Stefan Dittmaier, Philipp Maierhöfer, Christopher Schwan, Ramon Winterhalder
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It comprises the whole tower of next-to-leading-order contributions to the cross section, which scale like $$ {\\alpha}_{\\textrm{s}}^3 $$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:msubsup> <mml:mi>α</mml:mi> <mml:mi>s</mml:mi> <mml:mn>3</mml:mn> </mml:msubsup> </mml:math> α 4 , $$ {\\alpha}_{\\textrm{s}}^2 $$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:msubsup> <mml:mi>α</mml:mi> <mml:mi>s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> α 5 , α s α 6 , and α 7 in the strong and electroweak couplings α s and α . We present a detailed survey of numerical results confirming the occurrence of large pure electroweak corrections of the order of ~ −12% for integrated cross sections and even larger corrections in high-energy tails of distributions. 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引用次数: 0
摘要
摘要本文提出了在蒙特卡洛积分器B onsay中实现的大型强子对撞机强、电弱相互作用对w -玻色子散射的次一级修正的新计算。计算包括W玻色子的轻子衰变。在强耦合和电弱耦合α s和α中,它由整个次领先级贡献塔组成,其尺度为$$ {\alpha}_{\textrm{s}}^3 $$ α s 3 α 4, $$ {\alpha}_{\textrm{s}}^2 $$ α s 2 α 5, α s α 6和α 7。我们给出了详细的数值结果,证实了−12量级的大纯电弱修正的存在% for integrated cross sections and even larger corrections in high-energy tails of distributions. The electroweak corrections account for the major part of the complete next-to-leading-order correction, which amounts to 15–20% in size, depending on the details of the event selection chosen for analysing vector-boson-scattering. Moreover, we compare the full next-to-leading-order corrections to approximate results based on the neglect of contributions that are not enhanced by the vector-boson scattering kinematics (VBS approximation) and on resonance expansions for the W-boson decays (double-pole approximation) ; the quality of this approximation is good within ≲ 1 . 5% for integrated cross sections and the dominating parts of the differential distributions. Finally, for the leading-order predictions, we construct different versions of effective vector-boson approximations , which are based on cross-section contributions that are enhanced by collinear emission of W bosons off the initial-state (anti)quarks; in line with previous findings in the literature, it turns out that the approximative quality is rather limited for applications at the LHC.
Like-sign W-boson scattering at the LHC — approximations and full next-to-leading-order predictions
A bstract We present a new calculation of next-to-leading-order corrections of the strong and electroweak interactions to like-sign W-boson scattering at the Large Hadron Collider, implemented in the Monte Carlo integrator B onsay . The calculation includes leptonic decays of the W bosons. It comprises the whole tower of next-to-leading-order contributions to the cross section, which scale like $$ {\alpha}_{\textrm{s}}^3 $$ αs3 α 4 , $$ {\alpha}_{\textrm{s}}^2 $$ αs2 α 5 , α s α 6 , and α 7 in the strong and electroweak couplings α s and α . We present a detailed survey of numerical results confirming the occurrence of large pure electroweak corrections of the order of ~ −12% for integrated cross sections and even larger corrections in high-energy tails of distributions. The electroweak corrections account for the major part of the complete next-to-leading-order correction, which amounts to 15–20% in size, depending on the details of the event selection chosen for analysing vector-boson-scattering. Moreover, we compare the full next-to-leading-order corrections to approximate results based on the neglect of contributions that are not enhanced by the vector-boson scattering kinematics (VBS approximation) and on resonance expansions for the W-boson decays (double-pole approximation) ; the quality of this approximation is good within ≲ 1 . 5% for integrated cross sections and the dominating parts of the differential distributions. Finally, for the leading-order predictions, we construct different versions of effective vector-boson approximations , which are based on cross-section contributions that are enhanced by collinear emission of W bosons off the initial-state (anti)quarks; in line with previous findings in the literature, it turns out that the approximative quality is rather limited for applications at the LHC.
期刊介绍:
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