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3f33f@F5 ʚ;Xm8ʚ;g4IdId 0Dppp@ <4dddd@w 0tt ___PPT10D-3 00000}0xgtt 02DArial00}0xgtt 0" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA &Trigger efficiency from the simulation''$ Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3*Detector acceptance not including trigger ++$3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /T[ \ ]   0` ` ̙33` 333MMM` ff3333f` f` f` 3>?" dd@,~?" dd@   " @ ` n?" dd@   @@``PP    @ ` ` p@@ $(  $ $ 6 "  9Title  $ 0$ "  8cvcv  $ 0E "``  H*0C $ 0E " uq  E T*Photon2007, 9 July, 2007, S.Uehara, Belleb+0 #CC#CCC" $ 0PE " E J* 0CB $  `Do??"@@@B $  `Do??"ppp2  $ 3 rE jJ??"@ 8$0G2  $ 3 r@E jJ??"p  8$0G2  $ 3 rE jJ??" 8$0G2  $ 3 r!E jJ??"0  8$0G2  $ 3 rD$E jJ??"`  8$0GB $  `Do??" B $  `Do??" B $  `Do??" B $  `Do??" B $  `Do??" B $  `Do??" H $ 0޽h ? ̙3380___PPT10.xד 1_Title 0 H(  H H Ntp qڸqڸ    p  x* U**UU~~ H Np qڸqڸ C. p  z* U**UU~~d H c $ ?P< p  H Np qڸqڸ L( p  Z000 0000n0f_-[ ,{ 2 000 ,{ 3 000 ,{ 4 000 ,{ 5 000Z H Tp qڸqڸ  w  p  x* U**UU~~ H Tlz qڸqڸ C.w p  z* U**UU~~H H 0Crll ? 3380___PPT10.0 ((    N9z 'n'n    z  \* N''NNvv  NxKz 'n'n C. z  ^* N''NNvv  T$Uz 'n'n  w  z  \* N''NNvv  T[z 'n'n C.w z  ^* N''NNvvH  0Crll ? 3380___PPT10.ί  0  ,`(  ,~ , s * $    , <g:e :Study of pp production in two-photon collisions at Belle B; G G 0G  , <g=5  ^S.Uehara (KEK)CB ,@  `Do??7 ,  ` o??jd," ,  ` o??C"?<7T , C ,A bellelogo2   :  , 3 A!   ,  `g ?? H  u%on behalf of The Belle Collaboration4&0 CG I  ,  `Pg ?? W4  /BES-Belle-Cleo-Babar J.W.S, Nov., 2007, BeijingL00G3#G3G3H , 0޽h ? 33___PPT10i.`:+D=' p = @B +  0   0 (  0x 0 c $LXo$T o  0 0[o V4Hadron production from two quasi-real photons (|q2|<0.001GeV2, with no-tag condition) Exclusive processes with Wgg=0.6 - 4.5 GeV at KEKB/Belle Wide energy region --- Various physics aspects can be studied simultaneously. 0 Light-quark resonances, Charmonia Perturbative /Non-perturbative QCD, 00 0Hadron production mechanism 0XGGfOf GfOfcGfGCGfOfGfzG3C9C GfGf GfGf Gf9Gf GfGfG3L9<: 0 3 A  0  fpo jJ??  {9Resonance formation or Hard scattering with a quark line&:0:G 0  `to ??M m Ahadrons0CH 0 0޽h ? ̙33y___PPT10Y+D=' p = @B +   0 4, \(  \^ \ THo ??pt p+p- and p0p0 : Physics is almost the same, but gives independent information Electromagnetic production as mesons: s(p0p0)<<s(p+p-) Resonances (I=0, JPC=0++) decaying via strong interaction: 00000000000000s(p0p0):s(p+p-) =1:2 Test of QCD: s(p0p0)/s(p+p-) : ~0.03 (LO)  0.5 ( handbag ) c.m.-energy (W) and angular dependences must also be examined. t0GOGOGGGOGO G=GO+GGfOfGfOfGfOfGfOfGfGOGO!GC CGf OfGfOfGf GfGfOfGfOfGfGfGf GCGf OfGfOfGfOfGfOfGfC C&G3 G3G3E3G3<@~ \ s * o$   o : \ 3 AY \  `To ?? Ep(0C \  `}o ??}B Ep(0C: \ 3 A# +: \ 3 A{:  \ 3 AMJ s  \ <Tozf  C Resonance G  \ <|oM G ?quarkGf  \ <\oy Gsoft hadron exchangeA  \ <o Msoft production of mesonsAH \ 0޽h ? ̙33y___PPT10Y+D=' p = @B +   0    (  r  S , $      f<  ??T; i1(I=0, JPC=0++) mesons --- fJ or ccJ (J=even)20GOGOGGOGGO G4    fE  ??   $s(p0p0):s(p+p-) =1:20Gf OfGfOfGf GfGfOfGfOfGfGfR   `(  ??  Interferences a resonance and continuum component or among resonances make condition more complicated. We expect that continuum contribution is smaller in p0p0 than in p+p- in the intermediate or low energies0CCKCK CCKCK%C&  Tz  ??a  V- f2(1270) and f0(980) has been observed in p+p-. - Are any scalar mesons around 1500 MeV seen ? What we see in 1.5-1.9 GeV region where many resonances suggested? f2 or f4 around 2 GeV - The charmonia: cc0 and cc2<0CGOGCGOGCCKCK CGCGf"CCG3O3G3G3O3G3CG3G3O3G3G3O3,H  0޽h ? ̙3380___PPT10.j  0 y@ 8(  8X 8 6  @  &Results of ggp+p-   $ $C$$$$$$$ T 8  `  ??F j^ Phys. Rev. D075, 051101(R) (2007) arXiv:0704.3538[hep-ex], to appear in J. Phys. Soc. Jpn. (2007) Phys. Lett. B 615, 39 (2005)^0 A A!AeAA A< K 8 <# s gm  \"W = 0.8  1.5 GeVG3 8 <  g \"W = 2.4  4.1 GeVG3 8  `+  ??6 z /0  IBelle Collaboration0  8 T??C"? H 8 0޽h ? 33___PPT10i.~+D=' p = @B +M  0 d\P<(  <` < T6  ??q v  ,f0(980)  is an ordinary qq meson? - an exotic state? - some special theory needed? Its two-photon coupling is a crucial key. Prediction of Ggg : uu, dd --- 1.3  1.8 keV ss --- 0.3  0.5 keV KK molecule --- 0.2  0.6 keV0GOGRCC*CG GGOGG|Cw   ) < TH  ??  ?f0(980) appears as a small but statistically significant peak.J@0G3O3>G3F < S A40   < TO f??/O bf2(1270)> 0CKCB <@  fD3Ԕ??@" <  `T f??P# p af0(980)>0CKCB <  fD3o?? X  < s *TZ ?"6@`NNN?N9 q  Xp/m separation: by comparing energy deposit in the CsI calorimeter between data and MC2Yc "I"VB  <  `DjJ??/J/  <  `a  ?? O ((f0(980) in gg p+p-0G(O( G(G(((((,   <  `xm  ??  Z85.9fb-16 0GOB  < ZD??6 d6 B < ZD??6 t6 B < ZD?? d B < ZD?? 7 H < 0޽h ? 33___PPT10i.I" +D=' p = @B +Y  0 phpD(  D D s *y ?"6@`NNN?N'q > 2% D  `  ??w@  Fit to the f0(980) line shape\0 G$ffG$ffO$ffG$ffv D NA ??` n D  `  ??)    IInterference term0Az D 0A K?̙ ?"`w]  K D  `x  ??%    R |resonance|2* 0 AIz D T̵ f??p(  f0(980) p+p-0G 3O 3G 3 3 3 3 3 r ~ 6   D# #"`6 a  D 6 f?"6@ NNN?Nj  V @`U  D 6 f?"6@ NNN?N~  j Ggg =Jck"*  @`  D 6< f?"6@ NNN?Nj   V @`  D 6< f?"6@ NNN?N~ j  Gp+p- =~cckckc"  @` D 6* f?"6@ NNN?Nj6   V @` D 6 f?"6@ NNN?N~ 6 j  YM =$ @`B D 6o?"0@NNN?N~ 6 j6 B D 6o?"0@NNN?N~ jB D 6o?"0@NNN?N~ 6 ~ B D 6o?"0@NNN?N6  B D 6o?"0@NNN?Nj6 6 B D 6o?"0@NNN?N~ ~  B D 6o?"0@NNN?N  B D 6o?"0@NNN?N~  ~ B D 6o?"0@NNN?N B D 6o?"0@NNN?Nj` D c $A5 L??5 "Y  L` D c $A6 M?? P  M` D c $A7 N?? 7 N D  `  ??c ] MeV/c2 MeV eVB0CK C H D 0޽h ? 33___PPT10i.I" +D=' p = @B +   0 H @ L (  Lx L c $4 $   2 L T>  ??q No h p+p- enhancement is seen near 958MeV/c2 This is a P and CP mode; previous upper limit: Br (h p+p-) < 0.02 (HBC (1969)) New upper limit for Br(h p+p-) < 2.8 10-3 (interference with the non-resonant process allowed) < 3.3 10-4 (no interference)C0G ffG ffG ff ff ff ff ff 3GGGG33GG O 333>[9 B L@  `D3jJ??]*B L@  `D3jJ??: L 3 A  B L  fD3>?? tt  L  `D`  ??   ^h mass40G3G3H L 0޽h ? ̙3380___PPT10.B    0L0   P0 (  P` P c $A O?? <  OP P Tw ?? 's :GggBrcc0p+p-) 15.1 2.1 2.3 GggBrcc0K+K-) 14.3 1.6 2.3 GggBrcc2p+p-) 0.76 0.14 0.11 GggBrcc2K+K-) 0.44 0.76 0.14 0 C K"CC CGO C K"CC CGO C K"CC CG3O33333  C K"CC CG3O33333h&$F P T ?? '  \Two-photon measurements of 0Ggg(ccJ)Br (eV)/0 GGG GGOGGOGGEG4 F P S A M'  P T@  ??j > JPLB 615, 39 (2005)0 P N( _ж_ж $ "p+p- measurements at high energiesf# C ( K ( C ( K (C((   8  @ @ @: P 3 A&#  < P c $޽h ? ̙33y___PPT10Y+D=' p = @B +  0 @N(  @r @ S  $"    @ T??C"?H @ 0޽h ? 33___PPT10i.T+D=' p = @B +  0 8P(  8x 8 c $ $9   x 8 c $ $'    8  `$  ??j'z 6Based on data with an integrated luminosity of 95 fb-16704GOH 8 0޽h ? 33___PPT10i. @a+D=' p = @B +  0 0 P(   r  S  $'g   :  3 A*0    <LEC"?D  Trigger efficiency is determined by the trigger simulator, tsim after tunings of the energy thresholds for the total energy trigger (HiE)  1.15 GeV and for counting number of clusters (Clst4) - 110 MeV In each of 16 c.m. angular bins 0.0 < |cos q*| < 0.8, Fitted by a two-dimensional function of (W, |cos q*| )rgGCGC G3CGGff Gf CGGff6Gf,CC6CCCC,;I:  3 A/ ] 7H  0޽h ? 33___PPT10i. 0 E+D=' p = @B +F  0 ]U@%(  ~  s *$ $    0  `A ? ?$'    0  `A ? ?$      6 p0  8W (GeV)  XB  0Do:p  6 p ;0  8W (GeV)  XB @ 0Do 3    6 DD Q | cos q*|, CXB   0Do`Tp   s *  C   Q | cos q*|, CXB   0Doj    0p ,y i7About 1.26M events (before the background subtraction)88:  3 A   < 6  T |cos q*|<0.4, C  <  W (GeV)XB  0DԔ c XB  0DԔ 9:`   0`'   acc0B E MM  <,  g  acc2B E MM   ` 2 ??I U2.8 3.0 3.2 3.4 3.6 3.8 0 ^ ! S A$$% q N   "  `,0 ?? t<  NEstimated background03 # <d5 S j# M  j |cos q*|<0.8B C B $ ZD??I,I  %  `LA  ??  W = M(p0p0) h 0CCKCKCH  0޽h ? 33___PPT10i. $+D=' p = @B +0  0 G ? p (  ~  s *M $    :  3 A  :  3 A ';  <Q   1W=1.18GeV, |cosq*|=0.65 W>3.6GeV, |cosq*|<0.4N2CC, :   3 A       <X  7  LDots  experimental Histo.  Signal MC''   <^ i d4Histogram  experimental B  6b M 0pt-unbalanced backgrounds are seen in W<1.2 GeV1GOG!GG C G  B{E3ԔC"?5 Low-energy beam-background photons Intermediate or Higher energies Non-exclusive process sources not significantly seen<SE EHE=  <o T@k 3W=0.90GeV, |cosq*|=0.05 W=0.66GeV, |cosq*|=0.05N4CC,   Tr ??aT e/ 0 0.1 0.2 0.3 0.4 0.5000   < ~ t  |Spt| (GeV/c)DC     Ts ??Y e/ 0 0.1 0.2 0.3 0.4 0.5000 B @  fDԔ??"&"B @  fDԔ??s &s H  0޽h ? 33___PPT10i.Z|=+D=' p = @B +  0  $(  $~ $ s *8 $'    $ < ) s|cosq*| = 0.025&A   $ <̗ ) ~   W (GeV) $ <̓ p s|cosq*| = 0.725&A   $ < ) z   W (GeV)y  $ <  d2 Around 11% at maximum, typically 5 % Large angular dependence due to geometrical condition of the detector Overall efficiency = Acceptance * trigger efficiency Pl G  $ <( j* DCalculated from signal MC simulation and fitted by a smooth function*E%G C:  $ 3 A] < : $ 3 A] w H $ 0޽h ? 33___PPT10i.jPK.+D=' p = @B +^  0 um(  x  c $( $      0t jX W resolution --- ~ 1.4% W, almost independently of W (from signal MC) Apply Unfolding to the experimental W distribution (in each angle region) for the smearing effect in the W direction using an asymmetric Gaussian (1.3% higher side and 1.9 % lower side). Unfolding is applied in 0.9 GeV < W < 2.4 GeV. Wider bin-widths than the resolution are used in the other W regions.| G C4C GfpC=G3CxEff  T  ??  XW(GeV)0 0 6A% ?$pq3 g   "  T ??   .Before (orange) and After (blue) the unfoldingT/0f f   ft  ??F  9Yield0    `<  ?? B  } |cosq*|=0.22520C  f  S AC"?3    `  ??[  MHistogram: Data0B   `D??% gg%   T  ??Cp(  *Smearing func. peaking at the nominal mass+0+ B   `D??6 ts 6  0   <Experimental sample of h gg\EEEEH  0޽h ? 33___PPT10i.߫@z+D=' p = @B +?   0 VN (  r  S 0 $'g   #  0| f` _ mImportant note: After the Unfolding, different data bins and errors are no longer independent of each other.:n[fu  0D V   }Comparison with Crystal Ball at DORIS II (1990) They are consistent. Belle has ~103 times more data. Statistical errors only.|~0G"GOGCG3~  0 j3  XObtain first ds/d|cosq*| in each D|cos q*|=0.05 bin Then, accumulate them over the anglevYAAAA AAAA1A,  3:  3 AP %:  3 AO s    `(  ??zZ  K Preliminary$ 0 G3    f  ??   s9Data in the charmonium region are omitted from the plot.:0:fB   fD>?? P H  0޽h ? 33___PPT10i.Po@+D=' p = @B +  0 ,F(  ,r , S P $     , <! }d *A , 0% q  Trigger efficiency - - - 4% @ W > ~ 1.1 GeV (HiE) 5% - 30% @ W< ~1.1 GeV (Clst4) -p0 reconstruction efficiency - - - 6% Acceptance (dominated by pt-balance cut) - - 3% - 5% Background subtraction - - - 20% of the subtraction component 3% in High W where no subtraction applied. Luminosity function - - - 4% - 5% ------------------------------------------------------------------------- Total 55% - 10% @ W<~1.05GeV ~9% @ 1.05GeV~2.7GeVV---m---GfIC CCCCYC CCCCCCK CG)GG GG"PYH , 0޽h ? 33___PPT10i.+D=' p = @B +   0    N (    <I / g/Differential cross section (Angular dependence)00G x  0C"?,~ x  0C"?, :  3 A"z<<  0R D"  Low W High-W Large angle enhancement appears disappears Small angle enhancement disappears appears~CG G)G33 G3(G33 G3/   f~E ?? ds/d|cos q*| (nb)@0AA$/   fHa  ??S   ds/d|cos q*| (nb)@0AA$   `g  ??E b$Change ~ 2.0 GeV"0   ` k  ??M m K Preliminary$ 0 G3j   fdo  ??7| gg p0p0 0G  G O G O H  0޽h ? 33___PPT10i.tl+D=' p = @B +   0   0P (  r  S Xy $9      0z  0Resonances: Clearly seen: f0(980), f2(1270), ~1.65 GeV, ~1.95 GeV Hints with a lower significance : ~1.45 GeV, cc0, cc2 R G fGfCGGOGGOGC1G3G3O3G3G3O3<G3:  3 A20 R  0p 2q! n Sizes of the charmonia Ggg(cc0)B(cc0p0p0): 8.4 2.2 0.8 eV (4.5s) Ggg(cc2)B(cc2p0p0): 0.29 0.23 0.03 eV (1.4s) Upper limit < 0.75 eV (90%CL) Preliminary The central values are consistent with the expectations from isospin invariance between the p+p-/p0p0 decays o0G3AAAIAAIAIAIAAAAAAAAIAAIAIAIAAAAOA E3^AAIAIAIAIAE3FLA*  Z??C"?,%   <Ľ Z T |cos q*|<0.4, CH  0޽h ? 33___PPT10i.{_+D=' p = @B +  0 @ -(  r  S g$  g F  0ܮgf 7F Charmonium region is omitted from the plot. The ratio is 0.3  0.4 at W>2.7 GeV*Q,C%G3  0g   OError bars are statistical only. Systematic errors: About 10% at each measurement point, except p+p- above the charmonium masses (~25%).#GffGf/CCKCK$Cc&: ' 3 Azq`  ( Tg ??0   |cosq*|<0.6J 0 3 E3 33: ) 3 A0:@  * Tg ??>  K Preliminary$ 0 G3 +  `dg ??=H n K Preliminary$ 0 G3 , Z ??gm PH  0޽h ? 33___PPT10i._+D=' p = @B +$  0 $(  r  S  $    r  S 4 $]}   H  0޽h ? ̙3380___PPT10.pyh  0 `0(  x  c $ $    x  c $ $M=    H  0޽h ? 33___PPT10i.B+D=' p = @B +  0 (  r  S \ $g    H  0޽h ? ̙3380___PPT10.y[   0 4 ,   (  ~  s * $   V  C .ABellering4#    < '^   Asymmetric e- e+ collider b    0X"   wBeam crossing angle: 22mrad@$   0   LContinuous injectionH  0, '@  lLuminosity Lmax=1.71x1034 cm-2s-1 +" Ldt ~ 710 fb-100$ ,      E 4  6  <  "`  t8 GeV e- (HER) x 3.5 GeV e+ (LER) s=10.58 GeV (4S),;$33    `A ?$ q \      `@  ?? k BXHigh momentum/energy resolutions CDC+Solenoid, CsI Vertex measurement  Si strips Particle identification TOF, Si-aerogel, CDC-dE/dx, RPC for KL/muon0!GC CCG CG4CKC) xH  0޽h ? 33___PPT10i.@+D=' p = @B +  0 (  r  S l $      Z   ??kI ggcc2 gJ/y PLB 540, 33(2002) gg(f2'(1525)etc. )K+K- (1.4 - 2.4 GeV) EPJC 32, 323 (2003) gg (cc0,cc2)p+p-,K+K- (2.4 - 4.1 GeV) PLB 615, 39 (2005) gg (hc )pp (2.025 - 4.0 GeV) PLB 621, 41 (2005) gg cc2' DD PRL 96, 082003 (2006) gg (f0(980)etc. )p+p- (0.8 - 1.5 GeV) PRD 75, 051101(R) (2007), arXiv:0704.3538[hep-ex], to appear in Jour. Phys. Soc. Jpn. (2007) gg (cc0,cc2 )K+K- (2.4 - 4.0 GeV) hep-ex/0609042v2, submitted to PLB gg (hc,cc0,cc2 )p+p-p+p-,K+K-p+p-,K+K-K+K- arXiv:0706.3955[hep-ex], submitted to EPJC gg a2's -p+p-p0 (1.2 - 3.0 GeV) hep-ex/0610022 gg (hc )LL,S0S0 (2.3-4.0 GeV) hep-ex/0609048& 0CCKCCCC=CCCCCK CCKCK4CCCCKCCKCCKCKCKCK5CCCCKCGCCCCKCCQCCCCK CCCKCKCCCCKCCKCCKCKsCCCCKCCKCCKCCCKCKCKCKCKCKCKCKCKCKCKCKcCCCCKCCCCKCKCK5CCCCKCCCCCKCK5C JI[ F?B   `DjJ??B   `DjJ?? fB   `DjJ??   B   `DjJ??W IW H  0޽h ? ̙33___PPT10i.D:)+D=' p = @B +  0  lv(  l~ l s * $    ^ l 6X oMq  The cross sections observable there e+e-U(4S)BB --- 1.1 nb e+e-qq (uds) --- 2.1 nb e+e-cc --- 1.2 nb e+e-t+t- --- 0.9 nb gg hadrons (Wgg>0.8GeV) --- ~1 nb (within the acceptance) 0$GC"%  >@& , l T   ?? Dn  lRLuminosity Function for quasi-real gg collisions ds(in ee) = s(in gg) Lgg(W) dWpS0%GfGf GfGfGfOfGfOfG3G3O3G3O3O3G3GGGGf%  l0 ZA P? ?$@ j P   l  `  ??IC i/Calculated with equivalent-photon approximation000C l  `  ??  Ee+e-=10.58GeV Q2max=1GeV20G3G3O3G3O3 G3O3O3G3O3RB l s *DjJRB  l s *DjJ] k^RB  l s *DjJ?@  l  f ??Pm - &  QLuminosity function (1/GeV)0H l 0޽h ? 33___PPT10i.P0ۭ+D=' p = @B +  0  pl(  p p  `  ?? <  C = + resonances: Peak structure in the invariant mass distribution Test of QCD: c.m.-energy (W) dependence and angular dependence in high energies General Analysis strategy Invariant-mass of hadron pair = W (c.m. energy of gg) Quasi-real two-photon collisions with final state fully reconstructed --- strict transverse momentum balance is required (| Spt| <50 - 200 MeV/c ) This gives efficient background rejection  0CG6C G]CGfC!GffCCC GffCGff)CG3C.G3BCG3G3G3O3G3 C)G33CDIx p c $ $    : p 3 A  p  `  ??m " ;Meson0 p  `  ??P Pp ;Meson0H p 0޽h ? ̙33y___PPT10Y+D=' p = @B +Q  0 0tQ(  tx t c $8 $    x t c $ $    t  `  ??9 7Based on data with an integrated luminosity of 85.9fb-16805GOH t 0޽h ? ̙3380___PPT10.,  0 @x(  xx x c $ $    v x NA ??KS x  `  ?? ds/d|cos q*| (nb)j0GGGGG$H x 0޽h ? ̙3380___PPT10.`v  0 F>P|(  |x | c $  $    v | NA# ??* v | NA' ??m s B |  `Do??@ @ f  |  `#  ?? q  Red dashed lines --- Size of point-to-point systematic error Systematic structure near |cos q*|=0.45-0.55 could be due to a measurement biasX0?GffGG0GH | 0޽h ? ̙3380___PPT10.04  0 `4(  x  c $H. $    :  3 A(q :  3 A+ N H  0޽h ? ̙3380___PPT10.^0"  0 p(  x  c $h4 $    :  3 A,M    `6  ??  Close to |Y2|2\0 GOGO   `ԏg ??@z' =2 0E  T?  ??} \ Consistent with pure J=2 and l=2 But, mathematically the partial waves cannot be fully separated taking into account the interference between J=0 and 2.b0GGGCxCH  0޽h ? ̙3380___PPT10.0sa$   0  |  (  x  c $L $    :  3 A-P !   `DN  ??p-[ D  Econtinuum (sum)0B @  `D??% j    `R  ??   ]continuum (l=2)20 CB   `Do??     `0X  ??   MInterference +continuum0B    `D??6 J B    `D?? =)     `\  ??  ? resonance 0 B  @  `D??M ^ "    ``  ?? q rComponents: f2 (1270) resonance Smooth continuum: Interfering component (l=2) No-interfering component (I=0) s0 CG3O3G3GC>CB   `D??``  Tc  ?? P data and fit( 03  Zo  jJ?? 3 This is for consistency check: Known mass and width of f2(1270) (PDG2006) are used. The continuum and relative phase parameters etc. were floated.h08CCKCC?CH  0޽h ? ̙3380___PPT10.jC 0 ZR`(  `x ` c ${ $Ii   d ` 0}   .Correlation between the two triggers: HiE (Etot_trg>1.15GeV), Clst4 (>=4 clusters each with >110MeV) (The thresholds have been tuned.) * -- data, dashed histogram  trigger simulator (tsim) t&EffAEA@Gf>&: ` 3 Aq  ` Bd C dEtrg*  ` 6p 6   NEtrg ` 0ԕ F 6 (GeV) ` <l \& C : HiE in Clst4   ` <p  S  B Clst4 in HiE :  ` 3 A ,  ` 0Р ` `   LMinimum cluster energy (GeV)  ` 04 V3  LMinimum cluster energy (GeV)  ` < < dlarge p0 c.m. angle 4AI  ` <  &y  dsmall p0 c.m. angle 4AI  ` <8   Clst4 in HiE with Nclst=4 * ,  ` <  &C Clst4 in HiE with Nclst=4 * ,  ` <( 6   6 (GeV)2 ` # l ff?? 8$0GffH ` 0޽h ? 33___PPT10i. L|+D=' p = @B +  0 d(  d~ d s *\ $    : d 3 A  d 0 #  Dp W =1.96  2.00 GeV |cos q*| = 0.5  0.6 Dots -- experimental Curve  fit to data (considering backgrounds) (peak: 16 MeV/c) Histogram  signal MC (peak: 14 MeV/c)AAA AA E8AEA E3 AE3AK d < z Ethe pt-balance cut Efficiency is affected by pt-balance resolution.~FGCCGOGC^ d < 93   The resolution in the experimental data is by ~15% worse than the MC. Correction factor: 5% - 10%, depending on W and |cos q*| JGAE"AAA^ d 61g }2 d # l ff?? 8$0GffH d 0޽h ? 33___PPT10i.P{Ӄ+D=' p = @B +& 0 ~`@(  @d @ c $HP<  z r @ s *z HL(n  z VN___PPT90(  Backupk0_ P2 F2(1270)n0R^f Flatte Energy depon0UOn0R^ K0_0c0}0tag? 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" # $ % & ' ( ) * + , - . / 0 1 2 3 4 5 6 7 8 9 : ; < = > ? @ A B C D E F G H I J K L M N O P Q R S T U V W X Y Z [ \ ] ^ _ ` a b c d e f g h i j k l m n o p q r s t u v w x y z { | } ~  D rosoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0ԖD-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanPowerPoint Document(`WDocumentSummaryInformation8000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` LDxn|*&     "S5o).023 4.6  =?A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _t b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@F5 ʚ;Xm8ʚ;g4IdId 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0xgTTx 0x2DArial00}0xgTTx 0x" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA &Trigger efficiency from the simulation''$ Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3*Detector acceptance not including trigger ++$3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /T[ \ ] t  0 @ 8(  8X 8 6  @  &Results of ggp+p-   $ $C$$$$$$$ ^ 8  `  ??F jF Phys. Rev. D075, 051101(R) (2007) J. Phys. Soc. Jpn. 76, 074102 (2007) Phys. Lett. B 615, 39 (2005)^i0 A A!AJAA AL $ 06; 8 <# s gm  \"W = 0.8  1.5 GeVG3 8 <  g \"W = 2.4  4.1 GeVG3 8  `+  ??6 ]0  IBelle Collaboration0  8 T??C"? H 8 0޽h ? 33___PPT10i.~+D=' u= @B +  0 'p D(  D D s *y ?"6@`NNN?N'q > 2% D  `  ??w@  Fit to the f0(980) line shape\0 G$ffG$ffO$ffG$ffv D NA ??` n D  `  ??)    IInterference term0Az D 0A K?̙ ?"`w]  K D  `x  ??%    R |resonance|2* 0 AIz D T̵ f??p(  f0(980) p+p-0G 3O 3G 3 3 3 3 3 r ~ 6   D# #"`6 a  D 6 f?"6@ NNN?Nj  V @`U  D 6 f?"6@ NNN?N~  j Ggg =Jck"*  @`  D 6< f?"6@ NNN?Nj   V @`  D 6< f?"6@ NNN?N~ j  Gp+p- =~cckckc"  @` D 6* f?"6@ NNN?Nj6   V @` D 6 f?"6@ NNN?N~ 6 j  YM =$ @`B D 6o?"0@NNN?N~ 6 j6 B D 6o?"0@NNN?N~ jB D 6o?"0@NNN?N~ 6 ~ B D 6o?"0@NNN?N6  B D 6o?"0@NNN?Nj6 6 B D 6o?"0@NNN?N~ ~  B D 6o?"0@NNN?N  B D 6o?"0@NNN?N~  ~ B D 6o?"0@NNN?N B D 6o?"0@NNN?Nj` D c $A5 L??5 "Y  L` D c $A6 M?? P  M` D c $A7 N?? 7 N D  `  ??c ] MeV/c2 MeV eVB0CK C  D  `ؘ  ??_6 %f0(980) is observed as a clear peak.J&0G3O3$G3 D TDu ??'  > 0  D T  ??   > 0H D 0޽h ? 33___PPT10i.I" +D='  = @B +r6#KmMu'#b1CJ(/x _   000000 0000 LL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` ldr+՜.+,0h     画面に合わせるKEKW$ /ArialＭＳ ＰゴシックTimes New RomanＭＳ Ｐ明朝Symbol Calisto MTVerdanaTitle ビットマップ イメージMicrosoft 数式 3.0Microsoft Excel グラフ !Motivation of two-photon physics1 General physics in gg p+p-/p0p0 final states Resonances to appear in ggppスライド 5スライド 6スライド 7%New upper limit for Br (h’p+p-)スライド 9!Preliminary results of ggp0p0Selection of p0p0 candidatesRaw-event distribution of p0p0)pt-balance distributions and backgroundsDetection Efficiency!Unfolding and Energy calibrationCross sections of gg p0p0Systematic-error sourcesスライド 18Resonant structures $Cross section ratio s(p0p0)/s(p+p-)Conclusion of p+p- measurementSummary for p0p0 measurementBACKUP slides& KEKB Accelerator and Belle Detector.Measurements of two-photon processes at BelleReactions at KEKB/Belle!Two-meson exclusive final statesSelection of p+p- candidatesDifferential cross section*Angular dependences at some energy pointsFitting formula for f0&     "S5o).023 4.6 L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA &Trigger efficiency from the simulation''$ Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3*Detector acceptance not including trigger ++$3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /T[ \ ] rY!5b1CJ(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` LDxn|*&     "S5o).023 4.6  =?A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _t b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@F5 ʚ;Xm8ʚ;g4IdId 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0xgTTx 0x2DArial00}0xgTTx 0x" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA &Trigger efficiency from the simulation''$ Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3*Detector acceptance not including trigger ++$3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /T[ \ ] h 0 Hx(  H H Ntp "e"e    p  p* AAA H Np "e"e  t p  r* AAAd H c $ ?B l p  H Np "e"e s} p  Z000 0000n0f_-[ ,{ 2 000 ,{ 3 000 ,{ 4 000 ,{ 5 000Z  H Tp "e"e    p  p* AAA H Tlz "e"e  t p  r* AAAH H 0X—;g ? 3380___PPT10.0 ((    N9z aڰaڰ    z  \* :::XXuu  NxKz aڰaڰ  t z  ^* :::XXuu  T$Uz aڰaڰ    z  \* :::XXuu  T[z aڰaڰ  t z  ^* :::XXuuH  0X—;g ? 3380___PPT10.ί& 0 ~`@(  @d @ c $HB l  z r @ s *z Hp}n  z VN___PPT90(  Backupk0_ P2 F2(1270)n0R^f Flatte Energy depon0UOn0R^ K0_0c0}0tag? Pimu separationn0|^pP     p  H @ 0X—;g ? 3380___PPT10.+ib^' 0 Hn(  Hd H c $HB l  z  H s *,z Hp}  z  XBackupk0_ P2 $  H H 0X—;g ? 3380___PPT10.+ib) 0 Th(  Tp T 0 ?HB l  z  T 61z  Hs}  z  :  B T s *X—;g ? ̙33r(#&[0269_-!1;b1J(u _   000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D E =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA &Trigger efficiency from the simulation''$ Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3*Detector acceptance not including trigger ++$3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] dj 0` ` ̙33` 333MMM` ff3333f` f` f` 3>?" dd@,~?" dd@   " @ ` n?" dd@   @@``PP    @ ` ` p@@ rj (    61  "   9Title   0?  "   8cvcv   0C  "``   d*0Cw  0L  " uq    %BBCB-WS, Nov., 2007, S.Uehara, Beller&0C#CC#C CC6  0$]  "   F 0C B   `Do??"@@@B   `Do??"ppp2   3 re  jJ??"@ J$0G 2   3 ro  jJ??"p  J$0G 2   3 r|y  jJ??" J$0G 2   3 r  jJ??"0  J$0G 2   3 rX  jJ??"`  J$0G B   `Do??" B   `Do??" B   `Do??" B   `Do??" B   `Do??" B   `Do??" H  0޽h ? ̙3380___PPT10.8  Title 0  ,>(  ,~ , s *    , <Џ:e :Study of pp production in two-photon collisions at Belle B; G G 0G  , <=5  ^S.Uehara (KEK)CB ,@  `Do??7 ,  ` o??jd," ,  ` o??C"?<7T , C ,A bellelogo2   :  , 3 A!   ,  `؜ ?? H  u%on behalf of The Belle Collaboration4&0 CG '  ,  ` ?? W4  /BES-Belle-Cleo-Babar J.W.S, Nov., 2007, BeijingL00G3#G3G3H , 0޽h ? 33___PPT10i.`:+D='  = @B + 0   0 (  0x 0 c $'T '  0 0 ' V4Hadron production from two quasi-real photons (|q2|<0.001GeV2, with no-tag condition) Exclusive processes with Wgg=0.6 - 4.5 GeV at KEKB/Belle Wide energy region --- Various physics aspects can be studied simultaneously. 0 Light-quark resonances, Charmonia Perturbative /Non-perturbative QCD, 00 0Hadron production mechanism 0XGGfOf GfOfcGfGCGfOfGfzG3C9C GfGf GfGf Gf9Gf GfGfG3L9<: 0 3 A  0  f\!' jJ??  {9Resonance formation or Hard scattering with a quark line&:0:G 0  `"' ??M m Ahadrons0CH 0 0޽h ? ̙33y___PPT10Y+D='  = @B +  0 4, \(  \^ \ T:' ??pt p+p- and p0p0 : Physics is almost the same, but gives independent information ElectromagnetiFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#c production as mesons: s(p0p0)<<s(p+p-) Resonances (I=0, JPC=0++) decaying via strong interaction: 00000000000000s(p0p0):s(p+p-) =1:2 Test of QCD: s(p0p0)/s(p+p-) : ~0.03 (LO)  0.5 ( handbag ) c.m.-energy (W) and angular dependences must also be examined. t0GOGOGGGOGO G=GO+GGfOfGfOfGfOfGfOfGfGOGO!GC CGf OfGfOfGf GfGfOfGfOfGfGfGf GCGf OfGfOfGfOfGfOfGfC C&G3 G3G3E3G3<@~ \ s *<'   ' : \ 3 AY \  `H7' ?? Ep(0C \  `i' ??}B Ep(0C: \ 3 A# +: \ 3 A{:  \ 3 AMJ s  \ <G3F < S A40   < T,f??/O bf2(1270)> 0CKCB <@  fD3Ԕ??@" <  `<,f??P# p af0(980)>0CKCB <  fD3o?? X  < s *,?"6@`NNN?N9 q  Xp/m separation: by comparing energy deposit in the CsI calorimeter between data and MC2Yc "I"VB  <  `DjJ??/J/  <  `T, ?? O ((f0(980) in gg p+p-0G(O( G(G(((((,   <  `, ??  Z85.9fb-16 0GOB  < ZD??6 d6 B < ZD??6 t6 B < ZD?? d B < ZD?? 7 H < 0޽h ? 33___PPT10i.I" +D='  = @B + 0 'p D(  D D s *,?"6@`NNN?N'q > 2% D  `, ??w@  Fit to the f0(980) line shape\0 G$ffG$ffO$ffG$ffv D NA ??` n D  `, ??)    IInterference term0Az D 0A K?̙ ?"`w]  K D  `D, ??%    R |resonance|2* 0 AIz D T0,f??p(  f0(980) p+p-0G 3O 3G 3 3 3 3 3 r ~ 6   D# #"`6 a  D 6,f?"6@ NNN?Nj  V @`U  D 6,f?"6@ NNN?N~  j Ggg =Jck"*  @`  D 6T,f?"6@ NNN?Nj   V @`  D 6o f?"6@ NNN?N~ j  Gp+p- =~cckckc"  @` D 6o f?"6@ NNN?Nj6   V @` D 6@o f?"6@ NNN?N~ 6 j  YM =$ @`B D 6o?"0@NNN?N~ 6 j6 B D 6o?"0@NNN?N~ jB D 6o?"0@NNN?N~ 6 ~ B D 6o?"0@NNN?N6  B D 6o?"0@NNN?Nj6 6 B D 6o?"0@NNN?N~ ~  B D 6o?"0@NNN?N  B D 6o?"0@NNN?N~  ~ B D 6o?"0@NNN?N B D 6o?"0@NNN?Nj` D c $A5 L??5 "Y  L` D c $A6 M?? P  M` D c $A7 N?? 7 N D  `o  ??c ] MeV/c2 MeV eVB0CK C  D  `8%o  ??_6 %f0(980) is observed as a clear peak.J&0G3O3$G3 D T+o  ??'  > 0  D T,/o  ??   > 0H D 0޽h ? 33___PPT10i.I" +D='  = @B +  0 H @ L (  Lx L c $xJo   o  2 L TUo  ??q No h p+p- enhancement is seen near 958MeV/c2 This is a P and CP mode; previous upper limit: Br (h p+p-) < 0.02 (HBC (1969)) New upper limit for Br(h p+p-) < 2.8 10-3 (interference with the non-resonant process allowed) < 3.3 10-4 (no interference)C0G ffG ffG ff ff ff ff ff 3GGGG33GG O 333>[9 B L@  `D3jJ??]*B L@  `D3jJ??: L 3 A  B L  fD3>?? tt  L  `Tzo  ??   ^h mass40G3G3H L 0޽h ? ̙3380___PPT10.B   0N0   P0 (  P` P c $A O?? <  OP P THo ?? 's :GggBrcc0p+p-) 15.1 2.1 2.3 GggBrcc0K+K-) 14.3 1.6 2.3 GggBrcc2p+p-) 0.76 0.14 0.11 GggBrcc2K+K-) 0.44 0.76 0.14 0 C K"CC CGO C K"CC CGO C K"CC CG3O33333  C K"CC CG3O33333h&$F P T|o ?? '  \Two-photon measurements of 0Ggg(ccJ)Br (eV)/0 GGG GGOGGOGGEG4 F P S A M'  P To  ??j > JPLB 615, 39 (2005)0 P Nlo _ж_ж $ "p+p- measurements at high energiesf# C ( K ( C ( K (C((   8  @ @ @: P 3 A&#  < P c $޽h ? ̙33y___PPT10Y+D='  = @B + 0 @N(  @r @ S to "  o   @ T??C"?H @ 0޽h ? 33___PPT10i.T+D='  = @B + 0 8P(  8x 8 c $ 9   x 8 c $ '    8  `, ??j'z 6Based on data with an integrated luminosity of 95 fb-16704GOH 8 0޽h ? 33___PPT10i. @a+D='  = @B + 0 0 P(   r  S . 'g   :  3 A*0    <2 C"?D  Trigger efficiency is determined by the trigger simulator, tsim after tunings of the energy thresholds for the total energy trigger (HiE)  1.15 GeV and for counting number of clusters (Clst4) - 110 MeV In each of 16 c.m. angular bins 0.0 < |cos q*| < 0.8, Fitted by a two-dimensional function of (W, |cos q*| )rgGCGC G3CGGff Gf CGGff6Gf,CC6CCCC,;I:  3 A/ ] 7H  0޽h ? 33___PPT10i. 0 E+D='  = @B +F 0 ]U@%(  ~  s *tU     0  `A ? ?'    0  `A ? ?      6N p0  8W (GeV)  XB  0Do:p  6^ p ;0  8W (GeV)  XB @ 0Do 3    6a DD Q | cos q*|, CXB   0Do`Tp   s *Dh C   Q | cos q*|, CXB   0Doj    0m ,y i7About 1.26M events (before the background subtraction)88:  3 A   <o 6  T |cos q*|<0.4, C  <w  W (GeV)XB  0DԔ c XB  0DԔ 9:`   0z   acc0B E MM  <  g  acc2B E MM   `t ??I U2.8 3.0 3.2 3.4 3.6 3.8 0 ^ ! S A$% q N   "  `ȉ ?? t<  NEstimated background03 # < S j# M  j |cos q*|<0.8B C B $ ZD??I,I  %  `  ??  W = M(p0p0) h 0CCKCKCH  0޽h ? 33___PPT10i. $+D='  = @B +0 0 G ? p (  ~  s *<     :  3 A  :  3 A ';  <H   1W=1.18GeV, |cosq*|=0.65 W>3.6GeV, |cosq*|<0.4N2CC, :   3 A       <ĭ  7  LDots  experimental Histo.  Signal MC''   < i d4Histogram  experimental B  6l M 0pt-unbalanced backgrounds are seen in W<1.2 GeV1GOG!GG C G  B 3ԔC"?5 Low-energy beam-background photons Intermediate or Higher energies Non-exclusive process sources not significantly seen<SE EHE=  <Ɓ T@k 3W=0.90GeV, |cosq*|=0.05 W=0.66GeV, |cosq*|=0.05N4CC,   T΁ ??aT e/ 0 0.1 0.2 0.3 0.4 0.5000   <Lԁ t  |Spt| (GeV/c)DC     Tt܁ ??Y e/ 0 0.1 0.2 0.3 0.4 0.5000 B @  fDԔ??"&"B @  fDԔ??s &s H  0޽h ? 33___PPT10i.Z|=+D='  = @B + 0  $(  $~ $ s *@ '    $ < ) s|cosq*| = 0.025&A   $ <$ ) ~   W (GeV) $ < p s|cosq*| = 0.725&A   $ < ) z   W (GeV)y  $ <D  d2 Around 11% at maximum, typically 5 % Large angular dependence due to geometrical condition of the detector Overall efficiency = Acceptance * trigger efficiency Pl G  $ < j* DCalculated from signal MC simulation and fitted by a smooth function*E%G C:  $ 3 A] < : $ 3 A] w H $ 0޽h ? 33___PPT10i.jPK.+D='  = @B +^ 0 um(  x  c $t       0 jX W resolution --- ~ 1.4% W, almost independently of W (from signal MC) Apply Unfolding to the experimental W distribution (in each angle region) for the smearing effect in the W direction using an asymmetric Gaussian (1.3% higher side and 1.9 % lower side). Unfolding is applied in 0.9 GeV < W < 2.4 GeV. Wider bin-widths than the resolution are used in the other W regions.| G C4C GfpC=G3CxEff  T<  ??  XW(GeV)0 0 6A% ?pq3 g   "  T! ??   .Before (orange) and After (blue) the unfoldingT/0f f   f4)  ??F  9Yield0    `,  ?? B  } |cosq*|=0.22520C  f  S AC"?3    `4  ??[  MHistogram: Data0B   `D??% gg%   T9  ??Cp(  *Smearing func. peaking at the nominal mass+0+ B   `D??6 ts 6  0>   <Experimental sample of h gg\EEEEH  0޽h ? 33___PPT10i.߫@z+D='  = @B +?  0 VN (  r  S lI 'g   #  0J f` _ mImportant note: After the Unfolding, different data bins and errors are no longer independent of each other.:n[fu  0R V   }Comparison with Crystal Ball at DORIS II (1990) They are consistent. Belle has ~103 times more data. Statistical errors only.|~0G"GOGCG3~  0Z j3  XObtain first ds/d|cosq*| in each D|cos q*|=0.05 bin Then, accumulate them over the anglevYAAAA AAAA1A,  3:  3 AP %:  3 AO s    `Dg  ??zZ  K Preliminary$ 0 G3    fk  ??   s9Data in the charmonium region are omitted from the plot.:0:fB   fD>?? P H  0޽h ? 33___PPT10i.Po@+D='  = @B + 0 ,X(  ,r , S u     , < y }d <A  , 0| q  Trigger efficiency - - - 4% @ W > ~ 1.1 GeV (HiE) 5% - 30% @ W< ~1.1 GeV (Clst4) -p0 reconstruction efficiency - - - 6% Acceptance (dominated by pt-balance cut) - - 3% - 5% Background subtraction - - - 20% of the subtraction component 3% in High W where no subtraction applied. Luminosity function - - - 4% - 5% ------------------------------------------------------------------------- Total 55% - 10% @ W<~1.05GeV ~9% @ 1.05GeV~2.7GeVV---m---GfIC CCCCYC CCCCCCK CG)GG GG"PYH , 0޽h ? 33___PPT10i.+D='  = @B +  0    N (    <| / g/Differential cross section (Angular dependence)00G x  0C"?,~ x  0C"?, :  3 A"z<<  00 D"  Low W High-W Large angle enhancement appears disappears Small angle enhancement disappears appears~CG G)G33 G3(G33 G3/   f\  ?? ds/d|cos q*| (nb)@0AA$/   f  ??S   ds/d|cos q*| (nb)@0AA$   `  ??E b$Change ~ 2.0 GeV"0   `Ō  ??M m K Preliminary$ 0 G3j   fɌ  ??7| gg p0p0 0G  G O G O H  0޽h ? 33___PPT10i.tl+D='  = @B +  0   0P (  r  S |ӌ 9     0ٌ  0Resonances: Clearly seen: f0(980), f2(1270), ~1.65 GeV, ~1.95 GeV Hints with a lower significance : ~1.45 GeV, cc0, cc2 R G fGfCGGOGGOGC1G3G3O3G3G3O3<G3:  3 A20 R  0 2q! n Sizes of the charmonia Ggg(cc0)B(cc0p0p0): 8.4 2.2 0.8 eV (4.5s) Ggg(cc2)B(cc2p0p0): 0.29 0.23 0.03 eV (1.4s) Upper limit < 0.75 eV (90%CL) Preliminary The central values are consistent with the expectations from isospin invariance between the p+p-/p0p0 decays o0G3AAAIAAIAIAIAAAAAAAAIAAIAIAIAAAAOA E3^AAIAIAIAIAE3FLA*  Z??C"?,%   < Z T |cos q*|<0.4, CH  0޽h ? 33___PPT10i.{_+D='  = @B + 0 @ -(  r  S     F  0 f 7F Charmonium region is omitted from the plot. The ratio is 0.3  0.4 at W>2.7 GeV*Q,C%G3  0%    OError bars are statistical only. Systematic errors: About 10% at each measurement point, except p+p- above the charmonium masses (~25%).#GffGf/CCKCK$Cc&: ' 3 Azq`  ( T0  ??0   |cosq*|<0.6J 0 3 E3 33: ) 3 A0:@  * T6  ??>  K Preliminary$ 0 G3 +  `;  ??=H n K Preliminary$ 0 G3 , Z ??gm PH  0޽h ? 33___PPT10i._+D='  = @B +$ 0 $(  r  S pg   r  S Hh]}  H  0޽h ? ̙3380___PPT10.pyh 0 `0(  x  c $E    x  c $pE M=    H  0޽h ? 33___PPT10i.B+D='  = @B + 0 (  r  S ] g   H  0޽h ? ̙3380___PPT10.y[  0 4 ,   (  ~  s *S    V  C .ABellering4#    <XU '^   Asymmetric e- e+ collider b    0f   wBeam crossing angle: 22mrad@$   0$b$Ю`g,Gj  b$C#4eX!c0.8GeV) --- ~1 nb (within the acceptance) 0$GC"%  >@& , l TdP  ?? Dn  lRLuminosity Function for quasi-real gg collisions ds(in ee) = s(in gg) Lgg(W) dWpS0%GfGf GfGfGfOfGfOfG3G3O3G3O3O3G3GGGGf%  l0 ZA P? ?@ j P   l  ``c  ??IC i/Calculated with equivalent-photon approximation000C l  `h  ??  Ee+e-=10.58GeV Q2max=1GeV20G3G3O3G3O3 G3O3O3G3O3RB l s *DjJRB  l s *DjJ] k^RB  l s *DjJ?@  l  ft ??Pm - &  QLuminosity function (1/GeV)0H l 0޽h ? 33___PPT10i.P0ۭ+D='  = @B + 0  pl(  p p  `P  ?? <  C = + resonances: Peak structure in the invariant mass distribution Test of QCD: c.m.-energy (W) dependence and angular dependence in high energies General Analysis strategy Invariant-mass of hadron pair = W (c.m. energy of gg) Quasi-real two-photon collisions with final state fully reconstructed --- strict transverse momentum balance is required (| Spt| <50 - 200 MeV/c ) This gives efficient background rejection  0CG6C G]CGfC!GffCCC GffCGff)CG3C.G3BCG3G3G3O3G3 C)G33CDIx p c $䂞    : p 3 A  p  `D  ??m " ;Meson0 p  `  ??P Pp ;Meson0H p 0޽h ? ̙33y___PPT10Y+D='  = @B +Q 0 0tQ(  tx t c $    x t c $@     t  `x  ??9 7Based on data with an integrated luminosity of 85.9fb-16805GOH t 0޽h ? ̙3380___PPT10., 0 @x(  xx x c $    v x NA ??KS x  `H  ?? ds/d|cos q*| (nb)j0GGGGG$H x 0޽h ? ̙3380___PPT10.`v 0 F>P|(  |x | c $Ȟ    v | NA# ??* v | NA' ??m s B |  `Do??@ @ f  |  `˞  ?? q  Red dashed lines --- Size of point-to-point systematic error Systematic structure near |cos q*|=0.45-0.55 could be due to a measurement biasX0?GffGG0GH | 0޽h ? ̙3380___PPT10.04 0 `4(  x  c $՞    :  3 A(q :  3 A+ N H  0޽h ? ̙3380___PPT10.^0" 0 p(  x  c $۞    :  3 A,M    ``ޞ  ??  Close to |Y2|2\0 GOGO   `  ??@z' =2 0E  TX  ??} \ Consistent with pure J=2 and l=2 But, mathematically the partial waves cannot be fully separated taking into account the interference between J=0 and 2.b0GGGCxCH  0޽h ? ̙3380___PPT10.0sa$  0  |  (  x  c $    :  3 A-P !   `  ??p-[ D  Econtinuum (sum)0B @  `D??% j    `  ??   ]continuum (l=2)20 CB   `Do??     `  ??   MInterference +continuum0B    `D??6 J B    `D?? =)     `H  ??  ? resonance 0 B  @  `D??M ^ "    `   ?? q rComponents: f2 (1270) resonance Smooth continuum: Interfering component (l=2) No-interfering component (I=0) s0 CG3O3G3GC>CB   `D??``  T  ?? P data and fit( 03  Z  jJ?? 3 This is for consistency check: Known mass and width of f2(1270) (PDG2006) are used. The continuum and relative phase parameters etc. were floated.h08CCKCC?CH  0޽h ? ̙3380___PPT10.jU0 ld`(  `x ` c $d$ Ii   d ` 0xP  .Correlation between the two triggers: HiE (Etot_trg>1.15GeV), Clst4 (>=4 clusters each with >110MeV) (The thresholds have been tuned.) * -- data, dashed histogram  trigger simulator (tsim) t&EffAEA@Gf>&: ` 3 Aq  ` B0 C dEtrg*  ` 62 6   NEtrg ` 04 F 6 (GeV) ` <? \& C : HiE in Clst4   ` <C  S  B Clst4 in HiE :  ` 3 A ,  ` 00G ` `   LMinimum cluster energy (GeV)  ` 0K V3  LMinimum cluster energy (GeV)  ` <(P < dlarge p0 c.m. angle 4AI  ` <V  &y  dsmall p0 c.m. angle 4AI  ` <|\   Clst4 in HiE with Nclst=4 * ,  ` <b  &C Clst4 in HiE with Nclst=4 * ,  ` <8j 6   6 (GeV)2 ` # lo ff?? J$0Gff H ` 0޽h ? 33___PPT10i. L|+D='  = @B +  0 !d(  d~ d s *v     : d 3 A  d 0x #  Dp W =1.96  2.00 GeV |cos q*| = 0.5  0.6 Dots -- experimental Curve  fit to data (considering backgrounds) (peak: 16 MeV/c) Histogram  signal MC (peak: 14 MeV/c)AAA AA E8AEA E3 AE3AK d <8 z Ethe pt-balance cut Efficiency is affected by pt-balance resolution.~FGCCGOGC^ d < 93   The resolution in the experimental data is by ~15% worse than the MC. Correction factor: 5% - 10%, depending on W and |cos q*| JGAE"AAA^ d 61g }2 d # ld ff?? J$0Gff H d 0޽h ? 33___PPT10i.P{Ӄ+D='  = @B + "0 (  X  C HB l    S  Hs}    H  0X—;g ? 3380___PPT10.``Pr;;& 7Evf*+PM/]/oz1;G0~KP a.J^C`P%  "a;d1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` ldr}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA &Trigger efficiency from the simulation''$ Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 $L(  $~ $ s *@ '   `  $ < [ ? VDetermined by signal MC simulation and fitted with smooth functions of (W, |cos q*|)`W$G%C G3G3G3N:  $ 3 A` I6 : $ 3 A* , $ 0 U9 M  8 W (GeV) z $ Z 7 ??mq  Trigger efficiency is determined by the trigger simulator after tunings of the energy thresholds the total energy trigger  1.15 GeV counting number of clusters (>=4) - 110 MeV Close to 100% above W>1.3 GeV0EAEA E3AEEfE1Efb* $ <W "+ Acceptance Around 11% at maximum, typically 5 % Large angular dependence due to geometrical condition of the detector Overall efficiency = Acceptance * trigger efficiency L E3lE5GEH $ 0޽h ? 33___PPT10i.jPK.+D=' = @B +r`Z dd1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant struct%{Ub$0!_{P) 5e$b$[k.R(2 b$R9ϙAev\ b$zOQgɌ>Z}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$ures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d 0 @V(  x  c $d#'g  # :  3 A*0    <M,C"?D  Trigger efficiency is determined by the trigger simulator, tsim after tunings of the energy thresholds for the total energy trigger (HiE)  1.15 GeV and for counting number of clusters (Clst4) - 110 MeV In each of 16 c.m. angular bins 0.0 < |cos q*| < 0.8, Fitted by a two-dimensional function of (W, |cos q*| )rgGCGC G3CGGff Gf CGGff6Gf,CC6CCCC,;I:  3 A/ ] 7H  0޽h ? 33___PPT10i. 0 E+D=' = @B +rIde:%de1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+'Invariant-mass resolution and Unfolding(($,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0   7 (  x  c $t      0 j W resolution Apply Unfolding to the experimental W distribution (in each angle region) for the smearing effect in the W direction using an asymmetric Gaussian (1.3% higher side and 1.9 % lower side). Unfolding is applied in 0.9 GeV < W < 2.4 GeV.z GC GfpC=G3C1Eff  T<  ??  XW(GeV)0 0 6A% ?pq3 g   "  T! ??   .Before (orange) and After (blue) the unfoldingT/0f f   f4)  ??F  9Yield0    `,  ?? B  } |cosq*|=0.22520C  f  S AC"?3    `4  ??[  MHistogram: Data0B   `D??% gg%   T9  ??Cp(  *Smearing func. peaking at the nominal mass+0+ B   `D??6 ts   0> P  vExperimental sample of h gg The energy scale is correct.l<EEEEE3H  0޽h ? 33___PPT10i.߫@z+D=' = @B +rӶ+je1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0   7 (  x  c $t      0 j W resolution Apply Unfolding to the experimental W distribution (in each angle region) for the smearing effect in the W direction using an asymmetric Gaussian (1.3% higher side and 1.9 % lower side). Unfolding is applied in 0.9 GeV < W < 2.4 GeV.z GC GfpC=G3C1Eff  T<  ??  XW(GeV)0 0 6A% ?pq3 g   "  T! ??   .Before (orange) and After (blue) the unfoldingT/0f f   f4)  ??F  9Yield0    `,  ?? B  } |cosq*|=0.22520C  f  S AC"?3    `4  ??[  MHistogram: Data0B   `D??% gg%   T9  ??Cp(  *Smearing func. peaking at the nominal mass+0+ B   `D??6 ts   0> P  vExperimental sample of h gg The energy scale is correct.l<EEEEE3H  0޽h ? 33___PPT10i.߫@z+D='  = @B +r>+Yfge1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of thW-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0Le angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0   9 (  x  c $t      0 jX W resolution Apply Unfolding to the experimental W distribution (in each angle region) for the smearing effect in the W direction using an asymmetric Gaussian (1.3% higher side and 1.9 % lower side). Unfolding is applied in 0.9 GeV < W < 2.4 GeV.z GC GfpC=G3C3Eff  T<  ??  XW(GeV)0 0 6A% ?pq3 g   "  T! ??   .Before (orange) and After (blue) the unfoldingT/0f f   f4)  ??F  9Yield0    `,  ?? B  } |cosq*|=0.22520C  f  S AC"?3    `4  ??[  MHistogram: Data0B   `D??% gg%   T9  ??Cp(  *Smearing func. peaking at the nominal mass+0+ B   `D??6 ts   0> P  vExperimental sample of h gg The energy scale is correct.l<EEEEE3H  0޽h ? 33___PPT10i.߫@z+D='  = @B +rg+2~g̿e1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 '  0 (  r  S |ӌ 9     0ٌ w Resonances: Clearly seen: f0(980) and f2(1270) New broad peaks ~1.65 GeV and ~1.95 GeV Hints with a lower significance : ~1.45 GeV, cc0 (and cc2) @ GfC3GGO GGONGC2G3G3O3G3G3O3<G3:  3 A` R  0 | A Sizes of the charmonia Ggg(cc0)B(cc0p0p0): 8.4 2.2 0.8 eV (4.5s) Ggg(cc2)B(cc2p0p0): 0.29 0.23 0.03 eV (1.4s) Upper limit < 0.75 eV (90%CL) Preliminary The central values are consistent with the expectations from isospin invariance between the p+p-/p0p0 decays o0G3AAAIAAIAIAIAAAAAAAAIAAIAIAIAAAAOA E3^AAIAIAIAIAE3FLA*  Z??C"?,%   < Z T |cos q*|<0.4, CH  0޽h ? 33___PPT10i.{_+D=' = @B +r. e1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d 0   0 (  r  S |ӌ 9     0ٌ w lDgg Resonance p0p0 Clearly seen: f0(980) and f2(1270) New broad peaks ~1.65 GeV and ~1.95 GeV Hints with lower significance : ~1.45 GeV, cc0 (and cc2) #GfGf ffffffC3GGO GGONGC0G3G3O3G3G3O3<G36n:  3 A` R  0 | A Sizes of the charmonia Ggg(cc0)B(cc0p0p0): 8.4 2.2 0.8 eV (4.5s) Ggg(cc2)B(cc2p0p0): 0.29 0.23 0.03 eV (1.4s) Upper limit < 0.75 eV (90%CL) Preliminary The central values are consistent with the expectations from isospin invariance between the p+p-/p0p0 decays o0G3AAAIAAIAIAIAAAAAAAAIAAIAIAIAAAAOA E3^AAIAIAIAIAE3FLA*  Z??C"?,%   < Z T |cos q*|<0.4, CH  0޽h ? 33___PPT10i.{_+D=' = @B +r.|biqe1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC   $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] drqq5e1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanLL$+Ԗ0Ԗ"D-3 00000TomanLL$+Ԗ0Ԗ2 DTimes New RomanLL$+Ԗ0Ԗ0D-3 0fgew RomanLL$+Ԗ0Ԗ@DSymbolew RomanLL$+Ԗ0ԖPDCalisto MTomanLL$+Ԗ0Ԗ`DVerdanaMTomanLL$+Ԗ0Ԗ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4YdYd 0ppp@ <4ddddA10L+ ___PPT10D-3 000000;t^LLp0p2DArial000;t^LLp0p" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] driE e1J(u _   000000 0000 Paint.Picture0000Root EntrydO))+| PicturestdCurrent User5SummaryInformation( U                          ! " # $ % & ' ( ) * + , - . / 0 C < = > ? @ A B C D E F G H I J K L M N O P Q R S T U V W X Y Z [ \ ] ^ _ ` a b c d e f g h i j k l m n o p q r s t u v w x y { | } ~  ;                           ! " # $ % & ' ( ) * + , - . / 0 1 2 3 4 5 6 7 8 9 : ; < = > ? @ A B C D E F G H I J K L M N O P Q R S T U V W X Y Z [ \ ] ^ _ ` a b c d e f g h i j k l m n o p q r s t u v w x y z { } ~  | {                          ! " # $ % & ' ( ) * + , - . / 0 1 2 3 4 5 6 7 8 9 : ; < = > ? @ A B C D E F G H I J K L M N O P Q R S T U V W X Y Z [ \ ] ^ _ ` a b c d e f g h i j k l m n o p q r s t u v w x y z | } ~  )   (980)&Angular dependence in f2(1270) regionFit to f2(1270) line shapeTrigger efficiency study'Trigger efficiency from the simulation3pt-balance resolution and correction to efficiency "使用されているフォント デザイン テンプレート$埋め込まれた OLE サーバースライド タイトル$$イトル$_Wuehara2uehara2                         ! " # $ % & ' ( * A + , B { E F G H I J K L M N O P Q R S T U V W X Y Z [ \ ] ^ _ ` a b c d e f g h i j k l m n o p q r s t u v w x y z   } ~ 9 % 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4IdId\ 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d   0    (  r  S <       f=  ??T; a1(I=0, JPC=0++) mesons --- fJ or ccJ (J=even)20GOGOGGOGGO G,    fG  ??) I  $s(p0p0):s(p+p-) =1:20Gf OfGfOfGf GfGfOfGfOfGfGfq   `pR  ??9 ' Interference between a resonance and continuum component modifies the ratio. We expect that continuum contribution is smaller in p0p0 than in p+p- in the intermediate or low energies0NC3G3G3O3G3O3 G3G3O3G3O3%G3&  Tde  ??a  6f2(1270) has been observed in p+p-. f0(980) not significantly seen in the past experiments. Are any mesons previously reported seen ? f0 1.3-1.5GeV f2 1.6  2.1GeV f4(2050) etc. - The charmonia: cc0 and cc2$--8-0*-u-0GOGCCKCKCG OG GG9CGCCK$CCK&CCKCG3G3O3G3G3O3H  0޽h ? ̙3380___PPT10.r- aQ 9  E_ e1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4IdId\ 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =.G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3$fF  "3G3O33f+ 33fGO%33 3GUC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular depend ence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d   0 "   (  r  S <       f=  ??T; a1(I=0, JPC=0++) mesons --- fJ or ccJ (J=even)20GOGOGGOGGO G,    fG  ??6 P "V  $s(p0p0):s(p+p-) =1:20Gf OfGfOfGf GfGfOfGfOfGfGf   `pR  ?? p Interference between a resonance and continuum component modifies the ratio. We expect that continuum contribution in p0p0 is smaller than in p+p-, in the intermediate or low energies0OC(G3G3O3G3O3 G3CG3G3O3G3O3G3%G3'  Tde  ??3  4f2(1270) has been observed in p+p-. f0(980) not significantly seen in the past experiments. Are any mesons previously reported seen ? f0 1.3-1.5GeV f2 1.6  2.1GeV f4(2050) etc. - The charmonia: cc0 and cc2$--8-0*-u-0GOGCCKCKCG OG GG9CGCCK$CCK&CCKCG3G3O3G3G3O3H  0޽h ? ̙3380___PPT10.r_ a 9]_ ˷ e1J(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4IdId\ 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =a/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3"Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP<-PP-PxP3#ffffF  "3G3O33f+ 33fGO%33 3GSC  FWC  reRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] dL  0   L (  r  S <       f=  ??T; a1(I=0, JPC=0++) mesons --- fJ or ccJ (J=even)20GOGOGGOGGO G,    fG  ??6 P "V  $s(p0p0):s(p+p-) =1:20Gf OfGfOfGf GfGfOfGfOfGfGf   `pR  ?? p Interference between a resonance and continuum component modifies the ratio. We expect that continuum contribution in p0p0 is smaller than in p+p-, in the intermediate or low energies0OC(G3G3O3G3O3 G3CG3G3O3G3O3G3%G3',  Tde  ??3  hf2(1270) has been observed in p+p- and in p0p0 as a big peak. f0(980) not significantly seen in the past experiments. Are any mesons previously reported seen ? f0 1.3-1.5GeV f2 1.6  2.1GeV f4(2050) etc. - The charmonia: cc0 and cc2>--8-0*-u-0GOGCCKCKCCCCKCKCG OG GG9CGCCK$CCK&CCKCG3G3O3G3G3O3H  0޽h ? ̙3380___PPT10.  0 8P(  8x 8 c $> 9   x 8 c $x?     8  ` B  ??jT 6Based on data with an integrated luminosity of 95 fb-16704GOH 8 0޽h ? 33___PPT10i. @a+D=' 3= @B +r _ a     e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4IdId\ 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 &  0 (  0x 0 c $OT O  0 0,O j8Hadron production from two quasi-real photons (|q2|<0.001GeV2, with no-tag condition) Exclusive processes with WWgg=0.6 - 4.5 GeV at KEKB/Belle Wide energy region --- Various physics aspects can be studied simultaneously. 0 Light-quark resonances, Charmonia Perturbative /Non-perturbative QCD, 00 0Hadron production mechanism 0XGGfOf GfOfcGfGCGfOfGfzG3C9C GfGf GfGf Gf9Gf GfGfG3L9<: 0 3 A  0  fO jJ??  {9Resonance formation or Hard scattering with a quark line&:0:G 0  `O ??M m Ahadrons0CH 0 0޽h ? ̙33y___PPT10Y+D=' 3= @B +  0 8P(  8x 8 c $> 9   x 8 c $x?     8  ` B  ??jT 6Based on data with an integrated luminosity of 95 fb-16704GOH 8 0޽h ? 33___PPT10i. @a+D=' 3= @B +rT cl H\` #0 p e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@c5 ʚ;Xm8ʚ;g4IdId\ 0Dppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%3      !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~3 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0   0 (  0x 0 c $OT O  0 0,O :NHadron production from two quasi-real photons (|q2|<0.001GeV2, with zero-tag condition) Exclusive processes with gg c.m. energy WWgg=0.6 - 4.5 GeV at KEKB/Belle Wide energy region --- Various physics aspects can be studied simultaneously. Light-quark resonances, charmonia Perturbative /Non-perturbative QCD, Hadron production mechanism(0XGGfOf GfOfeGfGCC;CGfOfGfG3cG3C GfFGf GfGfG34:: 0 3 A  0  fO jJ??  {9Resonance formation or Hard scattering with a quark line&:0:G 0  `O ??M m Ahadrons0CH 0 0޽h ? ̙33y___PPT10Y+D=' 3= @B +rXp H` #4p 7 e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33f33f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 @%(  ~  s *W     0  `A ? ?'    0  `A ? ?      6Y p0  8W (GeV)  XB  0Do:p  6^ p ;0  8W (GeV)  XB @ 0Do 3    6` DD Q | cos q*|, CXB   0Do`Tp   s * f C   Q | cos q*|, CXB   0Doj    0@n ,y i7About 1.26M events (before the background subtraction)88:  3 A   <o 6  T |cos q*|<0.4, C  <tv  W (GeV)XB  0DԔ c XB  0DԔ 9:`   0|y   acc0B E MM  < q  g  acc2B E MM   ` ??I U2.8 3.0 3.2 3.4 3.6 3.8 0 ^ ! S A$% q N   "  ` ?? t<  NEstimated background03 # <ԋ S j# M  j |cos q*|<0.8B C B $ ZD??I,I %  `t  ??e M#W = M(p0p0) |cosq*| in gg c.m.s$0G3G3O3G3O3G3G3 G3G3G3> H  0޽h ? 33___PPT10i. $+D=' 3= @B +&  0 = 5 p (  ~  s *Ч     :  3 A  :  3 A ';  <BF  1W=1.18GeV, |cosq*|=0.65 W>3.6GeV, |cosq*|<0.4N2CC, :   3 A       <`  7  LDots  experimental Histo.  Signal MC''   < i d4Histogram  experimental B  6H M 0pt-unbalanced backgrounds are seen in W<1.2 GeV1GOG!GG C G  B 3ԔC"?5 Low-energy beam-background photons Intermediate or Higher energies Non-exclusive process sources not significantly seen<SE EHE=  <T T@k 3W=0.90GeV, |cosq*|=0.05 W=0.66GeV, |cosq*|=0.05N4CC,   T ??aT e/ 0 0.1 0.2 0.3 0.4 0.5000   < ]  |Spt| (GeV/c):A    T ??Y e/ 0 0.1 0.2 0.3 0.4 0.5000 B @  fDԔ??"&"B @  fDԔ??s &s H  0޽h ? 33___PPT10i.Z|=+D=' 3= @B +   0   $(  $~ $ s *0 '   >  $ <PuF[ ? VDetermined by signal MC simulation and fitted with smooth functions of (W, |cos q*|)`W$G%C G3G3G3:  $ 3 A` I6 : $ 3 A* , $ 0` 9 M  8 W (GeV)  $ Z  ??mq  Trigger efficiency is determined by the trigger simulator after tunings of the energy thresholds the total energy trigger  1.15 GeV counting number of clusters (>=4) - 110 MeV Close to 100% above W>1.3 GeV0EAEA E3AEEfE1Ef` $ < W "+ VAcceptance Around 11% at maximum, typically 5 % Large angular dependence due to geometrical condition of the detector Overall efficiency = trigger efficiency Acceptance  E3lE'GC3 GEH $ 0޽h ? 33___PPT10i.jPK.+D=' 3= @B +r s { # 1 O ; e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d   0   $(  $~ $ s *0 '   >  $ <PuF[ ? 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B  } |cosq*|=0.22520C  f  S AC"?3    ` 9  ??[  MHistogram: Data0B   `D??% gg%   TP>  ??Cp(  *Smearing func. peaking at the nominal mass+0+ B   `D??6 ts   0A P  vExperimental sample of h gg The energy scale is correct.l<EEEEE3H  0޽h ? 33___PPT10i.߫@z+D=' 3= @B +r<  + ; e1K(u _   000000 0000 Paint.Picture0000000 0000#000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] dr ܞ  e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls}+&     "S5o).023 4.6  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>$b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$W-!M*WZp!b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"b$[`˄jke2 *$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. 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F˛"Y>T'VJ)»(R24)ɜ~!6a +lӰ`$P&$^wŹ^=U!!4#OEj5$#'JPU{YHuޘI7zk;Ӑ M:,m´O S!JCԂ 3띚o`xc޼y}}}iY`/p: p|d-C*U0Eb%IJ'9J$PdmBb OkdhhHl :@~nCJwĎF'⬮^{@^Ŕ$@%"@X56FPVMSV@Wn(<)` C[AJoH(x|v& wIa;pbzK2̌H @3N$@)LBP&JH #.Ɍ+Y`L4#:3"GL\e'=Ȉ6Ir$@#|fM$4 \YLc)eAE#0%qISRLG$P(2 RLx #$~lrk@$PLalH Lbt4!.e:U&a $@e% 3*qZ-r t#@֍'(*YX=D|ŞEer !@f# BJ 1[?hg\J0SĐ+HrOɄ$y: KXB   j?Z uXۈ%$  &j+kE$@$@$P|ao#HHHêٮ @ PXB   jfV$@$@$@'@V6b IHHI:Z "*6IENDB`nM;\#fPPNG  IHDR( WxysRGB pHYs^wݾ0PLTE"""333DDDUUUwwwfffIDATXOhU'vl9H1fR!m -jr(""v[%5E#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*$b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0Vppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d5   0 LD (  r  S TO 'g     0P f@`  cNote: After the Unfolding, different data bins and errors are no longer independent of each other.:d[fu  0X V   }Comparison with Crystal Ball at DORIS II (1990) They are consistent. Belle has ~103 times more data. Statistical errors only.|~0G"GOGCG3~  0`   XObtain first ds/d|cosq*| in each D|cos q*|=0.05 bin Then, accumulate them over the anglevYAAAA AAAA1A,  3:  3 AP %:  3 AO s    `l  ??zZ  K Preliminary$ 0 G3    f|q  ??   s9Data in the charmonium region are omitted from the plot.:0:fB   fD>?? P H  0޽h ? 33___PPT10i.Po@+D='  = @B +  0   0b (  r  S  9     04 w B>gg Resonance p0p0 Clearly seen: f0(980) and f2(1270) New broad peaks ~1.65 GeV and ~1.95 GeV Hints with lower significance : ~1.45 GeV, cc0 (and cc2)  GfGf ffffffC3GGO GGOKGC0G3G3O3G3G3O3<G3:  3 A` R  0 | A Sizes of the charmonia Ggg(cc0)B(cc0p0p0): 8.4 2.2 0.8 eV (4.5s) Ggg(cc2)B(cc2p0p0): 0.29 0.23 0.03 eV (1.4s) Upper limit < 0.75 eV (90%CL) Preliminary The central values are consistent with the expectations from isospin invariance between the p+p-/p0p0 decays o0G3AAAIAAIAIAIAAAAAAAAIAAIAIAIAAAAOA E3^AAIAIAIAIAE3FLA*  Z??C"?,%   <L' Z T |cos q*|<0.4, CH  0޽h ? 33___PPT10i.{_+D='  = @B +  0 @ 1T(  r  S 6     F  07 f 7F Charmonium region is omitted from the plot. The ratio is 0.3  0.4 at W>2.7 GeV*Q,C%G3  0F   OError bars are statistical only. Systematic errors: About 10% at each measurement point, except p+p- above the charmonium masses (~25%).#GffGf/CCKCK$Cc& , Z ??-3 P: . 3 AT  / T  ??MG4  |cosq*|<0.6J 0 3 E3 33 0  `  ??  K Preliminary$ 0 G3 1 T^  ??#  K Preliminary$ 0 G3H  0޽h ? 33___PPT10i._+D='  = @B +r:C ,B .  B C e1K(u _   000000 0000 Paint.Pictur_ct^?Ǒ{k'5% ݬG !T~~" .zPC=&Nfا "隃Q?hL`*xF[e4tYŕ$?3 ;NV騡8|ٿh/b r,q^6%>ku- 9ۛl 'J"V_ uCVT1S%X X٪vT#X7Ji/=zjY_=nMbAB*}Q PB9^;mh!-儢݀H=_樢to)X sϐm(6a=+ F:,;N/nX%xD#H`$ |Hk0h.jɏ KhzH=I{do˯1ކaR5k嗖ޖ@+L.;տJ/}!K66ReXafH.jmp$3LPp SZP͠S3X hh ua#U[l5r !&fh 3qYXh)J%-\T+@;g৶MA"MNNOA)kRUeEmhJKFpmv ⵟ׎7$f ڐފ+ۡ~QlHC:L1;7+#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0Vppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 @ 2(  r  S 6     F  07 f 7F Charmonium region is omitted from the plot. The ratio is 0.3  0.4 at W>2.7 GeV*Q,C%G3  0F   OError bars are statistical only. Systematic errors: About 10% at each measurement point, except p+p- above the charmonium masses (~25%).#GffGf/CCKCK$Cc& , Z ??-3 P: . 3 A&  / T  ??MG4  |cosq*|<0.6J 0 3 E3 33 0  `  ??  K Preliminary$ 0 G3 1 T^  ??#  K Preliminary$ 0 G3: 2 3 A]p/S H  0޽h ? 33___PPT10i._+D='  = @B +r? /G  > e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls~+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d   0 @ 3<(  r  S 6       07 f 7F J The ratio is 0.3  0.4 at W>2.7 GeV*&C%G3  0F%  OError bars are statistical only. Systematic errors: About 10% at each measurement point, except p+p- above the charmonium masses (~25%).#GffGf/CCKCK$Cc& , Z ??-3 P: . 3 A&  / T  ??G  |cosq*|<0.6J 0 3 E3 33 0  `  ??  K Preliminary$ 0 G3 1 T^  ??#  K Preliminary$ 0 G3: 2 3 A]p/S  3  `|}  ?? z "4  d,Charmonium region is omitted from the plot.-0-AH  0޽h ? 33___PPT10i._+D=' = @B +rz /N V X e1K(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls~+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =e/G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained. 8P2-P-PGP-PE-PCCKCKC  ^CCD> 7C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  uCCh CKCKCKCKC C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d   0 @ 3,(  r  S 6       07  \ HThe ratio is 0.3  0.4 at W>2.7 GeV%%G3  0F%  OError bars are statistical only. Systematic errors: About 10% at each measurement point, except p+p- above the charmonium masses (~25%).#GffGf/CCKCK$Cc& , Z ??-3 P: . 3 A&  / T  ??G  |cosq*|<0.6J 0 3 E3 33 0  `  ??  K Preliminary$ 0 G3 1 T^  ??#  K Preliminary$ 0 G3: 2 3 A]p/S  3  `|}  ?? z "4  d,Charmonium region is omitted from the plot.-0-AH  0޽h ? 33___PPT10i._+D=' = @B +r[X /c 7X e1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls~+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$      !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{}~$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d$  0 $(  r  S T     r  S TU ]}   H  0޽h ? ̙3380___PPT10.pyh  0 `0(  x  c $H  H x  c $HM= H H  0޽h ? 33___PPT10i.B+D=' 3= @B +r, 1h ;<  e1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls~+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4IdId\ 0&ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0L HTTx 0x2DArial00}0L HTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] dr=  MJe1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls~+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4TdTd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LNTTx 0x2DArial00}0LNTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d#  0 JB \(  \t \ T  ??pt  p+p- and p0p0 : Physics is almost the same, but gives independent information Electromagnetic production as mesons: s(p0p0)<<s(p+p-) Resonances (I=0, JPC=even++) decaying via strong interaction: 00000000000000s(p0p0):s(p+p-) =1:2 Test of QCD: s(p0p0)/s(p+p-) : ~0.03 (LO)  0.5 ( handbag ) c.m.-energy (W) and angular dependences must also be examined. 0GOGOGGGOGO G=GO+GGfOfGfOfGfOfGfOfGfGOG O!GC CGf OfGfOfGf GfGfOfGfOfGfGfGf GCGf OfGfOfGfOfGfOfGfC C&G3 G3G3E3G3<C~ \ s *|     : \ 3 AY \  `x  ?? Ep(0C \  ` S ??}B Ep(0C: \ 3 A# +: \ 3 A{:  \ 3 AMJ s  \ <X zf  C Resonance G  \ <8 M G ?quarkGf  \ < y Gsoft hadron exchangeA  \ <D  Msoft production of mesonsAH \ 0޽h ? ̙33y___PPT10Y+D='  = @B +_  0   _ (  r  S #        f%  ??T; t4(I=0, JPC=even++) mesons --- fJ or ccJ (J=even)50GOG OGGOGGO G,    f3  ??6 P "V  $s(p0p0):s(p+p-) =1:20Gf OfGfOfGf GfGfOfGfOfGfGf   `D  ?? p Interference between a resonance and continuum component modifies the ratio. We expect that continuum contribution in p0p0 is smaller than in p+p-, in the intermediate or low energies0OC(G3G3O3G3O3 G3CG3G3O3G3O3G3%G3',  TX  ??3  hf2(1270) has been observed in p+p- and in p0p0 as a big peak. f0(980) not significantly seen in the past experiments. Are any mesons previously reported seen ? f0 1.3-1.5GeV f2 1.6  2.1GeV f4(2050) etc. - The charmonia: cc0 and cc2>--8-0*-u-0GOGCCKCKCCCCKCKCG OG GG9CGCCK$CCK&CCKCG3G3O3G3G3O3H  0޽h ? ̙3380___PPT10.{   0    " (  ~  s *x     V  C .ABellering4#    <\{ '^   Asymmetric e- e+ collider b    0   wBeam crossing angle: 22mrad@$   0   LContinuous injection  0 '@  FLuminosity Lmax=1.71x1034 cm-2s-1 +" Ldt ~ 740 fb-1 (Nov.2007)00^ >      E   4 6  <  "`  t8 GeV e- (HER) x 3.5 GeV e+ (LER) s=10.58 GeV (4S),;$33    `A ? q \      `  ?? k BXHigh momentum/energy resolutions CDC+Solenoid, CsI Vertex measurement  Si strips Particle identification TOF, Si-aerogel, CDC-dE/dx, RPC for KL/muon0!GC CCG CG4CKC) xH  0޽h ? 33___PPT10i.@+D='  = @B +rJIa #8]Je1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖD-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cʚ;Xm8ʚ;g4XdXd\ 0rppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LNTTx 0x2DArial00}0LNTTx 0x pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0   @(  @r @ S ~"    @ T??C"?b  @  f ?? -  BarXiv:0711.1926v1 [hep-ex]0(2007)<"0C CC*  @  `XR ?? z  IBelle Collaboration0H @ 0޽h ? 33___PPT10i.T+D=' = @B +r  e1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cDvʚ;Xm8ʚ;g4XdXd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LOTTx 0x2DArial00}0LOTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 <(  r  S      J  Z  ??ko bggcc2 gJ/y PLB 540, 33(2002) gg(f2'(1525)etc. )K+K- (1.4 - 2.4 GeV) EPJC 32, 323 (2003) gg (cc0,cc2)p+p-,K+K- (2.4 - 4.1 GeV) PLB 615, 39 (2005) gg (hc )pp (2.025 - 4.0 GeV) PLB 621, 41 (2005) gg cc2' DD PRL 96, 082003 (2006) gg (f0(980)etc. )p+p- (0.8 - 1.5 GeV) PRD 75, 051101(R) (2007), Phys. Soc. Jpn. 76, 074102 (2007) gg (cc0,cc2 )K+K- (2.4 - 4.0 GeV) PLB 651, 15 (2007) gg (hc,cc0,cc2 )p+p-p+p-,K+K-p+p-,K+K-K+K- arXiv:0706.3955[hep-ex], to appear inEPJC gg a2's -p+p-p0 (1.2 - 3.0 GeV) hep-ex/0610022 gg (hc )LL,S0S0 (2.3-4.0 GeV) hep-ex/0609048 gg p0p0 arXiv:0711.1926v1 [hep-ex]0 20CCKCCCC=CCCCCK CCKCK4CCCCKCCKCCKCKCKCK5CCCCKCGCCCCKCCQCCCCK CCCKCKCACCCKCCKCCKCK1CCCCKCCKCCKCCCKCKCKCKCKCKCKCKCKCKCKCK]CCCCKCCCCKCKCK5CCCCKCCCCCKCK5CCCCKCMKA AIH JI[C^ F?e 0RWB   `DjJ??B   `DjJ?? fB   `DjJ??   B   `DjJ??W IW H  0޽h ? ̙33___PPT10i.D:)+D=' Q = @B +r4`D_7we1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cDvʚ;Xm8ʚ;g4XdXd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LOTTx 0x2DArial00}0LOTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] ds  0 (  r  S      (  Z  ??ko dggcc2 gJ/y PLB 540, 33(2002) gg(f2'(1525)etc. )K+K- (1.4 - 2.4 GeV) EPJC 32, 323 (2003) gg (cc0,cc2)p+p-,K+K- (2.4 - 4.1 GeV) PLB 615, 39 (2005) gg (hc )pp (2.025 - 4.0 GeV) PLB 621, 41 (2005) gg cc2' DD PRL 96, 082003 (2006) gg (f0(980)etc. )p+p- (0.8 - 1.5 GeV) PRD 75, 051101(R) (2007), Phys. Soc. Jpn. 76, 074102 (2007) gg (cc0,cc2 )K+K- (2.4 - 4.0 GeV) PLB 651, 15 (2007) gg (hc,cc0,cc2 )p+p-p+p-,K+K-p+p-,K+K-K+K- arXiv:0706.3955[hep-ex], to appear in EPJC gg a2's -p+p-p0 (1.2 - 3.0 GeV) hep-ex/0610022 gg (hc )LL,S0S0 (2.3-4.0 GeV) hep-ex/0609048 gg p0p0 arXiv:0711.1926v1 [hep-ex]0 30CCKCCCC=CCCCCK CCKCK4CCCCKCCKCCKCKCKCK5CCCCKCGCCCCKCCQCCCCK CCCKCKCACCCKCCKCCKCK1CCCCKCCKCCKCCCKCKCKCKCKCKCKCKCKCKCKCK^CCCCKCCCCKCKCK5CCCCKCCCCCKCK5CCCCKCMKA AI$ JI[CF?e 0RWB   `DjJ??B   `DjJ?? fB   `DjJ??   B   `DjJ??W IW H  0޽h ? ̙33___PPT10i.D:)+D=' Q = @B +rx`-7we1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&      !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cDvʚ;Xm8ʚ;g4XdXd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LOTTx 0x2DArial00}0LOTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 >(  r  S      L  Z  ??ko vggcc2 gJ/y PLB 540, 33(2002) gg(f2'(1525)etc. )K+K- (1.4 - 2.4 GeV) EPJC 32, 323 (2003) gg (cc0,cc2)p+p-,K+K- (2.4 - 4.1 GeV) PLB 615, 39 (2005) gg (hc )pp (2.025 - 4.0 GeV) PLB 621, 41 (2005) gg cc2' DD PRL 96, 082003 (2006) gg (f0(980)etc. )p+p- (0.8 - 1.5 GeV) PRD 75, 051101(R) (2007), Phys. Soc. Jpn. 76, 074102 (2007) gg (cc0,cc2 )K+K- (2.4 - 4.0 GeV) PLB 651, 15 (2007) gg (hc,cc0,cc2 )p+p-p+p-,K+K-p+p-,K+K-K+K- arXiv:0706.3955[hep-ex], to appear in EPJC gg a2's -p+p-p0 (1.2 - 3.0 GeV) hep-ex/0610022 gg (hc )LL,S0S0 (2.3-4.0 GeV) hep-ex/0609048 gg p0p0 arXiv:0711.1926v1 [hep-ex]0 <0CCKCCCC=CCCCCK CCKCK4CCCCKCCKCCKCKCKCK5CCCCKCGCCCCKCCQCCCCK CCCKCKCACCCKCCKCCKCK:CCCCKCCKCCKCCCKCKCKCKCKCKCKCKCKCKCKCK^CCCCKCCCCKCKCK5CCCCKCCCCCKCK5CCCCKCMKA AI6 JI[, F?e 0RWB   `DjJ??B   `DjJ?? fB   `DjJ??   B   `DjJ??W IW H  0޽h ? ̙33___PPT10i.D:)+D=' ]= @B +r`(7Ae1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cDvʚ;Xm8ʚ;g4XdXd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LOTTx 0x2DArial00}0LOTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] du  0 (  r  S      *  Z  ??ko tggcc2 gJ/y PLB 540, 33(2002) gg(f2'(1525)etc. )K+K- (1.4 - 2.4 GeV) EPJC 32, 323 (2003) gg (cc0,cc2)p+p-,K+K- (2.4 - 4.1 GeV) PLB 615, 39 (2005) gg (hc )pp (2.025 - 4.0 GeV) PLB 621, 41 (2005) gg cc2' DD PRL 96, 082003 (2006) gg (f0(980)etc. )p+p- (0.8 - 1.5 GeV) PRD 75, 051101(R) (2007), Phys. Soc. Jpn. 76, 074102 (2007) gg (cc0,cc2 )K+K- (2.4 - 4.0 GeV) PLB 651, 15 (2007) gg (hc,cc0,cc2 )p+p-p+p-,K+K-p+p-,K+K-K+K- arXiv:0706.3955[hep-ex], to appear in EPJC gg a2's p+p-p0 (1.2 - 3.0 GeV) hep-ex/0610022 gg (hc )LL,S0S0 (2.3-4.0 GeV) hep-ex/0609048 gg p0p0 arXiv:0711.1926v1 [hep-ex]0 ;0CCKCCCC=CCCCCK CCKCK4CCCCKCCKCCKCKCKCK5CCCCKCGCCCCKCCQCCCCK CCCKCKCACCCKCCKCCKCK:CCCCKCCKCCKCCCKCKCKCKCKCKCKCKCKCKCKCK^CCCCKCCCKCKCK5CCCCKCCCCCKCK5CCCCKCMKA AI$ JI[LE?e 0RWB   `DjJ??B   `DjJ?? fB   `DjJ?? 9 B   `DjJ?? I H  0޽h ? ̙33___PPT10i.D:)+D=' Q = @B +rA`ߍ7A\e1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖ"D-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cDvʚ;Xm8ʚ;g4XdXd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LOTTx 0x2DArial00}0LOTTx 0x" pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  P.Reactions at KEKB/Belle(Q/ Two-meson exclusive final states!!R0Selection of p+p- candidatesZ (C(K(C(K( (  - Two charged tracks (oppositely charged) with pt>0.3 GeV/c, -0.47 %qb` *S1Differential cross section( T2)Angular dependences at some energy points**  U3Fitting formula for f0(980)F$$$$ V4%Angular dependence in f2(1270) region6&$$ $$ W5Fit to f2(1270) line shapeF$$$$ X+Trigger efficiency study( e:&Trigger efficiency from the simulation''$ Y,2pt-balance resolution and correction to efficiency63 ff ff1 ff /p[ \ ] d  0 4(  r  S      B  Z  ??ko zggcc2 gJ/y PLB 540, 33(2002) gg(f2'(1525)etc. )K+K- (1.4 - 2.4 GeV) EPJC 32, 323 (2003) gg (cc0,cc2)p+p-,K+K- (2.4 - 4.1 GeV) PLB 615, 39 (2005) gg (hc )pp (2.025 - 4.0 GeV) PLB 621, 41 (2005) gg cc2' DD PRL 96, 082003 (2006) gg (f0(980)etc. )p+p- (0.8 - 1.5 GeV) PRD 75, 051101(R) (2007), Phys. Soc. Jpn. 76, 074102 (2007) gg (cc0,cc2 )K+K- (2.4 - 4.0 GeV) PLB 651, 15 (2007) gg (hc,cc0,cc2 )p+p-p+p-,K+K-p+p-,K+K-K+K- arXiv:0706.3955[hep-ex], to appear in EPJC gg a2's p+p-p0 (1.2 - 3.0 GeV) hep-ex/0610022 gg (hc )LL,S0S0 (2.3-4.0 GeV) hep-ex/0609048 gg p0p0 arXiv:0711.1926 [hep-ex]0 >0CCKCCCC=CCCCCK CCKCK4CCCCKCCKCCKCKCKCK5CCCCKCGCCCCKCCQCCCCK CCCKCKCACCCKCCKCCKCK:CCCCKCCKCCKCCCKCKCKCKCKCKCKCKCKCKCKCK^CCCCKCCCKCKCK5CCCCKCCCCCKCK5CCCCKCRKA AI6 JI[LE?R 0RWB   `DjJ??B   `DjJ?? fB   `DjJ?? 9 B   `DjJ?? I H  0޽h ? ̙33___PPT10i.D:)+D=' Q = @B +r`7t= e1L(u _   000000 0000 Paint.Picture0000000 0000000000 0000 Paint.Picture0000000 00005000000 0000 Paint.Picture0000000 0000K@pe_ Equation.30 Microsoft pe_ 3.0LApe_ Equation.30 Microsoft pe_ 3.0MBpe_ Equation.30 Microsoft pe_ 3.0NCpe_ Equation.30 Microsoft pe_ 3.0ODpe_ Equation.30 Microsoft pe_ 3.0PE000 Excel.Chart.80&Microsoft Excel 000/ 0DArialaMTomanTTtܖ 0ܖD-3 00000TomanTTtܖ 0ܖ2 DTimes New RomanTTtܖ 0ܖ0D-3 0fgew RomanTTtܖ 0ܖ@DSymbolew RomanTTtܖ 0ܖPDCalisto MTomanTTtܖ 0ܖ`DVerdanaMTomanTTtܖ 0ܖ" C0.  @n?" dd@  @@`` tls+&     "S5o).023 446  =A B D EFG!HI J KMNO Q RSTUVWXY[Z ] ^ _`bdt b$B  `ib$4}x;gib$-pSο6 "$9AA*֨[K ؊b$P|4h\ +SF>#b$Se8iCab$#"X82KnNb$NYqSQV.IPMD"aR$phh.i0U Vb$61B%h}#nOv9 2$4yS b$uXJcE*u1f`?Ab$([>b$WVʯp Cci b$Ю`g,Gj  b$C#4eX!cZ}|R$/< r ̅b$.At(EAb$_]]?%CΜ)G0b$6)plxf>x (b$h[D4Ј}qcb$@+NȡJ@*b$M;\#fP^b$M(y]ӼgN&2$4bkX]l:8I1dt2$L3N!iF b$8 w{lU4W. b$8RkaE䶼z( b$UJ24P#^<> b$$-ܨwyTo[) b$3Sxlr)02 b$Üp7bko??[ 2$Z5Zu$1%^@ouR b$j2zT2\@my0L $b$aY+y8~s!b$4H z xkgb$ xE~1/3Qb$zc>?CkJW$b$_Զ(?̀Tc"$$$$b$ј( =% 2$ |qw̺2$#J ƫ u2$< BF8Oe8 \ 0e0e A@A5%8c8c     ?1d0u0@Ty2 NP'p<'p@A)BCD|E? 33333f@cDvʚ;Xm8ʚ;g4XdXd\ 0ppp@ <4dddd w 0Tt ___PPT10D-3 00000}0LQTTx 0x2DArial00}0LQTTx 0x pp6___PPT9{? -O  =m0G" ( H# Motivation of two-photon physics!!( I*\ General physics in gg p+p-/p0p0 final states/    C  C K C K C K C K  "a9:Resonances to appear in ggpp2(C(( K%  L&M'N(@New upper limit for Br (h p+p-)!$$$C$$$$$$$$ O)   <Preliminary results of ggp0p0~  $$C$$$$$$  Selection of p0p0 candidatesr (3G(3O(3G(3O(3 (3&Only 4 photons are visible - Triggered by Calorimeter triggers - No reconstructed track with pt>0.1GeV/c, dr<5cm, |dz|<5cm0 - 2 or more photons OR 1 or more p0s ------------------------------------------- - Just 2 p0s with E(decay product photon)>70MeV, pt>0.15GeV/c - Transverse-momentum (pt)-balance of the two p0 s |Spt|<0.05GeV/c - Satisfying a rough trigger condition at offline: N_gamma=4 or Esum_lab>1.25 GeV in the ECL-trigger region, 17<qlab<128.7degP>-PP-PxP3#ffffF  "3G3O33f+ 33f GO%33 3GSC  FWC  rgRA Raw-event distribution of p0p0d(3G(3O(3G(3O(3 (pt-balance distributions and backgrounds6)$3$3'$3Detection Efficiency6 (3  (3(3+ Unfolding and Energy calibration!!$,4Cross sections of gg p0p0n(C((C(K(C(K( Systematic-error sources* (  (( -  .Resonant structures ( /#Cross section ratio s(p0p0)/s(p+p-)$$C$$C$K$C$K$C$$C$K$C$K$C$ ;!Conclusion of p+p- measurementZ(C(K(C(K( (- We measure the process gg p+p- with 85.9 fb-1 data. The differential cross sections are obtained in 0.8 GeV < W < 1.5 GeV and |cos q*|<0.6 in the gg c.m. frame. (# We separately published before for the region 2.4 GeV<W<4.1GeV) - We confirm small but statistically significant peak from f0(980). New upper limit for P and CP violating process h p+p- is obtained.  8P2-P-PGP-PE-PCCKCKC  ^CCD$33330C X~1Summary for p0p0 measurementf  ((C(K(C(K( (- We measure the process gg p0p0 with 95fb-1 data. Preliminary results of the differential cross sections are obtained in 0.6 GeV < W < 4.0 GeV and |cos q*|<0.8 in the gg c.m. frame. - Several resonant structures are seen, including a statistically significant peak from f0(980). Behavior of the angular dependence (forward- and/or large-angle enhancements) changes drastically at around W= 2.0 GeV. The cross section ratio s(p0p0)/s(p+p-) in 3 GeV region is obtained. 6PE-PG-PePx-PPJ-PCCKCKC  p3G33 C3%33333,3 33G3O3G3O3G3O3G3O3G3C C,5^6 BACKUP slides(    b8% KEKB Accelerator and Belle Detector&&(3 `7-Measurements of two-photon processes at Belle..  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