English
Related papers

Related papers: Width Difference in the $B_s-\bar{B_s}$ System

200 papers

We compute the Darwin operator contribution ($1/m_b^3$ correction) to the width of the inclusive non-leptonic decay of a $B$ meson ($B^+$, $B_d$ or $B_s$), stemming from the quark flavour-changing transition $b \to q_1 \bar q_2 q_3$, where…

High Energy Physics - Phenomenology · Physics 2021-01-25 Alexander Lenz , Maria Laura Piscopo , Aleksey V. Rusov

Branching fractions of B^0s decays into specific CP eigenstates are presented, and these and other results are combined in world averages to evaluate implications on the width difference between mass or CP eigenstates, \Delta\Gamma_s. New…

High Energy Physics - Experiment · Physics 2008-11-26 R. Van Kooten

Using an operator product expansion (OPE) approach an updated Standard Model prediction of the $B_c$ lifetime is presented. The computation in three different mass schemes for the heavy quarks leads to three different values consistent with…

High Energy Physics - Phenomenology · Physics 2021-11-16 Jason Aebischer , Benjamín Grinstein

Muon electron scattering experiments such as the proposed MUonE experiment, offer an opportunity for an improved measurement of the Leading Order hadronic running of $\alpha$, denoted $\Delta \alpha_{\rm{had}}$. Such a measurement could be…

High Energy Physics - Phenomenology · Physics 2019-09-04 Ulrich Schubert , Ciaran Williams

Studying our semirelativistic potential model and the numerical results, which succeeds in predicting and reproducing recently discovered higher resonances of $D$, $D_s$, $B$, and $B_s$, we find a simple expression for the mass gap between…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takayuki Matsuki , Toshiyuki Morii , Kazutaka Sudoh

We present a determination of the b-quark mass accurate through O(\alpha_s^2) in perturbation theory and including partial contributions at O(\alpha_s^3). Nonperturbative input comes from the calculation of the Upsilon and B_s energies in…

High Energy Physics - Lattice · Physics 2013-04-29 A. J. Lee , C. J. Monahan , R. R. Horgan , C. T. H. Davies , R. J. Dowdall , J. Koponen

Using a specific scheme of the QCD sum rules for heavy quarkonium in the leading approximation over the inverse heavy quark mass, one gets the estimate of the difference between the masses of the heavy meson and heavy quark $\bar \Lambda =…

High Energy Physics - Phenomenology · Physics 2008-02-03 V. V. Kiselev

The QCD corrections for the box diagrams are revisited for the case of a heavy top quark with $\mt = 174 \GeV$. We resolve first a longstanding discrepancy between two methods of calculation by showing that they give the same results when…

High Energy Physics - Phenomenology · Physics 2019-08-17 Amitava Datta , E. A. Paschos , J. -M. Schwarz , M. N. Sinha Roy

We compute the electromagnetic mass differences of mesons containing a single heavy quark in terms of measurable data using QCD-based arguments in heavy-quark effective theory. We derive an unsubtracted dispersion relation that shows that…

High Energy Physics - Phenomenology · Physics 2016-09-01 Markus A. Luty , Raman Sundrum

We study the improvement of staggered fermions using hypercubically smeared (HYP) links. We calculate the strange quark mass and the kaon B-parameter, $B_K$, in quenched QCD on a $16^3 \times 64$ lattice at $\beta=6.0$. We find…

High Energy Physics - Lattice · Physics 2014-11-17 Weonjong Lee , Tanmoy Bhattacharya , George T. Fleming , Rajan Gupta , Gregory Kilcup , Stephen R. Sharpe

The relation between the on-shell and $\bar{\rm MS}$ mass can be expressed through scalar and vector part of the quark propagator. In principle these two-point functions have to be evaluated on-shell which is a non-trivial task at…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. G. Chetyrkin , M. Steinhauser

We present measurements of the lifetimes and polarization amplitudes for B_s --> J/psi phi and B_d --> J/psi K*0 decays. Lifetimes of the heavy (H) and light (L) mass eigenstates in the B_s system are separately measured for the first time…

High Energy Physics - Experiment · Physics 2010-05-12 D. Acosta

$B_d$ and $B_s$ meson systems play a fundamental role to test and improve our understanding of Standard Model flavor dynamics. The mixing parameters $\Delta m_{d,s}$ represent important constraints in the unitarity triangle analysis. Their…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Tarantino

We measure the mass difference, \Delta m_0, between the D*(2010)+ and the D0 and the natural line width, \Gamma, of the transition D*(2010)+ -> D0 pi+. The data were recorded with the BABAR detector at center-of-mass energies at and near…

High Energy Physics - Experiment · Physics 2013-09-17 The BaBar Collaboration

We use QCD sum rule approach to calculate the masses of the ground-state Lambda_Q and Sigma_Q^(*) baryons. Contributions of the operators up to dimension six are included in operator product expansion. The resulting heavy baryonic masses…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jian-Rong Zhang , Ming-Qiu Huang

Using a sample of 471 million BBbar events collected with the BaBar detector, we study the sum of seven exclusive final states B->X_s(d) gamma, where X_s(d) is a strange (non-strange) hadronic system with a mass of up to 2.0GeV/c^2. After…

High Energy Physics - Experiment · Physics 2014-11-21 The BABAR Collaboration , P. del Amo Sanchez

We review the theoretical status of the lifetime ratios $\tau_{B^+} / \tau_{B_d}$ and $\tau_{B_s} / \tau_{B_d}$ and of the mixing quantities $\Delta M_s$, $\Delta \Gamma_s$ and $\phi_s$. We show that the ratio $\Delta \Gamma_s / \Delta M_s$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alexander Lenz

We consider penguin contributions to the lifetime splitting between the $B_s$ and the $B_d$ meson. In the Standard Model the penguin effects are found to be opposite in sign, but of similar magnitude as the contributions of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. -Y. Keum

In the large $N_c$ limit, the nonleptonic width of the B meson is determined by the lepton mass spectrum in semileptonic B decay and the hadron mass spectrum in $\tau$ decay. This result can be compared with the nonleptonic width computed…

High Energy Physics - Phenomenology · Physics 2009-06-12 Zoltan Ligeti , Aneesh V. Manohar

We present a lattice calculation of the B meson B-parameter B_B using the NRQCD action. The heavy quark mass dependence is explicitly studied over a mass range between m_b and 4m_b with the $O(1/m_Q)$ and $O(1/m_Q^2)$ actions. We find that…

High Energy Physics - Lattice · Physics 2009-10-31 S. Hashimoto , K-I. Ishikawa , H. Matsufuru , T. Onogi , N. Yamada