首页> 外文OA文献 >The Complete $O(\alpha_s^2)$ Non-Singlet Heavy Flavor Corrections to the Structure Functions $g_{1,2}^{ep}(x,Q^2)$, $F_{1,2,L}^{ep}(x,Q^2)$, $F_{1,2,3}^{ u(\bar{ u})}(x,Q^2)$ and the Associated Sum Rules
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The Complete $O(\alpha_s^2)$ Non-Singlet Heavy Flavor Corrections to the Structure Functions $g_{1,2}^{ep}(x,Q^2)$, $F_{1,2,L}^{ep}(x,Q^2)$, $F_{1,2,3}^{ u(\bar{ u})}(x,Q^2)$ and the Associated Sum Rules

机译:完整的$ O(\ alpha_s ^ 2)$非单重态重味道修正   结构函数$ g_ {1,2} ^ {ep}(x,Q ^ 2)$,$ F_ {1,2,L} ^ {ep}(x,Q ^ 2)$,   $ F_ {1,2,3} ^ {\ nu(\ bar {\ nu})}(x,Q ^ 2)$和关联总和规则

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摘要

We calculate analytically the flavor non-singlet $O(\alpha_s^2)$ massiveWilson coefficients for the inclusive neutral current non-singlet structurefunctions $F_{1,2,L}^{ep}(x,Q^2)$ and $g_{1,2}^{ep}(x,Q^2)$ and charged currentnon-singlet structure functions $F_{1,2,3}^{\nu(\bar{\nu})p}(x,Q^2)$, atgeneral virtualities $Q^2$ in the deep-inelastic region. Numerical results arepresented. We illustrate the transition from low to large virtualities forthese observables, which may be contrasted to basic assumptions made in theso-called variable flavor number scheme. We also derive the correspondingresults for the Adler sum rule, the unpolarized and polarized Bjorken sum rulesand the Gross-Llewellyn Smith sum rule. There are no logarithmic corrections atlarge scales $Q^2$ and the effects of the power corrections due to the heavyquark mass are of the size of the known $O(\alpha_s^4)$ corrections in the caseof the sum rules. The complete charm and bottom corrections are compared to theapproach using asymptotic representations in the region $Q^2 \gg m_{c,b}^2$. Wealso study the target mass corrections to the above sum rules.
机译:我们分析性地计算了包含性中性电流非单一结构函数$ F_ {1,2,L} ^ {ep}(x,Q ^ 2)$的风味非单一$ O(\ alpha_s ^ 2)$ Massilson系数和$ g_ {1,2} ^ {ep}(x,Q ^ 2)$和带电电流非单一结构函数$ F_ {1,2,3} ^ {\ nu(\ bar {\ nu})p}( x,Q ^ 2)$,深无弹性区域的一般虚拟度$ Q ^ 2 $。给出了数值结果。我们说明了从低虚拟度到大型虚拟度的可观转变,这可以与所谓的可变风味数方案中的基本假设形成对比。我们还导出了Adler和规则,非极化和极化Bjorken和规则以及Gross-Llewellyn Smith和规则的相应结果。在总和规则的情况下,在大尺度$ Q ^ 2 $上没有对数校正,并且由于重夸克质量而导致的功率校正的作用与已知的$ O(\ alpha_s ^ 4)$校正相同。使用区域$ Q ^ 2 \ gg m_ {c,b} ^ 2 $中的渐近表示,将完整的魅力和底部校正与方法进行比较。我们还研究了上述总和规则的目标质量校正。

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