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Related papers: A New Charged Lepton Flavor Violation Program at F…

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Charged lepton flavor violation (CLFV) is expected in a diverse set of new physics scenarios. The current generation of experiments probe CLFV in the muon sector in three complementary channels: $\mu^-N \rightarrow e^- N$ (Mu2e, COMET),…

High Energy Physics - Experiment · Physics 2025-01-28 Sophie Middleton

Since its discovery, the muon has proven to be an invaluable probe of the Standard Model (SM). Muons are readily available in tertiary beams in facilities around the world. They do not decay hadronically and have a lifetime of a few $\mu$…

High Energy Physics - Experiment · Physics 2025-02-04 Sophie Middleton

The Mu2e experiment will search for the neutrino-less conversion of a muon into an electron in the field of an aluminum nucleus. An observation would be the first signal of charged lepton flavor violation and de facto evidence for new…

High Energy Physics - Experiment · Physics 2020-07-15 Manolis Kargiantoulakis

The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less $\mu \to e$ coherent conversion in the field of an aluminum nucleus. About $7 \cdot 10^{17}$ muons, provided by a dedicated muon…

High Energy Physics - Experiment · Physics 2017-05-22 G. Pezzullo

Charged-lepton flavor violation (cLFV) is one of the most powerful probes for New Physics (NP). Since lepton flavor conservation is an accidental symmetry in the Standard Model (SM), it is naturally violated in many NP models, with…

High Energy Physics - Experiment · Physics 2025-03-31 M. Aoki , A. M. Baldini , R. H. Bernstein , C. Carloganu , S. Mihara , S. Miscetti , T. Mori , W. Ootani , F. Renga , S. Ritt , A. Schoening

The Mu2e experiment at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for…

Instrumentation and Detectors · Physics 2015-03-18 L. Bartoszek , E. Barnes , J. P. Miller , J. Mott , A. Palladino , J. Quirk , B. L. Roberts , J. Crnkovic , V. Polychronakos , V. Tishchenko , P. Yamin , C. -h. Cheng , B. Echenard , K. Flood , D. G. Hitlin , J. H. Kim , T. S. Miyashita , F. C. Porter , M. Röhrken , J. Trevor , R. -Y. Zhu , E. Heckmaier , T. I. Kang , G. Lim , W. Molzon , Z. You , A. M. Artikov , J. A. Budagov , Yu. I. Davydov , V. V. Glagolev , A. V. Simonenko , Z. U. Usubov , S. H. Oh , C. Wang , G. Ambrosio , N. Andreev , D. Arnold , M. Ball , R. H. Bernstein , A. Bianchi , K. Biery , R. Bossert , M. Bowden , J. Brandt , G. Brown , H. Brown , M. Buehler , M. Campbell , S. Cheban , M. Chen , J. Coghill , R. Coleman , C. Crowley , A. Deshpande , G. Deuerling , J. Dey , N. Dhanaraj , M. Dinnon , S. Dixon , B. Drendel , N. Eddy , R. Evans , D. Evbota , J. Fagan , S. Feher , B. Fellenz , H. Friedsam , G. Gallo , A. Gaponenko , M. Gardner , S. Gaugel , K. Genser , G. Ginther , H. Glass , D. Glenzinski , D. Hahn , S. Hansen , B. Hartsell , S. Hays , J. A. Hocker , E. Huedem , D. Huffman , A. Ibrahim , C. Johnstone , V. Kashikhin , V. V. Kashikhin , P. Kasper , T. Kiper , D. Knapp , K. Knoepfel , L. Kokoska , M. Kozlovsky , G. Krafczyk , M. Kramp , S. Krave , K. Krempetz , R. K. Kutschke , R. Kwarciany , T. Lackowski , M. J. Lamm , M. Larwill , F. Leavell , D. Leeb , A. Leveling , D. Lincoln , V. Logashenko , V. Lombardo , M. L. Lopes , A. Makulski , A. Martinez , D. McArthur , F. McConologue , L. Michelotti , N. Mokhov , J. Morgan , A. Mukherjee , P. Murat , V. Nagaslaev , D. V. Neuffer , T. Nicol , J. Niehoff , J. Nogiec , M. Olson , D. Orris , R. Ostojic , T. Page , C. Park , T. Peterson , R. Pilipenko , A. Pla-Dalmau , V. Poloubotko , M. Popovic , E. Prebys , P. Prieto , V. Pronskikh , D. Pushka , R. Rabehl , R. E. Ray , R. Rechenmacher , R. Rivera , W. Robotham , P. Rubinov , V. L. Rusu , V. Scarpine , W. Schappert , D. Schoo , A. Stefanik , D. Still , Z. Tang , N. Tanovic , M. Tartaglia , G. Tassotto , D. Tinsley , R. S. Tschirhart , G. Vogel , R. Wagner , R. Wands , M. Wang , S. Werkema , H. B. White , J. Whitmore , R. Wielgos , R. Woods , C. Worel , R. Zifko , P. Ciambrone , F. Colao , M. Cordelli , G. Corradi , E. Dane , S. Giovannella , F. Happacher , A. Luca , S. Miscetti , B. Ponzio , G. Pileggi , A. Saputi , I. Sarra , R. S. Soleti , V. Stomaci , M. Martini , P. Fabbricatore , S. Farinon , R. Musenich , D. Alexander , A. Daniel , A. Empl , E. V. Hungerford , K. Lau , G. D. Gollin , C. Huang , D. Roderick , B. Trundy , D. Na. Brown , D. Ding , Yu. G. Kolomensky , M. J. Lee , M. Cascella , F. Grancagnolo , F. Ignatov , A. Innocente , A. L'Erario , A. Miccoli , A. Maffezzoli , P. Mazzotta , G. Onorato , G. M. Piacentino , S. Rella , F. Rossetti , M. Spedicato , G. Tassielli , A. Taurino , G. Zavarise , R. Hooper , D. No. Brown , R. Djilkibaev , V. Matushko , C. Ankenbrandt , S. Boi , A. Dychkant , D. Hedin , Z. Hodge , V. Khalatian , R. Majewski , L. Martin , U. Okafor , N. Pohlman , R. S. Riddel , A. Shellito , A. L. de Gouvea , F. Cervelli , R. Carosi , S. Di Falco , S. Donati , T. Lomtadze , G. Pezzullo , L. Ristori , F. Spinella , M. Jones , M. D. Corcoran , J. Orduna , D. Rivera , R. Bennett , O. Caretta , T. Davenne , C. Densham , P. Loveridge , J. Odell , R. Bomgardner , E. C. Dukes , R. Ehrlich , M. Frank , S. Goadhouse , R. Group , E. Ho , H. Ma , Y. Oksuzian , J. Purvis , Y. Wu , D. W. Hertzog , P. Kammel , K. R. Lynch , J. L. Popp

Since the discovery of the muon, particle physicists have carried out a series of experiments aimed at measuring flavor violation in charged-lepton interactions. To date, no such violation has been observed. The Mu2e experiment at Fermilab…

Instrumentation and Detectors · Physics 2014-01-20 Robert Craig Group , Yuri Oksuzian

The search for lepton flavour violation in charged lepton decays is highly sensitive to physics beyond the Standard Model. Among the possible processes, $\mu$-decays are considered to have the largest discovery potential in most of the…

High Energy Physics - Experiment · Physics 2019-06-26 Luca Galli

The Mu2e experiment will search for a Standard Model violating rate of neutrinoless conversion of a muon into an electron in the presence of an aluminum nucleus. Observation of this charged lepton flavor violating process would be an…

High Energy Physics - Experiment · Physics 2022-10-28 Michael Thomas Hedges

The observation of lepton flavour violation (LFV) in the charged lepton sector would be an unambiguous sign of physics beyond the Standard Model (BSM), and thus, it is the channel of choice for many BSM searches. LFV searches in muon decays…

High Energy Physics - Experiment · Physics 2023-08-23 Ann-Kathrin Perrevoort

Mu2e at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for this process. The…

Instrumentation and Detectors · Physics 2012-12-06 The Mu2e Project , Collaboration , : , R. J. Abrams , D. Alezander , G. Ambrosio , N. Andreev , C. M. Ankenbrandt , D. M. Asner , D. Arnold , A. Artikov , E. Barnes , L. Bartoszek , R. H. Bernstein , K. Biery , V. Biliyar , R. Bonicalzi , R. Bossert , M. Bowden , J. Brandt , D. N. Brown , J. Budagov , M. Buehler , A. Burov , R. Carcagno , R. M. Carey , R. Carosi , M. Cascella , D. Cauz , F. Cervelli , A. Chandra , J. K. Chang , C. Cheng , P. Ciambrone , R. N. Coleman , M. Cooper , M. C. Corcoran , M. Cordelli , Y. Davydov , A. L. de Gouvea , L. De Lorenzis , P. T. Debevec , F. DeJongh , C. Densham , G. Deuerling , J. Dey , S. Di Falco , S. Dixon , R. Djilkibaev , B. Drendel , E. C. Dukes , A. Dychkant , B. Echenard , R. Ehrlich , N. Evans , D. Evbota , I. Fang , J. E. Fast , S. Feher , M. Fischler , M. Frank , E. Frlez , S. S. Fung , G. Gallo , G. Galucci , A. Gaponenko , K. Genser , S. Giovannella , V. Glagolev , D. Glenzinski , D. Gnani , S. Goadhouse , G. D. Gollin , C. Grace , F. Grancagnolo , C. Group , J. Hanson , S. Hanson , F. Happacher , E. Heckmaier , D. Hedin , D. W. Hertzog , R. Hirosky , D. G. Hitlin , E. Ho , X. Huang , E. Huedem , P. Q. Hung , E. V. Hungerford , T. Ito , W. Jaskierny , R. Jedziniak , R. P. Johnson , C. Johnstone , J. A. Johnstone , S. A. Kahn , P. Kammel , T. I. Kang , V. S. Kashikhin , V. V. Kashikhin , P. Kasper , D. M. Kawall , V. Khalatian , M. Kim , A. Klebaner , D. Kocen , Y. Kolomensky , I. Kourbanis , J. Kowalkowski , J. Kozminski , K. Krempetz , K. S. Kumar , R. K. Kutschke , R. Kwarciany , T. Lackowski , M. Lamm , M. Larwill , K. Lau , M. J. Lee , A. L'Erario , T. Leveling , G. Lim , C. Lindenmeyer , V. Logashenko , T. Lontadze , M. Lopes , A. Luca , K. R. Lynch , T. Ma , A. Maffezzoli , W. J. Marciano , M. Martini , W. Masayoshi , V. Matushko , M. McAteer , R. McCrady , A. Moccoli , L. Michelotti , J. P. Miller , S. Miscetti , W. Molzon , J. Morgan , A. Mukherjee , S. Nagaitsev , V. Nagaslaev , J. Niehoff , D. V. Neuffer , T. Nicol , A. J. Norman , B. Norris , J. Odell , S. Oh , Y. Oksuzian , G. Onorato , J. Orduna , D. Orris , R. Ostojic , T. Page , K. D. Paschke , G. Pauletta , T. Peterson , G. M. Piacentino , G. Pileggi , A. Pla-Dalmau , D. Pocanic , C. C. Polly , V. Polychronakos , B. Ponzio , M. Popovic , J. L. Popp , F. Porter , E. Presbys , P. Prieto , V. Pronskikh , F. Puccinelli , R. Rabehl , J. Ramsey , R. E. Ray , R. Rechenmacher , S. Rella , L. Ristori , R. Rivera , B. L. Roberts , T. J. Roberts , P. Rubinov , V. L. Rusu , A. Saputi , I. Sarra , Y. Smertzidis , P. Shanahan , A. Simonenko , J. Steward , I. Suslov , C. Sylvester , Z. Tang , M. Tartaglia , G. Tassielli , V. Tereshchenko , J. Theilacker , J. Tompkins , R. Tschirhart , G. Van Zandbergen , C. Vannini , G. Venanzoni , H. von der Lippe , R. Wagner , J. P. Walder , R. Walton , S. Wands , S. Wang , G. Warren , S. Werkema , H. B. White , R. Wielgos , L. S. Wood , M. Woodward , J. Wu , M. Xiao , R. Yamada , P. Yamin , K. Yarritu , K. Yonehara , C. Yoshikawa , Z. You , G. Yu , A. Yurkewicz , G. Zavarise , R. Y. Zhu

Flavor violating processes in the lepton sector have highly suppressed branching ratios in the standard model. Thus, observation of lepton flavor violation (LFV) constitutes a clear indication of physics beyond the standard model (BSM). We…

High Energy Physics - Phenomenology · Physics 2022-03-09 Alexey A. Petrov , Renae Conlin , Cody Grant

A muon collider would be a powerful probe of flavor violation in new physics. There is a strong complementary case for collider measurements and precision low-energy probes of lepton flavor violation (as well as CP violation). We illustrate…

High Energy Physics - Phenomenology · Physics 2022-08-01 Samuel Homiller , Qianshu Lu , Matthew Reece

We briefly overview some theoretical aspects of charged lepton flavour violation in rare muon transitions and decays. Relying on the effective field theory approach (model-independent), we discuss the probing power of charged lepton flavour…

High Energy Physics - Phenomenology · Physics 2023-12-19 Ana M. Teixeira

The Mu2e Experiment at Fermilab will search for the coherent, neutrinoless conversion of muons into electrons in the field of an aluminium nucleus with an unprecedented sensitivity. Such a charged lepton flavor-violating reaction probes new…

High Energy Physics - Experiment · Physics 2016-09-08 Luca Morescalchi

Charged-lepton flavour-violating (cLFV) processes offer deep probes for new physics with discovery sensitivity to a broad array of new physics models - SUSY, Higgs Doublets, Extra Dimensions, and, particularly, models explaining the…

High Energy Physics - Experiment · Physics 2018-12-18 A. Baldini , D. Glenzinski , F Kapusta , Y. Kuno , M. Lancaster , J. Miller , S. Miscetti , T. Mori , A. Papa , A. Schoning , Y. Uchida

With the planned turn-on of the PIP-II 800 MeV superconducting proton linac, Fermilab will potentially become the world's best laboratory at which to carry out fundamental muon measurements, sensitive searches for symmetry violation, and…

Searches for charged lepton flavor violation in the muon sector stand out among the most sensitive and clean probes for physics beyond the Standard Model. Currently, $\mu^+ \to \mathrm{e}^+ \gamma$ experiments provide the best constraints…

Charged lepton flavour violating transitions would be a clear signal of new physics beyond the Standard Model. Their search has been carried out in a variety of channels, the most sensitive being those involving a muon: however no positive…

High Energy Physics - Phenomenology · Physics 2018-02-05 Lorenzo Calibbi , Giovanni Signorelli

The Muon Campus at Fermilab provides world class accelerator infrastructure supporting the next generation intensity frontier experiments. The anti-proton source from the Tevatron era was converted to the present day Muon Campus at the end…

Accelerator Physics · Physics 2022-08-08 S. Ganguly
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