English
Related papers

Related papers: Model independent analysis of a class of $\bar{B}_…

200 papers

I discuss a model independent determination of the widths of a class of two-body $\bar{B}_s^0 $ decays induced by $b \to c \bar u d$ and $b \to c \bar u s$ transitions. The analysis is based on $SU(3)_F$ symmetry and exploits existing…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Ferrandes

Based on the assumption of two-quark structure for the light scalar mesons, within the framework of perturbative QCD approach, we investigate the $B_{q}\to D_{(s)}^{(*)} S(q=u,d,s)$ decays induced by $b\to u $ transition, where $S$ denotes…

High Energy Physics - Phenomenology · Physics 2017-02-08 Zhi-Tian Zou , Ying Li , Xin liu

The $\Delta S = 2$ transition $b \to s s \bar d$ is extremely small in the standard model, proceeding only via box diagrams. Such decays are thus an appropriate ground for searching new physics. We present a study of several two-body and…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Fajfer , J. Kamenik , P. Singer

Motivated by the anomalies present in $b \to s\,l^+\,l^-$ neutral current decays, we study the corresponding $B_c \to (D_s,\,D^{\ast}_s)\mu^+\mu^-$ decays within the standard model and beyond. We use a model independent effective theory…

High Energy Physics - Phenomenology · Physics 2019-10-30 Rupak Dutta

Two- and three-body decays of $\Upsilon (5S)$ into $BB, $$ BB^*, $ $ B^*B^*,$ $ B_sB_s, $ $B_sB_s^*, $ $B_s^* B_s^*$ and $BB^*\pi, B^*B^*\pi$ are evaluated using the theory, developed earlier for dipion bottomonium transitions. The theory…

High Energy Physics - Phenomenology · Physics 2009-02-19 Yu. A. Simonov , A. I. Veselov

The decays of $B$ mesons to two-body hadronic final states are analyzed within the context of broken flavor SU(3) symmetry, extending a previous analysis involving pairs of light pseudoscalars to decays involving one or two charmed quarks…

High Energy Physics - Phenomenology · Physics 2010-11-01 Michael Gronau , Oscar F. Hernandez , David London , Jonathan L. Rosner

In this article, we study the two-body strong decays of the bottom mesons with the heavy meson effective theory in the leading order approximation, and obtain all the analytical expressions of the decay widths of the light pseudoscalar…

High Energy Physics - Phenomenology · Physics 2014-09-09 Zhi-Gang Wang

The b to d d s bar transition gives extremely small branching ratios within the standard model, thus providing an appropriate ground for testing new physics. Using renormalization group technique we determine the Wilson coefficients and the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Svjetlana Fajfer , Jernej Kamenik , Nejc Kosnik

The charmed B decays, $B\to DP, ~D^*P$ and $DV$, are re-analyzed using the latest experimental data, where $P$ and $V$ denote the pseudoscalar meson and vector meson, respectively. We perform global fits under the assumption of flavor SU(3)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Cheng-Wei Chiang , Eibun Senaha

We study two-body hadronic $B_s\to PT$ decays, with $P (T)$ being a light pseudoscalar (tensor) meson, in the perturbative QCD approach. The CP-averaged branching ratios and the direct CP asymmetries of the $\Delta S=0$ modes are predicted,…

High Energy Physics - Phenomenology · Physics 2014-03-25 Qin Qin , Zhi-Tian Zou , Xin Yu , Hsiang-nan Li , Cai-Dian Lü

The $\Delta S = 2$ $b \to \bar d ss$ transition proceeds via the box - diagram in the Standard Model with a branching ratio calculated to be below $10^{-11}$, thus providing an appropriate testing ground for physics beyond the Standard…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. Fajfer , P. Singer

We re-analyze hadronic decays of B mesons to a pseudoscalar (P) and a tensor meson (T), or a vector meson (V) and a tensor meson, through a $b \to c$ transition. We discuss possible large uncertainties to branching ratios (BR's) of the…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. S. Kim , Jong-Phil Lee , Sechul Oh

As a consequence of the Ward identity for hadronic matrix elements, we find relations between the differential decay rates of semileptonic decay modes with the underlying quark-level transition $b\rightarrow c\tau \nu$, which are valid in…

High Energy Physics - Phenomenology · Physics 2020-12-02 Stefan Schacht , Amarjit Soni

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

Various nonleptonic decay channels mediated by the quark-level subprocess $b\to s\bar{s} s$ show hints of deviation from the Standard Model expectations. We analyse the double-vector decay $B\to\phi K^\ast$ with different generic new…

High Energy Physics - Phenomenology · Physics 2009-11-11 Soumitra Nandi , Anirban Kundu

Decays of the D mesons to two pseudoscalars, to two vectors, and to pseudoscalar plus vector are discussed in the context of broken flavor SU(3). A few assumptions are used to reduce the number of parameters. Amplitudes are fit to the…

High Energy Physics - Phenomenology · Physics 2016-09-01 Ian Hinchliffe , Thomas A. Kaeding

psi and Upsilon decays may be used to search for light neutral spin-1 or spin-0 bosons associated with a broken extra-U(1) symmetry, local or global, acting axially on quarks and leptons, as may be present in supersymmetric theories with a…

High Energy Physics - Phenomenology · Physics 2011-03-28 Pierre Fayet

We report the results of the first search for Standard Model and baryon-number-violating two-body decays of the neutral $B$ mesons to $\Lambda^{0}$ and $\Omega^{(*)0}_c$ using 711~${\rm fb^{-1}}$ of data collected at the $\Upsilon(4S)$…

High Energy Physics - Experiment · Physics 2024-05-21 Belle Collaboration , V. Savinov , I. Adachi , J. K. Ahn , H. Aihara , D. M. Asner , H. Atmacan , R. Ayad , Sw. Banerjee , J. Bennett , M. Bessner , V. Bhardwaj , D. Biswas , A. Bobrov , D. Bodrov , J. Borah , M. Bračko , P. Branchini , T. E. Browder , A. Budano , D. Červenkov , M. -C. Chang , P. Chang , B. G. Cheon , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , N. Dash , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , S. Dubey , P. Ecker , D. Epifanov , D. Ferlewicz , B. G. Fulsom , V. Gaur , A. Giri , P. Goldenzweig , E. Graziani , T. Gu , Y. Guan , K. Gudkova , C. Hadjivasiliou , H. Hayashii , S. Hazra , M. T. Hedges , W. -S. Hou , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , Y. Jin , D. Kalita , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , R. Kumar , T. Kumita , A. Kuzmin , Y. -J. Kwon , Y. -T. Lai , T. Lam , J. S. Lange , L. K. Li , Y. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , T. Luo , Y. Ma , M. Masuda , T. Matsuda , S. K. Maurya , F. Meier , M. Merola , I. Nakamura , M. Nakao , Z. Natkaniec , L. Nayak , M. Nayak , S. Nishida , S. Ogawa , H. Ono , P. Pakhlov , G. Pakhlova , S. Pardi , H. Park , J. Park , S. -H. Park , A. Passeri , S. Patra , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , G. Russo , S. Sandilya , L. Santelj , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , W. Shan , C. Sharma , J. -G. Shiu , E. Solovieva , M. Starič , M. Sumihama , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , R. Tiwary , K. Trabelsi , M. Uchida , Y. Unno , S. Uno , K. E. Varvell , E. Wang , S. Watanuki , E. Won , X. Xu , B. D. Yabsley , W. Yan , J. H. Yin , C. Z. Yuan , L. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

The in-medium partial decay widths of $\Upsilon (4S) \rightarrow B\bar B$ in magnetized asymmetric nuclear matter are studied using a field theoretic model for composite hadrons with quark (and antiquark) constituents. The medium…

Nuclear Theory · Physics 2022-06-15 Amruta Mishra , S. P. Misra

We consider two body decays of B meson into a light vector (V) and a pseudoscalar (P) meson. The constraint obtained from the $B\to P P$ modes on the parameter space of the input parameters is imposed also on $B\to V P$ modes. In particular…

High Energy Physics - Phenomenology · Physics 2009-10-30 N. G. Deshpande , B. Dutta , Sechul Oh
‹ Prev 1 2 3 10 Next ›