Determining the strange and antistrange quark distributions of the nucleon

The difference between the strange and antistrange quark distributions,δs(x) = s(x) ˉs(x),and the combination of light quark sea and strange quark sea,Δ(x) =ˉ d(x) + uˉ(x) s(x) ˉs(x),are originated from non-perturbative processes and can be calculated using non-perturbative models of the nucleon.We...

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Bibliographic Details
Published inChinese physics C Vol. 34; no. 9; pp. 1414 - 1416
Main Author 曹福广 陈洪 A. I. signal
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.09.2010
Institute of Fundamental Sciences,Massey University,Private Bag 11 222,Palmerston North,New Zealand%School of Physical Science and Technology,Southwest University,Chongqing 400715,People's Republic of China
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ISSN1674-1137
0254-3052
2058-6132
DOI10.1088/1674-1137/34/9/058

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Summary:The difference between the strange and antistrange quark distributions,δs(x) = s(x) ˉs(x),and the combination of light quark sea and strange quark sea,Δ(x) =ˉ d(x) + uˉ(x) s(x) ˉs(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.
Bibliography:strange and antistrange quark distributions; nucleon; meson cloud model
meson cloud model
O572.3
O572.33
11-5641/O4
nucleon
strange and antistrange quark distributions
ISSN:1674-1137
0254-3052
2058-6132
DOI:10.1088/1674-1137/34/9/058