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We present new precision predictions for semitauonic decays involving $\rho$ and $\omega$ final state mesons. These decay channels offer an interesting orthogonal probe to study the existing B anomalies in semitauonic transitions and are…

High Energy Physics - Phenomenology · Physics 2020-01-20 Markus Tobias Prim , Florian Urs Bernlochner , Dean J. Robinson

Strangeness-changing decays of $B$ mesons to three-body final states of pions and kaons are studied, assuming that they are dominated by a $\Delta I=0$ penguin amplitude with flavor structure $\bar b \to \bar s$. Numerous isospin relations…

High Energy Physics - Phenomenology · Physics 2009-11-11 Michael Gronau , Jonathan L. Rosner

Within the factorization-assisted topological-amplitude approach, we studied the 33 charmless $B_{(s)} \to VV$ decays, where $V$ stands for a light vector meson. According to the flavor flows, the amplitude of each process can be decomposed…

High Energy Physics - Phenomenology · Physics 2017-06-01 Chao Wang , Qi-An Zhang , Ying Li , Cai-Dian Lu

New results on B decays to charm-related modes from the Belle and CLEO experiments are presented.

High Energy Physics - Experiment · Physics 2009-11-07 P. Krokovny

The semileptonic decays of $B_q$ mesons ($q=u,d,s$) to $J^P=2^+$ charmed mesons are investigated. The form factors parametrising the hadronic matrix elements of the weak vector and axial-vector quark currents are evaluated using light-cone…

High Energy Physics - Phenomenology · Physics 2026-04-30 Pietro Colangelo , Fulvia De Fazio , Carlo la Torre , Giuseppe Roselli

We improve upon previous explicit estimates of charm rescattering contributions to the decay $B^0\to K^0\bar{\ell}\ell$ by including contributions from dipole interactions with the intermediate charm-meson states, and by further…

High Energy Physics - Phenomenology · Physics 2025-11-07 Gino Isidori , Zachary Polonsky , Arianna Tinari

We report on preliminary measurements of branching fractions, charge-parity-violating asymmetries, and longitudinal polarization fractions in charmless bottom-meson decays from the Belle~II experiment. We use samples of electron-positron…

High Energy Physics - Experiment · Physics 2021-05-24 Riccardo Manfredi

A Gaussian wave function is used for detailed study of mass spectra of the $B$ and $B_S$ mesons using a Cornell potential incorporated with a $\mathcal{O}(1/m)$ correction in the potential energy term and expansion of the kinetic energy…

High Energy Physics - Phenomenology · Physics 2017-08-17 Virendrasinh Kher , Nayneshkumar Devlani , Ajay Kumar Rai

We consider the branching ratios and CP asymmetry in the B meson decays into two pseudoscalar mesons in the generalized factorization approximation. We also investigate the possible effects of the enhanced chromomagnetic interaction b --> s…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ji-Ho Jang , Yeong Gyun Kim , Pyungwon Ko

In the study of two-body charmless B decays as a mean of looking for direct CP-violation and measuring the CKM mixing parameters in the Standard Model, the short-distance penguin contribution with its absorptive part generated by charm…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. N. Pham

Light cone hadron wave functions support Fock states of arbitrarily high particle number: their heavy quark content arises naturally through QCD interactions. We discuss what role c\bar c pairs, intrinsic to a hadron's structure, can play…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Gardner

In this paper, we briefly review results on rare decays of $B$ mesons from the Belle experiment, based on 10.4 fb$^{-1}$ data collected on the $\Upsilon$(4S) resonance. The topics include measurements of Cabibbo suppressed decays $B \to…

High Energy Physics - Experiment · Physics 2016-11-23 Toru Iijima

We analyze the charmless two-body decays of the $B$ meson into a pseudoscalar and a vector meson, referred to as $B\to PV$ decay, within the framework of the modified perturbative QCD (PQCD) approach. Based on the conventional PQCD…

High Energy Physics - Phenomenology · Physics 2025-11-26 Sheng Lü , Ru-Xuan Wang , Mao-Zhi Yang

General relations between the form factors of B decays to light mesons are derived using the heavy quark and large recoil expansion. On their basis the complete account of contributions of second order in the ratio of the light meson mass…

High Energy Physics - Phenomenology · Physics 2014-11-17 D. Ebert , R. N. Faustov , V. O. Galkin

We discuss multichannel inelastic rescatterring effects in B decays into a pair $PP$ of pseudoscalar mesons ($PP = \pi \pi$ or $K\bar{K}$). In agreement with short-distance models it is assumed that initially $B$ meson decays dominantly…

High Energy Physics - Phenomenology · Physics 2009-10-31 P. Zenczykowski

We report on the reconstruction of various charmless $B$ decays from electron-positron collisions at the energy corresponding to the $\Upsilon(4S)$ resonance collected with the Belle II detector at the SuperKEKB collider. We use simulation…

High Energy Physics - Experiment · Physics 2020-06-05 Belle II Collaboration , F. Abudinén , I. Adachi , R. Adak , K. Adamczyk , P. Ahlburg , J. K. Ahn , H. Aihara , N. Akopov , A. Aloisio , F. Ameli , L. Andricek , N. Anh Ky , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , V. Aushev , T. Aziz , V. Babu , S. Bacher , S. Baehr , S. Bahinipati , A. M. Bakich , P. Bambade , Sw. Banerjee , S. Bansal , M. Barrett , W. Bartel , G. Batignani , J. Baudot , A. Beaulieu , J. Becker , P. K. Behera , M. Bender , J. V. Bennett , E. Bernieri , F. U. Bernlochner , M. Bertemes , M. Bessner , S. Bettarini , V. Bhardwaj , B. Bhuyan , F. Bianchi , T. Bilka , S. Bilokin , D. Biswas , A. Bobrov , A. Bondar , G. Bonvicini , A. Bozek , M. Bračko , P. Branchini , N. Braun , R. A. Briere , T. E. Browder , D. N. Brown , A. Budano , L. Burmistrov , S. Bussino , M. Campajola , L. Cao , G. Caria , G. Casarosa , C. Cecchi , D. Červenkov , M. -C. Chang , P. Chang , R. Cheaib , V. Chekelian , Y. Q. Chen , Y. -T. Chen , B. G. Cheon , K. Chilikin , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , D. Cinabro , L. Corona , L. M. Cremaldi , D. Cuesta , S. Cunliffe , T. Czank , N. Dash , F. Dattola , E. De La Cruz-Burelo , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , B. Deschamps , M. Destefanis , S. Dey , A. De Yta-Hernandez , F. Di Capua , S. Di Carlo , J. Dingfelder , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , K. Dort , D. Dossett , S. Dubey , S. Duell , G. Dujany , S. Eidelman , M. Eliachevitch , D. Epifanov , J. E. Fast , T. Ferber , D. Ferlewicz , G. Finocchiaro , S. Fiore , P. Fischer , A. Fodor , F. Forti , A. Frey , M. Friedl , B. G. Fulsom , M. Gabriel , N. Gabyshev , E. Ganiev , M. Garcia-Hernandez , R. Garg , A. Garmash , V. Gaur , A. Gaz , U. Gebauer , M. Gelb , A. Gellrich , J. Gemmler , T. Geßler , D. Getzkow , R. Giordano , A. Giri , A. Glazov , B. Gobbo , R. Godang , P. Goldenzweig , B. Golob , P. Gomis , P. Grace , W. Gradl , E. Graziani , D. Greenwald , Y. Guan , C. Hadjivasiliou , S. Halder , K. Hara , T. Hara , O. Hartbrich , T. Hauth , K. Hayasaka , H. Hayashii , C. Hearty , M. Heck , M. T. Hedges , I. Heredia de la Cruz , M. Hernández Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , H. Hirata , S. Hirose , M. Hoek , M. Hohmann , S. Hollitt , T. Hotta , C. -L. Hsu , Y. Hu , K. Huang , T. Iijima , K. Inami , G. Inguglia , J. Irakkathil Jabbar , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , S. Iwata , P. Jackson , W. W. Jacobs , I. Jaegle , D. E. Jaffe , E. -J. Jang , M. Jeandron , H. B. Jeon , S. Jia , Y. Jin , C. Joo , K. K. Joo , I. Kadenko , J. Kahn , H. Kakuno , A. B. Kaliyar , J. Kandra , K. H. Kang , P. Kapusta , G. Karyan , Y. Kato , H. Kawai , T. Kawasaki , T. Keck , C. Ketter , H. Kichimi , C. Kiesling , B. H. Kim , C. -H. Kim , D. Y. Kim , H. J. Kim , J. B. Kim , K. -H. Kim , K. Kim , S. -H. Kim , Y. -K. Kim , Y. Kim , T. D. Kimmel , H. Kindo , K. Kinoshita , B. Kirby , C. Kleinwort , B. Knysh , P. Kodyš , T. Koga , S. Kohani , S. Koirala , I. Komarov , T. Konno , S. Korpar , N. Kovalchuk , T. M. G. Kraetzschmar , P. Križan , R. Kroeger , J. F. Krohn , P. Krokovny , H. Krüger , W. Kuehn , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , T. Kumita , T. Kunigo , M. Künzel , S. Kurz , A. Kuzmin , P. Kvasnička , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , C. La Licata , K. Lalwani , L. Lanceri , J. S. Lange , K. Lautenbach , P. J. Laycock , F. R. Le Diberder , I. -S. Lee , S. C. Lee , P. Leitl , D. Levit , P. M. Lewis , C. Li , L. K. Li , S. X. Li , Y. M. Li , Y. B. Li , J. Libby , K. Lieret , L. Li Gioi , J. Lin , Z. Liptak , Q. Y. Liu , Z. A. Liu , D. Liventsev , S. Longo , A. Loos , P. Lu , M. Lubej , T. Lueck , F. Luetticke , T. Luo , C. MacQueen , Y. Maeda , M. Maggiora , S. Maity , R. Manfredi , E. Manoni , S. Marcello , C. Marinas , A. Martini , M. Masuda , T. Matsuda , K. Matsuoka , D. Matvienko , J. McNeil , F. Meggendorfer , J. C. Mei , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , K. Miyabayashi , H. Miyake , H. Miyata , R. Mizuk , K. Azmi , G. B. Mohanty , H. Moon , T. Moon , J. A. Mora Grimaldo , A. Morda , T. Morii , H. -G. Moser , M. Mrvar , F. Mueller , F. J. Müller , Th. Muller , G. Muroyama , R. Mussa , K. Nakagiri , I. Nakamura , K. R. Nakamura , E. Nakano , M. Nakao , H. Nakayama , H. Nakazawa , T. Nanut , Z. Natkaniec , M. Nayak , G. Nazaryan , D. Neverov , C. Niebuhr , M. Niiyama , J. Ninkovic , N. K. Nisar , S. Nishida , K. Nishimura , M. Nishimura , M. H. A. Nouxman , B. Oberhof , K. Ogawa , S. Ogawa , S. L. Olsen , Y. Onishchuk , H. Ono , Y. Onuki , P. Oskin , E. R. Oxford , H. Ozaki , P. Pakhlov , G. Pakhlova , A. Paladino , T. Pang , A. Panta , E. Paoloni , C. Park , H. Park , S. -H. Park , B. Paschen , A. Passeri , A. Pathak , S. Patra , S. Paul , T. K. Pedlar , I. Peruzzi , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , V. Popov , C. Praz , E. Prencipe , M. T. Prim , M. V. Purohit , P. Rados , S. Raiz , M. Reif , S. Reiter , M. Remnev , P. K. Resmi , I. Ripp-Baudot , M. Ritter , M. Ritzert , G. Rizzo , L. B. Rizzuto , S. H. Robertson , D. Rodríguez Pérez , J. M. Roney , C. Rosenfeld , A. Rostomyan , N. Rout , M. Rozanska , S. Rummel , G. Russo , D. Sahoo , Y. Sakai , D. A. Sanders , S. Sandilya , A. Sangal , L. Santelj , P. Sartori , J. Sasaki , Y. Sato , V. Savinov , B. Scavino , M. Schram , H. Schreeck , J. Schueler , C. Schwanda , A. J. Schwartz , B. Schwenker , R. M. Seddon , Y. Seino , A. Selce , K. Senyo , I. S. Seong , M. E. Sevior , C. Sfienti , V. Shebalin , C. P. Shen , H. Shibuya , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , S. Skambraks , K. Smith , R. J. Sobie , A. Soffer , A. Sokolov , Y. Soloviev , E. Solovieva , S. Spataro , B. Spruck , M. Starič , S. Stefkova , Z. S. Stottler , R. Stroili , J. Strube , J. Stypula , M. Sumihama , K. Sumisawa , T. Sumiyoshi , D. J. Summers , W. Sutcliffe , K. Suzuki , S. Y. Suzuki , M. Tabata , M. Takahashi , M. Takizawa , U. Tamponi , S. Tanaka , K. Tanida , H. Tanigawa , N. Taniguchi , Y. Tao , P. Taras , F. Tenchini , D. Tonelli , E. Torassa , K. Trabelsi , T. Tsuboyama , N. Tsuzuki , M. Uchida , I. Ueda , S. Uehara , T. Ueno , T. Uglov , K. Unger , Y. Unno , S. Uno , P. Urquijo , Y. Ushiroda , Y. Usov , S. E. Vahsen , R. van Tonder , G. S. Varner , K. E. Varvell , A. Vinokurova , L. Vitale , V. Vorobyev , A. Vossen , E. Waheed , H. M. Wakeling , K. Wan , W. Wan Abdullah , B. Wang , C. H. Wang , M. -Z. Wang , X. L. Wang , A. Warburton , M. Watanabe , S. Watanuki , I. Watson , J. Webb , S. Wehle , M. Welsch , C. Wessel , J. Wiechczynski , P. Wieduwilt , H. Windel , E. Won , L. J. Wu , X. P. Xu , B. Yabsley , S. Yamada , W. Yan , S. B. Yang , H. Ye , J. Yelton , I. Yeo , J. H. Yin , M. Yonenaga , Y. M. Yook , T. Yoshinobu , C. Z. Yuan , G. Yuan , W. Yuan , Y. Yusa , L. Zani , J. Z. Zhang , Y. Zhang , Z. Zhang , V. Zhilich , Q. D. Zhou , X. Y. Zhou , V. I. Zhukova , V. Zhulanov , A. Zupanc

New (preliminary) results for the form factors relevant for the semileptonic decays of heavy pseudoscalar to a light vector meson are presented. In particular, we discuss the form factors for D --> K* and B --> rho modes.

High Energy Physics - Lattice · Physics 2010-03-19 A. Abada , D. Becirevic , Ph. Boucaud , J. M. Flynn , J. P. Leroy , V. Lubicz , F. Mescia

We show that the QCD factorization approach for $B$-meson decays to charmless hadronic two-body final states can be extended to include electromagnetic corrections. The presence of electrically charged final-state particles complicates the…

High Energy Physics - Phenomenology · Physics 2020-12-02 Martin Beneke , Philipp Böer , Jan-Niklas Toelstede , K. Keri Vos

The exchange-degeneracy of the mesonic $f$, $\omega $, $\rho $ and $a_{2}$ Regge trajectories, dominant at moderate and high energies in hadron elastic scattering, is analyzed from two viewpoints. The first one concerns the masses of the…

High Energy Physics - Phenomenology · Physics 2009-01-07 P. Desgrolard , M. Giffon , E. Martynov , E. Predazzi

Measurements of mesons containing charm or bottom quarks at high transverse momentum (P_T) constitute an interesting set of probes for the nature of the interaction of hard partons with a QCD medium as created in ultrarelativistic heavy-ion…

High Energy Physics - Phenomenology · Physics 2014-05-21 Thorsten Renk
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