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Related papers: Flavour Physics in the Littlest Higgs Model with T…

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The Littlest Higgs with T-parity Model (LHT) is one of the attractive candidates of physics beyond the Standard Model. In this study we focus on heavy gauge bosons and heavy leptons that LHT imposes, which are detectable at ILC. The mass…

High Energy Physics - Phenomenology · Physics 2012-03-06 Eriko Kato , Masaki Asano , Keisuke Fujii , Shigeki Matsumoto , Yosuke Takubo , Hitoshi Yamamoto

In the littlest Higgs model with T-parity (LHT) the mirror quarks induce the special flavor structures and some new flavor-changing (FC) couplings which could greatly enhance the production rates of the FC processes. We in this paper study…

High Energy Physics - Phenomenology · Physics 2011-05-30 Xuelei Wang , Jinzhong Han , Wujun Li , Hao Wang

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

We construct a three-Higgs doublet model with a flavour non-universal ${\rm U}(1)\times \mathbb{Z}_2$ symmetry. That symmetry induces suppressed flavour-changing interactions mediated by neutral scalars. New scalars with masses below the…

High Energy Physics - Phenomenology · Physics 2022-03-04 Dipankar Das , P. M. Ferreira , António P. Morais , Ian Padilla-Gay , Roman Pasechnik , J. Pedro Rodrigues

Based on calculating the contributions of the littlest Higgs model with T-parity (called $LHT$ model) to the anomalous top coupling $tq\gamma$ ($q=u$ or $c$), we consider single top production via the t-channel partonic process $eq\to et$…

High Energy Physics - Phenomenology · Physics 2009-06-19 Chong-Xing Yue , Jia Wen , Jin-Yan Liu , Wei Liu

After the completion of the Standard Model (SM) through the Higgs discovery particle physicists are waiting for the discovery of new particles either directly with the help of the Large Hadron Collider (LHC) or indirectly through quantum…

High Energy Physics - Phenomenology · Physics 2015-05-05 Andrzej J. Buras

The Little Flavor model is a close cousin of the Little Higgs theory which aims to generate flavor structure around TeV scale. While the original Little Flavor only included the quark sector, here we build the lepton part of the Little…

High Energy Physics - Phenomenology · Physics 2016-01-25 Sichun Sun

We analyze flavor constraints in the littlest Higgs model with T-parity. In particular, we focus on neutral meson mixing in the K, B, and D systems due to one loop contributions from T-parity odd fermions and gauge bosons. We calculate the…

High Energy Physics - Phenomenology · Physics 2009-11-11 Jay Hubisz , Seung J. Lee , Gil Paz

Extending the scalar sector helps in studying the Higgs mechanism and some Standard Model problems. We implement the correspondence between the gauge-dependent elementary states and the non-perturbative non-abelian gauge-invariant…

High Energy Physics - Phenomenology · Physics 2022-04-15 Leonardo Pedro

The main purpose of Heavy Flavor experiments is to discover physics beyond the Standard Model, or characterize it, should it be found elsewhere. Thus, current limits on New Physics (NP) are reviewed. New results are presented, some…

High Energy Physics - Phenomenology · Physics 2011-09-23 Sheldon Stone

Precision measures of electroweak and flavour observables, at both low and high energies, are highly complementary to direct searches for New Physics at high-energy colliders. Despite the discovery of the Higgs boson at the Large Hadron…

High Energy Physics - Phenomenology · Physics 2022-03-01 Jonathan Kriewald

We study the low energy phenomenology of the little Higgs model. We first discuss the linearized effective theory of the "littlest Higgs model" and study the low energy constraints on the model parameters. We identify sources of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tao Han , Heather E. Logan , Bob McElrath , Lian-Tao Wang

Minimal Flavour Violation hypothesis can provide an attractive framework for Dark Matter (DM). We consider scalar DM candidates carrying flavour quantum numbers and whose representation under the flavour group guarantees DM stability. They…

High Energy Physics - Phenomenology · Physics 2015-06-15 Laura Lopez-Honorez , Luca Merlo

We review the sources and phenomenology of non-minimal flavour violation in the MSSM. We discuss in some detail the most important theoretical and experimental constraints, as well as promising observables to look for supersymmetric effects…

High Energy Physics - Phenomenology · Physics 2009-02-18 Sebastian Jager

The littlest $Higgs$ model with T-parity (called the $LHT$ model) predicts the existence of the T-odd leptons, which can generate contributions to some leptonic processes at the one-loop level. We calculate their contributions to the…

High Energy Physics - Phenomenology · Physics 2009-02-10 Chong-Xing Yue , Jin-Yan Liu , Shi-Hai Zhu

Little Higgs models with T-parity can easily satisfy electroweak precision tests and at the same time give a stable particle which is a candidate for cold dark matter. In addition to little Higgs heavy gauge bosons, this type of models…

High Energy Physics - Phenomenology · Physics 2010-04-14 G. Cacciapaglia , S. Rai Choudhury , A. Deandrea , N. Gaur

We present results of global fits of all relevant experimental data on rare $b \to s$ decays. We observe significant tensions between the Standard Model predictions and the data. After critically reviewing the possible sources of…

High Energy Physics - Phenomenology · Physics 2015-09-30 Wolfgang Altmannshofer , David M. Straub

Based on a view of current flavour physics and motivated by the hierarchy problem and by the pattern of quark masses and mixings, I describe a picture of flavour physics that should give rise in a not too distant future to observable…

High Energy Physics - Phenomenology · Physics 2021-07-07 Riccardo Barbieri

We shortly review and emphasize how l_j -> l_i gamma experiments and the searches for lepton e.d.m. are constraining New Physics model building. They are pure signals of new phenomena around the TeV scale since the SM contributions are…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. Masina , C. A. Savoy

While the LHC did not observe direct evidence for physics beyond the standard model, indirect hints for new physics were uncovered in the flavour sector in the decays $B\to K^*\mu^+\mu^-$, $B\to K\mu^+\mu^-/B\to Ke^+e^-$,…

High Energy Physics - Phenomenology · Physics 2016-06-22 Andreas Crivellin