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The sensitivity of the CKM angle $\gamma$ in $\Lambda_b^0 \to D \Lambda$ decays has been studied using the decay parameter $\alpha$ as an observable in addition to the decay rate asymmetry. Feasibility studies show that adding this…

High Energy Physics - Phenomenology · Physics 2021-12-30 Shunan Zhang , Yi Jiang , Zewen Chen , Wenbin Qian

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 report on the initial measurements of the angle gamma and the sum of angles 2 beta + gamma of the Unitarity Triangle. When compared with indirect information on the value of gamma from other measurements of CKM parameters, the…

High Energy Physics - Experiment · Physics 2007-05-23 Justin Albert

We evaluate the O(alpha_em/alpha_s) correction to the rate of B -> X_s gamma decay, i.e. we resum all the 0[ alpha_em ln M_W^2/m_b^2 x (alpha_s ln M_W^2/m_b^2)^n ] corrections for n=0,1,2,... Our calculation differs from the previously…

High Energy Physics - Phenomenology · Physics 2009-10-31 Konrad Baranowski , Mikolaj Misiak

Two loop electroweak corrections to b --> s gamma decays are computed. Fermion and photonic loop effects are found to reduce R = BR(b --> s gamma)/BR(b --> c e nu) by 8+-2% and lead to the standard model prediction BR(B --> X_s gamma)=(3.28…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andrzej Czarnecki , William J. Marciano

The angle $\gamma$ of the Cabibbo--Kobayashi--Maskawa unitarity triangle is a benchmark parameter of the Standard Model of particle physics. A method to determine $\gamma$ from $B^{\pm} \to D K^{\pm}$ with subsequent $D \to K_{\rm…

History and Philosophy of Physics · Physics 2020-06-23 A. Ceccucci , T. Gershon , M. Kenzie , Z. Ligeti , Y. Sakai , K. Trabelsi

Decays of the type $B\to D hh^\prime$, where a $b$~hadron decays to a neutral charm meson that can be an admixture of $D^0$ and $\overline{D}{}^0$ states together with two light particles that are typically a kaon and a pion, have…

High Energy Physics - Experiment · Physics 2019-08-13 Tim Gershon

The 3 X 3 CKM matrix defines six unitarity triangles in the complex plane, which will be carefully explored in the LHCb experiment and at the Super-B factory. We calculate the running effects of nine different inner angles and eighteen…

High Energy Physics - Phenomenology · Physics 2014-11-20 Shu Luo , Zhi-zhong Xing

We review the first measurements of the CKM angle gamma from LHCb. These measurements have been performed with b-hadron decays dominated by b -> u and b -> c tree-level amplitudes, from which gamma can be determined without theoretical…

High Energy Physics - Experiment · Physics 2015-06-15 Stefania Ricciardi

In presenting an up-to-date account of the experimental knowledge of the CKM matrix, special emphasis is placed on the exceptional degree of consistency shown by the current Standard Model determination of the unitarity triangle; some…

High Energy Physics - Phenomenology · Physics 2010-11-23 Pietro Faccioli

We present a complete calculation of the Leading Order QCD corrections to the quark level decay amplitude for b -> s gamma gamma and study their relevance for both the inclusive branching ratio BR(B -> X_s gamma gamma) and for the exclusive…

High Energy Physics - Phenomenology · Physics 2014-11-17 Laura Reina , Giulia Ricciardi , Amarjit Soni

Several time-independent methods have been devised for measuring the phase gamma of the Cabibbo-Kobayashi-Maskawa unitarity triangle. It is shown that such measurements generally suffer from discrete ambiguity which is at least 8-fold, not…

High Energy Physics - Phenomenology · Physics 2010-11-23 Abner Soffer

The LHCb collaboration has studied various promising ways to determine the Unitarity Triangle angle $\gamma$. Three complementary methods will be considered. The potential of the $B \to DK^{(*)}$ decays has been studied by employing the…

High Energy Physics - Experiment · Physics 2008-07-11 Jacopo Nardulli

The LHCb approach for a precise determination of the CKM angle $\gamma$ from tree--level decays is presented. Up to 16 independent determinations, using a variety of beauty and charm mesons decay modes, are available at LHCb. Not all of…

High Energy Physics - Experiment · Physics 2019-06-21 A. Bertolin

The unitarity triangle can be determined by means of two measurements of its sides or angles. Assuming the same relative errors on the angles $(\alpha,\beta,\gamma)$ and the sides $(R_b,R_t)$, we find that the pairs $(\gamma,\beta)$ and…

High Energy Physics - Phenomenology · Physics 2010-11-23 Andrzej J. Buras , Fabrizio Parodi , Achille Stocchi

The decay $B^{\pm}\to DK^{\pm}$ followed by the subsequent decay of the $D$ meson into final states involving a neutral kaon can be used to determine the CKM angle $\gamma$. We study CP violation effects due to mixing and decay of the final…

High Energy Physics - Phenomenology · Physics 2015-06-17 Yuval Grossman , Michael Savastio

It is shown that it is possible to perform a model-independent extraction of the CKM Unitarity Triangle angle $\gamma$ using only the decays $B^0\to D K^+\pi^-$ with $D\to K^0_S\pi^+\pi^-$ and $B^0\to D K^+\pi^-$ with flavour-specific $D$…

High Energy Physics - Phenomenology · Physics 2014-11-20 Tim Gershon , Anton Poluektov

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…

We find that the phase appearing in the unitarity relation between $\mathcal{B}(K_L\rightarrow \mu^+\mu^-)$ and $\mathcal{B}(K_L\rightarrow \gamma\gamma)$ is equal to the phase shift in the interference term of the time-dependent…

High Energy Physics - Phenomenology · Physics 2023-06-13 Avital Dery , Mitrajyoti Ghosh , Yuval Grossman , Teppei Kitahara , Stefan Schacht

We report a determination of the CKM angle $\phi_{3}$, also known as $\gamma$, from a combination of measurements using samples of up to 711~fb$^{-1}$ from the Belle experiment and up to 362~fb$^{-1}$ from the Belle II experiment. We…

High Energy Physics - Experiment · Physics 2024-08-13 Belle , Belle II Collaborations , : , I. Adachi , L. Aggarwal , H. Aihara , N. Akopov , A. Aloisio , S. Al Said , N. Anh Ky , D. M. Asner , H. Atmacan , V. Aushev , M. Aversano , R. Ayad , V. Babu , H. Bae , S. Bahinipati , P. Bambade , Sw. Banerjee , S. Bansal , M. Barrett , J. Baudot , A. Baur , A. Beaubien , F. Becherer , J. Becker , K. Belous , J. V. Bennett , F. U. Bernlochner , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , B. Bhuyan , F. Bianchi , L. Bierwirth , T. Bilka , S. Bilokin , D. Biswas , A. Bobrov , D. Bodrov , A. Bolz , A. Bondar , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , J. Cerasoli , M. -C. Chang , P. Chang , R. Cheaib , P. Cheema , B. G. Cheon , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , L. Corona , S. Das , F. Dattola , E. De La Cruz-Burelo , S. A. De La Motte , G. de Marino , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , R. Dhamija , A. Di Canto , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , M. Dorigo , K. Dort , D. Dossett , S. Dreyer , S. Dubey , G. Dujany , P. Ecker , M. Eliachevitch , D. Epifanov , P. Feichtinger , T. Ferber , D. Ferlewicz , T. Fillinger , G. Finocchiaro , A. Fodor , F. Forti , A. Frey , B. G. Fulsom , A. Gabrielli , E. Ganiev , M. Garcia-Hernandez , R. Garg , G. Gaudino , V. Gaur , A. Gaz , A. Gellrich , G. Ghevondyan , D. Ghosh , H. Ghumaryan , G. Giakoustidis , R. Giordano , A. Giri , B. Gobbo , R. Godang , O. Gogota , P. Goldenzweig , W. Gradl , T. Grammatico , S. Granderath , E. Graziani , D. Greenwald , Z. Gruberová , T. Gu , Y. Guan , K. Gudkova , S. Halder , Y. Han , T. Hara , H. Hayashii , S. Hazra , M. T. Hedges , A. Heidelbach , I. Heredia de la Cruz , M. Hernández Villanueva , T. Higuchi , M. Hoek , M. Hohmann , P. Horak , C. -L. Hsu , T. Humair , T. Iijima , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , P. Jackson , W. W. Jacobs , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , H. Junkerkalefeld , D. Kalita , A. B. Kaliyar , J. Kandra , T. Kawasaki , F. Keil , C. Kiesling , C. -H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , H. Kindo , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , K. Kojima , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , T. M. G. Kraetzschmar , P. Križan , P. Krokovny , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , T. Kunigo , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , T. Lam , L. Lanceri , J. S. Lange , M. Laurenza , M. J. Lee , D. Levit , P. M. Lewis , C. Li , L. K. Li , Y. Li , Y. B. Li , J. Libby , M. H. Liu , Q. Y. Liu , Z. Q. Liu , D. Liventsev , S. Longo , T. Lueck , C. Lyu , Y. Ma , M. Maggiora , S. P. Maharana , R. Maiti , S. Maity , G. Mancinelli , R. Manfredi , E. Manoni , M. Mantovano , D. Marcantonio , S. Marcello , C. Marinas , L. Martel , C. Martellini , A. Martini , T. Martinov , L. Massaccesi , M. Masuda , D. Matvienko , S. K. Maurya , J. A. McKenna , R. Mehta , F. Meier , M. Merola , F. Metzner , C. Miller , M. Mirra , K. Miyabayashi , H. Miyake , G. B. Mohanty , N. Molina-Gonzalez , S. Mondal , S. Moneta , H. -G. Moser , M. Mrvar , R. Mussa , I. Nakamura , K. R. Nakamura , M. Nakao , Y. Nakazawa , A. Narimani Charan , M. Naruki , D. Narwal , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , G. Nazaryan , M. Neu , C. Niebuhr , S. Nishida , S. Ogawa , Y. Onishchuk , H. Ono , P. Oskin , F. Otani , P. Pakhlov , G. Pakhlova , A. Panta , S. Pardi , K. Parham , H. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , G. Pinna Angioni , P. L. M. Podesta-Lerma , T. Podobnik , S. Pokharel , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , P. Rados , G. Raeuber , S. Raiz , N. Rauls , M. Reif , S. Reiter , M. Remnev , I. Ripp-Baudot , G. Rizzo , S. H. Robertson , M. Roehrken , J. M. Roney , A. Rostomyan , N. Rout , G. Russo , D. A. Sanders , S. Sandilya , L. Santelj , Y. Sato , V. Savinov , B. Scavino , C. Schmitt , G. Schnell , C. Schwanda , M. Schwickardi , Y. Seino , A. Selce , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , W. Shan , X. D. Shi , T. Shillington , T. Shimasaki , J. -G. Shiu , D. Shtol , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , J. Skorupa , R. J. Sobie , M. Sobotzik , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , B. Spruck , M. Starič , P. Stavroulakis , S. Stefkova , R. Stroili , M. Sumihama , K. Sumisawa , W. Sutcliffe , N. Suwonjandee , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , O. Tittel , R. Tiwary , D. Tonelli , E. Torassa , K. Trabelsi , I. Tsaklidis , M. Uchida , I. Ueda , Y. Uematsu , T. Uglov , K. Unger , Y. Unno , K. Uno , S. Uno , P. Urquijo , Y. Ushiroda , S. E. Vahsen , R. van Tonder , K. E. Varvell , M. Veronesi , A. Vinokurova , V. S. Vismaya , L. Vitale , V. Vobbilisetti , R. Volpe , B. Wach , M. Wakai , S. Wallner , E. Wang , M. -Z. Wang , X. L. Wang , Z. Wang , A. Warburton , S. Watanuki , C. Wessel , E. Won , X. P. Xu , B. D. Yabsley , S. Yamada , W. Yan , S. B. Yang , J. Yelton , J. H. Yin , K. Yoshihara , C. Z. Yuan , B. Zhang , Y. Zhang , V. Zhilich , Q. D. Zhou , V. I. Zhukova