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Related papers: The Decay $B\to K^*\gamma$ from QCD Sum Rules

200 papers

We suggest a new technique to determine the CKM phase $\gamma$ {\em without} neglecting the (soft) final state rescattering effects. We use (time integrated) $B$ meson decay rates to $\pi$'s and $K$'s. A set of 5 $\Delta S = 0$ (or 1…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. Agashe , N. G. Deshpande

The decays $B^\pm\to \pi^\pm K$ and $B_d\to \pi^\mp K^\pm$ were observed by the CLEO collaboration last year; they may play an important role to probe the angle $\gamma$ of the unitarity triangle of the CKM matrix. After a general…

High Energy Physics - Phenomenology · Physics 2010-11-23 Robert Fleischer

We calculate the tree and penguin amplitudes in the $B^0\to\pi^+\pi^-$ decay channel employing the perturbative QCD factorization approach. Using the amplitudes as input with the theoretical uncertainties sufficiently considered, we…

High Energy Physics - Phenomenology · Physics 2017-11-21 Qin Qin , Zhi-Tian Zou , Cai-Dian Lü , Ying Li

We reanalyze the decay $B_d\to\pi^+\pi^-$ without assuming dominance of QCD penguins with internal top-quark exchanges. In that case the weak phase of the $\bar b \to\bar d$ QCD penguin amplitude is not related in a simple way to the CKM…

High Energy Physics - Phenomenology · Physics 2009-10-28 Robert Fleischer , Thomas Mannel

The decay rates for $B^0 \to K^+ \pi^-$, $B^+ \to K^0 \pi^+$, and the charge-conjugate processes were found to provide information on the weak phase $\gamma \equiv {\rm Arg}(V_{ub}^*)$ when the ratio $r$ of weak tree and penguin amplitudes…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michael Gronau , Jonathan L. Rosner

Precision tests of the Standard Model and searches for New Physics in the quark flavor sector depend on accurate theoretical calculations of decay rates and spectra for rare, flavor-changing processes. The theoretical status and recent…

High Energy Physics - Phenomenology · Physics 2008-01-07 Matthias Neubert

The decays $B_d\to\pi^\mp K^\pm$ and $B^\pm\to\pi^\pm K$ provide interesting constraints on the angle $\gamma$ of the unitarity triangle of the CKM matrix. It is shown that bounds on $\gamma$ can also be obtained from the time evolution of…

High Energy Physics - Phenomenology · Physics 2014-11-17 Robert Fleischer

We compute branching ratios of $B\to K\pi$ decays in the framework of perturbative QCD factorization theorem. Decay amplitudes are classified into the topologies of tree, penguin and annihilation, all of which contain both factorizable and…

High Energy Physics - Phenomenology · Physics 2009-07-09 Y. -Y. Keum , H. -n. Li , A. I. Sanda

New physics contributions to B decays often arise through chromo-magnetic penguin operators. To look for new physics effects in B decays, it is useful to be able to estimate the hadronic matrix elements for the chromo-magnetic operator. We…

High Energy Physics - Phenomenology · Physics 2009-11-10 Satoshi Mishima , A. I. Sanda

By employing the QCD factorization approach, we calculated the next-to-leading order new physics contributions to the branching ratios, CP asymmetries, isospin and U-spin symmetry breaking of the exclusive decays $B \to V \gamma$ ($V=K^*,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Zhenjun Xiao , Ci Zhuang

We give a more complete calculation of $b \to s\gamma $ decay, including leading log QCD corrections from $m_{top}$ to $M_W$ in addition to corrections from $M_{W}$ to $m_b$. We have included the full set of dimension-6 operators and…

High Energy Physics - Phenomenology · Physics 2009-10-28 Chong-Shong Gao , Jing-Liang Hu , Cai-Dian Lu , Zhao-Ming Qiu

We employ the $B\to\pi$ form factors obtained from QCD light-cone sum rules and calculate the $B\to \pi \ell \nu_l$ width ($\ell=e,\mu$) in units of $1/|V_{ub}|^2$, integrated over the region of accessible momentum transfers, $0\leq q^2\leq…

High Energy Physics - Phenomenology · Physics 2011-06-07 A. Khodjamirian , Th. Mannel , N. Offen , Y. -M. Wang

Using the method of QCD light-cone sum rules, we calculate the $B \to \pi\pi$ hadronic matrix elements with annihilation topology. We obtain a finite result, including the related strong phase. Numerically, the annihilation effects in $B\to…

High Energy Physics - Phenomenology · Physics 2014-11-18 A. Khodjamirian , Th. Mannel , M. Melcher , B. Melic

We study a relation between the weak phase $\gamma$ and the rates and CP asymmetries of several $K \pi$ decays of $B^+$, $B^0$, and $B_s$, emphasizing the impact of the latter measurements. Current data indicate large SU(3) breaking in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Cheng-Wei Chiang , Michael Gronau , Jonathan L. Rosner

We present a preliminary determination of the inclusive branching fraction for the rare radiative penguin transition B -> X_{s} gamma. The measurement is based on a data sample of 60 million BB pairs collected between 1999 and 2001 with the…

High Energy Physics - Experiment · Physics 2009-09-29 B. Aubert , BaBar Collaboration

We present a preliminary measurement of the branching fraction of the exclusive penguin decay B^0 -> K^*0 gamma using (8.6+/-0.3) x 10^6 B-anti-B decays BF(B^0 -> K^*0 gamma) = (5.2+/-0.82 (stat.) +/- 0.47 (sys.)) x 10^-5. In addition we…

High Energy Physics - Experiment · Physics 2016-08-31 Colin Jessop

Efforts to predict the rare exclusive decay $B\to K^{\ast}\gamma$ from the well known inclusive decay $b\to s\gamma$ are frustrated by the effect of the large recoil momentum. We show how to reduce the large uncertainty in calculating this…

High Energy Physics - Phenomenology · Physics 2009-10-22 Patrick J. O'Donnell , Humphrey K. K. Tung

We report the first search for the penguin-dominated process $B^0 \rightarrow K_S^0 K_S^0 \gamma$ using the full data sample of $772\times 10^6$ $B\bar{B}$ pairs collected with the Belle detector at the KEKB asymmetric-energy $e^+ e^-$…

High Energy Physics - Experiment · Physics 2023-01-24 Belle Collaboration , H. B. Jeon , K. H. Kang , H. Park , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , P. Behera , K. Belous , J. Bennett , F. Bernlochner , M. Bessner , V. Bhardwaj , B. Bhuyan , T. Bilka , A. Bobrov , D. Bodrov , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , P. Chang , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Das , N. Dash , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Giri , P. Goldenzweig , B. Golob , E. Graziani , T. Gu , K. Gudkova , C. Hadjivasiliou , T. Hara , K. Hayasaka , H. Hayashii , M. T. Hedges , T. Higuchi , W. -S. Hou , C. -L. Hsu , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , K. K. Joo , J. Kahn , H. Kakuno , A. B. Kaliyar , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , K. T. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , M. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , Y. -T. Lai , K. Lalwani , T. Lam , J. S. Lange , M. Laurenza , S. C. Lee , C. H. Li , J. Li , Y. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , A. Martini , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , M. Merola , F. Metzner , K. Miyabayashi , R. Mizuk , G. B. Mohanty , M. Nakao , D. Narwal , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , H. Ono , Y. Onuki , P. Oskin , P. Pakhlov , G. Pakhlova , T. Pang , S. Pardi , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , V. Popov , E. Prencipe , M. T. Prim , M. V. Purohit , M. Röhrken , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , S. Sandilya , A. Sangal , L. Santelj , T. Sanuki , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. Sharma , V. Shebalin , C. P. Shen , J. -G. Shiu , J. B. Singh , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , J. F. Strube , M. Sumihama , T. Sumiyoshi , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , S. E. Vahsen , R. Van Tonder , G. Varner , K. E. Varvell , A. Vinokurova , A. Vossen , E. Waheed , C. H. Wang , M. -Z. Wang , S. Watanuki , E. Won , B. D. Yabsley , W. Yan , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , C. Z. Yuan , Y. Yusa , Y. Zhai , Z. P. Zhang , V. Zhilich , V. Zhukova

We compute the rate of the decay $B^- \to \mu^- {\bar \nu}_\mu \gamma$ by a QCD relativistic potential model, with the result: ${\cal B}(B^- \to \mu^- {\bar \nu}_\mu \gamma)=0.9 \cdot 10^{-6}$. We also discuss how this decay mode can be…

High Energy Physics - Phenomenology · Physics 2008-02-03 F. De Fazio

Motivated by the observation of the decay B to K* gamma by the CLEO collaboration, we have systematically analyzed the weak radiative decay Lambda_b to Lambda gamma, evaluating the confined effects of quarks in the covariant oscillator…

High Energy Physics - Phenomenology · Physics 2009-10-31 Rukmani Mohanta , Anjan K. Giri , Mohinder P. Khanna , Muneyuki Ishida , Shin Ishida