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Related papers: T-violation tests for relativity principles

200 papers

Supersymmetry with R-parity violation (RPV) provides an interesting framework for naturally accommodating small neutrino masses. Within this framework, we discuss the lepton-flavour violating (LFV) processes mu -> e gamma, mu -> eee, and mu…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. de Gouvea , S. Lola , K. Tobe

We point out two simple but instructive possibilities to modify the tri-bimaximal neutrino mixing ansatz, such that leptonic CP violation can naturally be incorporated into the resultant scenarios of nearly tri-bimaximal flavor mixing. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-zhong Xing

If observed, charged lepton flavour violation is a clear sign of new physics - beyond the Standard Model minimally extended to accommodate neutrino oscillation data. We briefly review several extensions of the Standard Model which could…

High Energy Physics - Phenomenology · Physics 2017-10-11 Ana M. Teixeira

We study the possibility of measuring T (time reversal) violation in a future long baseline neutrino oscillation experiment. By assuming a neutrino factory as a staging scenario of a muon collider at the J-PARC site, we find that the…

High Energy Physics - Phenomenology · Physics 2024-12-19 Ryuichiro Kitano , Joe Sato , Sho Sugama

Heavy singlet neutrinos admit Majorana masses which are not possible for the Standard Model particles. This suggest new possibilities for generating the masses and mixing angles of light neutrinos. We present a model of neutrino physics…

High Energy Physics - Phenomenology · Physics 2008-11-26 Micheal S. Berger , Samuel Santana

We study whether the individual violation of the lepton numbers L_{e,mu,tau} in the charged sector can lead to measurable rates for BR(mu->e gamma) and BR(tau->mu gamma). We consider three different scenarios, the fist one corresponds to…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. E. Gomez , D. F. Carvalho

We examine the impact of Lorentz Invariance Violation (LIV) in measuring the octant of $\theta_{23}$ and CP phases in the context of the Deep Underground Neutrino Experiment (DUNE). We consider the CPT-violating LIV parameters involving $e…

High Energy Physics - Phenomenology · Physics 2021-03-10 Sanjib Kumar Agarwalla , Mehedi Masud

In this report we have studied the implication of a parity and charge-parity (PCP) violating interaction in varying alpha theory. Due to this interaction, the state of photon polarization can change when it passes through a strong…

High Energy Physics - Phenomenology · Physics 2011-11-15 Debaprasad Maity , Pisin Chen

We show that experimental probes of the P-conserving, T-violating triple correlation in polarized neutron or nuclear $\beta$-decay provide a unique probe of possible T-violation at the TeV scale in the presence of right-handed neutrinos. In…

High Energy Physics - Phenomenology · Physics 2017-12-22 Basem Kamal El-Menoufi , Michael J. Ramsey-Musolf , Chien-Yeah Seng

If observed, charged lepton flavour violation is a clear sign of new physics - beyond the Standard Model minimally extended to accommodate neutrino oscillation data. After a brief review of several charged lepton flavour violation…

High Energy Physics - Phenomenology · Physics 2016-12-20 Ana M. Teixeira

With only three flavors it is possible to account for various neutrino oscillation experiments. The masses and mixing angles for three neutrinos can be determined from the available experimental data on neutrino oscillation and from the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Rathin Adhikari , Gordana Omanovic

This talk will address how various experiments will address the following issues: the $\nu_e$ flavor content of the 3rd neutrino mass eigenstates, $\sin^2 \theta_{13}$, the mass ordering of the neutrinos, ${\rm sign}(\delta m^2_{31})$ and…

High Energy Physics - Phenomenology · Physics 2008-07-22 Stephen J. Parke

Global analyses of neutrino data suggest that the mixing angle $\theta_{23}$ is likely to be nonmaximal with two closely matched solutions emerging: one representing a smaller angle ($\theta_{23}$ < $\pi/4$) and the other a larger angle…

High Energy Physics - Phenomenology · Physics 2024-10-01 Saurabh Shukla , Shashank Mishra , Lakhwinder Singh , Venktesh Singh

We analyze possible violations of the Equivalence Principle in scalar-tensor gravity at finite temperature $T.$ Before we present an approach where the Equivalence Principle violation is achieved within the framework of Quantum Field…

General Relativity and Quantum Cosmology · Physics 2019-04-19 Massimo Blasone , Salvatore Capozziello , Gaetano Lambiase , Luciano Petruzziello

The two long-baseline experiments T2K and NO$\nu$A have recently presented new findings. T2K has shown the first $\bar \nu_e$ appearance data while NO$\nu$A has released the first $\nu_e$ appearance results. These data are of particular…

High Energy Physics - Phenomenology · Physics 2016-05-04 Antonio Palazzo

A class of extensions of the Standard Model allows Lorentz and CPT violations, which can be identified by the observation of sidereal modulations in the neutrino interaction rate. A search for such modulations was performed using the T2K…

High Energy Physics - Experiment · Physics 2017-07-05 K. Abe , J. Amey , C. Andreopoulos , M. Antonova , S. Aoki , A. Ariga , S. Assylbekov , D. Autiero , S. Ban , F. C. T. Barbato , M. Barbi , G. J. Barker , G. Barr , C. Barry , P. Bartet-Friburg , M. Batkiewicz , V. Berardi , S. Berkman , S. Bhadra , S. Bienstock , A. Blondel , S. Bolognesi , S. Bordoni , S. B. Boyd , D. Brailsford , A. Bravar , C. Bronner , M. Buizza Avanzini , R. G. Calland , T. Campbell , S. Cao , S. L. Cartwright , R. Castillo , M. G. Catanesi , A. Cervera , A. Chappell , C. Checchia , D. Cherdack , N. Chikuma , G. Christodoulou , A. Clifton , J. Coleman , G. Collazuol , D. Coplowe , L. Cremonesi , A. Cudd , A. Dabrowska , G. De Rosa , T. Dealtry , P. F. Denner , S. R. Dennis , C. Densham , D. Dewhurst , F. Di Lodovico , S. Di Luise , S. Dolan , O. Drapier , K. E. Duffy , J. Dumarchez , M. Dunkman , M. Dziewiecki , S. Emery-Schrenk , A. Ereditato , T. Feusels , A. J. Finch , G. A. Fiorentini , M. Friend , Y. Fujii , D. Fukuda , Y. Fukuda , A. P. Furmanski , V. Galymov , A. Garcia , S. G. Giffin , C. Giganti , F. Gizzarelli , T. Golan , M. Gonin , N. Grant , D. R. Hadley , L. Haegel , J. T. Haigh , P. Hamilton , D. Hansen , J. Harada , T. Hara , M. Hartz , T. Hasegawa , N. C. Hastings , T. Hayashino , Y. Hayato , R. L. Helmer , M. Hierholzer , A. Hillairet , A. Himmel , T. Hiraki , A. Hiramoto , S. Hirota , M. Hogan , J. Holeczek , F. Hosomi , K. Huang , A. K. Ichikawa , K. Ieki , M. Ikeda , J. Imber , J. Insler , R. A. Intonti , T. J. Irvine , T. Ishida , T. Ishii , E. Iwai , K. Iwamoto , A. Izmaylov , A. Jacob , B. Jamieson , M. Jiang , S. Johnson , J. H. Jo , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , D. Karlen , I. Karpikov , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , D. Kielczewska , T. Kikawa , H. Kim , J. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , T. Koga , A. Konaka , K. Kondo , A. Kopylov , L. L. Kormos , A. Korzenev , Y. Koshio , K. Kowalik , W. Kropp , Y. Kudenko , R. Kurjata , T. Kutter , J. Lagoda , I. Lamont , M. Lamoureux , E. Larkin , P. Lasorak , M. Laveder , M. Lawe , M. Lazos , M. Licciardi , T. Lindner , Z. J. Liptak , R. P. Litchfield , X. Li , A. Longhin , J. P. Lopez , T. Lou , L. Ludovici , X. Lu , L. Magaletti , K. Mahn , M. Malek , S. Manly , L. Maret , A. D. Marino , J. Marteau , J. F. Martin , P. Martins , S. Martynenko , T. Maruyama , V. Matveev , K. Mavrokoridis , W. Y. Ma , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , P. Mijakowski , A. Minamino , O. Mineev , S. Mine , A. Missert , M. Miura , S. Moriyama , J. Morrison , Th. A. Mueller , S. Murphy , J. Myslik , T. Nakadaira , M. Nakahata , K. G. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakanishi , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , C. Nielsen , M. Nirkko , K. Nishikawa , Y. Nishimura , P. Novella , J. Nowak , H. M. O'Keeffe , R. Ohta , K. Okumura , T. Okusawa , W. Oryszczak , S. M. Oser , T. Ovsyannikova , R. A. Owen , Y. Oyama , V. Palladino , J. L. Palomino , V. Paolone , N. D. Patel , P. Paudyal , M. Pavin , D. Payne , J. D. Perkin , Y. Petrov , L. Pickard , L. Pickering , E. S. Pinzon Guerra , C. Pistillo , B. Popov , M. Posiadala-Zezula , J. -M. Poutissou , R. Poutissou , P. Przewlocki , B. Quilain , T. Radermacher , E. Radicioni , P. N. Ratoff , M. Ravonel , M. A. Rayner , A. Redij , E. Reinherz-Aronis , C. Riccio , P. Rojas , E. Rondio , B. Rossi , S. Roth , A. Rubbia , A. C. Ruggeri , A. Rychter , R. Sacco , K. Sakashita , F. Sánchez , F. Sato , E. Scantamburlo , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , R. Shah , A. Shaikhiev , F. Shaker , D. Shaw , M. Shiozawa , T. Shirahige , S. Short , M. Smy , J. T. Sobczyk , H. Sobel , M. Sorel , L. Southwell , P. Stamoulis , J. Steinmann , T. Stewart , P. Stowell , Y. Suda , S. Suvorov , A. Suzuki , K. Suzuki , S. Y. Suzuki , Y. Suzuki , R. Tacik , M. Tada , S. Takahashi , A. Takeda , Y. Takeuchi , R. Tamura , H. K. Tanaka , H. A. Tanaka , D. Terhorst , R. Terri , T. Thakore , L. F. Thompson , S. Tobayama , W. Toki , T. Tomura , C. Touramanis , T. Tsukamoto , M. Tzanov , Y. Uchida , A. Vacheret , M. Vagins , Z. Vallari , G. Vasseur , C. Vilela , T. Vladisavljevic , T. Wachala , K. Wakamatsu , C. W. Walter , D. Wark , W. Warzycha , M. O. Wascko , A. Weber , R. Wendell , R. J. Wilkes , M. J. Wilking , C. Wilkinson , J. R. Wilson , R. J. Wilson , C. Wret , Y. Yamada , K. Yamamoto , M. Yamamoto , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , J. Yoo , K. Yoshida , T. Yuan , M. Yu , A. Zalewska , J. Zalipska , L. Zambelli , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito , J. Żmuda

It is well known that a fundamental theorem of Quantum Field Theory (QFT) set in at spacetime ensures the CPT invariance of the theory. This symmetry is strictly connected to the Lorentz covariance, and consequently to the fundamental…

High Energy Physics - Phenomenology · Physics 2021-10-19 Vito Antonelli , Lino Miramonti , Marco Danilo Claudio Torri

Lorentz invariance is one of the fundamental principles of physics, and, as such, it must be experimentally tested. The purpose of this work is to obtain, within the Standard-Model Extension, the dynamics of a Lorentz-violating spinor in a…

High Energy Physics - Phenomenology · Physics 2013-11-12 Yuri Bonder

Neutrino flavour oscillation is one of the primary indication of the existence of new physics beyond standard model. The presence of small neutrino mass is indispensable to explicate the oscillation among different flavours of neutrino. By…

High Energy Physics - Phenomenology · Physics 2023-01-31 Trisha Sarkar

A relativistic theory for neutrino superluminality is presented (in principle, the same mechanism applies also to other fermions). The theory involves the standard-model particles and one additional heavy sterile neutrino with an…

High Energy Physics - Phenomenology · Physics 2017-08-23 F. R. Klinkhamer