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The extension of the standard model with pairs of the vector-like families is studied. The quark mixing matrices for the left- and right-handed charged currents, as well as those for the flavour changing neutral currents, the Z and Higgs…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yu. F. Pirogov , O. V. Zenin

The Heavy Flavor Averaging Group provides with this document input to the European Strategy for Particle Physics. Research in heavy-flavor physics is an essential component of the particle-physics program, both within and beyond the…

I calculate heavy-light decay constants in a nonrelativistic potential model. The resulting estimate of heavy quark symmetry breaking conflicts with similar estimates from lattice QCD. I show that a semirelativistic potential model…

High Energy Physics - Phenomenology · Physics 2011-07-19 James F. Amundson

The Littlest Higgs model contains a new vector-like heavy quark in the up sector. There are two interesting features of its existence. One is that it extends the $3\times3$ CKM matrix in the Standard Model to a $4\times3$ matrix and the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jae Yong Lee

Some of the open questions on jet quenching are expected to be clarified by measuring heavy-flavored mesons at high transverse momentum. The formalism based on radiative in-medium energy-loss, which describes other high-pt results at RHIC,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Carlos A. Salgado

Heavy flavor physics entered a new era when the Belle II experiment observed its first collision. There are several hints found so far by BaBar, Belle, and LHCb in particular, that suggest the physics beyond the Standard Model appearing in…

High Energy Physics - Lattice · Physics 2019-02-26 Shoji Hashimoto

We apply heavy-quark effective theory to separate long- and short-distance effects of heavy quarks in lattice gauge theory. In this approach, the inverse heavy-quark mass and the lattice spacing are treated as short distances, and their…

High Energy Physics - Lattice · Physics 2014-11-17 Junpei Harada , Shoji Hashimoto , Ken-Ichi Ishikawa , Andreas S. Kronfeld , Tetsuya Onogi , Norikazu Yamada

We demonstrate that flavour-changing neutral currents in the top sector, mediated by leptophilic scalars at the electroweak scale, can easily arise in scenarios of new physics, and in particular in composite Higgs models. We moreover show…

High Energy Physics - Phenomenology · Physics 2020-10-14 Nuno Castro , Mikael Chala , Ana Peixoto , Maria Ramos

We consider correlation functions containing the axial current of one light and one heavy quark in the static approximation as well as in full QCD, using the lattice regularization. Up to one-loop order of perturbation theory, we study the…

High Energy Physics - Lattice · Physics 2016-09-01 ALPHA Collaboration , Martin Kurth , Rainer Sommer

Motivated by the success of the flavour physics programme carried out over the last decade at the Large Hadron Collider (LHC), we characterize in detail the physics potential of its High-Luminosity and High-Energy upgrades in this domain of…

High Energy Physics - Phenomenology · Physics 2019-02-25 A. Cerri , V. V. Gligorov , S. Malvezzi , J. Martin Camalich , J. Zupan , S. Akar , J. Alimena , B. C. Allanach , W. Altmannshofer , L. Anderlini , F. Archilli , P. Azzi , S. Banerjee , W. Barter , A. E. Barton , M. Bauer , I. Belyaev , S. Benson , M. Bettler , R. Bhattacharya , S. Bifani , A. Birnkraut , F. Bishara , T. Blake , S. Blusk , E. Boos , M. Borsato , C. Bozzi , A. Bragagnolo , J. Brod , J. Brodzicka , A. J. Buras , L. Cadamuro , A. Carbone , M. Carena , I. Carli , A. Carmona , F. R. Cavallo , A. Celis , M. Cepeda , G. S. Chahal , M. Chala , J. Charles , M. Charles , K. F. Chen , V. Chobanova , M. Chrzaszcz , G. Ciezarek , V. Cirigliano , M. Ciuchini , H. Cliff , J. Cogan , G. Colangelo , A. Contu , R. Covarelli , G. Cowan , A. Crivellin , G. D'Ambrosio , M. D'Onofrio , N. P. Dang , A. Davis , O. A. De Aguiar Francisco , K. De Bruyn , U. De Sanctis , H. De la Torre , W. Dekens , F. Deliot , M. Della Morte , S. Demers , D. Derkach , O. Deschamps , S. Descotes-Genon , F. Dettori , A. Di Canto , M. Dinardo , P. Dini , F. Dordei , M. Dorigo , A. dos Reis , L. Dudko , L. Dufour , G. Durieux , S. Dutta , A. Dziurda , U. Eitschberger , A. Esposito , M. Estevez , S. Fajfer , A. Falkowski , D. A. Faroughy , G. Fedi , S. Fiorendi , F. Fiori , C. Fitzpatrick , R. Fleischer , M. Fontana , P. J. Fox , M. Freytsis , E. Gámiz , E. Gabriel , P. Gambino , J. García Pardiñas , L. S. Geng , E. Gersabeck , M. Gersabeck , T. Gershon , A. Gilbert , M. Gonzalez-Alonso , P. Govoni , G. Graziani , A. Greljo , L. Grillo , B. Grinstein , A. Grohsjean , Y. Grossman , D. Guadagnoli , F. -K. Guo , L. Guzzi , J. Haller , B. Hamilton , T. Han , R. Harnik , D. Hill , G. Hiller , K. Hoepfner , J. M. Hogan , T. Hurth , O. Igonkina , P. Ilten , G. Isidori , Sa. Jain , M. John , D. Johnson , M. Jung , N. Jurik , S. Jäger , M. Kado , A. L. Kagan , J. F. Kamenik , M. Karliner , M. Kenzie , B. Khanji , J. Kieseler , T. Kitahara , T. Klijnsma , M. Knecht , N. Košnik , R. Kogler , P. Koppenburg , A. Korytov , M. Kreps , C. Langenbruch , U. Langenegger , T. Latham , R. F. Lebed , A. J. Lenz , N. Leonardo , O. Leroy , Q. Li , T. Li , F. Ligabue , Z. Ligeti , K. Long , E. Lunghi , F. Mahmoudi , G. Mancinelli , P. Mandrik , T. Mannel , X. Marcano , J. F. Marchand , D. Martínez Santos , A. Martin , M. Martinelli , F. Martinez Vidal , D. Marzocca , J. Matias , P. Matorras Cuevas , O. Matsedonskyi , A. Mauri , K. Mazumdar , M. Merk , A. B. Meyer , E. Michielin , G. Mitselmakher , L. Mittnacht , S. Monteil , M. J. Morello , M. Morgenstern , M. Narain , M. Nardecchia , M. Needham , N. Neri , M. Neubert , S. Neubert , U. Nierste , J. Nieves , Y. Nir , A. Nisati , D. P. O'Hanlon , E. Oset , P. Owen , O. Ozcelik , S. Pagan Griso , E. Palencia Cortezon , F. Palla , M. Palutan , M. Pappagallo , C. Parkes , S. Pascoli , G. Passaleva , E. Passemar , M. Patel , A. Pearce , K. Pedro , S. Perazzini , M. Perfilov , L. Perrozzi , L. Pescatore , B. A. Petersen , A. A. Petrov , A. Pich , A. Pilloni , F. Polci , A. D. Polosa , S. Prelovsek , A. Puig Navarro , G. Punzi , J. Rademacker , M. Rama , M. Reboud , A. Reimers , P. Reznicek , D. J. Robinson , J. L. Rosner , R. Ruiz , S. Saito , S. Sarkar , A. Savin , S. Sawant , S. Schacht , M. Schlaffer , A. Schmidt , B. Schneider , A. Schopper , M. H. Schune , J. Segovia , M. Selvaggi , N. Serra , G. Servant , L. Sestini , D. Shih , R. Silva Coutinho , L. Silvestrini , K. Skovpen , T. Skwarnicki , M. Smizanska , A. Soni , Y. Soreq , M. Spannowsky , P. Spradlin , E. Stamou , S. Stone , S. Stracka , D. M. Straub , A. P Szczepaniak , S. T'Jampens , Y. Takahashi , F. Teubert , E. Thomas , V. Tisserand , R. Torre , F. Tresoldi , D. Tsiakkouri , S. Turchikhin , K. A. Ulmer , V. Vagnoni , D. van Dyk , J. van Tilburg , S. Vecchi , R. Venditti , M. Vesterinen , J. Virto , P. Volkov , G. Vorotnikov , E. Vryonidou , J. Walder , W. Walkowiak , J. Wang , W. Wang , C. Weiland , M. Whitehead , G. Wilkinson , J. M. Williams , M. R. J. Williams , F. Wilson , Y. Xie , Z. Yang , E. Yazgan , T. You , F. Yu , C. Zhang , L. Zhang , W. Zhang

Heavy Quarks will be abundantly produced in Heavy Ion Collisions at LHC energies. Both, the production of open heavy flavoured mesons and quarkonia will probe the strongly interacting medium created in these reactions. In particular, the…

Nuclear Experiment · Physics 2008-11-26 Gines Martinez , the ALICE collaboration

We discuss the phenomenology of effective field theories with new scalar or vector representations of the Standard Model quark flavor symmetry group, allowing for large flavor breaking involving the third generation. Such field content can…

High Energy Physics - Phenomenology · Physics 2015-05-30 Benjamin Grinstein , Alexander L. Kagan , Michael Trott , Jure Zupan

We present the result for the first moment of the scalar and axial-vector current correlator in third order of the strong coupling constant alpha_s and give the details of a recent evaluation of the pseudo-scalar correlator. The results can…

High Energy Physics - Phenomenology · Physics 2009-01-06 Christian Sturm

We point out that there exist two different formulations of the Heavy Quark Effective Theory (HQET). One formulation of HQET was mostly developed at Harvard and involves the use of the equation of motion to eliminate the small components of…

High Energy Physics - Phenomenology · Physics 2009-09-25 S. Balk , A. Ilakovac , J. G. Korner , D. Pirjol

We review recent lattice results for quark masses and low-energy hadronic parameters relevant for flavor physics. We do that by describing the FLAG initiative, with emphasis on its scope and rating criteria. The emerging picture is that…

High Energy Physics - Phenomenology · Physics 2015-07-16 Michele Della Morte

The Large Hadron Collider (LHC), where lead nuclei will collide at the unprecedented c.m.s. energy of 5.5 TeV per nucleon-nucleon pair, will offer new and unique opportunities for the study of the properties of strongly interacting matter…

Nuclear Experiment · Physics 2008-11-26 A. Dainese

The purpose of these lectures is to provide the reader with an idea of how we can probe New Physics with quark flavour observables using effective theory techniques. After giving a concise review of the quark flavour structure of the…

High Energy Physics - Phenomenology · Physics 2021-05-03 Luca Silvestrini

Moriond QCD brings together particle physicists of varied interests. This review and introduction to heavy flavour physics is aimed at those not in the heavy-flavour field to describe the motivation and methodology of precision flavour…

High Energy Physics - Experiment · Physics 2011-05-09 Robert W. Lambert

SU(3) gauge theories with increasing number of light fermions are the templates of strongly interacting sectors and studying their low-energy dynamics and spectrum is important, both for understanding the strong dynamics of QCD itself, but…

Drawing on experimental data for baryon resonances, Hamiltonian effective field theory (HEFT) is used to predict the positions of the finite-volume energy levels to be observed in lattice QCD simulations of the lowest-lying $J^P=1/2^-$…

High Energy Physics - Lattice · Physics 2016-03-01 Zhan-Wei Liu , Waseem Kamleh , Derek B. Leinweber , Finn M. Stokes , Anthony W. Thomas , Jia-Jun Wu
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