THE QCD BEHAVIOURS OF THE XF3 (X, Q2) UP TO THE LEADING LOG IN THE NEUTRINO DEEPINELASTIC PROCESSES

SHEN Qi-Xing; WU Ji-Min; LU Jing-Xian; ZHAO Pei-Ying

Chinese Physics C> 1983, Vol. 7> Issue(3) : 309-315

THE QCD BEHAVIOURS OF THE XF₃ (X, Q²) UP TO THE LEADING LOG IN THE NEUTRINO DEEPINELASTIC PROCESSES

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Abstract：
The QCD behaviours of the structure functions xF₃ in the neutrino deep-inelastic processes are discussed by using the analytic expression for the distribution function of valence quarks in hadrons up to the leading log approximation given by a previous paper^[9]. The theoretical predictions are in good agreement with experimental data. The error arising from an approximation in solving the A-p equation is discussed. The calculation shows that relative error remains smaller than 1% even in the case of Q²=200 GeV and x=0.1

References

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SHEN Qi-Xing, WU Ji-Min, LU Jing-Xian and ZHAO Pei-Ying. THE QCD BEHAVIOURS OF THE XF₃ (X, Q²) UP TO THE LEADING LOG IN THE NEUTRINO DEEPINELASTIC PROCESSES[J]. Chinese Physics C, 1983, 7(3): 309-315.

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Received: 1900-01-01
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

THE QCD BEHAVIOURS OF THE XF₃ (X, Q²) UP TO THE LEADING LOG IN THE NEUTRINO DEEPINELASTIC PROCESSES

Corresponding author: SHEN Qi-Xing,

Received Date: 1900-01-01

Accepted Date: 1900-01-01

Available Online: 1983-06-05

Abstract: The QCD behaviours of the structure functions xF₃ in the neutrino deep-inelastic processes are discussed by using the analytic expression for the distribution function of valence quarks in hadrons up to the leading log approximation given by a previous paper^[9]. The theoretical predictions are in good agreement with experimental data. The error arising from an approximation in solving the A-p equation is discussed. The calculation shows that relative error remains smaller than 1% even in the case of Q²=200 GeV and x=0.1

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THE QCD BEHAVIOURS OF THE XF₃ (X, Q²) UP TO THE LEADING LOG IN THE NEUTRINO DEEPINELASTIC PROCESSES

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THE QCD BEHAVIOURS OF THE XF₃ (X, Q²) UP TO THE LEADING LOG IN THE NEUTRINO DEEPINELASTIC PROCESSES

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