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Related papers: QCD corrections to neutralino annihilation

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We compute the QCD next-to-leading order matching conditions of the (chromo)-magnetic operators relevant for B\to X_s \gamma in supersymmetric models with minimal flavour violation. The calculation is performed under the assumption that the…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Ciuchini , G. Degrassi , P. Gambino , G. F. Giudice

The next-to-leading order (NLO) quantum chromodynamics (QCD) corrections for $\chi_{cJ}(^3P_J^{[1]},^3S_1^{[8]})$, the P-wave charmoniums inclusive production at $B$ factories are calculated utilizing the non-relativistic QCD (NRQCD)…

High Energy Physics - Phenomenology · Physics 2015-06-03 Long-Bin Chen , Jun Jiang , Cong-Feng Qiao

QED radiative corrections to the cross-section of muon-antimuon annihilation into Higgs boson and photon are calculated within the 1-loop approximation. We write down the expression for cross-section in the form of Drell-Yan process, taking…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. B. Arbuzov , E. A. Kuraev , F. F. Tikhonin , B. G. Shaikhatdenov

In the framework of nonrelativistic QCD (NRQCD) factorization, we compute both the polarized and the unpolarized decay widths for the processes $\eta_b(\chi_{bJ})\to J/\psi J/\psi$, accurate up to next-to-next-to-leading-order (NNLO) in…

High Energy Physics - Phenomenology · Physics 2023-10-13 Yu-Dong Zhang , Xiao-Wei Bai , Feng Feng , Wen-Long Sang , Ming-Zhen Zhou

We compute the next to leading QCD corrections to weak four fermion interactions introducing a scheme that does not require an explicit definition of $\gamma_5$ in $d$ dimensions. This scheme reduces greatly the difficulties in calculating…

High Energy Physics - Phenomenology · Physics 2016-09-01 G. Curci , G. Ricciardi

We briefly present the status of QCD corrections to the inclusive total cross section for the production of a Higgs boson in association with a top-quark pair within the Standard Model at hadron colliders.

High Energy Physics - Phenomenology · Physics 2009-11-07 S. Dawson , L. Orr , L. Reina , D. Wackeroth

We calculate the radiative corrections to helicity amplitudes for chargino production in electron-positron collisions. We include all weak self-energy, triangle, and box diagrams, and find that the three are important and should be…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marco A. Diaz , Douglas A. Ross

We compute the next-to-leading order QCD corrections to the spin-independent and spin-dependent cross-sections for the production of a single-hadron accompanied by an opposite jet in hadronic collisions. This process is being studied…

High Energy Physics - Phenomenology · Physics 2009-07-30 Daniel de Florian

The calculation of exclusive cross sections at next-to-next-to-leading order (NNLO) in QCD requires an analytic understanding of the infrared singular structure with up to two unresolved partons. This has so far only been achieved for…

High Energy Physics - Phenomenology · Physics 2024-08-22 Thomas Gehrmann , Markus Löchner

Electroweak, QCD, and QED radiative corrections to the nucleon low-energy coupling constants $g_V$ and $g_A$ are enhanced by large perturbative logarithms between the electroweak and hadronic scale, as well as between the hadronic scale and…

High Energy Physics - Phenomenology · Physics 2026-04-10 Oleksandr Tomalak , Yi-Bo Yang

We present a summary of the first calculation of NLO QCD corrections to WZjj production with leptonic decays at the LHC. Our results show that the next-to-leading order corrections reduce significantly the scale uncertainties.

High Energy Physics - Phenomenology · Physics 2013-10-17 Francisco Campanario , Matthias Kerner , Le Duc Ninh , Dieter Zeppenfeld

We discuss the production of top--anti-top quark pairs in association with a hard jet at the Tevatron and at the LHC and we report on the calculation of the next-to-leading order QCD corrections to this process. Numerical results for the…

High Energy Physics - Phenomenology · Physics 2009-04-14 Stefan Dittmaier , Peter Uwer , Stefan Weinzierl

Top quark production in electron-positron annihilation is one of the benchmark reactions at a future linear collider. Both electroweak and QCD corrections are large, amounting to 10% or even more in specific kinematic regions. In this note…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Kuehn , T. Hahn , R. Harlander

We discuss the supersymmetric O(alpha_s) QCD corrections to e+ e- -> squark_i + antisquark_j (i,j = 1,2) and to squark_i -> q' + chargino_j, q + neutralino_k (i,j = 1,2; k = 1...4) within the Minimal Supersymmetric Standard Model. In…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Bartl , H. Eberl , S. Kraml , W. Majerotto , W. Porod

Radiative corrections due to initial state radiation in electron-positron annihilation are calculated within the QED structure function approach. Results are shown in the next-to-leading logarithmic approximation up to $O(\alpha^4 L^3)$…

High Energy Physics - Phenomenology · Physics 2024-12-12 A. B. Arbuzov , U. E. Voznaya

We calculated the complete next-to-leading order(NLO) QCD corrections to the $t\bar t b \bar b$ production process at a $\gamma \gamma$ collider in the standard model(SM). The calculation of the one-loop QCD correction includes the…

High Energy Physics - Phenomenology · Physics 2008-04-15 Guo Lei , Ma Wen-Gan , Han Liang , Zhang Ren-You , Jiang Yi

We present the analytic total cross section of top quark pair production in electron-positron annihilation at next-to-next-to-leading order (NNLO) in Quantum Chromodynamics (QCD). By utilizing the optical theorem, the NNLO corrections are…

High Energy Physics - Phenomenology · Physics 2024-09-10 Long-Bin Chen , Jian Wang , Yefan Wang

We compute for the first time QCD corrections to the rare decays B -> X_{d,s} nu nubar, B_{d,s} -> l^+ l^-, K -> pi nu nubar and K_L -> mu^+ mu^-, where l=e or mu, in the context of a supersymmetric extension of the Standard Model (SM) with…

High Energy Physics - Phenomenology · Physics 2011-03-23 C. Bobeth , A. J. Buras , F. Krüger , J. Urban

We investigate the QCD effects in the associated production of the chargino and the neutralino, $\tilde\chi^\pm_{1}$ and $\tilde\chi^0_{2}$, in the Minimal Supersymmetric Standard Model (MSSM) at both the Fermilab Tevatron and the CERN…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chong Sheng Li , Zhao Li , Robert J. Oakes , Li Lin Yang

We compute the two-loop QCD corrections to $q g \to H q$ and $q \bar{q} \to H g$ amplitudes mediated by loops of nearly massless quarks. These amplitudes provide the last missing ingredient required to compute the NLO QCD corrections to the…

High Energy Physics - Phenomenology · Physics 2017-03-22 Kirill Melnikov , Lorenzo Tancredi , Christopher Wever