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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

The unique physics opportunities accessible with nuclear collisions at the CERN Future Circular Collider (FCC) are summarized. Lead-lead (PbPb) and proton-lead (pPb) collisions at $\sqrt{s_{NN}}$ = 39 and 63 TeV respectively with…

While strong attenuation of single particle production and particle correlations has provided convincing evidence for large parton energy loss in the QGP, its application to jet tomography has inherent limitations due to the inclusive…

High Energy Physics - Phenomenology · Physics 2009-11-18 Ben-Wei Zhang

The Electron-Ion Collider (EIC) is a next-generation accelerator primarily designed to study the internal structure of nucleons through high-precision electron-hadron collisions. In this work, we explore the feasibility of employing a 1 MW…

High Energy Physics - Phenomenology · Physics 2026-03-06 Nishat Fiza , Mehedi Masud , Kim Siyeon , Guang Yang

High-energy electron scattering is a clean and precise probe for measurements of hadronic and nuclear structure, with a key role in understanding the role of high-momentum nucleons (and quarks) in nuclei. Jefferson Lab has dramatically…

Nuclear Experiment · Physics 2022-03-08 John Arrington , Nadia Fomin , Axel Schmidt

The nucleon energy-energy correlator (NEEC) was proposed in 2209.02080 as a new way of studying nucleon intrinsic dynamics. In this work, we present a detailed derivation of the factorization theorem that enables the measurement of the…

High Energy Physics - Phenomenology · Physics 2023-03-06 Haotian Cao , Xiaohui Liu , Hua Xing Zhu

The confining transition from asymptotically free partons to hadrons remains one of the most mysterious aspects of Quantum Chromodynamics. With the wealth of high quality jet substructure data we can hope to gain new experimental insights…

High Energy Physics - Phenomenology · Physics 2023-08-03 Kyle Lee , Ian Moult

These proceedings present a brief overview of the main results on jet-modifications in heavy ion collisions at RHIC. In heavy ion collisions, jets are studied using single hadron spectra and di-hadron correlations with a high-\pt{} trigger…

Nuclear Experiment · Physics 2008-08-07 M. van Leeuwen

The sensitivity of calorimetric energy-energy correlation function to the medium-induced energy loss of fast partons in high multiplicity heavy ion interactions is demonstrated at the appropriate selection of events for the analysis,…

High Energy Physics - Phenomenology · Physics 2015-12-30 I. P. Lokhtin , L. I. Sarycheva , A. M. Snigirev

Collimated sprays of hadrons, called jets, are an emergent phenomenon of Quantum Chromodynamics (QCD) at collider experiments, whose detailed internal structure encodes valuable information about the interactions of high energy quarks and…

High Energy Physics - Phenomenology · Physics 2021-04-01 Hao Chen , Ian Moult , Hua Xing Zhu

An Electron-Ion Collider (EIC) would enable next-generation measurements of deep-inelastic scattering (DIS) on the deuteron with detection of a forward-moving nucleon (p, n) and measurement of its recoil momentum ("spectator tagging"). Such…

High Energy Physics - Phenomenology · Physics 2016-04-20 W. Cosyn , V. Guzey , M. Sargsian , M. Strikman , C. Weiss

We propose the lepton-jet correlation in deep inelastic scattering as a unique tool for nucleon/nucleus tomography at the electron-ion collider. The azimuthal angular correlation between the final state lepton and jet depends on the…

High Energy Physics - Phenomenology · Physics 2019-05-22 Xiaohui Liu , Felix Ringer , Werner Vogelsang , Feng Yuan

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

Cold nuclear matter effects in reactions with nuclei at a future electron-ion collider (EIC) lead to a modification of semi-inclusive hadron production, jet cross sections, and jet substructure when compared to the vacuum. At leading order…

High Energy Physics - Phenomenology · Physics 2018-11-21 Matthew D. Sievert , Ivan Vitev

The medium-modifications of processes characterized by the presence of a hard scale provide the most diverse tools to characterize the properties of the matter created in high-energy nuclear collisions. Indeed, jet quenching, the…

High Energy Physics - Phenomenology · Physics 2015-05-30 Carlos A. Salgado

Hard-jet correlations probe parton energy loss and the microscopic structure of the quark-gluon plasma formed in ultra-relativistic heavy-ion collisions. The correlation of high-$p_\mathrm{T}$ jets with other jets, hadrons, or electroweak…

Nuclear Experiment · Physics 2025-05-02 Riccardo Longo

The LHeC and the FCC-he will open a new realm in our understanding of nuclear structure and the dynamics in processes involving nuclei, in an unexplored kinematic domain. We review some of the recent studies as shown in the update of the…

High Energy Physics - Phenomenology · Physics 2020-10-13 Heikki Mäntysaari

Pions constitute nearly $70\%$ of final state particles in ultra high energy collisions. They act as a probe to understand the statistical properties of Quantum Chromodynamics (QCD) matter i.e. Quark Gluon Plasma (QGP) created in such…

Data Analysis, Statistics and Probability · Physics 2021-03-31 Yogesh Verma , Satyajit Jena

We define a new strategy to scan jet substructure in heavy-ion collisions. The scope is multifold: (i) test the dominance of vacuum jet dynamics at early times, (ii) capture the transition from coherent to incoherent jet energy loss, and…

High Energy Physics - Phenomenology · Physics 2024-09-05 Leticia Cunqueiro , Daniel Pablos , Alba Soto-Ontoso , Martin Spousta , Adam Takacs , Marta Verweij

Lepto-nuclear colliders offer unique experimental opportunities to probe QCD in an extended medium. Of the many possibilities, three experiments are described here that are clearly feasible and of high scientific importance. First, a direct…

Nuclear Experiment · Physics 2010-11-19 W K Brooks