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Related papers: NNLO QCD corrections to the B -> X_s gamma matrix …

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We calculate the next-to-next-to-leading order QCD corrections to the leptonic invariant mass ($q^2$) spectrum of semileptonic $b \to c$ inclusive decays, taking into account the mass of the charm quark and the charged lepton in the final…

High Energy Physics - Phenomenology · Physics 2024-03-08 Matteo Fael , Florian Herren

Many contributions to the decay rate of the inclusive radiative $\bar{B}\rightarrow X_s \gamma$ transition have been calculated to NNLO in QCD during the past decades. However, there are still a few unknown contributions from multi-parton…

High Energy Physics - Phenomenology · Physics 2026-01-30 Kevin Brune , Tobias Huber , Lars-Thorben Moos

We calculate the QCD corrected effective Hamiltonian for $B\bbar$--Mixing in heavy quark effective theory including corrections of the order $\Lambda_{QCD} / m_b$. The matrix elements of the subleading operators are estimated using the…

High Energy Physics - Phenomenology · Physics 2009-10-22 Wolfgang Kilian , Thomas Mannel

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

The matrix element of the weak transition {\Lambda}_b\rightarrow{\Lambda}_c can be expressed in terms of six form factors. {\Lambda}_Q(Q = b;c) can be regarded as composed of a heavy quark Q(Q = b;c) and a diquark which is made up of the…

High Energy Physics - Phenomenology · Physics 2016-08-17 L. Zhang , X. -H. Guo , M. -H. Weng

We give a summary about the various contributions which have to be calculated in order to obtain the next-to-leading logarithmic result for the branching ratio $BR(B \to X_s \gamma)$. Combining all these ingredients, which were obtained by…

High Energy Physics - Phenomenology · Physics 2016-11-03 C. Greub , T. Hurth

A theoretical analysis of the partial inclusive B-->X_s gamma decay rate with a cut E_gamma>E_0 on photon energy must deal with short-distance contributions associated with three different mass scales: the hard scale m_b, an intermediate…

High Energy Physics - Phenomenology · Physics 2009-11-11 Thomas Becher , Matthias Neubert

We review the NLL QCD calculations for the branching ratio of B -> X_s gamma in the SM. In particular, we emphasize the problem related to the definition of the charm quark mass which leads to a rather large uncertainty of the NLL…

High Energy Physics - Phenomenology · Physics 2014-11-17 Kay Bieri , Christoph Greub

We calculate the fermionic corrections to the photon-energy spectrum of Bbar -> X_sgamma which arise from the self-interference of the chromomagnetic dipole operator Q_8 at next-to-next-to-leading order by applying naive non-abelianization.…

High Energy Physics - Phenomenology · Physics 2010-12-13 Andrea Ferroglia , Ulrich Haisch

It is shown that the inclusive rate of the rare weak radiative decays $B \to X_s \gamma$ contains a series of nonperturbative corrections, whose `short distance' scale is set by $m_c^{-1}$, rather than by $m_b^{- 1}$. The first correction…

High Energy Physics - Phenomenology · Physics 2016-09-06 M. B. Voloshin

We compute the real part of the 2-loop vertex corrections for charmless hadronic B decays, completing the NNLO calculation of the topological tree amplitudes in QCD factorization. Among the technical aspects we show that the hard-scattering…

High Energy Physics - Phenomenology · Physics 2009-09-28 Guido Bell

We review and update the branching ratios for the $B \to (\rho,\omega) \gamma$ decays, calculated in the QCD factorization approach in the next-to-leading order (NLO) in the strong coupling $\alpha_s$ and to leading power in $\Lambda_{\rm…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ahmed Ali , Alexander Parkhomenko

We compute non-perturbative contributions to b->s l+ l- that are not explicitly suppressed by powers of the b-quark mass. They are proportional to lambda_2 and arise from an interference between the free-quark amplitude and higher order…

High Energy Physics - Phenomenology · Physics 2011-01-27 Jiunn-Wei Chen , Gautam Rupak , Martin J. Savage

We calculate the hadronic tensor for inclusive semileptonic B decay to O(alpha_s). This allows O(alpha_s Lambda_{QCD}/mb) corrections to hadronic invariant mass observables to be directly evaluated with experimentally required cuts on phase…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michael Trott

We compute by QCD sum rules the matrix elements of the relevant four-quark operators appearing in the expression of the $\Lambda_b$ inclusive decay rates at the order $1/m_b^3$. The results suggest that $1/m_b^3$ corrections are not…

High Energy Physics - Phenomenology · Physics 2011-01-27 P. Colangelo , F. De Fazio

The gluino-induced contributions to the decay b-> s gamma are investigated in supersymmetric frameworks with generic sources of flavour violation. It is shown that, when QCD corrections are taken into account, the relevant operator basis of…

High Energy Physics - Phenomenology · Physics 2011-01-05 F. Borzumati , C. Greub , T. Hurth , D. Wyler

Using heavy meson chiral perturbation theory, we consider the light quark-mass and spatial volume dependence of the matrix elements of \Delta B=2 and \Delta C=2 four-quark operators relevant for B^{0}_{(s)}{-}\bar{B}^{0}_{(s)} and…

High Energy Physics - Lattice · Physics 2008-11-26 William Detmold , C. -J. David Lin

We compute perturbative QCD corrections to $B \to D$ form factors at leading power in $\Lambda/m_b$, at large hadronic recoil, from the light-cone sum rules (LCSR) with $B$-meson distribution amplitudes in HQET. QCD factorization for the…

High Energy Physics - Phenomenology · Physics 2017-06-28 Yu-Ming Wang , Yan-Bing Wei , Yue-Long Shen , Cai-Dian Lü

We study the spectra of the bottomonium and B_c states within perturbative QCD up to order alpha_s^4. The O(Lambda_QCD) renormalon cancellation between the static potential and the pole mass is performed in the epsilon-expansion scheme. We…

High Energy Physics - Phenomenology · Physics 2009-06-12 N. Brambilla , Y. Sumino , A. Vairo

We reconsider the prediction of the semileptonic branching ratio of B mesons, using a recent calculation of the radiative corrections with account for finite quark masses in nonleptonic decays and taking into account 1/m_b^2 corrections.…

High Energy Physics - Phenomenology · Physics 2009-10-28 E. Bagan , Patricia Ball , V. M. Braun , P. Gosdzinsky
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