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Conceptual designs of a superconducting dipole magnet for a Storage Ring of a Muon Collider with a 1.5 TeV center of mass (c.o.m.) energy and an average luminosity of 10 34 cm-2s-1 are presented. In contrast to proton machines, the dipoles…

Accelerator Physics · Physics 2015-06-04 I. Novitski , V. V. Kashikhin , N. Mokhov , A. V. Zlobin

This proposal describes an experimental search for sterile neutrinos beyond the Standard Model with a new CERN-SPS neutrino beam. The experiment is based on two identical LAr-TPC's followed by magnetized spectrometers, observing the…

Instrumentation and Detectors · Physics 2012-03-30 M. Antonello , D. Bagliani , B. Baibussinov , H. Bilokon , F. Boffelli , M. Bonesini , E. Calligarich , N. Canci , S. Centro , A. Cesana , K. Cieslik , D. B. Cline , A. G. Cocco , D. Dequal , A. Dermenev , R. Dolfini , M. De Gerone , S. Dussoni , C. Farnese , A. Fava , A. Ferrari , G. Fiorillo , G. T. Garvey , F. Gatti , D. Gibin , S. Gninenko , F. Guber , A. Guglielmi , M. Haranczyk , J. Holeczek , A. Ivashkin , M. Kirsanov , J. Kisiel , I. Kochanek , A. Kurepin , J. Łagoda , G. Lucchini , W. C. Louis , S. Mania , G. Mannocchi , S. Marchini , V. Matveev , A. Menegolli , G. Meng , G. B. Mills , C. Montanari , M. Nicoletto , S. Otwinowski , T. J. Palczewski , G. Passardi , F. Perfetto , P. Picchi , F. Pietropaolo , P. Płoński , A. Rappoldi , G. L. Raselli , M. Rossella , C. Rubbia , P. Sala , A. Scaramelli , E. Segreto , D. Stefan , J. Stepaniak , R. Sulej , O. Suvorova , M. Terrani , D. Tlisov , R. G. Van de Water , G. Trinchero , M. Turcato , F. Varanini , S. Ventura , C. Vignoli , H. G. Wang , X. Yang , A. Zani , K. Zaremba , M. Benettoni , P. Bernardini , A. Bertolin , C. Bozza , R. Brugnera , A. Cecchetti , S. Cecchini , G. Collazuol , P. Creti , F. Dal Corso , I. De Mitri , G. De Robertis , M. De Serio , L. Degli Esposti , D. Di Ferdinando , U. Dore , S. Dusini , P. Fabbricatore , C. Fanin , R. A. Fini , G. Fiore , A. Garfagnini , G. Giacomelli , R. Giacomelli , G. Grelli , C. Guandalini , M. Guerzoni , U. Kose , G. Laurenti , M. Laveder , I. Lippi , F. Loddo , A. Longhin , P. Loverre , G. Mancarella , G. Mandrioli , A. Margiotta , G. Marsella , N. Mauri , E. Medinaceli , A. Mengucci , M. Mezzetto , R. Michinelli , M. T. Muciaccia , D. Orecchini , A. Paoloni , A. Pastore , L. Patrizii , M. Pozzato , R. Rescigno , G. Rosa , S. Simone , M. Sioli , G. Sirri , M. Spurio , L. Stanco , S. Stellacci , A. Surdo , M. Tenti , V. Togo , M. Ventura , M. Zago

A 1.8 T dipole magnet using thin grain oriented silicon steel laminations has been constructed as a prototype for a muon synchrotron ramping at 400 Hz. Following the practice in large 3 phase transformers and our own Opera-2d simulations,…

Accelerator Physics · Physics 2012-08-27 D. J. Summers , L. M. Cremaldi , T. L. Hart , L. P. Perera , M. Reep , H. Witte , S. Hansen , M. L. Lopes , J. Reidy,

The SHiP experiment is designed to search for very weakly interacting particles beyond the Standard Model which are produced in a 400 GeV/c proton beam dump at the CERN SPS. An essential task for the experiment is to keep the Standard Model…

Instrumentation and Detectors · Physics 2017-05-19 SHiP collaboration , A. Akmete , A. Alexandrov , A. Anokhina , S. Aoki , E. Atkin , N. Azorskiy , J. J. Back , A. Bagulya , A. Baranov , G. J. Barker , A. Bay , V. Bayliss , G. Bencivenni , A. Y. Berdnikov , Y. A. Berdnikov , M. Bertani , C. Betancourt , I. Bezshyiko , O. Bezshyyko , D. Bick , S. Bieschke , A. Blanco , J. Boehm , M. Bogomilov , K. Bondarenko , W. M. Bonivento , A. Boyarsky , R. Brenner , D. Breton , R. Brundler , M. Bruschi , V. Büscher , A. Buonaura , S. Buontempo , S. Cadeddu , A. Calcaterra , M. Campanelli , J. Chauveau , A. Chepurnov , M. Chernyavsky , K. -Y. Choi , A. Chumakov , P. Ciambrone , G. M. Dallavalle , N. D'Ambrosio , G. D'Appollonio , G. De Lellis , A. De Roeck , M. De Serio , L. Dedenko , A. Di Crescenzo , N. Di Marco , C. Dib , H. Dijkstra , V. Dmitrenko , D. Domenici , S. Donskov , A. Dubreuil , J. Ebert , T. Enik , A. Etenko , F. Fabbri , L. Fabbri , O. Fedin , G. Fedorova , G. Felici , M. Ferro-Luzzi , R. A. Fini , P. Fonte , C. Franco , T. Fukuda , G. Galati , G. Gavrilov , S. Gerlach , L. Golinka-Bezshyyko , D. Golubkov , A. Golutvin , D. Gorbunov , S. Gorbunov , V. Gorkavenko , Y. Gornushkin , M. Gorshenkov , V. Grachev , E. Graverini , V. Grichine , A. M. Guler , Yu. Guz , C. Hagner , H. Hakobyan , E. van Herwijnen , A. Hollnagel , B. Hosseini , M. Hushchyn , G. Iaselli , A. Iuliano , R. Jacobsson , M. Jonker , I. Kadenko , C. Kamiscioglu , M. Kamiscioglu , M. Khabibullin , G. Khaustov , A. Khotyantsev , S. H. Kim , V. Kim , Y. G. Kim , N. Kitagawa , J. -W. Ko , K. Kodama , A. Kolesnikov , D. I. Kolev , V. Kolosov , M. Komatsu , N. Konovalova , M. A. Korkmaz , I. Korol , I. Korol'ko , A. Korzenev , S. Kovalenko , I. Krasilnikova , K. Krivova , Y. Kudenko , V. Kurochka , E. Kuznetsova , H. M. Lacker , A. Lai , G. Lanfranchi , O. Lantwin , A. Lauria , H. Lebbolo , K. Y. Lee , J. -M. Lévy , V. Likacheva , L. Lopes , V. Lyubovitskij , J. Maalmi , A. Magnan , V. Maleev , A. Malinin , A. Mefodev , P. Mermod , S. Mikado , Yu. Mikhaylov , D. A. Milstead , O. Mineev , A. Montanari , M. C. Montesi , K. Morishima , S. Movchan , N. Naganawa , M. Nakamura , T. Nakano , A. Novikov , B. Obinyakov , S. Ogawa , N. Okateva , P. H. Owen , A. Paoloni , B. D. Park , L. Paparella , A. Pastore , M. Patel , D. Pereyma , D. Petrenko , K. Petridis , D. Podgrudkov , V. Poliakov , N. Polukhina , M. Prokudin , A. Prota , A. Rademakers , F. Ratnikov , T. Rawlings , M. Razeti , F. Redi , S. Ricciardi , T. Roganova , A. Rogozhnikov , H. Rokujo , G. Rosa , T. Rovelli , O. Ruchayskiy , T. Ruf , V. Samoylenko , A. Saputi , O. Sato , E. S. Savchenko , W. Schmidt-Parzefall , N. Serra , A. Shakin , M. Shaposhnikov , P. Shatalov , T. Shchedrina , L. Shchutska , V. Shevchenko , H. Shibuya , A. Shustov , S. B. Silverstein , S. Simone , M. Skorokhvatov , S. Smirnov , J. Y. Sohn , A. Sokolenko , N. Starkov , B. Storaci , P. Strolin , S. Takahashi , I. Timiryasov , V. Tioukov , N. Tosi , D. Treille , R. Tsenov , S. Ulin , A. Ustyuzhanin , Z. Uteshev , G. Vankova-Kirilova , F. Vannucci , P. Venkova , S. Vilchinski , M. Villa , K. Vlasik , A. Volkov , R. Voronkov , R. Wanke , J. -K. Woo , M. Wurm , S. Xella , D. Yilmaz , A. U. Yilmazer , C. S. Yoon , Yu. Zaytsev

The magnetic moment is a fundamental property of particles. The measurement of these magnetic moments and the comparison with the values predicted by the standard model of particle physics is a way to test our understanding of the…

High Energy Physics - Experiment · Physics 2015-12-23 M. Eads

The KM3NeT Collaboration has successfully deployed the first detection units of the next generation undersea neutrino telescopes in the Mediterranean Sea at the two sites in Italy and in France. The data sample collected between December…

High Energy Physics - Experiment · Physics 2022-08-11 Piotr Kalaczyński

We propose a new fixed-target experiment for the study of electromagnetic and hard probes of the Quark-Gluon Plasma (QGP) in heavy-ion collisions at the CERN SPS. The experiment aims at performing measurements of the dimuon spectrum from…

The Muon g-2 Experiment (E989) at Fermilab is seeking to measure the anomalous magnetic moment of muon ($a_{\mu}$) with a precision of 140 parts-per-billion (ppb) and aiming to resolve the discrepancy between the E821 measurement and the…

Instrumentation and Detectors · Physics 2018-10-10 Ran Hong

LumiCal is a sampling electromagnetic calorimeter designed for the precise measurement of integrated luminosity in electron positron linear collider experiments. The present report contains a description and results of the first beam test…

Instrumentation and Detectors · Physics 2019-08-13 Oleksandr Borysov

Multiscale simulation is a key research tool for the quest for new permanent magnets. Starting with first principles methods, a sequence of simulation methods can be applied to calculate the maximum possible coercive field and expected…

Large scale neutrino detectors and muon tomography rely on the muon direction in the detector to infer the muon's or parent neutrino's origin. However, muons accumulate deflections along their propagation path prior to entering the…

Instrumentation and Methods for Astrophysics · Physics 2023-02-03 Pascal Gutjahr , Jean-Marco Alameddine , Alexander Sandrock , Jan Soedingrekso , Mirco Hünnefeld , Wolfgang Rhode

The SHiP experiment will search for very weakly interacting particles beyond the Standard Model which are produced in a 400 \GeV/$c$ proton beam dump at the CERN SPS. About $10^{11}$ muons per spill will be produced in the dump. To design…

Instrumentation and Detectors · Physics 2020-01-15 SHiP Collaboration

The MUonE experiment proposes a novel approach to determine the leading hadronic contribution to the muon g-2, from a precise measurement of the differential cross section of the $\mu-e$ elastic scattering, achievable by using the CERN SPS…

High Energy Physics - Experiment · Physics 2024-01-09 E. Spedicato

The KM3NeT Collaboration has successfully deployed the first detection units of the next generation undersea neutrino telescopes in the Mediterranean Sea at the two sites in Italy and in France. A sample of the data collected between…

Instrumentation and Detectors · Physics 2021-10-20 Piotr Kalaczyński

Muon spin spectroscopy is one of the most powerful tools to investigate the microscopic properties of superconductors. In this manuscript, an overview on some of the main achievements obtained by this technique in the iron-based…

Superconductivity · Physics 2015-06-16 P. Carretta , R. De Renzi , G. Prando , S. Sanna

Muon ionization cooling provides the only practical solution to prepare high-brilliance beams necessary for a neutrino factory or muon collider. The Muon Ionization Cooling Experiment (MICE), under development at the Rutherford Appleton…

Accelerator Physics · Physics 2008-10-11 Terrence L. Hart , Daniel M. Kaplan

The Muon $(g-2)$ experiment, E821, at the Brookhaven AGS has the goal to measure the muon anomalous magnetic moment to a relative accuracy of $\pm 3.5 \times 10^{-7}$. A superferric 14 m diameter storage ring has been constructed and an…

High Energy Physics - Experiment · Physics 2007-05-23 B. Lee Roberts

We have re-purposed portable plastic scintillator muon detectors, designed by the CosmicWatch project, for the measurement of electrons emitted by the decay of radioactive sources. For the latter purpose we have first calibrated the…

Instrumentation and Detectors · Physics 2019-08-20 Joaquin Masias , Franco Delgado , Lucía Coll , Alicia Pérez , José Bazo , Alberto Gago

IceTop, the surface component of the IceCube detector, has been used to measure the energy spectrum of cosmic ray primaries in the range between 1.58 PeV and 1.26 EeV. It can also be used to study the low energy muons in air showers by…

High Energy Astrophysical Phenomena · Physics 2019-08-13 Javier G. Gonzalez

In 2018, a test run with muons in the North Area at CERN was performed, running parasitically downstream of the COMPASS spectrometer. The aim of the test was to investigate the elastic interactions of muons on atomic electrons, in an…