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Related papers: CPT and Lorentz tests with muons

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If there exists Lorentz and CPT violation in nature, then it is crucial to discover and understand the underlying mechanism. In this contribution, we discuss one such mechanism which relies on four-dimensional chiral gauge theories defined…

High Energy Physics - Theory · Physics 2018-10-25 F. R. Klinkhamer

We present a systematic phenomenological analysis of the tests of CPT symmetry that are possible within an {\em open} quantum-mechanical description of the neutral kaon system that is motivated by arguments based on quantum gravity and…

High Energy Physics - Phenomenology · Physics 2009-09-11 J. Ellis , J. Lopez , N. Mavromatos , D. Nanopoulos

Atomic clock comparisons provide some of the most precise tests of Lorentz and CPT symmetries in the laboratory. With data from multiple such experiments using different nuclei, it is possible to constrain new regions of the parameter space…

High Energy Physics - Phenomenology · Physics 2014-11-18 Brett Altschul

We have witnessed a persistent puzzling anomaly in the muon magnetic moment that cannot be accounted for in the Standard Model even considering the large hadronic uncertainties. A new measurement is forthcoming, and it might give rise to a…

High Energy Physics - Phenomenology · Physics 2022-08-30 Alvaro S. de Jesus , Sergey Kovalenko , Farinaldo S. Queiroz , Carlos A. de S. Pires , Yoxara S. Villamizar

In light of the increasing hints of new physics at the muon $g-2$ and neutrino oscillation experiments, we consider the recently observed tension in the long-baseline neutrino oscillation experiments as a potential indication of Lorentz…

High Energy Physics - Phenomenology · Physics 2022-06-08 Hai-Xing Lin , Pedro Pasquini , Jian Tang , Sampsa Vihonen

Muon neutrino and antineutrino disappearance probabilities are identical in the standard three-flavor neutrino oscillation framework, but CPT violation and non-standard interactions can violate this symmetry. In this work we report the…

High Energy Physics - Experiment · Physics 2023-10-17 K. Abe , N. Akhlaq , R. Akutsu , H. Alarakia-Charles , A. Ali , Y. I. Alj Hakim , S. Alonso Monsalve , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , T. Arihara , Y. Asada , Y. Ashida , E. T. Atkin , M. Barbi , G. J. Barker , G. Barr , D. Barrow , M. Batkiewicz-Kwasniak , F. Bench , V. Berardi , L. Berns , S. Bhadra , A. Blanchet , A. Blondel , S. Bolognesi , T. Bonus , S. Bordoni , S. B. Boyd , A. Bravar , C. Bronner , S. Bron , A. Bubak , M. Buizza Avanzini , J. A. Caballero , N. F. Calabria , S. Cao , D. Carabadjac , A. J. Carter , S. L. Cartwright , M. P. Casado , M. G. Catanesi , A. Cervera , J. Chakrani , D. Cherdack , P. S. Chong , G. Christodoulou , A. Chvirova , M. Cicerchia , J. Coleman , G. Collazuol , L. Cook , A. Cudd , C. Dalmazzone , T. Daret , P. Dasgupta , Yu. I. Davydov , A. De Roeck , G. De Rosa , T. Dealtry , C. C. Delogu , C. Densham , A. Dergacheva , F. Di Lodovico , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , A. J. Finch , G. A. Fiorentini Aguirre , G. Fiorillo , M. D. Fitton , J. M. Franco Patiño , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , K. Fusshoeller , L. Giannessi , C. Giganti , V. Glagolev , M. Gonin , J. González Rosa , E. A. G. Goodman , A. Gorin , M. Grassi , M. Guigue , D. R. Hadley , J. T. Haigh , P. Hamacher-Baumann , D. A. Harris , M. Hartz , T. Hasegawa , S. Hassani , N. C. Hastings , Y. Hayato , D. Henaff , A. Hiramoto , M. Hogan , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , M. Ishitsuka , H. T. Israel , K. Iwamoto , A. Izmaylov , N. Izumi , M. Jakkapu , B. Jamieson , S. J. Jenkins , C. Jesús-Valls , J. J. Jiang , J. Y. Ji , P. Jonsson , S. Joshi , C. K. Jung , P. B. Jurj , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , S. P. Kasetti , Y. Kataoka , Y. Katayama , T. Katori , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kikutani , S. King , V. Kiseeva , J. Kisiel , T. Kobata , H. Kobayashi , T. Kobayashi , L. Koch , S. Kodama , A. Konaka , L. L. Kormos , Y. Koshio , A. Kostin , T. Koto , K. Kowalik , Y. Kudenko , Y. Kudo , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , M. La Commara , L. Labarga , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , M. Lamoureux , A. Langella , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , Y. Lee , C. Lin , S. -K. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , K. R. Long , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , M. Mandal , S. Manly , A. D. Marino , L. Marti-Magro , D. G. R. Martin , M. Martini , J. F. Martin , T. Maruyama , T. Matsubara , V. Matveev , C. Mauger , K. Mavrokoridis , E. Mazzucato , N. McCauley , J. McElwee , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , P. Mehta , L. Mellet , C. Metelko , M. Mezzetto , E. Miller , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , L. Munteanu , K. Nagai , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , A. Nakamura , H. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , T. V. Ngoc , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , K. Nishizaki , T. Nosek , F. Nova , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , T. Ogawa , R. Okada , W. Okinaga , K. Okumura , T. Okusawa , N. Ospina , L. Osu , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , J. Parlone , S. Parsa , J. Pasternak , M. Pavin , D. Payne , G. C. Penn , D. Pershey , L. Pickering , C. Pidcott , G. Pintaudi , C. Pistillo , B. Popov , A. J. Portocarrero Yrey , K. Porwit , M. Posiadala-Zezula , Y. S. Prabhu , F. Pupilli , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , M. A. Ramírez , P. N. Ratoff , M. Reh , C. Riccio , E. Rondio , S. Roth , N. Roy , A. Rubbia , A. C. Ruggeri , C. A. Ruggles , A. Rychter , K. Sakashita , F. Sánchez , G. Santucci , T. Schefke , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikhiev , F. Shaker , M. Shiozawa , W. Shorrock , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , A. J. Speers , R. Spina , I. A. Suslov , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , S. Tairafune , S. Takayasu , A. Takeda , Y. Takeuchi , K. Takifuji , H. K. Tanaka , H. Tanigawa , Y. Tanihara , M. Tani , A. Teklu , V. V. Tereshchenko , N. Teshima , N. Thamm , L. F. Thompson , W. Toki , C. Touramanis , T. Towstego , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , D. Vargas , M. Varghese , G. Vasseur , C. Vilela , E. Villa , W. G. S. Vinning , U. Virginet , T. Vladisavljevic , T. Wachala , D. Wakabayashi , J. G. Walsh , Y. Wang , 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 , Y. -h. Xu , K. Yamamoto , T. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , M. Yu , R. Zaki , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , X. Zhao , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

Recent Standard Model predictions for the anomalous magnetic moments of the electron, muon and tau lepton are reviewed and compared to the latest experimental values.

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Passera

The limits on lepton radii and contact interaction scales are used to derive limits on the deviations of lepton anomalous magnetic dipole moments (g-2)/2 from the Standard Model predictions. In the case of quadratic dependence of the…

High Energy Physics - Phenomenology · Physics 2025-06-19 Dimitri Bourilkov

A search for a sidereal modulation in the MINOS near detector neutrino data was performed. If present, this signature could be a consequence of Lorentz and CPT violation as predicted by a class of extensions to the Standard Model. No…

High Energy Physics - Experiment · Physics 2019-08-13 P. Adamson

The feasibility of placing bounds on CPT violation from experiments with neutral-$B$ mesons is examined. We consider situations with uncorrelated mesons and ones with either unboosted or boosted correlated mesons. Analytical expressions…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alan Kostelecky , Rick Van Kooten

One of the current goals of neutrino experiments is to precisely determine standard unknown oscillation parameters such as the leptonic CP phase and mass hierarchy. Lorentz invariance violation represents a potential physics factor that…

High Energy Physics - Phenomenology · Physics 2024-12-02 Saurabh Shukla , Shashank Mishra , Lakhwinder Singh , Venktesh Singh

We present how to further the search for Lorentz and CPT violation in the top-quark sector after the first measurement in this sector by D0. We compute the Lorentz-violating matrix element for top pair production via gluon fusion, which…

High Energy Physics - Phenomenology · Physics 2020-11-13 Z. Liu

In this paper we investigate, within the standard model extension framework, the influence of Lorentz- and CPT-violating terms on gravitational quantum states of ultracold neutrons. Using a semiclassical wave packet, we derive the effective…

High Energy Physics - Theory · Physics 2018-06-06 A. Martín-Ruiz , C. A. Escobar

Recently Georgi has discussed the possible existence of `Unparticles' describable by operators having non-integral scaling dimensions. With the interaction of these with the Standard Model (SM) particles being constrained only by gauge and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Debajyoti Choudhury , Dilip Kumar Ghosh , Mamta

We investigate possible effects of unparticles at the MUonE experiment by considering a general model for unparticle with broken scale invariance, characterized by the scaling dimension $d$ and the energy scale $\mu$ at which the scale…

High Energy Physics - Phenomenology · Physics 2023-11-22 Duc Ninh Le , Van Dung Le , Duc Truyen Le , Van Cuong Le

We carry out a systematic study of the bounds that can be set on Planck-scale deformations of relativistic symmetries and CPT from precision measurements of particle and antiparticle lifetimes. Elaborating on our earlier work [1] we discuss…

High Energy Physics - Phenomenology · Physics 2020-09-08 Michele Arzano , Jerzy Kowalski-Glikman , Wojciech Wislicki

Although Lorentz symmetry has been tested at low energy with extremely good accuracy, its validity at very high energy is much less well established. If Lorentz symmetry violation (LSV) is energy-dependent (e.g. $\propto E^2$), it can be of…

General Physics · Physics 2016-10-26 Luis Gonzalez-Mestres

Quantitative bounds on Lorentz symmetry violation in the neutrino sector have been obtained by analyzing existing laboratory data on neutron $\beta$ decay and pion leptonic decays. In particular some parameters appearing in the…

High Energy Physics - Phenomenology · Physics 2009-11-11 E. Di Grezia , S. Esposito , G. Salesi

Proton decay experiments typically constrain baryon number violation to the scale of grand unified theories. From a phenomenological point of view, this makes direct probing of the associated new resonances, such as the X and Y bosons, out…

High Energy Physics - Phenomenology · Physics 2025-08-29 Amit Bhoonah , Francis Burk , Da Liu , Tong Ou , Deepak Sathyan

Fundamental physics could be described as having a muon problem. Discrepancies between theory and experiment in a number of muonic measurements ($r_P$, $a_\mu$, $H\rightarrow\mu\tau$, $\mathcal{R}_K$, $\mathcal{R}_{D^*}$) have been observed…

High Energy Physics - Phenomenology · Physics 2015-10-01 Henry Lamm