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A proton-driven Muon Collider, in the configuration that has resulted from the efforts of the International Muon Collider Collaboration (IMCC), poses multiple and exceptional magnet system challenges. Addressing these challenges will…

The status of the research on muon colliders is discussed and plans are outlined for future theoretical and experimental studies. Besides continued work on the parameters of a 3-4 and 0.5 TeV center-of-mass (CoM) energy collider, many…

Accelerator Physics · Physics 2009-04-17 Charles M. Ankenbrandt

The Compact Muon Solenoid (CMS) experiment at the Large Hadron Collider (LHC) is designed to study a wide range of high energy physics phenomena. It employs a large all-silicon tracker within a 3.8 T magnetic solenoid, which allows precise…

Instrumentation and Detectors · Physics 2019-10-29 Thomas James

Renewed international interest in muon colliders motivates the continued investigation of the impacts of beam-induced background on detector performance. This continues the effort initiated by the Muon Accelerator Program and carried out…

Several different scenarios for neutrino scattering experiments using a neutrino beam from the muon collider complex are discussed. The physics reach of a neutrino experiment at the front end of a muon collider is shown to extend far beyond…

High Energy Physics - Experiment · Physics 2010-02-02 Deborah A. Harris , Kevin S. McFarland

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

Heavy quarks are an ideal probe of the quark gluon plasma created in heavy ion collisions. They are produced in the initial hard scattering and therefore experience the full evolution of the medium. PHENIX has previously measured the…

Nuclear Experiment · Physics 2019-08-13 D. McGlinchey

In the RHIC run of 2006, PHENIX recorded data from about 20/nb of transversely polarized p+p collisions at sqrt(s) = 62.4 GeV and polarization of about 50%. Also in this last run PHENIX successfully commissioned a new lead-tungstate based…

Nuclear Experiment · Physics 2019-08-14 Mickey Chiu

Future collider detectors at muon colliders will be bombarded by Beam-Induced Backgrounds (BIB) due to the in-flight muon decays from the beam line. These backgrounds can inhibit the ability of the detector and subsequent data analysis to…

Instrumentation and Detectors · Physics 2022-07-01 D. Ally , L. Carpenter , T. Holmes , L. Lee , P. Wagenknecht

We have developed a silicon pixel detector to enhance the physics capabilities of the PHENIX experiment. This detector, consisting of two layers of sensors, will be installed around the beam pipe at the collision point and covers a…

Muon colliders are expected to naturally have a small spread in beam energy making them an ideal place to study the excitation curve. We present the parameter determinations that are possible from measuring the total cross section near…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. S. Berger

Transverse momentum (p_T) spectra of neutral pions and charged hadrons measured in Au+Au and d+Au collisions at sqrt{s_NN}=200 GeV by the PHENIX experiment at RHIC are compared to p+p reference spectra at the same sqrt{s_NN}. In central…

Nuclear Experiment · Physics 2019-08-14 Klaus Reygers

One of the fundamental goals of the PHENIX experiment is to understand the structure of cold nuclear matter, since this serves as the initial state for heavy-ion collisions. Knowing the initial state is vital for interpreting measurements…

Nuclear Experiment · Physics 2012-10-10 Mickey Chiu

A muon collider could produce the heavier Standard Model particles with a boost, for example in resonant processes such as $\mu^-\mu^+\to h$ or $\mu^-\mu^+\to Z$. We propose machine configurations that produce the boost (asymmetric beam…

High Energy Physics - Phenomenology · Physics 2023-09-27 Daniele Barducci , Alessandro Strumia

We have investigated the production potential of the spin-1/2 excited muons, predicted by the preonic models, at the four SPPC (Super Proton-Proton Collider)-based muon-proton colliders in different center-of-mass energies. For the signal…

High Energy Physics - Phenomenology · Physics 2019-10-23 Abdullatif Caliskan

Flavor-breaking interactions due to heavy new physics can be probed at a 10 TeV muon collider in the high-energy production of quarks and leptons. The high collision energy mitigates the suppression of the new interactions, offering…

High Energy Physics - Phenomenology · Physics 2025-12-23 Alfredo Glioti , David Marzocca , Andrea Wulzer

The COMPASS experiment makes use of the CERN SPS high-intensitymuon and hadron beams for the investigation of the nucleon spin structure and the spectroscopy of hadrons. One or more outgoing particles are detected in coincidence with the…

High Energy Physics - Experiment · Physics 2008-11-26 COMPASS Collaboration , P. Abbon

An electron-muon collider with an asymmetric collision profile targeting multi-ab$^{-1}$ integrated luminosity is proposed. This novel collider, operating at collisions energies of e.g. 20-200 GeV, 50-1000 GeV and 100-3000 GeV, would be…

High Energy Physics - Phenomenology · Physics 2020-11-16 Meng Lu , Andrew Michael Levin , Congqiao Li , Antonios Agapitos , Qiang Li , Fanqiang Meng , Sitian Qian , Jie Xiao , Tianyi Yang

This report presents double helicity asymmetry in inclusive $\pi^0$ production in polarized proton-proton collisions at a center-of-mass energy ($\sqrt{s}$) of 200 GeV. The data were collected with the PHENIX detector at the Relativistic…

High Energy Physics - Experiment · Physics 2019-08-14 Y. Fukao

ALICE is the LHC experiment dedicated to the study of heavy-ion collisions. At forward rapidity a muon spectrometer detects muons from low mass mesons, quarkonia, open heavy-flavor hadrons as well as weak bosons. A muon selection based on…

Instrumentation and Detectors · Physics 2019-08-13 Massimiliano Marchisone