Fast heating dissociation of ${ \Upsilon(1S) }$ in heavy ion collisions at RHIC

  • By adopting the adiabatic assumption in the cooling process, we discuss a novel mechanism of $ \Upsilon(1S) $ suppression that occurs due to the fast heating process at the early stage of the fireball, instead of its finite decay width in a finite temperature medium generated by heavy ion collisions. We calculate the transition probability after the fast heating dissociation as a function of the temperature of the medium and the nuclear modification factor in central collisions and find that the suppression is not negligible at RHIC, even if the width of $ \Upsilon(1S) $ becomes zero.
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Yunpeng Liu and Baoyi Chen. Fast Heating Dissociation of ${ \Upsilon(1S) }$ in Heavy Ion Collisions at RHIC[J]. Chinese Physics C. doi: 10.1088/1674-1137/abb4d7
Yunpeng Liu and Baoyi Chen. Fast Heating Dissociation of ${ \Upsilon(1S) }$ in Heavy Ion Collisions at RHIC[J]. Chinese Physics C. doi:10.1088/1674-1137/abb4d7 shu
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Received: 2020-07-13
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    Fast heating dissociation of ${ \Upsilon(1S) }$ in heavy ion collisions at RHIC

      Abstract:By adopting the adiabatic assumption in the cooling process, we discuss a novel mechanism of $ \Upsilon(1S) $ suppression that occurs due to the fast heating process at the early stage of the fireball, instead of its finite decay width in a finite temperature medium generated by heavy ion collisions. We calculate the transition probability after the fast heating dissociation as a function of the temperature of the medium and the nuclear modification factor in central collisions and find that the suppression is not negligible at RHIC, even if the width of $ \Upsilon(1S) $ becomes zero.

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        1. Introduction
        • The phase diagram of quark matter is among the most interesting topics in high-energy nuclear

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