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Polarized ion beams at the Electron Ion Collider are essential to address some of the most important open questions at the twenty-first century frontiers of understanding of the fundamental structure of matter. Here, we summarize the…

Beam polarisation is an integral part of the physics case of future Linear Colliders. In this contribution, important examples from Higgs coupling measurements, top and electroweak physics at high energies, the Z pole program as well as…

High Energy Physics - Experiment · Physics 2021-02-10 Jenny List

We analyze beam-induced depolarizing effects in the hydrogen jet target (HJET) at the Relativistic Heavy Ion Collider (RHIC) that has been used for absolute hadron beam polarimetry and shall be employed at the Electron-Ion Collider (EIC).…

A polarized ep/eA collider (Electron-Ion Collider, or EIC) with variable center-of-mass energy sqrt(s) ~ 20-70 GeV and a luminosity ~ 10^{34} cm^{-2} s^{-1} would be uniquely suited to address several outstanding questions of Quantum…

Nuclear Theory · Physics 2015-05-30 A. Accardi , V. Guzey , A. Prokudin , C. Weiss

Any future high energy e+e- linear collider aims at precision measurements of Standard Model quantities as well as of new, not yet discovered phenomena. In order to pursue this physics programme, excellent detectors at the interaction…

The physics program at the upgraded Jefferson Lab (JLab) and the physics program envisioned for the proposed electron-ion collider (EIC) include large efforts to search for interactions beyond the Standard Model (SM) using parity violation…

Accelerator Physics · Physics 2014-02-10 Prajwal Mohanmurthy , Dipangkar Dutta

The HERMES hydrogen and deuterium nuclear-polarized gas targets have been in use since 1996 with the polarized electron beam of HERA at DESY to study the spin structure of the nucleon. Polarized atoms from a Stern-Gerlach Atomic Beam Source…

Instrumentation and Detectors · Physics 2012-08-27 The HERMES Collaboration

Precision experiments in the parity violating electron scattering (PVES) sector is one the leading methods to probe physics beyond the standard model (SM). A large part of the physics program being envisioned for future facilities such as…

Accelerator Physics · Physics 2018-10-12 Prajwal Mohanmurthy , Dipangkar Dutta

The high-luminosity high-energy Electron-Ion Collider (EIC) to be built at Brookhaven National Laboratory (BNL) will provide a clean environment to study several fundamental questions in the high energy and nuclear physics fields. A high…

Instrumentation and Detectors · Physics 2023-05-09 Xuan Li

Since 2012, a BNL-MIT collaboration has worked to develop a polarized $^3$He ion source for the Relativistic Heavy Ion Collider (RHIC) using the existing Electron Beam Ionization Source (EBIS). $^3$He atoms are polarized using optical…

Instrumentation and Detectors · Physics 2023-08-08 Charles Epstein , Richard Milner

For the planned International Linear Collider it is intended to have both -- electron and positron -- beams polarised. This offers a great benefit for many physics studies, but also provides a challenge for the engineering of the machine. A…

High Energy Physics - Experiment · Physics 2008-11-26 Andreas Schälicke

In this talk, I demonstrate that the proposed Electron-Ion Collider (EIC) will be an ideal and unique future facility to address many overarching questions about QCD and strong interaction physics at one place. The EIC will be the world's…

High Energy Physics - Phenomenology · Physics 2015-06-23 Jian-Wei Qiu

An Electron-Ion Collider (EIC) with suitable forward detection capabilities would enable a unique experimental program of deep-inelastic scattering (DIS) from polarized light nuclei (deuterium 2H, helium 3He) with spectator nucleon tagging.…

High Energy Physics - Phenomenology · Physics 2014-11-03 V. Guzey , D. Higinbotham , Ch. Hyde , P. Nadel-Turonski , K. Park , M. Sargsian , M. Strikman , C. Weiss

This report describes the physics case, the resulting detector requirements, and the evolving detector concepts for the experimental program at the Electron-Ion Collider (EIC). The EIC will be a powerful new high-luminosity facility in the…

Instrumentation and Detectors · Physics 2023-04-24 R. Abdul Khalek , A. Accardi , J. Adam , D. Adamiak , W. Akers , M. Albaladejo , A. Al-bataineh , M. G. Alexeev , F. Ameli , P. Antonioli , N. Armesto , W. R. Armstrong , M. Arratia , J. Arrington , A. Asaturyan , M. Asai , E. C. Aschenauer , S. Aune , H. Avagyan , C. Ayerbe Gayoso , B. Azmoun , A. Bacchetta , M. D. Baker , F. Barbosa , L. Barion , K. N. Barish , P. C. Barry , M. Battaglieri , A. Bazilevsky , N. K. Behera , F. Benmokhtar , V. V. Berdnikov , J. C. Bernauer , V. Bertone , S. Bhattacharya , C. Bissolotti , D. Boer , M. Boglione , M. Bondì , P. Boora , I. Borsa , F. Bossù , G. Bozzi , J. D. Brandenburg , N. Brei , A. Bressan , W. K. Brooks , S. Bufalino , M. H. S. Bukhari , V. Burkert , N. H. Buttimore , A. Camsonne , A. Celentano , F. G. Celiberto , W. Chang , C. Chatterjee , K. Chen , T. Chetry , T. Chiarusi , Y. -T. Chien , M. Chiosso , X. Chu , E. Chudakov , G. Cicala , E. Cisbani , I. C. Cloet , C. Cocuzza , P. L. Cole , D. Colella , J. L. Collins , M. Constantinou , M. Contalbrigo , G. Contin , R. Corliss , W. Cosyn , A. Courtoy , J. Crafts , R. Cruz-Torres , R. C. Cuevas , U. D'Alesio , S. Dalla Torre , D. Das , S. S. Dasgupta , C. Da Silva , W. Deconinck , M. Defurne , W. DeGraw , K. Dehmelt , A. Del Dotto , F. Delcarro , A. Deshpande , W. Detmold , R. De Vita , M. Diefenthaler , C. Dilks , D. U. Dixit , S. Dulat , A. Dumitru , R. Dupré , J. M. Durham , M. G. Echevarria , L. El Fassi , D. Elia , R. Ent , R. Esha , J. J. Ethier , O. Evdokimov , K. O. Eyser , C. Fanelli , R. Fatemi , S. Fazio , C. Fernandez-Ramirez , M. Finger , M. Finger , D. Fitzgerald , C. Flore , T. Frederico , I. Friščić , S. Fucini , S. Furletov , Y. Furletova , C. Gal , L. Gamberg , H. Gao , P. Garg , D. Gaskell , K. Gates , M. B. Gay Ducati , M. Gericke , G. Gil da Silveira , F. -X. Girod , D. I. Glazier , K. Gnanvo , V. P. Goncalves , L. Gonella , J. O. Gonzalez Hernandez , Y. Goto , F. Grancagnolo , L. C. Greiner , W. Guryn , V. Guzey , Y. Hatta , M. Hattawy , F. Hauenstein , X. He , T. K. Hemmick , O. Hen , G. Heyes , D. W. Higinbotham , A. N. Hiller Blin , T. J. Hobbs , M. Hohlmann , T. Horn , T. -J. Hou , J. Huang , Q. Huang , G. M. Huber , C. E. Hyde , G. Iakovidis , Y. Ilieva , B. V. Jacak , P. M. Jacobs , M. Jadhav , Z. Janoska , A. Jentsch , T. Jezo , X. Jing , P. G. Jones , K. Joo , S. Joosten , V. Kafka , N. Kalantarians , G. Kalicy , D. Kang , Z. B. Kang , K. Kauder , S. J. D. Kay , C. E. Keppel , J. Kim , A. Kiselev , M. Klasen , S. Klein , H. T. Klest , O. Korchak , A. Kostina , P. Kotko , Y. V. Kovchegov , M. Krelina , S. Kuleshov , S. Kumano , K. S. Kumar , R. Kumar , L. Kumar , K. Kumerički , A. Kusina , K. Kutak , Y. S. Lai , K. Lalwani , T. Lappi , J. Lauret , M. Lavinsky , D. Lawrence , D. Lednicky , C. Lee , K. Lee , S. H. Lee , S. Levorato , H. Li , S. Li , W. Li , X. Li , X. Li , W. B. Li , T. Ligonzo , H. Liu , M. X. Liu , X. Liu , S. Liuti , N. Liyanage , C. Lorcé , Z. Lu , G. Lucero , N. S. Lukow , E. Lunghi , R. Majka , Y. Makris , I. Mandjavidze , S. Mantry , H. Mäntysaari , F. Marhauser , P. Markowitz , L. Marsicano , A. Mastroserio , V. Mathieu , Y. Mehtar-Tani , W. Melnitchouk , L. Mendez , A. Metz , Z. -E. Meziani , C. Mezrag , M. Mihovilovič , R. Milner , M. Mirazita , H. Mkrtchyan , A. Mkrtchyan , V. Mochalov , V. Moiseev , M. M. Mondal , A. Morreale , D. Morrison , L. Motyka , H. Moutarde , C. Muñoz Camacho , F. Murgia , M. J. Murray , P. Musico , P. Nadel-Turonski , P. M. Nadolsky , J. Nam , P. R. Newman , D. Neyret , D. Nguyen , E. R. Nocera , F. Noferini , F. Noto , A. S. Nunes , V. A. Okorokov , F. Olness , J. D. Osborn , B. S. Page , S. Park , A. Parker , K. Paschke , B. Pasquini , H. Paukkunen , S. Paul , C. Pecar , I. L. Pegg , C. Pellegrino , C. Peng , L. Pentchev , R. Perrino , F. Petriello , R. Petti , A. Pilloni , C. Pinkenburg , B. Pire , C. Pisano , D. Pitonyak , A. A. Poblaguev , T. Polakovic , M. Posik , M. Potekhin , R. Preghenella , S. Preins , A. Prokudin , P. Pujahari , M. L. Purschke , J. R. Pybus , M. Radici , R. Rajput-Ghoshal , P. E. Reimer , M. Rinaldi , F. Ringer , C. D. Roberts , S. Rodini , J. Rojo , D. Romanov , P. Rossi , E. Santopinto , M. Sarsour , R. Sassot , N. Sato , B. Schenke , W. B. Schmidke , I. Schmidt , A. Schmidt , B. Schmookler , G. Schnell , P. Schweitzer , J. Schwiening , I. Scimemi , S. Scopetta , J. Segovia , R. Seidl , S. Sekula , K. Semenov-Tian-Shanskiy , D. Y. Shao , N. Sherrill , E. Sichtermann , M. Siddikov , A. Signori , B. K. Singh , S. Širca , K. Slifer , W. Slominski , D. Sokhan , W. E. Sondheim , Y. Song , O. Soto , H. Spiesberger , A. M. Stasto , P. Stepanov , G. Sterman , J. R. Stevens , I. W. Stewart , I. Strakovsky , M. Strikman , M. Sturm , M. L. Stutzman , M. Sullivan , B. Surrow , P. Svihra , S. Syritsyn , A. Szczepaniak , P. Sznajder , H. Szumila-Vance , L. Szymanowski , A. S. Tadepalli , J. D. Tapia Takaki , G. F. Tassielli , J. Terry , F. Tessarotto , K. Tezgin , L. Tomasek , F. Torales Acosta , P. Tribedy , A. Tricoli , Triloki , S. Tripathi , R. L. Trotta , O. D. Tsai , Z. Tu , C. Tuvè , T. Ullrich , M. Ungaro , G. M. Urciuoli , A. Valentini , P. Vancura , M. Vandenbroucke , C. Van Hulse , G. Varner , R. Venugopalan , I. Vitev , A. Vladimirov , G. Volpe , A. Vossen , E. Voutier , J. Wagner , S. Wallon , H. Wang , Q. Wang , X. Wang , S. Y. Wei , C. Weiss , T. Wenaus , H. Wennlöf , N. Wickramaarachchi , A. Wikramanayake , D. Winney , C. P. Wong , C. Woody , L. Xia , B. W. Xiao , J. Xie , H. Xing , Q. H. Xu , J. Zhang , S. Zhang , Z. Zhang , Z. W. Zhao , Y. X. Zhao , L. Zheng , Y. Zhou , P. Zurita

Atomic nuclei can be used as spatial analyzers of the hadronization process in semi-inclusive deep inelastic scattering. The study of this process using fully-identified final state hadrons began with the HERMES program in the late 1990s,…

High Energy Physics - Phenomenology · Physics 2015-05-30 Will Brooks , Hayk Hakobyan , Cristian Peña , Miguel Arratia , Constanza Valdés

To achieve the extremely high luminosity for colliding electron-positron beams at the future International Linear Collider (ILC) an undulator-based source with about 230 meters helical undulator and a thin titanium-alloy target rim rotated…

Accelerator Physics · Physics 2017-08-23 A. Ushakov , O. S. Adeyemi , G. Moortgat-Pick , F. Staufenbiel , S. Riemann

The full exploitation of the physics potential of a future Linear Collider requires the development of polarised positron beams. A very promising scheme for the technical realisation is the use of helical undulators, generating circular…

High Energy Physics - Phenomenology · Physics 2011-09-13 Gudrid Moortgat-Pick

The Electron-Ion Collider (EIC) will be the next frontier project of nuclear physics in the United States. It is planned to be built in the Brookhaven National Laboratory (BNL) in close collaboration with Jefferson Lab. One of the key…

Instrumentation and Detectors · Physics 2022-02-15 Greg Kalicy

Several important and unique measurements, within the standard model and of possible physics beyond it, could be made with {\em polarized HERA} in which both the proton and the electron beams are polarized. With a $\sim$820 GeV proton beam…

High Energy Physics - Experiment · Physics 2007-05-23 A. Deshpande

An electron-proton/ion collider facility (eRHIC) is under consideration at Brookhaven National Laboratory (BNL). Such a new facility will require the design and construction of a new optimized detector profiting from the experience gained…

High Energy Physics - Experiment · Physics 2009-11-11 Bernd Surrow