The pp ? W(? l?) + ? process at next-to-next-to-leading order

نویسندگان

چکیده

We present details of the calculation $pp\to W(\to l\nu) \gamma$ process at next-to-next-to-leading order in QCD, calculated using jettiness slicing method. The is based entirely on analytic amplitudes. Because radiation zero, NLO QCD contribution from $gq$ channel as important Born $q\bar{q}$ process, disrupting normal counting leading and sub-leading contributions. also assess importance electroweak (EW) corrections, including EW corrections to both six-parton $0\to \bar{u} d \nu e^+\gamma g$ five-parton e^+ \gamma$. Previous experimental results have been shown agree with theoretical predictions, taking into account large errors. With advent run II data LHC, statistical errors will decrease, be competitive error predictions for first time. numerical $\sqrt{s}=7$ 13 TeV. Analytic one-loop amplitude tree-level seven-parton are presented appendices.

برای دانلود باید عضویت طلایی داشته باشید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Soft and virtual corrections to pp → H + X at next - to - next - to - leading order

The contributions of virtual corrections and soft gluon emission to the inclusive Higgs boson production cross section pp → H +X are computed at next-to-next-to-leading order in the heavy top quark limit. We show that this part of the total cross section is well behaved in the sense of perturbative convergence, with the NNLO corrections amounting to an enhancement of the NLO cross section by ∼ ...

متن کامل

W+W−+ dijet to next-to-leading order in QCD

I present the calculation of the production of a W-boson pair in association with two jets at the Tevatron and LHC, performed to next-to-leading order in QCD. This is an important background in Higgs boson production, whether it occurs through gluon fusion or weak boson fusion. In this calculation, the W-bosons decay leptonically and all spin correlations are included. Although we find that the...

متن کامل

Charm Quark Contribution to K L → μ + μ − at Next - to - Next - to - Leading Order

We calculate the charm quark contribution to the decay KL → μ μ in next-to-next-to-leading order of QCD. This new contribution reduces the theoretical uncertainty in the relevant parameter Pc from ±22% down to±7%, corresponding to scale uncertainties of±3% and ±6% in the short-distance part of the branching ratio and the determination of the Wolfenstein parameter ρ̄ from KL → μ μ. The error in P...

متن کامل

BFKL at next-to-leading order

This is a summary of the contributions on the next-to-leading order corrections to the BFKL equation which were presented to the ‘Small-x and Diffraction’ working group at the 1998 Durham Workshop on HERA Physics. The original BFKL equation [1] allowed the computation of elastic scattering amplitudes in the Regge limit to leading logarithmic (LO) accuracy, i.e. all terms ∼ (αs ln s)n are summed...

متن کامل

Next-to-leading-order QCD corrections to W+W-bb production at hadron colliders.

Top-antitop quark pairs belong to the most abundantly produced and precisely measurable heavy-particle signatures at hadron colliders and allow for crucial tests of the standard model and new physics searches. Here we report on the calculation of the next-to-leading order (NLO) QCD corrections to hadronic W(+)W(-)bb production, which provides a complete NLO description of the production of top-...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

ژورنال

عنوان ژورنال: Journal of High Energy Physics

سال: 2021

ISSN: ['1127-2236', '1126-6708', '1029-8479']

DOI: https://doi.org/10.1007/jhep07(2021)079