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The performed systematic meta-analysis of the quality of data description (QDD) of existing event generators of nucleus-nucleus collisions allows us to extract a very important physical information. Our meta-analysis is dealing with the…

High Energy Physics - Phenomenology · Physics 2015-04-27 V. A. Kizka , V. S. Trubnikov , K. A. Bugaev , D. R. Oliinychenko

I review recent progress in the determination of the parton structure of the nucleon, in particular from deep-inelastic structure functions. I explain how the needs of current and future precision phenomenology, specifically at the LHC,…

High Energy Physics - Phenomenology · Physics 2015-06-25 Stefano Forte

The angular structure of collisional and radiative energy losses of a hard parton jet propagating through the quark-gluon plasma is analyzed. The possibility to observe the energy losses of quark- and gluon-initiated jets in dense…

High Energy Physics - Phenomenology · Physics 2016-09-06 I. P. Lokhtin

The Large Hadron Collider at CERN will provide Pb-Pb collisions at energies up to $\sqrt{s_{NN}}$ = 5.5 TeV. We speculate on global observables, i.e. the charged particle density at mid-rapidity, chemical freeze-out conditions and…

Nuclear Experiment · Physics 2009-01-16 K. Schweda

The capabilities of the CMS experiment to study the low-x parton structure and QCD evolution in the proton and the nucleus at LHC energies are presented through four different measurements, to be carried out in Pb-Pb at sqrt(s_NN) = 5.5…

High Energy Physics - Experiment · Physics 2008-11-26 David d'Enterria

The transverse structure of the nucleon as probed in hard exclusive processes plays critical role in the understanding of the structure of the underlying event in hard collisions at the LHC, and multiparton interactions. We summarize…

High Energy Physics - Phenomenology · Physics 2011-12-19 Mark Strikman

QCD and Spin physics are playing important role in our understanding of hadron structure. I will give a short overview of origin of hadron structure in QCD and highlight modern understanding of the subject. Jefferson Laboratory is…

High Energy Physics - Phenomenology · Physics 2015-06-12 A. Prokudin

A brief overview is given on the physics and future lepton-nucleon collider facilities to explore the domain of high parton densities at low Bjorken $x$, with HERA, the electron-ion collider (EIC) and with THERA - in $ep$, polarised…

High Energy Physics - Phenomenology · Physics 2017-08-23 M. Klein

We review recent progress in hadron structure using lattice QCD simulations, with main focus in the evaluation of nucleon quantities such as the axial and tensor charges, and the spin con- tent of the nucleon, using simulations at pion…

High Energy Physics - Lattice · Physics 2015-11-24 Martha Constantinou

The intrinsic transverse momentum distribution of partons in the nucleon can be used to explain a large amount of high-$p_T$ hadron and photon production data in high-energy nucleon-nucleon collisions at energies $\sqrt{s} \approx 20$ to…

Nuclear Theory · Physics 2007-05-23 Gabor Papp , Gergely Barnafoeldi , George Fai , Peter Levai , Yi Zhang

The multi-TeV proton and ion beams of the LHC would allow for the most energetic fixed-target experiment ever. In particular, $pp$, $p$d and $p$A collisions could be performed at $\sqrt{s_{NN}}$ = 115~GeV, as well as Pb$p$ and PbA…

We argue that hadron production in coherent diffraction of proton on a heavy nucleus provides a very sensitive probe of the low-x QCD dynamics. This process probes the BFKL dynamics in proton and the non-linear gluon evolution in nucleus.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yang Li , Kirill Tuchin

We review a microscopic model of the nuclear parton distribution functions, which accounts for a number of nuclear effects including Fermi motion and nuclear binding, nuclear meson-exchange currents, off-shell corrections to bound nucleon…

High Energy Physics - Phenomenology · Physics 2017-04-26 S. A. Kulagin

We consider a possibility that inside the proton and, more generally, inside the hadrons there are additional partons - tensor-gluons, which can carry a part of the proton momentum. The tensor-gluons have zero electric charge, like gluons,…

High Energy Physics - Theory · Physics 2015-06-17 George Savvidy

The Spin Physics Detector at the constructing NICA collider (JINR, Dubna) is a universal facility to investigate the spin structure of the proton and deuteron and the other spin-related phenomena with polarized proton and deuteron beams at…

High Energy Physics - Experiment · Physics 2021-10-19 Alexey Guskov

The Spin Physics Detector (SPD) is a future multipurpose experiment foreseen to run at the NICA collider, which is currently under construction at the Joint Institute for Nuclear Research (JINR, Dubna, Russia). The physics program of the…

Hard processes in nucleus-nucleus interactions at relativistic energies are reviewed with emphasis on recent PHENIX results from the first run of the Relativistic Heavy-Ion Collider at BNL. The observed suppression of moderately high $p_T$…

High Energy Physics - Experiment · Physics 2019-08-14 David G. d'Enterria

This report is based on a ten-week program on "Gluons and the quark sea at high-energies", which took place at the Institute for Nuclear Theory in Seattle in Fall 2010. The principal aim of the program was to develop and sharpen the science…

Nuclear Theory · Physics 2015-03-19 D. Boer , M. Diehl , R. Milner , R. Venugopalan , W. Vogelsang , A. Accardi , E. Aschenauer , M. Burkardt , R. Ent , V. Guzey , D. Hasch , K. Kumar , M. A. C. Lamont , Y. Li , W. J. Marciano , C. Marquet , F. Sabatie , M. Stratmann , F. Yuan , S. Abeyratne , S. Ahmed , C. Aidala , S. Alekhin , M. Anselmino , H. Avakian , A. Bacchetta , J. Bartels , H. BC , J. Beebe-Wang , S. Belomestnykh , I. Ben-Zvi , G. Beuf , J. Blumlein , M . Blaskiewicz , A. Bogacz , S. J. Brodsky , T. Burton , R. Calaga , X. Chang , I. O. Cherednikov , P. Chevtsov , G. A. Chirilli , C. Ciofi degli Atti , I. C. Cloet , A. Cooper-Sarkar , R. Debbe , Ya. Derbenev , A. Deshpande , F. Dominguez , A. Dumitru , R. Dupre , B. Erdelyi , C. Faroughy , S. Fazio , A. Fedotov , J. R. Forshaw , R. Geraud , K. Gallmeister , L. Gamberg , J. -H. Gao , D. Gassner , F. Gelis , G. P. Gilfoyle , G. Goldstein , K. Golec-Biernat , V. P. Goncalves , M. Gonderinger , M. Guzzi , P. Hagler , H. Hahn , L. Hammons , Y. Hao , P. He , T. Horn , W. A. Horowitz , M. Huang , A. Hutton , B. Jager , W. Jackson , A. Jain , E. C. Johnson , Z. -B. Kang , L. P. Kaptari , D. Kayran , J. Kewisch , Y. Koike , A. Kondratenko , B. Z. Kopeliovich , Y. V. Kovchegov , G. Krafft , P. Kroll , S. Kumano , K. Kumericki , T. Lappi , T. Lautenschlager , R. Li , Z. -T. Liang , V. N. Litvinenko , S. Liuti , Y. Luo , D. Muller , G. Mahler , A. Majumder , S. Manikonda , F. Marhauser , G. McIntyre , M. Meskauskas , W. Meng , A. Metz , C. B. Mezzetti , G. A. Miller , M. Minty , S. -O. Moch , V. Morozov , U. Mosel , L. Motyka , H. Moutarde , P. J. Mulders , B. Musch , P. Nadel-Turonski , P. Nadolsky , F. Olness , P. N. Ostrumov , B. Parker , B. Pasquini , K. Passek-Kumericki , A. Pikin , F. Pilat , B. Pire , H. Pirner , C. Pisano , E. Pozdeyev , A. Prokudin , V. Ptitsyn , X. Qian , J. -W. Qiu , M. Radici , A. Radyushkin , T. Rao , R. Rimmer , F. Ringer , S. Riordan , T. Rogers , J. Rojo , T. Roser , R. Sandapen , R. Sassot , T. Satogata , H. Sayed , A. Schafer , G. Schnell , P. Schweitzer , B. Sheehy , J. Skaritka , G. Soyez , M. Spata , H. Spiesberger , A. M. Stasto , N. G. Stefanis , M. Strikman , M. Sullivan , L. Szymanowski , K. Tanaka , S. Taneja , S. Tepikian , B. Terzic , Y. Than , T. Toll , D. Trbojevic , E. Tsentalovich , N. Tsoupas , K. Tuchin , J. Tuozzolo , T. Ullrich , A. Vossen , S. Wallon , G. Wang , H. Wang , X. -N. Wang , S. Webb , C. Weiss , Q. Wu , B. -W. Xiao , W. Xu , B. Yunn , A. Zelenski , Y. Zhang , J. Zhou , P. Zurita

The Quark-Gluon Plasma (QGP) is created in high energy heavy ion collisions at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC). This medium is transparent to electromagnetic probes but nearly opaque to colored…

Nuclear Experiment · Physics 2018-10-17 Christine Nattrass

Nuclear parton distributions and structure functions are determined in an effective chiral quark theory. We also discuss an extension of our model to fragmentation functions.

Nuclear Theory · Physics 2009-03-27 W. Bentz , I. C. Cloët , T. Ito , A. W. Thomas , K. Yazaki
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