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Related papers: Flavor physics and Jarlskog determinant

200 papers

The introduction of a Flavour Symmetry can represent an interesting way in which one can try to find an answer to some intriguing problems in Flavour Physics, like the hierarchy between the fermion masses or the particular values of mixing…

High Energy Physics - Phenomenology · Physics 2009-05-07 Alfredo Urbano

Chiral thermodynamics of charmed mesons is formulated at finite temperature within a $2+1+1$-flavored effective Lagrangian incorporating heavy quark symmetry. The chiral mass splittings are shown to be less sensitive to the light-quark…

High Energy Physics - Phenomenology · Physics 2015-03-02 Chihiro Sasaki

We study a finite SU(5) grand unified model based on the non-Abelian discrete symmetry A_4. This model leads to the democratic structure of the mass matrices for the quarks and leptons. In the soft supersymmetry breaking sector, the scalar…

High Energy Physics - Phenomenology · Physics 2009-11-07 K. S. Babu , Tatsuo Kobayashi , Jisuke Kubo

Motivated by the success of A_4 in explaining neutrino tribimaximal mixing, and its approximate residual Z_3 symmetry in the quark and charged-lepton sectors, the notion of "flavor triality" is proposed. Under this hypothesis, certain…

High Energy Physics - Phenomenology · Physics 2011-11-23 Ernest Ma

Recent work on flavour changing neutral current effects in supersymmetric models is reviewed. The emphasis is put on new issues related to solutions to the flavour problem through new symmetries: GUTs, horizontal symmetries, modular…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. A. Savoy

The physics underlying quark and lepton masses and mixings (the "flavor problem") is the least well understood aspect of the Standard Model. Some questions of flavor physics, and ways in which the LHC can help shed light on this problem,…

High Energy Physics - Phenomenology · Physics 2014-11-20 Jonathan L. Rosner

It is pointed out that if a flavor symmetry (a discrete symmetry, a U(1) symmetry, and so on) exists, we cannot obtain the observed CKM quark mixing matrix V_q and MNS lepton mixing matrix U_\ell, even if we can obtain reasonable mass…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide

When the flavour content of QCD is increased sufficiently, the theory develops a non-trivial infra red fixed point. Thus, for a number of flavours above a certain critical value, but not yet so high that asymptotic freedom is lost, QCD…

High Energy Physics - Lattice · Physics 2010-01-21 Albert Deuzeman , Maria Paola Lombardo , Elisabetta Pallante

At non-zero lattice spacing the flavor symmetry of staggered fermions is broken to a discrete subgroup. We show that in the chiral limit the flavor symmetry of the pion effective Lagrangian enlarges to an SO(4) subgroup of the continuum…

High Energy Physics - Lattice · Physics 2009-10-31 Weonjong Lee , Stephen Sharpe

Previous work relating the flavour variation of the chiral order parameters $F_\pi$, $<\bar u u>$ and S-wave scattering data, based on chiral sum rules and chiral perturbation theory at order $p^4$, is extended to include $O(p^6)$…

High Energy Physics - Phenomenology · Physics 2011-07-19 Bachir Moussallam

The combination of flavor symmetries with grand unification is considered: GUT $ \times$ flavor . To accommodate three generations the flavor group SO(3) is used. All fermions transform as 3-vectors under this group. The Yukawa couplings…

High Energy Physics - Phenomenology · Physics 2011-01-07 Berthold Stech

This talk highlights, from a theoretical point of view, some recent exciting results in flavor physics, as well as future prospects. We discuss possible implications of a subset of the experimental results in tension with the standard…

High Energy Physics - Phenomenology · Physics 2016-06-21 Zoltan Ligeti

At the availability of a sharp interconnection, the difference in sizes with Dirac and Pauli form factors of a massive neutrino must constitute their linearly ordered set. Such a class of currents can lead in the field of a spinless nucleus…

General Physics · Physics 2013-11-26 Rasulkhozha S. Sharafiddinov

The chiral quark model with a broken U(3) symmetry gives a simple and unified account for the proton spin and flavor puzzles, as well as the octet baryon magnetic moments.

High Energy Physics - Phenomenology · Physics 2007-05-23 T. P. Cheng , Ling-Fong Li

This is a written version of a series of lectures aimed at graduate students and postdoctoral fellows in particle theory/string theory/particle experiment familiar with the basics of the Standard Model. We begin with an overview of flavor…

High Energy Physics - Phenomenology · Physics 2007-08-15 Yosef Nir

Orbifold grand unified theories (GUTs) solve several problems in GUT model building. Therefore, it is intriguing to investigate similar constructions in the flavor context. In this paper, we propose that a flavor symmetry might emerge due…

High Energy Physics - Phenomenology · Physics 2015-03-13 Adisorn Adulpravitchai , Michael A. Schmidt

Chiral symmetry restoration at nonzero temperature and quark densities are investigated in the framework of a linear sigma model with N_f=3 light quark flavors. After the derivation of the grand potential in mean-field approximation, the…

High Energy Physics - Phenomenology · Physics 2009-11-19 Bernd-Jochen Schaefer , Mathias Wagner

This review presents flavour related issues in the production and decays of heavy states at LHC, both from the experimental side and from the theoretical side. We review top quark physics and discuss flavour aspects of several extensions of…

High Energy Physics - Phenomenology · Physics 2008-12-18 T. Lari , L. Pape , W. Porod , J. A. Aguilar-Saavedra , F. del Aguila , B. C. Allanach , J. Alwall , Yu. Andreev , D. Aristizabal Sierra , A. Bartl , M. Beccaria , S. Bejar , L. Benucci , S. Bityukov , I. Borjanovic , G. Bozzi , G. Burdman , J. Carvalho , N. Castro , B. Clerbaux , F. de Campos , A. de Gouvea , C. Dennis , A. Djouadi , O. J. P. Eboli , U. Ellwanger , D. Fassouliotis , P. M. Ferreira , R. Frederix , B. Fuks , J. -M. Gerard , A. Giammanco , S. Gopalakrishna , T. Goto , B. Grzadkowski , J. Guasch , T. Hahn , S. Heinemeyer , A. Hektor , M. Herquet , B. Herrmann , K. Hidaka , M. K. Hirsch , K. Hohenwarter-Sodek , W. Hollik , G. W. S. Hou , T. Hurth , A. Ibarra , J. Illana , M. Kadastik , S. Kalinin , C. Karafasoulis , M. Karagoz Unel , T. Kernreiter , M. M. Kirsanov , M. Klasen , E. Kou , C. Kourkoumelis , S. Kraml , N. Krasnikov , F. Krauss , A. Kyriakis , V. Lemaitre , G. Macorini , M. B. Magro , W. Majerotto , F. Maltoni , R. Mehdiyev , M. Misiak , F. Moortgat , G. Moreau , M. Mühlleitner , M. Muntel , A. Onofre , E. Ozcan , F. Palla , L. Panizzi , L. Pape , S. Penaranda , R. Pittau , G. Polesello , A. Pukhov , M. Raidal , A. R. Raklev , L. Rebane , F. M. Renard , D. Restrepo , Z. Roupas , R. Santos , S. Schumann , G. Servant , F. Siegert , P. Skands , P. Slavich , J. Sola , M. Spira , S. Sultansoy , A. Toropin , A. Tricomi , J. Tseng , G. Unel , J. W. F. Valle , F. Veloso , A. Ventura , G. Vermisoglou , C. Verzegnassi , A. Villanova del Moral , G. Weiglein , M. Yilmaz

The quantum anomaly that breaks the U(1) axial symmetry of massless multi-flavored QCD leaves behind a discrete flavor-singlet chiral invariance. With massive quarks, this residual symmetry has a close connection with the strong…

High Energy Physics - Phenomenology · Physics 2011-07-14 Michael Creutz

This thesis is dedicated to the holographic study of flavor dynamics. The technique employed is a D7-brane probing of various D3-brane backgrounds. The first topic covered studies the influence of an external magnetic field on a flavored…

High Energy Physics - Theory · Physics 2008-09-29 Veselin G. Filev