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In the minimal left-right symmetric model, there are only two intrinsic CP violating phases to account for all CP violation in both the quark and lepton sectors, if CP is broken spontaneously by the complex phases in the VEV's of the scalar…

High Energy Physics - Phenomenology · Physics 2009-11-10 Mu-Chun Chen , K. T. Mahanthappa

We investigate the prediction on the lepton phases in theories with a non trivial correlation between quark (CKM) and lepton (PMNS) mixing matrices. We show that the actual evidence, under the only assumption that the correlation matrix…

High Energy Physics - Phenomenology · Physics 2008-12-18 Marco Picariello

We introduce the CP violating scalar leptoquark $S_3$ to explain the measured values of the lepton universality ratios $R_{K^{(*)}}$. We derive constraints on the CP-even and CP-odd components of the leptoquark Yukawa couplings stemming…

High Energy Physics - Phenomenology · Physics 2021-09-10 Nejc Košnik , Aleks Smolkovič

In the light of recent experimental results on $\theta_{13}^{pmns}$, we re-investigate the complementarity between the quark and lepton mixing matrices and obtain predictions for most unsettled neutrino mixing parameters like…

High Energy Physics - Phenomenology · Physics 2016-08-23 Gazal Sharma , B. C. Chauhan

The current laws of physics do not explain the observed imbalance of matter and antimatter in the universe. Sakharov proposed that an explanation would require the violation of CP symmetry between matter and antimatter. The only CP…

High Energy Physics - Experiment · Physics 2021-01-26 K. Abe , R. Akutsu , A. Ali , C. Alt , C. Andreopoulos , L. Anthony , M. Antonova , S. Aoki , A. Ariga , Y. Asada , Y. Ashida , E. T. Atkin , Y. Awataguchi , S. Ban , M. Barbi , G. J. Barker , G. Barr , C. Barry , M. Batkiewicz-Kwasniak , A. Beloshapkin , F. Bench , V. Berardi , S. Berkman , L. Berns , S. Bhadra , S. Bienstock , A. Blondel , S. Bolognesi , B. Bourguille , S. B. Boyd , D. Brailsford , A. Bravar , D. Bravo Berguño , C. Bronner , A. Bubak , M. Buizza Avanzini , J. Calcutt , T. Campbell , S. Cao , S. L. Cartwright , M. G. Catanesi , A. Cervera , A. Chappell , C. Checchia , D. Cherdack , N. Chikuma , G. Christodoulou , J. Coleman , G. Collazuol , L. Cook , D. Coplowe , A. Cudd , A. Dabrowska , G. De Rosa , T. Dealtry , P. F. Denner , S. R. Dennis , C. Densham , F. Di Lodovico , N. Dokania , S. Dolan , O. Drapier , J. Dumarchez , P. Dunne , L. Eklund , S. Emery-Schrenk , A. Ereditato , P. Fernandez , T. Feusels , A. J. Finch , G. A. Fiorentini , G. Fiorillo , C. Francois , M. Friend , Y. Fujii , R. Fujita , D. Fukuda , R. Fukuda , Y. Fukuda , K. Gameil , C. Giganti , T. Golan , M. Gonin , A. Gorin , M. Guigue , D. R. Hadley , J. T. Haigh , P. Hamacher-Baumann , M. Hartz , T. Hasegawa , N. C. Hastings , T. Hayashino , Y. Hayato , A. Hiramoto , M. Hogan , J. Holeczek , N. T. Hong Van , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , T. Ishii , M. Ishitsuka , K. Iwamoto , A. Izmaylov , B. Jamieson , S. J. Jenkins , C. Jesús-Valls , M. Jiang , S. Johnson , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , D. Karlen , S. P. Kasetti , Y. Kataoka , T. Katori , Y. Kato , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kim , J. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , T. Koga , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , H. Kubo , Y. Kudenko , N. Kukita , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , M. Lamoureux , M. Laveder , M. Lawe , M. Licciardi , T. Lindner , R. P. Litchfield , S. L. Liu , X. Li , A. Longhin , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , S. Manly , L. Maret , A. D. Marino , J. F. Martin , T. Maruyama , T. Matsubara , K. Matsushita , V. Matveev , K. Mavrokoridis , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , J. Morrison , Th. A. Mueller , L. Munteanu , S. Murphy , Y. Nagai , T. Nakadaira , M. Nakahata , Y. Nakajima , A. Nakamura , K. G. Nakamura , K. Nakamura , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , T. V. Ngoc , K. Niewczas , K. Nishikawa , Y. Nishimura , T. S. Nonnenmacher , F. Nova , P. Novella , J. Nowak , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , K. Okumura , T. Okusawa , S. M. Oser , R. A. Owen , Y. Oyama , V. Palladino , J. L. Palomino , V. Paolone , W. C. Parker , P. Paudyal , M. Pavin , D. Payne , G. C. Penn , L. Pickering , C. Pidcott , G. Pintaudi , E. S. Pinzon Guerra , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , A. Pritchard , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Ratoff , E. Reinherz-Aronis , C. Riccio , E. Rondio , S. Roth , A. Rubbia , A. C. Ruggeri , A. Rychter , K. Sakashita , F. Sánchez , C. M. Schloesser , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , R. Shah , A. Shaikhiev , F. Shaker , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , A. Smirnov , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , J. Steinmann , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , M. Tajima , A. Takeda , Y. Takeuchi , H. K. Tanaka , H. A. Tanaka , S. Tanaka , L. F. Thompson , W. Toki , C. Touramanis , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , W. Uno , M. Vagins , S. Valder , Z. Vallari , D. Vargas , G. Vasseur , C. Vilela , W. G. S. Vinning , T. Vladisavljevic , V. V. Volkov , T. Wachala , J. Walker , J. G. Walsh , Y. Wang , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , R. J. Wilson , K. Wood , C. Wret , Y. Yamada , K. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , S. Yen , N. Yershov , M. Yokoyama , T. Yoshida , M. Yu , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos , A. Zykova

We consider a class of models of neutrino mixing with $S_4$ lepton flavour symmetry combined with a generalised CP symmetry, which are broken to residual $Z_2$ and $Z_2 \times H^\nu_{\rm CP}$ symmetries in the charged lepton and neutrino…

High Energy Physics - Phenomenology · Physics 2017-12-07 J. T. Penedo , S. T. Petcov , A. V. Titov

I present the status of the elements and parameters of the Cabibbo-Kobayashi-Maskawa (CKM) matrix and summarise the related theoretical progress since "Lepton-Photon 2003". One finds |V_{us}| = 0.2227 +/- 0.0017 from K and tau decays and…

High Energy Physics - Phenomenology · Physics 2009-11-11 Ulrich Nierste

We study effects of CP violation in a modified bipair neutrino mixing scheme predicting $\sin^2\theta_{23}$ near both 0.4 and 0.6 currently consistent with experimentally allowed values. The source of CP violation is supplied by charged…

High Energy Physics - Phenomenology · Physics 2015-06-19 Jun Iizuka , Yoshikazu Kaneko , Teruyuki Kitabayashi , Naoto Koizumi , Masaki Yasue

We construct a supersymmetric model for leptons and quarks with the flavor symmetry Delta(384) and CP. The peculiar features of lepton and quark mixing are accomplished by the stepwise breaking of the flavor and CP symmetry. The correct…

High Energy Physics - Phenomenology · Physics 2020-02-17 Claudia Hagedorn , Johannes König

We derive predictions for the Dirac phase $\delta$ present in the $3\times 3$ unitary neutrino mixing matrix $U = U_e^{\dagger} \, U_{\nu}$, where $U_e$ and $U_{\nu}$ are $3\times 3$ unitary matrices which arise from the diagonalisation,…

High Energy Physics - Phenomenology · Physics 2015-11-10 I. Girardi , S. T. Petcov , A. V. Titov

The complex Clebsch-Gordon coefficients in the double tetrahedral group T' offers the possibility that CP violation can be entirely geometrical in origin, as pointed out by us recently. In this note, we investigate leptogenesis in a SUSY…

High Energy Physics - Phenomenology · Physics 2011-07-21 Mu-Chun Chen , K. T. Mahanthappa

We study the possibility of identifying the CP violating phases in the PMNS mixing matrix in the lepton sector and also that in the CKM mixing matrix in the quark sector with the phase responsible for the spontaneous CP violation in the…

High Energy Physics - Phenomenology · Physics 2011-03-21 Xiao-Gang He , Lu-Hsing Tsai

The high scale mixing unification hypothesis recently proposed by three of us (R. N. M., M. K. P. and G. R.) states that if at the seesaw scale, the quark and lepton mixing matrices are equal then for quasi-degenerate neutrinos, radiative…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. K. Agarwalla , M. K. Parida , R. N. Mohapatra , G. Rajasekaran

The area of the unitarity triangle is a measure of CP-violation. We introduce the leptonic unitarity triangles and study their properties. We consider the possibility of reconstructing the unitarity triangle in future oscillation and…

High Energy Physics - Phenomenology · Physics 2009-11-07 Y. Farzan , A. Yu. Smirnov

After the observation of non-zero $\theta_{13}$ the goal has shifted to observe $CP$ violation in the leptonic sector. Neutrino oscillation experiments can, directly, probe the Dirac $CP$ phases. Alternatively, one can measure $CP$…

High Energy Physics - Phenomenology · Physics 2016-05-04 Surender Verma , Shankita Bhardwaj

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

With the progress of increasingly precise measurements on the neutrino mixing angles, phenomenological relations such as quark-lepton complementarity (QLC) among mixing angles of quarks and leptons and self-complementarity (SC) among lepton…

High Energy Physics - Phenomenology · Physics 2012-11-20 Yijia Zhang , Xinyi Zhang , Bo-Qiang Ma

We explain all features of lepton and quark mixing in a scenario with the flavor symmetry Delta (384) and a CP symmetry, where these are broken in several steps. The residual symmetry in the neutrino and up quark sector is a Klein group and…

High Energy Physics - Phenomenology · Physics 2019-11-12 Claudia Hagedorn , Johannes König

We propose new classes of models which predict both tri-bimaximal lepton mixing and a right-angled Cabibbo-Kobayashi-Maskawa (CKM) unitarity triangle, alpha approximately 90 degrees. The ingredients of the models include a supersymmetric…

High Energy Physics - Phenomenology · Physics 2015-05-27 Stefan Antusch , Stephen F. King , Christoph Luhn , Martin Spinrath

Phenomenological issues of the CP violation in the quark sector of the Standard Model are discussed. We consider quark mixing in the SM, standard and Wolfenstein parametrization of the $CKM$ mixing matrix and unitarity triangle. We discuss…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Bilenky