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Related papers: $B^0-\bar{B}^0$ Mixing at Next-to-Leading Order

200 papers

We re-examine the theoretical uncertainty in the Standard Model expression for $B^0$-$\bar{B}^0$ mixing. We focus on lattice calculations of the ratio $\xi$, needed to relate the oscillation frequency of $B^0_s$-$\bar{B}^0_s$ mixing to the…

High Energy Physics - Phenomenology · Physics 2011-03-23 Andreas S. Kronfeld , Sinead M. Ryan

We briefly sketch the calculation of the effective low-energy $|\Delta S|=2$-hamiltonian in the next-to-leading order of renormalization group improved perturbation theory. The result for the coefficient $\eta_3^\star$ is discussed. Further…

High Energy Physics - Phenomenology · Physics 2007-05-23 Stefan Herrlich

We consider HQET including the first order correction in 1/m. A strategy for the computation of the b-quark mass is discussed. Only two quantities Phi_1/2 have to be considered in order to match QCD and HQET, since the spin-dependent…

High Energy Physics - Lattice · Physics 2007-05-23 Michele Della Morte , Nicolas Garron , Rainer Sommer , Mauro Papinutto

We calculate the B-parameters for operators arising in theories of new physics beyond the standard model (BSM) using HYP-smeared improved staggered fermions on the MILC asqtad lattices with N_f = 2+1 flavors. We use three different lattice…

B decay sum rules relate exclusive B semileptonic decay matrix elements to forward B-meson matrix elements of operators in HQET. At leading order the operators that occur are the b-quark kinetic energy $\lambda_1$ and chromomagnetic energy…

High Energy Physics - Phenomenology · Physics 2009-10-30 Mark B. Wise

We present a calculation of the QCD correction factors $\eta_{2B}$ and $\eta_{2K}$ up to Next-to-Leading Order within the MSSM. We took into account the region of low $\tan\beta$ for the Higgs- and chargino sector while neglecting the…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. Krauss , G. Soff

We present analytical next-to-leading order results for the correlator of baryonic currents at the three-loop level with one finite mass quark. We obtain the massless and the HQET limits of the correlator as particular cases from the…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Groote , J. G. Körner , A. A. Pivovarov

We comment on two recent calculations of the second order perturbative corrections in the heavy flavor semileptonic transitions within the Brodsky-Lepage-Mackenzie approach. It is pointed out that the results do not show significant…

High Energy Physics - Phenomenology · Physics 2010-11-01 M. Shifman , N. G. Uraltsev

In the model III 2HDM there are new CP violating phases which would affect the $B_{d,s}^0 - \bar{B}_{d,s}^0$ mixing. In this paper, we calculate the new physics contributions to the neutral B meson mass splitting $\Delta M_{B_q}$ (q=d, s)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chao-Shang Huang , Jian-Tao Li

In this study, we compute the radiative corrections to the $\Lambda_b \to p$ transition form factors at next-to-leading logarithmic accuracy, employing the framework of QCD light-cone sum rules with the light-cone distribution amplitudes of…

High Energy Physics - Phenomenology · Physics 2026-02-23 Jiang-Lin Zhou , Yong-Kang Huang

We present the complete next-to-leading order short-distance QCD corrections to the effective \dstwo -hamiltonian in the Standard Model. The calculation of the coefficient $\eta_3$ is described in great detail. It involves the two-loop…

High Energy Physics - Phenomenology · Physics 2009-10-28 Stefan Herrlich , Ulrich Nierste

We compute the next-to-leading order perturbative QCD corrections to the correlators of nucleon interpolating currents in relativistic nuclear matter. The main new result is the calculation of the O(alpha_s) perturbative corrections to the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Groote , J. G. Körner , A. A. Pivovarov

We compute the \alpha_s^2\beta_0 part of the two-loop QCD corrections to the charged lepton spectrum in b \to c \ell \bar\nu_\ell decays and find them to be about 50\% of the first order corrections at all lepton energies, except those…

High Energy Physics - Phenomenology · Physics 2008-11-26 Martin Gremm , Iain Stewart

We consider the effects of a non-vanishing strange-quark mass in the determination of the full basis of dimension six matrix elements for $B_{s}$ mixing, in particular we get for the ratio of the $V-A$ Bag parameter in the $B_s$ and $B_d$…

High Energy Physics - Phenomenology · Physics 2019-05-10 Daniel King , Alexander Lenz , Thomas Rauh

We consider in detail various theoretical uncertainties of the perturbative predictions for the decay width of $H^0\rightarrow b\overline{b}$ process in the region $50\ GeV< M_H\leq 2M_W$. We calculate the order…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. L. Kataev , V. T. Kim

By incorporating the available leading-power results at $\mathcal{O}(\alpha_s)$ and next-to-leading-power corrections at tree level, we improve the precision of the theoretical predictions for $B\to\pi$ form factors to the…

High Energy Physics - Phenomenology · Physics 2025-12-24 Yong-Kang Huang , Dong-Hao Li , Cai-Dian Lü , Bo-Xuan Shi , Hui-Xin Yu

The next-to-leading order (NLO) Standard Model Effective Field Theory (SMEFT) renormalization group equations are needed to account for phenomenologically relevant operator mixing and ensure renormalization scale independence in NLO…

High Energy Physics - Phenomenology · Physics 2026-03-19 Lukas Born , Javier Fuentes-Martín , Anders Eller Thomsen

We present the QCD corrections to the matching conditions of the Delta B =1 magnetic and chromo-magnetic operators in the Standard Model and in two-Higgs doublet models. We use an off-shell matching procedure which allows us to perform the…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Ciuchini , G. Degrassi , P. Gambino , G. F. Giudice

We calculate a class of three-loop Feynman diagrams which contribute to the next-to-next-to-leading logarithmic approximation for the width difference $\Delta\Gamma_{s}$ in the $B_s-\bar{B}_s$ system. The considered diagrams contain a…

High Energy Physics - Phenomenology · Physics 2017-12-15 H. M. Asatrian , Artyom Hovhannisyan , Ulrich Nierste , Arsen Yeghiazaryan

We discuss the renormalisation properties of parity-odd Delta B=2 operators with the heavy quark treated in the static approximation. Via twisted mass QCD (tmQCD), these operators provide the matrix elements relevant for the B0-B0bar mixing…

High Energy Physics - Lattice · Physics 2007-05-23 F. Palombi , M. Papinutto , C. Pena , H. Wittig