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Related papers: Jarlskog determinant and data on flavor matrices

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The Nelson-Barr mechanism to solve the strong CP problem requires vector-like quarks (VLQs) to transmit the spontaneous CP breaking to the SM. We study the scenario where only these VLQs are within reach at the TeV scale while the…

High Energy Physics - Phenomenology · Physics 2020-09-02 A. L. Cherchiglia , C. C. Nishi

Measurements of CP asymmetries in B decays will soon be made at $B$ factories and hadron machines. In light of this, we review and update the profile of the CKM unitarity triangle and the resulting CP asymmetries in B decays. This is done…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ahmed Ali , David London

There is still a problem in neutrino physics related to the configuration of neutrino masses: Are neutrinos arranged by masses following the Standard Model as three generations of fundamental particles, Gen III>Gen II>Gen I, thus forming a…

High Energy Physics - Phenomenology · Physics 2021-09-06 Z. B. Todorovic

Most of the free parameters in the Standard Model (SM) -- a quantum field theory which has successfully elucidated the behaviors of strong, weak and electromagnetic interactions of all the known fundamental particles, come from the lepton…

High Energy Physics - Phenomenology · Physics 2020-05-20 Zhi-zhong Xing

In this paper we give a geometric parametrization to the Cabibbo-Kobayashi-Maskawa (CKM) mixing matrix and the Jarlskog invariant, which is based on two flag manifolds $SU(3)/U(1)^{2}$. To treat a fourth generation of quarks on CP violation…

Mathematical Physics · Physics 2010-01-07 Kazuyuki Fujii

We construct a model based on SUSY SO(10) combined with U(2) family symmetry including complex phases leading to CP violation. In contrast with the commonly used effective operator approach, \bar{126}-dimensional Higgs fields are utilized…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mu-Chun Chen , K. T. Mahanthappa

We propose that the flavor structure of the quark sector of the Standard Model is determined by a vectorial SU(2) flavor symmetry, which we dub Flavorspin, under which quarks transform as triplets. The fundamental Yukawa couplings are real…

High Energy Physics - Phenomenology · Physics 2015-07-03 Jeffrey Berryman , Daniel Hernández

In the present paper, I have re-examined the weak basis invariants at low energies, proposed by C. Jarlskog and Branco et. al, respectively, in their earlier analyses, after confronting them with the assumptions of two zeros and an equality…

High Energy Physics - Phenomenology · Physics 2020-10-14 Madan Singh

The Standard Model quark and neutrino mixing matrices are of independent empirical origin, but they do suggest unification. In this paper I obtained two united one-parameter quark and neutrino mixing matrices inferred from two…

High Energy Physics - Phenomenology · Physics 2009-03-11 E. M. Lipmanov

We address the problem of the apparently very small magnitude of CP violation in the standard model, measured by the Jarlskog invariant J. In order to make statements about probabilities for certain values of J, we seek to find a natural…

High Energy Physics - Phenomenology · Physics 2010-04-21 Gary W. Gibbons , Steffen Gielen , C. N. Pope , Neil Turok

It is known that the Cabibbo-Kobayashi-Maskawa (CKM) $n\times n$ matrix can be represented by a real matrix iff there is no CP-violation, and then the Jarlskog invariants vanish. We investigate sufficient conditions for the opposite…

High Energy Physics - Theory · Physics 2021-04-22 Klaus Bering

We review and update the constraints on the parameters of the quark flavour mixing matrix $V_{CKM}$ in the standard model and estimate the resulting CP asymmetries in $B$ decays, taking into account recent experimental and theoretical…

High Energy Physics - Phenomenology · Physics 2010-11-23 A. Ali , D. London

We rewrite the Yukawa interactions of the standard model in terms of flavour-dependent vacuum structure to address the family mass hierarchy and CP violation in both the quark sector and lepton sector. It is realized for the first time that…

High Energy Physics - Phenomenology · Physics 2022-01-17 Ying Zhang

The semileptonic decay of heavy flavor mesons offers a clean environment for extraction of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements, which describes the CP-violating and flavor changing process in the Standard Model. The involved…

High Energy Physics - Phenomenology · Physics 2021-03-17 Lu Zhang , Xian-Wei Kang , Xin-Heng Guo , Ling-Yun Dai , Tao Luo , Chao Wang

We assume that all quark and lepton $3 \times 3$ mass matrices which appear in the standard model lagrangian (after spontaneous symmetry breaking) with neutrinos treated as Dirac patricles have the triangular form. Such matrices have not…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Tatur , J. Bartelski

Harrison, Perkins and Scott have proposed simple charged lepton and neutrino mass matrices that lead to the tribimaximal mixing $U_{\rm TBM}$. We consider in this work an extension of the mass matrices so that the leptonic mixing matrix…

High Energy Physics - Phenomenology · Physics 2015-05-28 Y. H. Ahn , Hai-Yang Cheng , Sechul Oh

Given the $3\times 3$ Cabibbo-Kobayashi-Maskawa (CKM) quark flavor mixing matrix $V$, we define a new set of rephasing invariants in terms of the "trios" of its nine elements: $\lozenge^{ijk}_{\alpha\beta\gamma} \equiv (V^{}_{\alpha i}…

High Energy Physics - Phenomenology · Physics 2025-08-25 Shu Luo , Zhi-zhong Xing

Bayesian analysis results require a choice of prior distribution. In long-baseline neutrino oscillation physics, the usual parameterisation of the mixing matrix induces a prior that privileges certain neutrino mass and flavour state…

High Energy Physics - Experiment · Physics 2025-12-16 The T2K Collaboration , K. Abe , S. Abe , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , L. Anthony , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , Y. Ashida , E. T. Atkin , N. Babu , V. Baranov , G. J. Barker , G. Barr , D. Barrow , P. Bates , L. Bathe-Peters , M. Batkiewicz-Kwasniak , N. Baudis , V. Berardi , L. Berns , S. Bhattacharjee , A. Blanchet , A. Blondel , P. M. M. Boistier , S. Bolognesi , S. Bordoni , S. B. Boyd , C. Bronner , A. Bubak , M. Buizza Avanzini , J. A. Caballero , F. Cadoux , N. F. Calabria , S. Cao , S. Cap , D. Carabadjac , S. L. Cartwright , M. P. Casado , M. G. Catanesi , J. Chakrani , A. Chalumeau , D. Cherdack , P. S. Chong , A. Chvirova , J. Coleman , G. Collazuol , F. Cormier , A. A. L. Craplet , A. Cudd , D. D'ago , C. Dalmazzone , T. Daret , P. Dasgupta , C. Davis , Yu. I. Davydov , P. de Perio , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , A. J. Finch , M. D. Fitton , C. Forza , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , J. García-Marcos , A. C. Germer , L. Giannessi , C. Giganti , M. Girgus , V. Glagolev , M. Gonin , R. González Jiménez , J. González Rosa , E. A. G. Goodman , K. Gorshanov , P. Govindaraj , M. Grassi , M. Guigue , F. Y. Guo , D. R. Hadley , S. Han , D. A. Harris , R. J. Harris , T. Hasegawa , C. M. Hasnip , S. Hassani , N. C. Hastings , Y. Hayato , I. Heitkamp , D. Henaff , Y. Hino , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , M. C. F. Hooft , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. Ishida , M. Ishitsuka , H. Ito , S. Ito , A. Izmaylov , N. Jachowicz , S. J. Jenkins , C. Jesús-Valls , M. Jia , J. J. Jiang , J. Y. Ji , T. P. Jones , P. Jonsson , S. Joshi , M. Kabirnezhad , A. C. Kaboth , H. Kakuno , J. Kameda , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , A. Kawabata , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , S. King , V. Kiseeva , J. Kisiel , A. Klustová , L. Kneale , H. Kobayashi , L. Koch , S. Kodama , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , Y. Kudenko , Y. Kudo , A. Kumar Jha , R. Kurjata , V. Kurochka , T. Kutter , L. Labarga , M. Lachat , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , A. Langella , D. H. Langridge , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , D. Leon Silverio , S. Levorato , S. V. Lewis , B. Li , C. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , K. K. Mahtani , M. Mandal , S. Manly , A. D. Marino , D. G. R. Martin , D. A. Martinez Caicedo , L. Martinez , M. Martini , T. Matsubara , R. Matsumoto , V. Matveev , C. Mauger , K. Mavrokoridis , N. McCauley , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , L. Mellet , C. Metelko , M. Mezzetto , S. Miki , V. Mikola , E. W. Miller , A. Minamino , O. Mineev , S. Mine , J. Mirabito , M. Miura , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , A. Muñoz , L. Munteanu , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , A. Nakano , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , D. T. Nguyen , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , Y. Noguchi , T. Nosek , F. Nova , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , R. Okazaki , W. Okinaga , K. Okumura , T. Okusawa , N. Onda , N. Ospina , L. Osu , N. Otani , Y. Oyama , V. Paolone , J. Pasternak , D. Payne , M. Pfaff , L. Pickering , B. Popov , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , M. A. Ramirez , R. Ramsden , P. N. Ratoff , M. Reh , G. Reina , C. Riccio , D. W. Riley , E. Rondio , S. Roth , N. Roy , A. Rubbia , L. Russo , A. Rychter , W. Saenz , K. Sakashita , S. Samani , F. Sánchez , E. M. Sandford , Y. Sato , T. Schefke , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , T. Sekiya , D. Seppala , D. Sgalaberna , A. Shaikhiev , M. Shiozawa , Y. Shiraishi , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , A. J. Speers , R. Spina , A. Srivastava , P. Stowell , Y. Stroke , I. A. Suslov , A. Suzuki , S. Y. Suzuki , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , K. Takeya , H. K. Tanaka , H. Tanigawa , V. V. Tereshchenko , N. Thamm , C. Touramanis , N. Tran , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , M. Varghese , I. Vasilyev , G. Vasseur , E. Villa , U. Virginet , T. Vladisavljevic , T. Wachala , S. -i. Wada , D. Wakabayashi , H. T. Wallace , J. G. Walsh , L. Wan , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , K. Yamamoto , T. Yamamoto , C. Yanagisawa , Y. Yang , T. Yano , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , R. Zaki , A. Zalewska , J. Zalipska , G. Zarnecki , J. Zhang , X. Y. Zhao , H. Zheng , H. Zhong , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

These lectures give an introduction and the current status of flavour physics in the quark sector, with special attention to the CKM matrix and CP violation. We describe the measurements which contribute to the determination of the CKM…

High Energy Physics - Phenomenology · Physics 2009-09-29 Achille Stocchi

We study the connection between quark and lepton mass matrices in a supersymmetric SO(10) GUT model in six dimensions, compactified on an orbifold. The physical quarks and leptons are mixtures of brane and bulk states. This leads to a…

High Energy Physics - Phenomenology · Physics 2009-01-06 Wilfried Buchmuller , Laura Covi , David Emmanuel-Costa , Soren Wiesenfeldt
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