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Related papers: Tau/Charm Factory Accelerator Report

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The project of Super Tau-Charm Facility (STCF) proposed in China, as a new-generation high-luminosity $e^+e^-$ collider in the low-energy region with the center-of-mass energy of 2-7 GeV, is well underway. The luminosity is targeted at…

Accelerator Physics · Physics 2024-03-04 Linhao Zhang , Tao Liu , Sangya Li , Jingyu Tang , Qing Luo

An overview of tau lepton physics is presented, using the tau lepton discovery and its precision measurements as examples to illustrate the importance of the energy region to be covered by the super tau-charm factory. By presenting the…

High Energy Physics - Experiment · Physics 2026-01-29 Zhiqing Zhang

A sensitivity study for the search for the charged lepton flavor violating process $\tau \to \gamma\mu$ at the Super $\tau$-Charm Facility is performed with a fast simulation. With the expected performance of the current detector design and…

High Energy Physics - Experiment · Physics 2023-10-17 Teng Xiang , Xiao-Dong Shi , Da-Yong Wang , Xiao-Rong Zhou

I review the sensitivities achieved by and projected for fixed-target charm experiments in CP violation, flavor-changing neutral-current and lepton-number-violating decays, and mixing, and I describe the Charm2000 experiment intended to run…

High Energy Physics - Experiment · Physics 2015-06-25 Daniel M. Kaplan

The possibility of exploring the flavor changing neutral current $tcZ/tc\gamma$ couplings in the production vertex for the reaction $\epem\to t\bar c + \bar tc$ is examined. Using a model independent parameterization for the effective…

High Energy Physics - Phenomenology · Physics 2016-08-25 Tao Han , JoAnne L. Hewett

A Monte Carlo study of possible background processes in a search for $\tau \to \mu \gamma$ decay has been performed for conditions of the Super $c-\tau$ factory (CTF) (at a center-of-mass energy 3.686 GeV, 3.77 GeV and 4.17 GeV). The…

High Energy Physics - Experiment · Physics 2012-06-12 A. V. Bobrov , A. E. Bondar

During the run III of the LHC, the forward experiments FASER$\nu$ and SND@LHC will be able to detect the Charged Current (CC) interactions of the high energy neutrinos of all three flavors produced at the ATLAS Interaction Point (IP). This…

High Energy Physics - Phenomenology · Physics 2022-07-13 Saeed Ansarifard , Yasaman Farzan

This is a review of the SuperB project, covering the accelerator, detector, and highlights of the broad physics programme. SuperB is a flavour factory capable of performing precision measurements and searches for rare and forbidden decays…

High Energy Physics - Experiment · Physics 2015-05-30 Adrian J. Bevan

The next generation tau-charm factory, the third Beijing Electron Spectrometer (BESIII) at the new Beijing Electron Positron Collider (BEPCII), has begun data collection. I discuss the flavor physics reach of the BESIII charm program and…

High Energy Physics - Experiment · Physics 2019-08-13 Peter Zweber

In tau physics, we are at the frontier between the completion of the LEP program and the start of analyses from b-factories, which are expected to produce results in the coming years. Nice results from CLEO are steadily delivered in the…

High Energy Physics - Phenomenology · Physics 2014-11-17 P. Roudeau

We report on the status and plans of experiments now running or proposed for electron-positron colliders at energies between the $\phi$ and the Z. The $e^{+}e^{-}$ B and charm factories we considered were PEP-II/BABAR, KEKB/Belle, superKEK,…

Both the B-factories BaBar and Belle have ended data-taking and have mostly completed the data analysis aimed at searching Lepton Flavor Violation in Tau decays. No evidence of LFV in tau decays has been found yet. We review in the…

High Energy Physics - Experiment · Physics 2010-12-20 Alberto Lusiani

In this Technical Design Report (TDR) we describe the SuperB detector that was to be installed on the SuperB e+e- high luminosity collider. The SuperB asymmetric collider, which was to be constructed on the Tor Vergata campus near the INFN…

Instrumentation and Detectors · Physics 2013-06-25 SuperB Collaboration , M. Baszczyk , P. Dorosz , J. Kolodziej , W. Kucewicz , M. Sapor , A. Jeremie , E. Grauges Pous , G. E. Bruno , G. De Robertis , D. Diacono , G. Donvito , P. Fusco , F. Gargano , F. Giordano , F. Loddo , F. Loparco , G. P. Maggi , V. Manzari , M. N. Mazziotta , E. Nappi , A. Palano , B. Santeramo , I. Sgura , L. Silvestris , V. Spinoso , G. Eigen , J. Zalieckas , Z. Zhuo , L. Jenkovszky , G. Balbi , M. Boldini , D. Bonacorsi , V. Cafaro , I. D'Antone , G. M. Dallavalle , R. Di Sipio , F. Fabbri , L. Fabbri , A. Gabrielli , D. Galli , P. Giacomelli , V. Giordano , F. M. Giorgi , C. Grandi , I. Lax , S. Lo Meo , U. Marconi , A. Montanari , G. Pellegrini , M. Piccinini , T. Rovelli , N. Semprini Cesari , G. Torromeo , N. Tosi , R. Travaglini , V. M. Vagnoni , S. Valentinetti , M. Villa , A. Zoccoli , J. -F. Caron , C. Hearty , P. F. -T. Lu , T. S. Mattison , J. A. McKenna , R. Y. -C. So , M. Yu. Barnyakov , V. E. Blinov , A. A. Botov , V. P. Druzhinin , V. B. Golubev , S. A. Kononov , E. A. Kravchenko , E. B. Levichev , A. P. Onuchin , S. I. Serednyakov , D. A. Shtol , Y. I. Skovpen , E. P. Solodov , A. Cardini , M. Carpinelli , D. S. -T. Chao , C. H. Cheng , D. A. Doll , B. Echenard , K. Flood , J. Hanson , D. G. Hitlin , P. Ongmongkolkul , F. C. Porter , R. Y. Zhu , N. Randazzo , E. De La Cruz Burelo , Y. Zheng , P. Campos , M. De Silva , A. Kathirgamaraju , B. Meadows , B. Pushpawela , Y. Shi , M. Sokoloff , G. Lopez Castro , V. Ciaschini , P. Franchini , F. Giacomini , A. Paolini , G. A. Calderon Polania , S. Laczek , P. Romanowicz , B. Szybinski , M. Czuchry , L. Flis , D. Harezlak , J. Kocot , M. Radecki , M. Sterzel , T. Szepieniec , T. Szymocha , P. Wójcik , M. Andreotti , W. Baldini , R. Calabrese , V. Carassiti , G. Cibinetto , A. Cotta Ramusino , F. Evangelisti , A. Gianoli , E. Luppi , R. Malaguti , M. Manzali , M. Melchiorri , M. Munerato , C. Padoan , V. Santoro , L. Tomassetti , M. M. Beretta , M. Biagini , M. Boscolo , E. Capitolo , R. de Sangro , M. Esposito , G. Felici , G. Finocchiaro , M. Gatta , C. Gatti , S. Guiducci , S. Lauciani , P. Patteri , I. Peruzzi , M. Piccolo , P. Raimondi , M. Rama , C. Sanelli , S. Tomassini , P. Fabbricatore , D. Delepine , M. A. Reyes Santos , M. Chrzaszcz , R. Grzymkowski , P. Knap , J. Kotula , T. Lesiak , J. Ludwin , J. Michalowski , B. Pawlik , B. Rachwal , M. Stodulski , J. Wiechczynski , M. Witek , L. Zawiejski , M. Zdybal , V. Y. Aushev , A. Ustynov , N. Arnaud , P. Bambade , C. Beigbeder , F. Bogard , M. Borsato , D. Breton , J. Brossard , L. Burmistrov , D. Charlet , V. Chaumat , O. Dadoun , M. El Berni , J. Maalmi , V. Puill , C. Rimbault , A. Stocchi , V. Tocut , A. Variola , S. Wallon , G. Wormser , F. Grancagnolo , E. Ben-Haim , S. Sitt , M. Baylac , O. Bourrion , J. -M. Deconto , Y. Gomez Martinez , N. Monseu , J. -F. Muraz , J. -S. Real , C. Vescovi , R. Cenci , A. Jawahery , D. Roberts , E. W. Twedt , R. Cheaib , D. Lindemann , S. Nderitu , P. Patel , S. H. Robertson , D. Swersky , A. Warburton , E. Cuautle Flores , G. Toledo Sanchez , P. Biassoni , L. Bombelli , M. Citterio , S. Coelli , C. Fiorini , V. Liberali , M. Monti , B. Nasri , N. Neri , F. Palombo , F. Sabatini , A. Stabile , A. Berra , A. Giachero , C. Gotti , D. Lietti , M. Maino , G. Pessina , M. Prest , J. -P. Martin , M. Simard , N. Starinski , P. Taras , A. Drutskoy , S. Makarychev , A. V. Nefediev , A. Aloisio , S. Cavaliere , G. De Nardo , M. Della Pietra , A. Doria , R. Giordano , A. Ordine , S. Pardi , G. Russo , C. Sciacca , I. I. Bigi , C. P. Jessop , W. Wang , M. Bellato , M. Benettoni , M. Corvo , A. Crescente , F. Dal Corso , U. Dosselli , C. Fanin , A. Gianelle , S. Longo , M. Michelotto , F. Montecassiano , M. Morandin , R. Pengo , M. Posocco , M. Rotondo , G. Simi , R. Stroili , L. Gaioni , A. Manazza , M. Manghisoni , L. Ratti , V. Re , G. Traversi , S. Zucca , S. Bizzaglia , M. Bizzarri , C. Cecchi , S. Germani , M. Lebeau , P. Lubrano , E. Manoni , A. Papi , A. Rossi , G. Scolieri , G. Batignani , S. Bettarini , G. Casarosa , A. Cervelli , A. Fella , F. Forti , M. Giorgi , L. Lilli , A. Lusiani , B. Oberhof , A. Paladino , F. Pantaleo , E. Paoloni , A. L. Perez Perez , G. Rizzo , J. Walsh , A. Fernández Téllez , G. Beck , M. Berman , A. Bevan , F. Gannaway , G. Inguglia , A. J. Martin , J. Morris , V. Bocci , M. Capodiferro , G. Chiodi , I. Dafinei , N. V. Drenska , R. Faccini , F. Ferroni , C. Gargiulo , P. Gauzzi , C. Luci , R. Lunadei , G. Martellotti , F. Pellegrino , V. Pettinacci , D. Pinci , L. Recchia , D. Ruggeri , A. Zullo , P. Camarri , R. Cardarelli , C. De Santis , A. Di Ciaccio , V. Di Felice , F. Di Palma , A. Di Simone , L. Marcelli , R. Messi , D. Moricciani , R. Sparvoli , S. Tammaro , P. Branchini , A. Budano , S. Bussino , M. Ciuchini , F. Nguyen , A. Passeri , F. Ruggieri , E. Spiriti , F. Wilson , I. Leon Monzon , J. R. Millan-Almaraz , P. L. M. Podesta-Lerma , D. Aston , B. Dey , A. Fisher , P. D. Jackson , D. W. G. S. Leith , S. Luitz , D. MacFarlane , M. McCulloch , S. Metcalfe , A. Novokhatski , S. Osier , R. Prepost , B. Ratcliff , J. Seeman , M. Sullivan , J. Va'vra , U. Wienands , W. Wisniewski , B. D. Altschul , M. V. Purohit , J. Baudot , I. Ripp-Baudot , G. A. P. Cirrone , G. Cuttone , O. Bezshyyko , G. Dolinska , A. Soffer , F. Bianchi , F. De Mori , A. Filippi , D. Gamba , S. Marcello , M. Bomben , L. Bosisio , P. Cristaudo , L. Lanceri , B. Liberti , I. Rashevskaya , C. Stella , E. S. Vallazza , L. Vitale , G. Auriemma , C. Satriano , F. Martinez Vidal , J. Mazorra de Cos , A. Oyanguren , P. Ruiz Valls , A. Beaulieu , S. Dejong , J. Franta , M. J. Lewczuk , M. Roney , R. Sobie

SuperB is a next generation asymmetric e+e- flavor factory with a baseline luminosity of 10^36 cm^-2 s^-1, 50-100 times the peak luminosity of the existing B-factories. The physics motivation is presented and the complementarity with the…

High Energy Physics - Experiment · Physics 2014-11-20 Matteo Rama

In February this year Google proposed a new Transformer variant called FLASH, which has a faster speed, lower VRAM footprint and better performance. This is achieved by designing a performant layer named GAU (Gated Attention Unit), which…

Computation and Language · Computer Science 2022-05-19 Zhenjie Liu

The charm physics program accessible to a Tau-Charm Factory is summarized. Semileptonic, leptonic, hadronic, rare and forbidden charm decay modes are discussed, as well as \dmix\ mixing and CP violation in the charm sector. The theoretical…

High Energy Physics - Phenomenology · Physics 2009-09-25 J. L. Hewett

We consider theories where lepton flavor is violated, in particular concentrating on the four fermion operator consisting of three electrons and a tau. Strong constraints are available from existing searches for tau -> eee, requiring the…

High Energy Physics - Phenomenology · Physics 2015-01-14 Brandon Murakami , Tim M. P. Tait

Leptophilic axion-like particles (ALPs) extend the Standard Model (SM) with brand-new interactions between the ALP and leptons. In this work, we focus on studying exotic $\tau$ decays to explore such ALPs. Both the tauphilic and lepton…

High Energy Physics - Phenomenology · Physics 2025-12-02 Xu-Hui Jiang , Chih-Ting Lu

Today the B-factories BaBar and Belle have accumulated largest samples of tau-tau events and are competing to be called tau-factories. Among the problems to be tested and measurements to be done by BaBar and Belle are check of CP and CPT…

High Energy Physics - Experiment · Physics 2008-11-26 O. Igonkina

A search for the nonconservation of lepton flavor number in the decay tau -> mu gamma has been performed using 2.07 x 10^8 e+e- -> tau+ tau- events produced at a center-of-mass energy near 10.58 GeV with the BABAR detector at the PEP-II…

High Energy Physics - Experiment · Physics 2008-11-26 B. Aubert , The BABAR Collaboration