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Related papers: Lifetime Difference of Neutral $B_s$ Mesons and it…

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The lifetime difference ($y_D=\Delta\Gamma_D/2\Gamma_D$) and mass difference ($x_D=\Delta m_D/\Gamma_D$) of neutral $D$ meson have been measured with $y_D=(0.80\pm 0.13)%$ and $x_D=(0.59 \pm 0.20)%$, respectively. Intriguingly, in contrast…

High Energy Physics - Phenomenology · Physics 2011-06-13 Chuan-Hung Chen , C. S. Kim

We update the theory predictions for the mass difference $\dm_s$, the width difference $\dg_s$ and the CP asymmetry in flavour-specific decays, $a_{\rm fs}^{s}$, for the \bbs system. In particular we present a new expression for the element…

High Energy Physics - Phenomenology · Physics 2010-10-27 Alexander Lenz , Ulrich Nierste

The Bs meson is an interesting particle to study because a sizable mixing induced CP violation in the Bs-Bsbar system would be an indication for physics beyond the Standard Model. In this paper we present a measurement of the lifetime…

High Energy Physics - Experiment · Physics 2019-08-13 Thomas Kuhr

We present lattice QCD results for the matrix elements of $R_2$ and other dimension-7, $\Delta B = 2$ operators relevant for calculations of $\Delta \Gamma_s$, the $B_s-\bar{B}_s$ width difference. We have computed correlation functions…

High Energy Physics - Lattice · Physics 2018-03-29 Christine Davies , Judd Harrison , G Peter Lepage , Christopher Monahan , Junko Shigemitsu , Matthew Wingate

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 investigate new physics models that can increase the lifetime differences in the $B_q$--$\bar{B}_q$ systems ($q = d,s$) above their standard model values. If both $B_q$ as well as $\bar{B}_q$ can decay to a final state through flavour…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amol Dighe , Anirban Kundu , Soumitra Nandi

Suggestions for efficiently determining the lifetimes and mass difference of the light and heavy $B_s$ mesons ($B_s^L, B_s^H$) from $B_s \to J/ \psi \phi, D_s^{*+}D_s^{*-}$ decays are given. Using appropriate weighting functions for the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Amol Dighe , Isard Dunietz , Robert Fleischer

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

The $B_s$ system is analyzed in light of a possible width difference $\Delta\Gamma_s$ between its mass eigenstates. If $\Delta\Gamma_s$ is sizable, untagged $B_s$-meson decays may allow a probe of CP violation and moreover the extraction…

High Energy Physics - Phenomenology · Physics 2007-05-23 Robert Fleischer

We present O(alpha_s^2) corrections to the decay t-->bW in the limit of a very large top quark mass, m_t >> m_W. We find that the O(alpha_s^2) effects decrease the top quark decay width Gamma_t by about 2%: Gamma_t =…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andrzej Czarnecki , Kirill Melnikov

The LHCb experiment has recently established a sizable width difference between the mass eigenstates of the $B_s$-meson system. This phenomenon leads to a subtle difference at the 10% level between the experimental branching ratios of $B_s$…

High Energy Physics - Phenomenology · Physics 2015-06-11 Robert Fleischer

We have made the first observation of Bs->Ds(*)+Ds(*)- decays using 23.6 fb-1 of data recorded by the Belle experiment running on the Upsilon(5S) resonance. The branching fractions are measured to be B(B^0_s\ra D^+_s D^-_s) =…

High Energy Physics - Experiment · Physics 2010-12-09 S. Esen , A. J. Schwartz , I. Adachi , H. Aihara , K. Arinstein , V. Aulchenko , T. Aushev , T. Aziz , A. M. Bakich , V. Balagura , E. Barberio , A. Bay , M. Bischofberger , A. Bondar , A. Bozek , M. Bracko , T. E. Browder , M. -C. Chang , P. Chang , A. Chen , P. Chen , B. G. Cheon , C. -C. Chiang , Y. Choi , J. Dalseno , M. Dash , Z. Dolezal , Z. Drasal , A. Drutskoy , S. Eidelman , P. Goldenzweig , B. Golob , H. Ha , J. Haba , T. Hara , K. Hayasaka , T. Higuchi , Y. Hoshi , W. -S. Hou , Y. B. Hsiung , H. J. Hyun , T. Iijima , K. Inami , R. Itoh , M. Iwabuchi , N. J. Joshi , T. Julius , J. H. Kang , T. Kawasaki , H. Kichimi , H. J. Kim , H. O. Kim , J. H. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , P. Kodys , S. Korpar , P. Krizan , P. Krokovny , T. Kuhr , T. Kumita , Y. -J. Kwon , S. -H. Kyeong , J. S. Lange , S. -H. Lee , Y. Liu , D. Liventsev , R. Louvot , A. Matyja , S. McOnie , H. Miyata , R. Mizuk , G. B. Mohanty , E. Nakano , M. Nakao , H. Nakazawa , Z. Natkaniec , S. Neubauer , S. Nishida , O. Nitoh , T. Ohshima , S. Okuno , S. L. Olsen , P. Pakhlov , C. W. Park , H. Park , H. K. Park , M. Petric , L. E. Piilonen , M. Rohrken , S. Ryu , H. Sahoo , Y. Sakai , O. Schneider , C. Schwanda , K. Senyo , M. E. Sevior , M. Shapkin , C. P. Shen , J. -G. Shiu , P. Smerkol , E. Solovieva , M. Staric , K. Sumisawa , T. Sumiyoshi , Y. Teramoto , K. Trabelsi , S. Uehara , Y. Unno , S. Uno , P. Urquijo , Y. Usov , G. Varner , K. E. Varvell , K. Vervink , C. H. Wang , M. -Z. Wang , P. Wang , Y. Watanabe , R. Wedd , J. Wicht , E. Won , B. D. Yabsley , Y. Yamashita , Z. P. Zhang , V. Zhilich , A. Zupanc

Combining our results for various O(alpha_s^2) corrections to the weak radiative B-meson decay, we are able to present the first estimate of the branching ratio at the next-to-next-to-leading order in QCD. We find BR(B -> X_s gamma) = (3.15…

The B meson lifetime ratios are calculated to the order of $1/m_b^3$ in the heavy quark expansion. The predictions of those ratios are dependent on four unknown hadronic parameters $B_1$, $B_2$, $\epsilon_1$ and $\epsilon_2$, where $B_1$…

High Energy Physics - Phenomenology · Physics 2009-10-31 Hai-Yang Cheng , Kwei-Chou Yang

We study the impact of the Randall-Sundrum setup on the width difference $\Delta\Gamma_s$ and the CP-violating phase $\phi_s$ in the $\bar B_s^0$-$B_s^0$ system. Our calculations are performed in the general framework of an effective…

High Energy Physics - Phenomenology · Physics 2015-03-19 Florian Goertz , Torsten Pfoh

About 90% of Bs-bar Bs pairs produced at the Upsilon(5s) resonance are initially Bs*-bar Bs* pairs which decay radiatively to Bs-bar Bs. This implies that the Bs pair will then be in an eigenstate of charge conjugation (i.e. C=-1) and…

High Energy Physics - Phenomenology · Physics 2014-11-20 David Atwood , Amarjit Soni

We study the Standard Model prediction for the mass difference between the two neutral D meson mass eigenstates, $\Delta m$. We derive a dispersion relation based on heavy quark effective theory that relates $\Delta m$ to an integral of the…

High Energy Physics - Phenomenology · Physics 2010-04-06 Adam F. Falk , Yuval Grossman , Zoltan Ligeti , Yosef Nir , Alexey A. Petrov

We report on the calculation of next-to-next-to-leading order (NNLO) QCD corrections to the width difference $\Delta \Gamma_s$ in the neutral $B$-meson mixing process $B^0_s - \bar{B}^0_s$. These contributions represent an important step in…

High Energy Physics - Phenomenology · Physics 2021-10-26 Vladyslav Shtabovenko

We compute perturbative QCD corrections to the lifetime splitting between the charged and neutral $B$ meson in the framework of the heavy quark expansion. These next-to-leading logarithmic corrections are necessary for a meaningful use of…

High Energy Physics - Phenomenology · Physics 2009-10-09 M. Beneke , G. Buchalla , C. Greub , A. Lenz , U. Nierste

The experimentally established non-zero decay width difference of the B_s meson system gives us access to a mass eigenstate rate asymmetry for each B_s transition. This observable is not only the key ingredient in converting between…

High Energy Physics - Phenomenology · Physics 2014-12-18 Robert Knegjens