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Manifestations of P-,T-odd weak interaction between nucleons in nucleus are considered. Renormalization of this interaction due to residual strong interaction is studied. Mean squared matrix elements of P-,T-odd weak interaction between…

Nuclear Theory · Physics 2008-11-26 V. V. Flambaum , O. K. Vorov

Spin precession of channelled particles in bent crystals at the LHC gives unique possibility for measurements as electric and magnetic moments of charm, beauty and strange charged baryons so and constants determining CP ($T_{odd}, P_{odd}$)…

High Energy Physics - Phenomenology · Physics 2018-07-09 V. G. Baryshevsky

We calculate the electric dipole moments (EDM) of the neutral Hg(199) atom, deuteron, nucleons and neutral hyperons Lambda, Sigma(0) and Xi(0) in the framework of a generic SUSY model without R-parity conservation (RPV SUSY) on the basis of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Amand Faessler , Thomas Gutsche , Sergey Kovalenko , Valery E. Lyubovitskij

We investigate the constraints on four-Fermi contact interactions from low-energy lepton-quark and lepton-lepton scattering experiments --- polarization asymmetries in electron (muon)-nucleon scattering experiments, cesium and thallium atom…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gi-Chol Cho , Kaoru Hagiwara , Seiji Matsumoto

The T2K experiment reports updated measurements of neutrino and antineutrino oscillations using both appearance and disappearance channels. This result comes from an exposure of $14.9~(16.4) \times 10^{20}$ protons on target in neutrino…

High Energy Physics - Experiment · Physics 2021-06-23 T2K Collaboration , K. Abe , N. Akhlaq , R. Akutsu , A. Ali , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , T. Arihara , Y. Asada , Y. Ashida , E. T. Atkin , Y. Awataguchi , G. J. Barker , G. Barr , D. Barrow , M. Batkiewicz-Kwasniak , A. Beloshapkin , F. Bench , V. Berardi , L. Berns , S. Bhadra , A. Blanchet , A. Blondel , S. Bolognesi , T. Bonus , B. Bourguille , S. B. Boyd , A. Bravar , D. Bravo Bergu , C. Bronner , S. Bron , A. Bubak , M. Buizza Avanzini , S. Cao , S. L. Cartwright , M. G. Catanesi , A. Cervera , D. Cherdack , G. Christodoulou , M. Cicerchia , J. Coleman , G. Collazuol , L. Cook , D. Coplowe , A. Cudd , G. De Rosa , T. Dealtry , C. C. Delogu , S. R. Dennis , C. Densham , A. Dergacheva , F. Di Lodovico , S. Dolan , D. Douqa , T. A. Doyle , J. Dumarchez , P. Dunne , A. Eguchi , L. Eklund , S. Emery-Schrenk , A. Ereditato , A. J. Finch , G. Fiorillo , C. Francois , M. Friend , Y. Fujii , R. Fukuda , Y. Fukuda , K. Fusshoeller , C. Giganti , M. Gonin , A. Gorin , M. Grassi , M. Guigue , D. R. Hadley , P. Hamacher-Baumann , D. A. Harris , M. Hartz , T. Hasegawa , S. Hassani , N. C. Hastings , Y. Hayato , A. Hiramoto , M. Hogan , J. Holeczek , N. T. Hong Van , T. Honjo , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , M. Ishitsuka , K. Iwamoto , A. Izmaylov , N. Izumi , M. Jakkapu , B. Jamieson , S. J. Jenkins , C. Jes , P. Jonsson , C. K. Jung , P. B. Jurj , M. Kabirnezhad , H. Kakuno , J. Kameda , S. P. Kasetti , Y. Kataoka , Y. Katayama , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kikutani , S. King , J. Kisiel , T. Kobata , T. Kobayashi , L. Koch , A. Konaka , L. L. Kormos , Y. Koshio , A. Kostin , K. Kowalik , Y. Kudenko , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , M. Lamoureux , D. Last , M. Laveder , M. Lawe , R. P. Litchfield , S. L. Liu , A. Longhin , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , S. Manly , L. Maret , A. D. Marino , L. Marti-Magro , T. Maruyama , T. Matsubara , K. Matsushita , C. Mauger , K. Mavrokoridis , E. Mazzucato , N. McCauley , J. McElwee , K. S. McFarland , C. McGrew , A. Mefodiev , M. Mezzetto , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , Th. A. Mueller , L. Munteanu , Y. Nagai , T. Nakadaira , M. Nakahata , Y. Nakajima , A. Nakamura , K. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , T. V. Ngoc , V. Q. Nguyen , K. Niewczas , Y. Nishimura , E. Noah , T. S. Nonnenmacher , F. Nova , J. Nowak , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , T. Ogawa , R. Okada , K. Okumura , T. Okusawa , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , W. C. Parker , S. Parsa , J. Pasternak , M. Pavin , D. Payne , G. C. Penn , L. Pickering , C. Pidcott , G. Pintaudi , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , A. Pritchard , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Ratoff , C. Riccio , E. Rondio , S. Roth , A. Rubbia , A. C. Ruggeri , C. Ruggles , A. Rychter , K. Sakashita , F. S , G. Santucci , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikhiev , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , K. Skwarczynski , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , R. Spina , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , M. Tajima , A. Takeda , Y. Takeuchi , H. K. Tanaka , Y. Tanihara , M. Tani , N. Teshima , L. F. Thompson , W. Toki , C. Touramanis , T. Towstego , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , S. Valder , D. Vargas , G. Vasseur , C. Vilela , W. G. S. Vinning , T. Vladisavljevic , 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 , K. Wood , C. Wret , J. Xia , K. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , N. Yershov , M. Yokoyama , T. Yoshida , Y. Yoshimoto , M. Yu , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , M. Ziembicki , M. Zito , S. Zsoldos

(Abridged) Neutrino interactions beyond the standard model may affect the cosmological evolution and can be constrained through observations. We consider the possibility that neutrinos possess secret scalar or pseudoscalar interactions…

Cosmology and Nongalactic Astrophysics · Physics 2015-07-15 Francesco Forastieri , Massimiliano Lattanzi , Paolo Natoli

We study the effects of non-standard interactions (NSI) and the genuine CP phase $\delta_D$ in neutrino oscillations at low, $E_\nu \lesssim 1\,\mbox{GeV}$, and very low, $E_\nu \lesssim 0.1\,\mbox{GeV}$, energies. For experimental setup…

High Energy Physics - Phenomenology · Physics 2018-05-18 Shao-Feng Ge , Alexei Yu. Smirnov

Heavy quarks, namely, the top and bottom quarks, may show great sensitiveness to new physics effects. In particular, they might have unusually large electric dipole moments. This possibility is analyzed via the corresponding one-loop…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Cordero-Cid , J. M. Hernandez , G. Tavares-Velasco , J. J. Toscano

We discuss time reversal (T) violation in neutrino oscillations in generic new physics scenarios. A general parameterization is adopted to describe flavour evolution, which captures a wide range of new physics effects, including…

High Energy Physics - Phenomenology · Physics 2022-03-14 Thomas Schwetz , Alejandro Segarra

We present the first experimental test of Lorentz invariance using the frequency difference between counter-propagating modes in an asymmetric odd-parity optical resonator. This type of test is $\sim10^{4}$ more sensitive to odd-parity and…

General Relativity and Quantum Cosmology · Physics 2015-05-30 Fred Baynes , Andre Luiten , Michael Tobar

We constrain generic nonstandard neutrino interactions with existing experimental data on neutrino transition magnetic moments and derive strong bounds on tensorial couplings of neutrinos to charged fermions. We also discuss how some of…

High Energy Physics - Phenomenology · Physics 2014-04-24 Kristopher J. Healey , Alexey A. Petrov , Dmitry Zhuridov

The violation of parity (P) and time-reversal (T) symmetry is enhanced in the LaS, LaO and LuO molecules due to the existence of states of opposite parity with small energy differences and the presence of heavy nuclei. We calculate the…

Collective effects in deformed atomic nuclei present possible avenues of study on the non-spherical distribution of neutrons and the violation of the local Lorentz invariance. We introduce the weak quadrupole moment of nuclei, related to…

Nuclear Theory · Physics 2018-09-18 Bryce G. C. Lackenby , Victor V. Flambaum

We present a study of parity (P) violating contributions to the eigenenergies of stationary systems containing atoms in spatially inhomogeneous external electric fields. In this context the subtle interplay of P-violation and time reversal…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Bruss , T. Gasenzer , O. Nachtmann

We consider the decays of a correlated neutral-meson--antimeson state with C-parity +1. We show that there is CPT noninvariance in the mixing of the neutral mesons if, for any two decay modes f and g, the decay rate has a component R_A…

High Energy Physics - Phenomenology · Physics 2010-02-03 G. V. Dass , W. Grimus , L. Lavoura

From the recent measurement of parity nonconservation (PNC) in the Cs atom we have extracted the constant of the nuclear spin dependent electron-nucleon PNC interaction, $\kappa = 0.442 (63)$; the anapole moment constant, $\kappa_a = 0.364…

Nuclear Theory · Physics 2008-11-26 V. V. Flambaum , D. W. Murray

Parity violation experiments involving only two nucleons provide a way to study the non-leptonic, strangeness conserving part of the weak interaction in a clean measurement free of nuclear structure uncertainties. Although simple in…

Nuclear Experiment · Physics 2009-11-07 W. D. Ramsay

In Minkowski flat space-time, it is perceived that time inversion is unitary rather than antiunitary, with energy being a time vector changing sign under time inversion. The Dirac equation, in the case of electromagnetic interaction, is not…

Quantum Physics · Physics 2007-05-23 Wei Min Jin

Measurements are ordinarily described with respect to absolute "Newtonian" time. In reality however, the switching-on of the measuring device at the instance of the measurement requires a timing device. Hence the classical time $t$ must be…

Quantum Physics · Physics 2009-10-31 Aharon Casher , Benni Reznik

We employ the $Z$-vector method in the four-component relativistic coupled-cluster framework to calculate the parity (${\mathcal{P}}$) and time-reversal (${\mathcal{T}}$) symmetry violating scalar-pseudoscalar (S-PS) nucleus-electron…

Atomic Physics · Physics 2019-03-27 Kaushik Talukdar , Malaya K. Nayak , Nayana Vaval , Sourav Pal