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相关论文: Full one-loop electroweak radiative corrections to…

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We study the 1-loop corrections to the charged Higgs production both in the Minimal Supersymmetric Standard Model (MSSM) and in a more general type II two-Higgs-doublet model (THDM-II). We consider the full set of corrections (including…

高能物理 - 唯象学 · 物理学 2007-05-23 A. Arhrib , G. Moultaka

We calculate the full one-loop electroweak radiative corrections to the cross section of single W-boson inclusive hadroproduction at finite transverse momentum (p_T). This includes the O(alpha) corrections to W+j production, the O(alpha_s)…

高能物理 - 唯象学 · 物理学 2008-11-26 W. Hollik , T. Kasprzik , B. A. Kniehl

Using the automatic system GRACE-LOOP, the full $O(\alpha)$ electroweak corrections has been calculated for the process $e^+e^- \to W^+\mu \bar{\nu}_{\mu}$. The total correction to the cross section is found to be typically -6.4% at…

高能物理 - 唯象学 · 物理学 2007-05-23 J. Fujimoto , T. Ishikawa , Y. Kurihara , Y. Shimizu , K. Kato , N. Nakazawa , T. Kaneko

We study the impact of the two-loop electroweak corrections on the production of a Higgs boson via gluon-fusion in proton-proton collisions at LHC energies. We discuss the prescritpion to include the corrections to the hard scattering…

高能物理 - 唯象学 · 物理学 2007-05-23 U. Aglietti , R. Bonciani , G. Degrassi , A. Vicini

Full O(alpha) electroweak corrections for gamma-gamma-> W+W- are calculated including virtual corrections, soft and hard real photon and Z-boson emission. The corrections are quite large ranging from -2.5% at 500 GeV to -18% at 2 TeV,…

高能物理 - 唯象学 · 物理学 2009-10-30 G. Jikia

We review recent theoretical progress in the computation of radiative corrections beyond one loop within the standard model of electroweak interactions, both in the gauge and Higgs sectors. In the gauge sector, we discuss universal…

高能物理 - 唯象学 · 物理学 2007-05-23 Bernd A. Kniehl

We compute analytically the complete electroweak two-loop corrections to the $B^0-{\bar B}^0$ mixing. These corrections fix the normalization of the electroweak coupling employed in the extraction of $|V_{td}|$ and reduce the theoretical…

高能物理 - 唯象学 · 物理学 2009-10-31 P. Gambino , A. Kwiatkowski , N. Pott

We compute the electroweak corrections due to the light fermions to the production cross section $\sigma(g g \to H)$ and to the partial decay widths $\Gamma (H \to \gamma \gamma)$ and $\Gamma (H \to g g)$. We present analytic results for…

高能物理 - 唯象学 · 物理学 2011-09-29 U. Aglietti , R. Bonciani , G. Degrassi , A. Vicini

We describe the impact of the full one-loop electroweak terms of O(alpha_s alpha_EM^3) entering the electron-positron into three-jet cross-section from sqrt(s)=M_Z to TeV scale energies. We include both factorisable and non-factorisable…

高能物理 - 唯象学 · 物理学 2022-03-02 C. M. Carloni Calame , S. Moretti , F. Piccinini , D. A. Ross

QCD corrections to the electroweak one-loop result for the partial width $\Gamma(H\rightarrow b\bar{b})$ are studied. For the decay channel into bottom quarks the rate is affected by a virtual top quark through electroweak interactions. The…

高能物理 - 唯象学 · 物理学 2009-10-28 A. Kwiatkowski , M. Steinhauser

The prospective Higgs factories, exemplified by ILC, FCC-ee and CEPC, plan to conduct the precision Higgs measurements at the $e^+e^-$ center-of-mass energy around 250 GeV. The cross sections for the dominant Higgs production channel, the…

高能物理 - 唯象学 · 物理学 2017-09-13 Qing-Feng Sun , Feng Feng , Yu Jia , Wen-Long Sang

We present the first complete calculation of the one-loop electroweak effect in the process of semi-inclusive bottom-Higgs production at LHC in the MSSM. The size of the electroweak contribution depends on the choice of the final produced…

高能物理 - 唯象学 · 物理学 2010-12-23 M. Beccaria , G. O. Dovier , G. Macorini , E. Mirabella , L. Panizzi , F. M. Renard , C. Verzegnassi

The electroweak O(alpha) contribution to the resonant single W production in a general 4-fermion process is discussed with particular emphasis on a gauge invariant decomposition into a QED-like and weak part. The cross section in the…

高能物理 - 唯象学 · 物理学 2008-11-26 Doreen Wackeroth , Wolfgang Hollik

The Higgs-boson production in association with a W-boson pair at $e^+e^-$ linear colliders is one of the important processes in probing the coupling between Higgs-boson and vector gauge bosons and discovering the signature of new physics.…

高能物理 - 唯象学 · 物理学 2009-11-18 Song Mao , Ma Wen-Gan , Zhang Ren-You , Guo Lei , Wang Shao-Ming

The complete electroweak O(alpha) corrections are calculated for the charged-current four-fermion production processes e+e- --> nu_tau tau+ mu- anti-nu_mu, u anti-d mu- anti-nu_mu, and u anti-d s anti-c. The calculation is performed using…

高能物理 - 唯象学 · 物理学 2011-08-30 A. Denner , S. Dittmaier , M. Roth , L. H. Wieders

We calculate the $O(\alpha_{ew}m_{t(b)}^{2}/m_{W}^{2})$ and $O(\alpha_{ew} m_{t(b)}^4/m_W^4)$ supersymmetric electroweak corrections to the cross section for the charged Higgs boson production in association with a top quark at the Tevatron…

高能物理 - 唯象学 · 物理学 2009-10-31 Li Gang Jin , Chong Sheng Li , Robert J. Oakes , Shou Hua Zhu

The selfcoupling of the Higgs field grows with the mass of the Higgs particle and induces potentially large radiative corrections in the electroweak model. The technical aspects of performing multiloop calculations in the massive case are…

高能物理 - 唯象学 · 物理学 2014-11-17 Adrian Ghinculov

We study the complete ${\cal O}(\alpha_{ew})$ electroweak (EW) corrections to the production of three $Z^0$-bosons in the the framework of the standard model(SM) at the ILC. The leading order and the EW next-to-leading order corrected cross…

高能物理 - 唯象学 · 物理学 2008-11-26 Su Ji-Juan , Ma Wen-Gan , Zhang Ren-You , Wang Shao-Ming , Guo Lei

Full one-loop electroweak corrections to the on-shell decay $H^+ \to W^+A^0$ are computed in the framework of models with two Higgs doublets (THDM). Such a decay may be dominant for $H^{\pm}$ over a wide range of parameter space relevant at…

高能物理 - 唯象学 · 物理学 2008-11-26 A. G. Akeroyd , A. Arhrib , E. Naimi

We present an analytical calculation of the leading three-loop radiative correction to the S-parameter in the Standard Model in the large Higgs mass limit. Numerically, S^(3) = 1.1105*g^4/(1024 pi^3)*m_H^4/M_W^4. When combined with the…

高能物理 - 唯象学 · 物理学 2010-04-05 R. Boughezal , J. B. Tausk , J. J. van der Bij