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Generalized parton distributions (GPDs) encoding multidimensional information of hadron partonic structure appear as the building blocks in a factorized description of hard exclusive reactions. The nucleon GPDs have been accessed by deeply…

Nuclear Experiment · Physics 2016-07-01 Takahiro Sawada , Wen-Chen Chang , Shunzo Kumano , Jen-Chieh Peng , Shinya Sawada , Kazuhiro Tanaka

QCD gives rise to a rich spectrum of excited baryon states. Understanding their internal structure is important for many areas of nuclear physics, such as nuclear forces, dense matter, and neutrino-nucleus interactions. Generalized parton…

This dissertation explores two main topics: 1) Color Transparency and quasi-elastic knockout reactions involving pions and $\rho$ mesons; and 2) determination of the $J/\psi$-nucleon scattering amplitude and scattering length via $J/\psi$…

Nuclear Theory · Physics 2013-03-13 Gary T. Howell

The future opportunities for high-density QCD studies with ion and proton beams at the LHC are presented. Four major scientific goals are identified: the characterisation of the macroscopic long wavelength Quark-Gluon Plasma (QGP)…

High Energy Physics - Phenomenology · Physics 2019-02-26 Z. Citron , A. Dainese , J. F. Grosse-Oetringhaus , J. M. Jowett , Y. -J. Lee , U. A. Wiedemann , M. Winn , A. Andronic , F. Bellini , E. Bruna , E. Chapon , H. Dembinski , D. d'Enterria , I. Grabowska-Bold , G. M. Innocenti , C. Loizides , S. Mohapatra , C. A. Salgado , M. Verweij , M. Weber , J. Aichelin , A. Angerami , L. Apolinario , F. Arleo , N. Armesto , R. Arnaldi , M. Arslandok , P. Azzi , R. Bailhache , S. A. Bass , C. Bedda , N. K. Behera , R. Bellwied , A. Beraudo , R. Bi , C. Bierlich , K. Blum , A. Borissov , P. Braun-Munzinger , R. Bruce , G. E. Bruno , S. Bufalino , J. Castillo Castellanos , R. Chatterjee , Y. Chen , Z. Chen , C. Cheshkov , T. Chujo , Z. Conesa del Valle , J. G. Contreras Nuno , L. Cunqueiro Mendez , T. Dahms , N. P. Dang , H. De la Torre , A. F. Dobrin , B. Doenigus , L. Van Doremalen , X. Du , A. Dubla , M. Dumancic , M. Dyndal , L. Fabbietti , E. G. Ferreiro , F. Fionda , F. Fleuret , S. Floerchinger , G. Giacalone , A. Giammanco , P. B. Gossiaux , G. Graziani , V. Greco , A. Grelli , F. Grosa , M. Guilbaud , T. Gunji , V. Guzey , C. Hadjidakis , S. Hassani , M. He , I. Helenius , P. Huo , P. M. Jacobs , P. Janus , M. A. Jebramcik , J. Jia , A. P. Kalweit , H. Kim , M. Klasen , S. R. Klein , M. Klusek-Gawenda , M. Konyushikhin , J. Kremer , G. K. Krintiras , F. Krizek , E. Kryshen , A. Kurkela , A. Kusina , J. -P. Lansberg , R. Lea , M. van Leeuwen , W. Li , J. Margutti , A. Marin , C. Marquet , J. Martin Blanco , L. Massacrier , A. Mastroserio , E. Maurice , C. Mayer , C. Mcginn , G. Milhano , A. Milov , V. Minissale , C. Mironov , A. Mischke , N. Mohammadi , M. Mulders , M. Murray , M. Narain , P. Di Nezza , A. Nisati , J. Noronha-Hostler , A. Ohlson , V. Okorokov , F. Olness , P. Paakkinen , L. Pappalardo , J. Park , H. Paukkunen , C. C. Peng , H. Pereira Da Costa , D. V. Perepelitsa , D. Peresunko , M. Peters , N. E. Pettersson , S. Piano , T. Pierog , J. Pires , M. PS. Plumari , F. Prino , M. Puccio , R. Rapp , K. Redlich , K. Reygers , C. L. Ristea , P. Robbe , A. Rossi , A. Rustamov , M. Rybar , M. Schaumann , B. Schenke , I. Schienbein , L. Schoeffel , I. Selyuzhenkov , A. M. Sickles , M. Sievert , P. Silva , T. Song , M. Spousta , J. Stachel , P. Steinberg , D. Stocco , M. Strickland , M. Strikman , J. Sun , D. Tapia Takaki , K. Tatar , C. Terrevoli , A. Timmins , S. Trogolo , B. Trzeciak , A. Trzupek , R. Ulrich , A. Uras , R. Venugopalan , I. Vitev , G. Vujanovic , J. Wang , T. W. Wang , R. Xiao , Y. Xu , C. Zampolli , H. Zanoli , M. Zhou , Y. Zhou

Study of in-medium mass modification has attracted interest in terms of the restoration of the spontaneously broken chiral symmetry, which is responsible for the generation of hadron mass. Many experiments were performed to measure…

Nuclear Experiment · Physics 2019-08-14 Kazuya Aoki

The designed 2m propane bubble chambers(PBC) with modern power technologies for PC and high precision digital photographic methods is a unique multi-propose, competitive capable and higher-informative 4$\pi$ detector for study of exotic…

High Energy Physics - Experiment · Physics 2010-12-21 Aslanyan P. Zh

We review a unique prediction of Quantum Chromo Dynamics, called color transparency (CT), where the final (and/or initial) state interactions of hadrons with the nuclear medium must vanish for exclusive processes at high momentum transfers.…

Nuclear Theory · Physics 2015-06-12 D. Dutta , K. Hafidi , M. Strikman

Generalized Parton Distributions (GPDs) have emerged as a powerful framework for exploring the internal structure of hadrons in terms of their partonic constituents. Over the past three decades, the field has witnessed significant…

High quality polarized electron beams at Jefferson Lab make possible precision measurements of hadronic properties in the regime of strongly interacting QCD. We will describe a few programs at Jefferson Lab that are making measurements that…

Nuclear Experiment · Physics 2014-11-18 Elton S. Smith

The COMPASS experiment at CERN SPS will use hadron beams (pion, kaon and proton) and muons at 50-280 GeV/c and virtual photon targets to investigate, via Primakoff effect, important hadron properties: polarizability, chiral anomaly,…

High Energy Physics - Experiment · Physics 2007-05-23 Murray A. Moinester , Victor Steiner , Serguei Prakhov

Generalized parton distributions (GPDs) encoding multidimensional information of hadron partonic structure appear as the building blocks in a factorized description of hard exclusive reactions. The nucleon GPDs have been accessed by deeply…

High Energy Physics - Phenomenology · Physics 2017-09-06 Kazuhiro Tanaka

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental programs at the next generation of lepton accelerators. In the context of the hadronic physics program at Jefferson Lab (JLab),…

Nuclear Experiment · Physics 2021-09-15 A. Accardi , A. Afanasev , I. Albayrak , S. F. Ali , M. Amaryan , J. R. M. Annand , J. Arrington , A. Asaturyan , H. Atac , H. Avakian , T. Averett , C. Ayerbe Gayoso , X. Bai , L. Barion , M. Battaglieri , V. Bellini , R. Beminiwattha , F. Benmokhtar , V. V. Berdnikov , J. C. Bernauer , V. Bertone , A. Bianconi , A. Biselli , P. Bisio , P. Blunden , M. Boer , M. Bondì , K. -T. Brinkmann , W. J. Briscoe , V. Burkert , T. Cao , A. Camsonne , R. Capobianco , L. Cardman , M. Carmignotto , M. Caudron , L. Causse , A. Celentano , P. Chatagnon , J. -P. Chen , T. Chetry , G. Ciullo , E. Cline , P. L. Cole , M. Contalbrigo , G. Costantini , A. D'Angelo , L. Darmé , D. Day , M. Defurne , M. De Napoli , A. Deur , R. De Vita , N. D'Hose , S. Diehl , M. Diefenthaler , B. Dongwi , R. Dupré , H. Dutrieux , D. Dutta , M. Ehrhart , L. El Fassi , L. Elouadrhiri , R. Ent , J. Erler , I. P. Fernando , A. Filippi , D. Flay , T. Forest , E. Fuchey , S. Fucini , Y. Furletova , H. Gao , D. Gaskell , A. Gasparian , T. Gautam , F. -X. Girod , K. Gnanvo , J. Grames , G. N. Grauvoge , P. Gueye , M. Guidal , S. Habet , T. J. Hague , D. J. Hamilton , O. Hansen , D. Hasell , M. Hattawy , D. W. Higinbotham , A. Hobart , T. Horn , C. E. Hyde , H. Ibrahim , A. Ilyichev , A. Italiano , K. Joo , S. J. Joosten , V. Khachatryan , N. Kalantarians , G. Kalicy , B. Karky , D. Keller , C. Keppel , M. Kerver , M. Khandaker , A. Kim , J. Kim , P. M. King , E. Kinney , V. Klimenko , H. -S. Ko , M. Kohl , V. Kozhuharov , B. T. Kriesten , G. Krnjaic , V. Kubarovsky , T. Kutz , L. Lanza , M. Leali , P. Lenisa , N. Liyanage , Q. Liu , S. Liuti , J. Mammei , S. Mantry , D. Marchand , P. Markowitz , L. Marsicano , V. Mascagna , M. Mazouz , M. McCaughan , B. McKinnon , D. McNulty , W. Melnitchouk , A. Metz , Z. -E. Meziani , S. Migliorati , M. Mihovilovic , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , H. Moutarde , M. Muhoza , C. Muñoz Camacho , J. Murphy , P. Nadel-Turonski , E. Nardi , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , J. F. Owens , M. Paolone , L. Pappalardo , R. Paremuzyan , B. Pasquini , E. Pasyuk , T. Patel , I. Pegg , C. Peng , D. Perera , M. Poelker , K. Price , A. J. R. Puckett , M. Raggi , N. Randazzo , M. N. H. Rashad , M. Rathnayake , B. Raue , P. E. Reimer , M. Rinaldi , A. Rizzo , Y. Roblin , J. Roche , O. Rondon-Aramayo , F. Sabatié , G. Salmè , E. Santopinto , R. Santos Estrada , B. Sawatzky , A. Schmidt , P. Schweitzer , S. Scopetta , V. Sergeyeva , M. Shabestari , A. Shahinyan , Y. Sharabian , S. Širca , E. S. Smith , D. Sokhan , A. Somov , N. Sparveris , M. Spata , H. Spiesberger , M. Spreafico , S. Stepanyan , P. Stoler , I. Strakovsky , R. Suleiman , M. Suresh , P. Sznajder , H. Szumila-Vance , V. Tadevosyan , A. S. Tadepalli , A. W. Thomas , M. Tiefenback , R. Trotta , M. Ungaro , P. Valente , M. Vanderhaeghen , L. Venturelli , H. Voskanyan , E. Voutier , B. Wojtsekhowski , M. H. Wood , S. Wood , J. Xie , W. Xiong , Z. Ye , M. Yurov , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhang , S. Zhao , Z. W. Zhao , X. Zheng , J. Zhou , C. Zorn

Intense and well-characterized neutrino sources, coupled with large and high-performance detectors, are essential for elucidating the unknowns in leptonic mixing through neutrino oscillation measurements. The J-PARC accelerator and neutrino…

High Energy Physics - Experiment · Physics 2024-10-23 Son Cao , Megan Friend

Parton luminosities are convenient for estimating how the physics potential of Large Hadron Collider experiments depends on the energy of the proton beams. I quantify the advantage of increasing the beam energy from 3.5 TeV to 4 TeV. I…

High Energy Physics - Phenomenology · Physics 2011-02-02 Chris Quigg

Novel considerations are presented on the physics, apparatus and accelerator designs for a future, luminous, energy frontier electron-hadron ($eh$) scattering experiment at the LHC in the thirties for which key physics topics and their…

We outline major ideas involved in discussion of color coherence phenomena (CCP) at intermediate energies. We point out that the recent advances in calculating cross sections of hard exclusive processes off light nuclei allow to use the…

High Energy Physics - Phenomenology · Physics 2011-08-17 Mark Strikman , Michail Zhalov

An overview is presented of the upgrade of JLab's cw electron accelerator from a maximum beam energy of currently 6 GeV to 12 GeV. Construction of the 12 GeV upgrade project has started in 2008. A broad experimental program has been…

Nuclear Experiment · Physics 2012-03-13 Volker D. Burkert

Color transparency occurs if a small-sized wave packet, formed in a high momentum transfer process, escapes the nucleus before expanding. The time required for the expansion depends on the masses of the baryonic components of the wave…

High Energy Physics - Phenomenology · Physics 2009-10-22 B. K. Jennings , G. A. Miller

We show that the QCD color transparency of higher-twist contributions to inclusive hadroproduction cross sections, where baryons are produced directly in a short-distance subprocess, can explain several remarkable features of high-$p_T$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Stanley J. Brodsky , Anne Sickles

An "ultimate" high intensity proton source for neutrino factories and/or muon colliders was projected to be a ~4 MW multi-GeV proton source providing short, intense proton pulses at ~15 Hz. The JPARC ~1 MW accelerators provide beam at…

Accelerator Physics · Physics 2017-04-27 D. Neuffer