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A sequential fourth generation is still viable, but the t' and b' quarks are constrained to be not too far apart in mass. The t'{\to}bW and b'{\to}tW decay channels are still being pursued at the Tevatron, which would soon be surpassed by…

High Energy Physics - Phenomenology · Physics 2011-08-09 Yuan Chao , Kai-Feng Chen , Shing-Kuo Chen , Wei-Shu Hou , Bo-Yan Huang , Yeong-Jyi Lei

We compute the decay rate of the Standard Model Higgs boson to bottom quarks to order $\alpha\alpha_s$. We apply the optical theorem and calculate the imaginary part of three-loop corrections to the Higgs boson propagator using asymptotic…

High Energy Physics - Phenomenology · Physics 2015-11-11 Luminita Mihaila , Barbara Schmidt , Matthias Steinhauser

We propose a direct method to calculate the decay width of a hadron decaying to two photons, which is conventionally obtained by an extrapolation for various off-shell form factors. The new method provides an simple way to examine the…

High Energy Physics - Lattice · Physics 2022-09-21 Yu Meng

We study the radiative $B \to K \eta^{(\prime)} \gamma$ decays, which are important to investigate CP violation, and are also relevant to assess the role of the exclusive modes induced by the $b \to s \gamma$ transition to saturate the…

High Energy Physics - Phenomenology · Physics 2015-06-04 Pietro Biancofiore , Pietro Colangelo , Fulvia De Fazio

Radiative QCD corrections significantly influence the theoretical predictions for the decay rates of the $Z$ and the Higgs boson. The status of the QCD calculations to the hadronic $Z$ width is reviewed. The role of mass corrections from…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. G. Chetyrkin , J. H. Kühn , A. Kwiatkowski

In this paper, we calculate the decay widths and branching fractions for the decays $Z \to H+ \gamma$ up to ${\cal O}(\alpha_{s} v^2)$ accuracy within the framework of nonrelativistic QCD, where $H$ stands for the $S$-wave quarkonium…

High Energy Physics - Phenomenology · Physics 2023-12-15 Guang-Yu Wang , Xu-Chang Zheng , Xing-Gang Wu , Guang-Zhi Xu

The Higgs boson decay into bottom quarks is the dominant decay channel contributing to its total decay width, which can be used to measure the bottom quark Yukawa coupling and mass. This decay width has been computed up to…

High Energy Physics - Phenomenology · Physics 2025-03-25 Jian Wang , Xing Wang , Yefan Wang

The main challenge faced by Higgsless models of electroweak symmetry breaking is to reconcile the experimental constraints imposed by the precision electroweak data and the top quark phenomenology with the unitarity constraints imposed by…

High Energy Physics - Phenomenology · Physics 2009-11-11 Roshan Foadi , Carl Schmidt

We report the first analytic calculation of the Higgs boson decay width to gluons up to next-to-leading order in quantum chromodynamics including full dependence on the bottom and charm quark masses. The interference between top- and…

High Energy Physics - Phenomenology · Physics 2025-09-16 Jian Wang , Yefan Wang

The recent Tevatron result on the top quark forward-backward asymmetry, which deviates from its standard model prediction by 3.4$\sigma$, has prompted many authors to build new models to account for this anomaly. Among the various…

High Energy Physics - Phenomenology · Physics 2015-05-27 Chuan-Hung Chen , Sandy S. C. Law , Run-Hui Li

Observing a heavy charged Higgs boson produced in the near future at the Tevatron or at the LHC would be instant evidence of physics beyond the Standard Model. Whether such a Higgs boson would be supersymmetric or not it could only be…

High Energy Physics - Phenomenology · Physics 2010-01-28 J. A. Coarasa , David Garcia , Jaume Guasch , Ricardo A. Jimenez , Joan Sola

In the light of the top quark discovered very recently by CDF, we investigate the possibility of narrowing down the allowed top quark masses by combining for the first time only two strongest constraints present in the no-scale $SU(5)\times…

High Energy Physics - Phenomenology · Physics 2015-06-25 Gye T. Park

The Higgs boson decay to a massive bottom quark pair provides the dominant contribution to the Higgs boson width. We present an exact result for such a decay induced by the bottom quark Yukawa coupling with next-to-next-to-leading order…

High Energy Physics - Phenomenology · Physics 2024-03-13 Jian Wang , Yefan Wang , Da-Jiang Zhang

We calculate the spectrum and wave functions (WFs) of various states of bottomonium mesons ($b\overline{b}$) using a non-relativistic quark potential model (NRQPM). The calculated WFs are used to compute the radiative widths of various…

High Energy Physics - Phenomenology · Physics 2023-09-28 Ishrat Asghar , Nosheen Akbar

We present a detailed study of the exclusive radiative decays $Z\to\eta^{(\prime)}\gamma$ employing the QCD factorization approach. We derive a factorization formula for the decay amplitudes valid at leading power in an expansion in…

High Energy Physics - Phenomenology · Physics 2016-03-23 Stefan Alte , Matthias Koenig , Matthias Neubert

We present a comparative study of various approaches for modelling of the $e^+ \nu_e \mu^- \bar{\nu}_\mu b\bar{b} \gamma$ final state in $t\bar{t}\gamma$ production at the LHC. Working at the NLO in QCD we compare the fully realistic…

High Energy Physics - Phenomenology · Physics 2020-03-31 G. Bevilacqua , H. B. Hartanto , M. Kraus , T. Weber , M. Worek

We give a more complete calculation of $b \to s\gamma $ decay, including leading log QCD corrections from $m_{top}$ to $M_W$ in addition to corrections from $M_{W}$ to $m_b$. We have included the full set of dimension-6 operators and…

High Energy Physics - Phenomenology · Physics 2009-10-28 Chong-Shong Gao , Jing-Liang Hu , Cai-Dian Lu , Zhao-Ming Qiu

A generalisation of the narrow-width approximation (NWA) is formulated which allows for a consistent treatment of interference effects between nearly mass-degenerate particles in the factorisation of a more complicated process into…

High Energy Physics - Phenomenology · Physics 2014-11-19 Elina Fuchs , Silja Thewes , Georg Weiglein

We evaluate the effect of a virtual top quark on the coefficient of $\alpha_{s}^{2}$ in the decay rates $\Gamma(Z \rightarrow {\rm hadrons})$ and $\Gamma(Z \rightarrow b\overline{b} )$. We treat the dependence on the top quark mass exactly…

High Energy Physics - Phenomenology · Physics 2009-10-28 Davison E. Soper , Levan R. Surguladze

The lowest-order expression for the partial $W$ width to $e \nu ,~\Gamma (W \to e \nu) = G_\mu M_W^3 /(6 \pi \sqrt{2})$, has no oblique radiative corrections from new physics if the measured $W$ mass is used. Here $G_\mu = (1.16639 \pm…

High Energy Physics - Phenomenology · Physics 2009-10-22 Jonathan L. Rosner , Mihir P. Worah , Tatsu Takeuchi
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