Chinese Physics C > 2010, Vol. 34 > Issue(9): 1414-1416 DOI: 10.1088/1674-1137/34/9/058

Determining the strange and antistrange quark distributions of the nucleon

CAO Fu-Guang,
CHEN Hong^,

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Abstract：

The difference between the strange and antistrange quark distributions, δs(x)=s(x)－s(x), and the combination of light quark sea and strange quark sea, Δ(x)=d(x)+u(x)－s(x)－s(x), are originated from non-perturbative processes and can be calculated using non-perturbative models of the nucleon. We report calculations of δs(x) and Δ(x) using the meson cloud model. Combining our calculations of Δ(x) with relatively well known light antiquark distributions obtained from global analysis of available experimental data, we estimate the total strange sea distributions of the nucleon.

References

[1]

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CAO Fu-Guang and CHEN Hong. Determining the strange and antistrange quark distributions of the nucleon[J]. Chinese Physics C, 2010, 34(9): 1414-1416. doi: 10.1088/1674-1137/34/9/058

CAO Fu-Guang and CHEN Hong. Determining the strange and antistrange quark distributions of the nucleon[J]. Chinese Physics C, 2010, 34(9): 1414-1416. doi:10.1088/1674-1137/34/9/058 shu

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Received: 2010-03-04
Revised: 1900-01-01

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通讯作者:陈斌, bchen63@163.com

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沈阳化工大学材料科学与工程学院沈阳 110142

Determining the strange and antistrange quark distributions of the nucleon

Corresponding author:CHEN Hong,

Received Date:2010-03-04

Accepted Date:1900-01-01

Available Online:2010-09-05

Abstract:

The difference between the strange and antistrange quark distributions, δs(x)=s(x)－s(x), and the combination of light quark sea and strange quark sea, Δ(x)=d(x)+u(x)－s(x)－s(x), are originated from non-perturbative processes and can be calculated using non-perturbative models of the nucleon. We report calculations of δs(x) and Δ(x) using the meson cloud model. Combining our calculations of Δ(x) with relatively well known light antiquark distributions obtained from global analysis of available experimental data, we estimate the total strange sea distributions of the nucleon.

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Determining the strange and antistrange quark distributions of the nucleon

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