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Related papers: Antisymmetric rank--2 tensor unparticle physics

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The anomalous magnetic moment of the muon is one of the most precisely measured quantities in physics. Its experimental value exhibits a $4.2 \, \sigma$ discrepancy $\delta a_\mu=(251 \pm 59) \times 10^{-11}$ with its theoretical value…

General Physics · Physics 2021-04-20 Laurent Nottale

We study the muon anomalous magnetic moment $(g-2)_{\mu}$ in the context of the reduced minimal 3-3-1 model recently proposed in the literature. In particular, its spectrum contains a doubly charged scalar ($H^{\pm \pm}$) and gauge boson…

High Energy Physics - Phenomenology · Physics 2014-06-20 Chris Kelso , P. R. D. Pinheiro , Farinaldo S. Queiroz , William Shepherd

We study $SU(n)$ symmetry breaking by rank three and rank two antisymmetric tensor fields. Using tensor analysis, we derive branching rules for the adjoint and antisymmetric tensor representations, and explain why for general $SU(n)$ one…

High Energy Physics - Theory · Physics 2015-05-22 Stephen L. Adler

The role of nonvalence, {\it e.g.} sea quarks and/or meson degrees of freedom in static and quasistatic baryon electroweak observables, is discussed within the phenomenological sum rule approach. The inclusion of nonvalence degrees of…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. B. Gerasimov

In models with a low quantum gravity scale, one might expect sizable effects from nonrenormalizable interactions that violate the global symmetries of the standard model. While some mechanism must be invoked in such theories to suppress…

High Energy Physics - Phenomenology · Physics 2009-11-07 Carl E. Carlson , Christopher D. Carone

The recent measurement of the muon anomalous magnetic dipole moment shows 2.6$\sigma$ deviation of $a_\mu$ from the standard model prediction which can be explained by a chargino-sneutrino loop correction in the supersymmetric models. In…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yasuhiro Daikoku

We show that lepton number violating muon decays, \mu^+ -> e^+ + \nu_e-bar + \nu_i-bar (i=e, \mu or \tau), can consistently explain the neutrino anomaly reported by the LSND experiment. Two effective operators in the Standard Model are…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. S. Babu , Sandip Pakvasa

The electromagnetic structure of axial-vector mesons is investigated via elastic and two-photon transition form factors (TFFs). To this end, we employ a framework based on the Dyson-Schwinger and Bethe-Salpeter equations within a contact…

High Energy Physics - Phenomenology · Physics 2025-09-23 Zanbin Xing , Lei Chang , Khépani Raya

We search for evidence of a light scalar boson in the radiative decays of the Upsilon(2S) and Upsilon(3S) resonances: Upsilon(2S,3S)-> gamma A0, A0 -> mu^+ mu^-. Such a particle appears in extensions of the Standard Model, where a light…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

As one of the extensions of the Standard Model, we investigate the anomalous four-point $\tau-W-\nu_\tau-\gamma$ scalar- and tensor-type interactions, which originate from the gauge invariant dimension-five operators. The coupling constants…

High Energy Physics - Phenomenology · Physics 2017-03-16 N. Shimizu , D. Epifanov , J. Sasaki

Low energy phenomenology of the unparticle physics associated with an exact scale invariant sector possessing a non-trivial infrared fixed point at a higher energy scale is explored for both electron-positron and hadronic colliders. Feynman…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kingman Cheung , Wai-Yee Keung , Tzu-Chiang Yuan

We study the effects of extra dimension on the muon anomalous magnetic moment in the stabilized Randall-Sundrum scenario. The effects of the Kaluza-Klein states heavier than the cut-off scale expected to be of order $\Lambda_\pi$ are…

High Energy Physics - Phenomenology · Physics 2009-11-07 Seong Chan Park , H. S. Song

Asymmetry measurements in $e^+e^-\to\tau^+\tau^-$ constitute a promising avenue to obtain competitive constraints on the $\tau$ dipole moments, the anomalous magnetic moment $a_\tau$ and the electric dipole moment $d_\tau$, especially, once…

High Energy Physics - Phenomenology · Physics 2026-04-21 Joël Gogniat , Martin Hoferichter , Gabriele Levati

Supersymmetric contributions to all leptonic electromagnetic dipole operators have essentially identical diagramatic structure. With approximate slepton universality this allows the muon anomalous magnetic moment to be related to the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Michael Graesser , Scott Thomas

We have studied the leptonic EDM and the LFV decays relating with the recent data of anomalous magnetic moment of muon, $(g-2)_{\mu}$ in the leptonic dipole operator. We have adopted the successful $\Gamma_2$ modular invariant model by…

High Energy Physics - Phenomenology · Physics 2024-12-18 Takaaki Nomura , Morimitsu Tanimoto , Xing-Yu Wang

We analyze allowed region of muon anomalous magnetic moment (muon $g-2$), satisfying lepton flavor violations, $Z$ boson decays, and collider physics, in a framework of multi-charged particles. Then we explore the typical size of the muon…

High Energy Physics - Phenomenology · Physics 2020-02-05 Takaaki Nomura , Hiroshi Okada

We present a combined study of the muon anomalous magnetic moment, $a_{\mu} \equiv (g-2)_{\mu} /2$, and $b \to s \gamma$ decay in the minimal supersymmetric standard model with gauge-mediated supersymmetry-breaking. Combining new…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. T. Mahanthappa , Sechul Oh

Theories beyond the standard model often predict the existence of an additional neutral boson, the $Z^{\prime}$. Using data collected by the Belle II experiment during 2018 at the SuperKEKB collider, we perform the first searches for the…

High Energy Physics - Experiment · Physics 2020-04-07 Belle II Collaboration , I. Adachi , P. Ahlburg , H. Aihara , N. Akopov , A. Aloisio , N. Anh Ky , D. M. Asner , H. Atmacan , T. Aushev , V. Aushev , T. Aziz , V. Babu , S. Baehr , P. Bambade , Sw. Banerjee , V. Bansal , M. Barrett , J. Baudot , J. Becker , P. K. Behera , J. V. Bennett , E. Bernieri , F. U. Bernlochner , M. Bertemes , M. Bessner , S. Bettarini , F. Bianchi , D. Biswas , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , L. Burmistrov , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , D. Červenkov , M. -C. Chang , R. Cheaib , V. Chekelian , Y. Q. Chen , Y. -T. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. Cho , S. -K. Choi , S. Choudhury , D. Cinabro , L. Corona , L. M. Cremaldi , S. Cunliffe , T. Czank , F. Dattola , E. De La Cruz-Burelo , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , S. Dey , A. De Yta-Hernandez , F. Di Capua , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , K. Dort , D. Dossett , S. Dubey , S. Duell , G. Dujany , S. Eidelman , M. Eliachevitch , J. E. Fast , T. Ferber , D. Ferlewicz , G. Finocchiaro , S. Fiore , A. Fodor , F. Forti , B. G. Fulsom , E. Ganiev , M. Garcia-Hernandez , R. Garg , V. Gaur , A. Gaz , A. Gellrich , J. Gemmler , T. Geßler , R. Giordano , A. Giri , B. Gobbo , R. Godang , P. Goldenzweig , B. Golob , P. Gomis , W. Gradl , E. Graziani , D. Greenwald , Y. Guan , C. Hadjivasiliou , S. Halder , T. Hara , O. Hartbrich , K. Hayasaka , H. Hayashii , C. Hearty , M. T. Hedges , I. Heredia de la Cruz , M. Hernández Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , M. Hoek , C. -L. Hsu , Y. Hu , T. Iijima , K. Inami , G. Inguglia , J. Irakkathil Jabbar , A. Ishikawa , R. Itoh , Y. Iwasaki , W. W. Jacobs , D. E. Jaffe , E. -J. Jang , H. B. Jeon , S. Jia , Y. Jin , C. Joo , K. K. Joo , J. Kahn , H. Kakuno , A. B. Kaliyar , J. Kandra , G. Karyan , Y. Kato , T. Kawasaki , B. H. Kim , C. -H. Kim , D. Y. Kim , K. -H. Kim , S. -H. Kim , Y. K. Kim , Y. Kim , T. D. Kimmel , H. Kindo , C. Kleinwort , P. Kodyš , T. Koga , S. Kohani , I. Komarov , S. Korpar , N. Kovalchuk , T. M. G. Kraetzschmar , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , S. Kurz , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , C. La Licata , L. Lanceri , J. S. Lange , K. Lautenbach , I. -S. Lee , S. C. Lee , P. Leitl , D. Levit , L. K. Li , Y. B. Li , J. Libby , K. Lieret , L. Li Gioi , Z. Liptak , Q. Y. Liu , D. Liventsev , S. Longo , T. Luo , Y. Maeda , M. Maggiora , E. Manoni , S. Marcello , C. Marinas , A. Martini , M. Masuda , T. Matsuda , K. Matsuoka , D. Matvienko , F. Meggendorfer , J. C. Mei , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , K. Miyabayashi , H. Miyake , R. Mizuk , K. Azmi , G. B. Mohanty , T. Moon , T. Morii , H. -G. Moser , F. Mueller , F. J. Müller , Th. Muller , G. Muroyama , R. Mussa , E. Nakano , M. Nakao , M. Nayak , G. Nazaryan , D. Neverov , C. Niebuhr , N. K. Nisar , S. Nishida , K. Nishimura , M. Nishimura , B. Oberhof , K. Ogawa , Y. Onishchuk , H. Ono , Y. Onuki , P. Oskin , H. Ozaki , P. Pakhlov , G. Pakhlova , A. Paladino , A. Panta , E. Paoloni , H. Park , B. Paschen , A. Passeri , A. Pathak , S. Paul , T. K. Pedlar , I. Peruzzi , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , V. Popov , C. Praz , E. Prencipe , M. T. Prim , M. V. Purohit , P. Rados , R. Rasheed , S. Reiter , M. Remnev , P. K. Resmi , I. Ripp-Baudot , M. Ritter , G. Rizzo , L. B. Rizzuto , S. H. Robertson , D. Rodríguez Pérez , J. M. Roney , C. Rosenfeld , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , A. Sangal , L. Santelj , P. Sartori , Y. Sato , V. Savinov , B. Scavino , J. Schueler , C. Schwanda , R. M. Seddon , Y. Seino , A. Selce , K. Senyo , C. Sfienti , C. P. Shen , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , R. J. Sobie , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , B. Spruck , M. Starič , S. Stefkova , Z. S. Stottler , R. Stroili , J. Strube , M. Sumihama , T. Sumiyoshi , D. J. Summers , S. Y. Suzuki , M. Tabata , M. Takizawa , U. Tamponi , S. Tanaka , K. Tanida , N. Taniguchi , P. Taras , F. Tenchini , E. Torassa , K. Trabelsi , T. Tsuboyama , M. Uchida , K. Unger , Y. Unno , S. Uno , Y. Ushiroda , S. E. Vahsen , R. van Tonder , G. S. Varner , K. E. Varvell , A. Vinokurova , L. Vitale , A. Vossen , M. Wakai , H. M. Wakeling , W. Wan Abdullah , C. H. Wang , M. -Z. Wang , A. Warburton , M. Watanabe , J. Webb , S. Wehle , C. Wessel , J. Wiechczynski , H. Windel , E. Won , B. Yabsley , S. Yamada , W. Yan , S. B. Yang , H. Ye , J. H. Yin , M. Yonenaga , C. Z. Yuan , Y. Yusa , L. Zani , Z. Zhang , V. Zhilich , Q. D. Zhou , X. Y. Zhou , V. I. Zhukova

In a model of supersymmetric SU(5) Grand Unification with a spatial dimension described by the orbifold $S^1/(Z_2 \times Z_2')$, proton decay is naturally suppressed at all orders. This is achieved by a suitable implementation of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gautam Bhattacharyya , K. Sridhar

Recent experimental results on muon anomalous magnetic dipole moment have shown a $4.2\sigma$ tension with the SM prediction, which has blown a fresh wind into the elementary particle physics community. The problem is believed to be…

High Energy Physics - Phenomenology · Physics 2023-08-09 D. N. Dinh