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One of the unanswered and most fundamental questions in physics regards the nature of the confinement mechanism of quarks and gluons in QCD. Exotic hybrid mesons manifest gluonic degrees of freedom and their spectroscopy will provide the…

High Energy Physics - Experiment · Physics 2008-11-26 Daniel S. Carman

We obtain the deuteron's wave functions as eigenstates of the light-front quantum chromodynamics (QCD) Hamiltonian using a fully relativistic and nonperturbative approach based on light-front quantization, without an explicit confining…

High Energy Physics - Phenomenology · Physics 2025-05-20 Chandan Mondal , Satvir Kaur , Jiatong Wu , Siqi Xu , Xingbo Zhao , James P. Vary

Recent measurements of selected QCD processes at the Tevatron are reviewed and confronted with theoretical calculations. Results on inclusive jet production at large transverse momentum are compared to predictions from next-to-leading order…

High Energy Physics - Experiment · Physics 2007-05-23 Marek Zielinski

New predictions regarding the role of color flow in high energy Quantum Chromodynamics (QCD) processes have emerged in the last decade. In particular, the role of color flow is now being explored through many different observables; one such…

High Energy Physics - Experiment · Physics 2018-06-21 Joseph D. Osborn

The LHCb collaboration has recently announced the discovery of two hidden-charm pentaquark states with also strange quark content, $P_{cs}(4338)$ and $P_{cs}(4459)$; its analysis points towards having both hadrons isospin equal to zero and…

High Energy Physics - Phenomenology · Physics 2023-11-03 Gang Yang , Jialun Ping , Jorge Segovia

It is usually assumed -- following the parton model -- that the leading-twist structure functions measured in deep inelastic lepton-proton scattering are simply the probability distributions for finding quarks and gluons in the target…

High Energy Physics - Phenomenology · Physics 2009-09-11 S. J. Brodsky

Deep-inelastic production of heavy quarks at HERA, especially charm, is an excellent signal to measure the gluon distribution in the proton at small $x$ values. By measuring various differential distributions of the heavy quarks this…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. Laenen , M. Buza , B. W. Harris , Y. Matiounine , R. Migneron , S. Riemersma , J. Smith , W. L. van Neerven

We present measurements of $\Omega$ and $\phi$ production at mid-rapidity from Au+Au collisions at nucleon-nucleon center-of-mass energies $\sqrt{s_{NN}}$ = 7.7, 11.5, 19.6, 27 and 39 GeV by the STAR experiment at the Relativistic Heavy Ion…

Nuclear Experiment · Physics 2016-03-02 STAR Collaboration , L. Adamczyk , J. K. Adkins , G. Agakishiev , M. M. Aggarwal , Z. Ahammed , I. Alekseev , J. Alford , A. Aparin , D. Arkhipkin , E. C. Aschenauer , G. S. Averichev , V. Bairathi , A. Banerjee , R. Bellwied , A. Bhasin , A. K. Bhati , P. Bhattarai , J. Bielcik , J. Bielcikova , L. C. Bland , I. G. Bordyuzhin , J. Bouchet , A. V. Brandin , I. Bunzarov , J. Butterworth , H. Caines , M. Calderón de la Barca Sánchez , J. M. Campbell , D. Cebra , M. C. Cervantes , I. Chakaberia , P. Chaloupka , Z. Chang , S. Chattopadhyay , J. H. Chen , X. Chen , J. Cheng , M. Cherney , W. Christie , G. Contin , H. J. Crawford , S. Das , L. C. De Silva , R. R. Debbe , T. G. Dedovich , J. Deng , A. A. Derevschikov , B. di Ruzza , L. Didenko , C. Dilks , X. Dong , J. L. Drachenberg , J. E. Draper , C. M. Du , L. E. Dunkelberger , J. C. Dunlop , L. G. Efimov , J. Engelage , G. Eppley , R. Esha , O. Evdokimov , O. Eyser , R. Fatemi , S. Fazio , P. Federic , J. Fedorisin , Z. Feng , P. Filip , Y. Fisyak , C. E. Flores , L. Fulek , C. A. Gagliardi , D. Garand , F. Geurts , A. Gibson , M. Girard , L. Greiner , D. Grosnick , D. S. Gunarathne , Y. Guo , A. Gupta , S. Gupta , W. Guryn , A. Hamad , A. Hamed , R. Haque , J. W. Harris , L. He , S. Heppelmann , S. Heppelmann , A. Hirsch , G. W. Hoffmann , D. J. Hofman , S. Horvat , B. Huang , H. Z. Huang , X. Huang , P. Huck , T. J. Humanic , G. Igo , W. W. Jacobs , H. Jang , K. Jiang , E. G. Judd , S. Kabana , D. Kalinkin , K. Kang , K. Kauder , H. W. Ke , D. Keane , A. Kechechyan , Z. H. Khan , D. P. Kikoła , I. Kisel , A. Kisiel , L. Kochenda , D. D. Koetke , T. Kollegger , L. K. Kosarzewski , A. F. Kraishan , P. Kravtsov , K. Krueger , I. Kulakov , L. Kumar , R. A. Kycia , M. A. C. Lamont , J. M. Landgraf , K. D. Landry , J. Lauret , A. Lebedev , R. Lednicky , J. H. Lee , X. Li , Z. M. Li , Y. Li , W. Li , X. Li , C. Li , M. A. Lisa , F. Liu , T. Ljubicic , W. J. Llope , M. Lomnitz , R. S. Longacre , X. Luo , G. L. Ma , R. Ma , Y. G. Ma , L. Ma , N. Magdy , R. Majka , A. Manion , S. Margetis , C. Markert , H. Masui , H. S. Matis , D. McDonald , K. Meehan , N. G. Minaev , S. Mioduszewski , D. Mishra , B. Mohanty , M. M. Mondal , D. A. Morozov , M. K. Mustafa , B. K. Nandi , Md. Nasim , T. K. Nayak , G. Nigmatkulov , L. V. Nogach , S. Y. Noh , J. Novak , S. B. Nurushev , G. Odyniec , A. Ogawa , K. Oh , V. Okorokov , D. Olvitt , B. S. Page , R. Pak , Y. X. Pan , Y. Pandit , Y. Panebratsev , B. Pawlik , H. Pei , C. Perkins , A. Peterson , P. Pile , M. Planinic , J. Pluta , N. Poljak , K. Poniatowska , J. Porter , M. Posik , A. M. Poskanzer , J. Putschke , H. Qiu , A. Quintero , S. Ramachandran , R. Raniwala , S. Raniwala , R. L. Ray , H. G. Ritter , J. B. Roberts , O. V. Rogachevskiy , J. L. Romero , A. Roy , L. Ruan , J. Rusnak , O. Rusnakova , N. R. Sahoo , P. K. Sahu , I. Sakrejda , S. Salur , J. Sandweiss , A. Sarkar , J. Schambach , R. P. Scharenberg , A. M. Schmah , W. B. Schmidke , N. Schmitz , J. Seger , P. Seyboth , N. Shah , E. Shahaliev , P. V. Shanmuganathan , M. Shao , M. K. Sharma , B. Sharma , W. Q. Shen , S. S. Shi , Q. Y. Shou , E. P. Sichtermann , R. Sikora , M. Simko , M. J. Skoby , N. Smirnov , D. Smirnov , L. Song , P. Sorensen , H. M. Spinka , B. Srivastava , T. D. S. Stanislaus , M. Stepanov , R. Stock , M. Strikhanov , B. Stringfellow , M. Sumbera , B. Summa , Z. Sun , X. M. Sun , Y. Sun , X. Sun , B. Surrow , N. Svirida , M. A. Szelezniak , Z. Tang , A. H. Tang , T. Tarnowsky , A. Tawfik , J. H. Thomas , A. R. Timmins , D. Tlusty , M. Tokarev , S. Trentalange , R. E. Tribble , P. Tribedy , S. K. Tripathy , B. A. Trzeciak , O. D. Tsai , T. Ullrich , D. G. Underwood , I. Upsal , G. Van Buren , G. van Nieuwenhuizen , M. Vandenbroucke , R. Varma , A. N. Vasiliev , R. Vertesi , F. Videbæk , Y. P. Viyogi , S. Vokal , S. A. Voloshin , A. Vossen , G. Wang , H. Wang , J. S. Wang , Y. Wang , Y. Wang , F. Wang , J. C. Webb , G. Webb , L. Wen , G. D. Westfall , H. Wieman , S. W. Wissink , R. Witt , Y. F. Wu , Z. G. Xiao , W. Xie , K. Xin , Y. F. Xu , Q. H. Xu , H. Xu , N. Xu , Z. Xu , Y. Yang , C. Yang , S. Yang , Y. Yang , Q. Yang , Z. Ye , P. Yepes , L. Yi , K. Yip , I. -K. Yoo , N. Yu , H. Zbroszczyk , W. Zha , J. B. Zhang , Z. Zhang , J. Zhang , S. Zhang , X. P. Zhang , J. Zhang , Y. Zhang , F. Zhao , J. Zhao , C. Zhong , L. Zhou , X. Zhu , Y. Zoulkarneeva , M. Zyzak

We propose to create a secondary beam of neutral kaons in Hall D at Jefferson Lab to be used with the GlueX experimental setup for strange hadron spectroscopy. The superior CEBAF electron beam will enable a flux on the order of $1\times…

Nuclear Experiment · Physics 2021-03-05 KLF Collaboration , Moskov Amaryan , Mikhail Bashkanov , Sean Dobbs , James Ritman , Justin Stevens , Igor Strakovsky , Shankar Adhikari , Arshak Asaturyan , Alexander Austregesilo , Marouen Baalouch , Vitaly Baturin , Vladimir Berdnikov , Olga Cortes Becerra , Timothy Black , Werner Boeglin , William Briscoe , William Brooks , Volker Burkert , Eugene Chudakov , Geraint Clash , Philip Cole , Volker Crede , Donal Day , Pavel Degtyarenko , Alexandre Deur , Gail Dodge , Anatoly Dolgolenko , Simon Eidelman , Hovanes Egiyan , Denis Epifanov , Paul Eugenio , Stuart Fegan , Alessandra Filippi , Sergey Furletov , Liping Gan , Franco Garibaldi , Ashot Gasparian , Gagik Gavalian , Derek Glazier , Colin Gleason , Vladimir Goryachev , Lei Guo , David Hamilton , Avetik Hayrapetyan , Garth Huber , Andrew Hurley , Charles Hyde , Isabella Illari , David Ireland , Igal Jaegle , Kyungseon Joo , Vanik Kakoyan , Grzegorz Kalicy , Mahmoud Kamel , Christopher Keith , Chan Wook Kim , Eberhard Klemp , Geoffrey Krafft , Sebastian Kuhn , Sergey Kuleshov , Alexander Laptev , Ilya Larin , David Lawrence , Daniel Lersch , Wenliang Li , Kevin Luckas , Valery Lyubovitskij , David Mack , Michael McCaughan , Mark Manley , Hrachya Marukyan , Vladimir Matveev , Mihai Mocanu , Viktor Mokeev , Curtis Meyer , Bryan McKinnon , Frank Nerling , Matthew Nicol , Gabriel Niculescu , Alexander Ostrovidov , Zisis Papandreou , KiJun Park , Eugene Pasyuk , Peter Pauli , Lubomir Pentchev , William Phelps , John Price , Jorg Reinhold , Dimitri Romanov , Carlos Salgado , Todd Satogata , Susan Schadmand , Amy Schertz , Axel Schmidt , Daniel Sober , Alexander Somov , Sergei Somov , Victor Tarasov , Simon Taylor , Annika Thiel , Guido Maria Urciuoli , Holly Szumila-Vance , Daniel Watts , Lawrence Weinstein , Timothy Whitlatch , Nilanga Wickramaarachchi , Bogdan Wojtsekhowski , Nicholas Zachariou , Jonathan Zarling , Jixie Zhang , Alexey Anisovich , Alexei Bazavov , Rene Bellwied , Veronique Bernard , Gilberto Colangelo , Ales Cieply , Michael Doring , Ali Eskanderian , Jose Goity , Helmut Haberzettl , Mirza Hadzimehmedovic , Robert Jaffe , Boris Kopeliovich , Heinrich Leutwyler , Maxim Mai , Terry Mart , Maxim Matveev , Ulf-G. Meissner , Colin Morningstar , Bachir Moussallam , Kanzo Nakayama , Wolfgang Ochs , Youngseok Oh , Rifat Omerovic , Hedim Osmanovic , Eulogio Oset , Antimo Palano , Jose Pelaez , Alessandro Pilloni , Maxim Polyakov , David Richards , Arkaitz Rodas , Dan-Olof Riska , Jacobo Ruiz de Elvira , Hui-Young Ryu , Elena Santopinto , Andrey Sarantsev , Jugoslav Stahov , Alfred Svarc , Adam Szczepaniak , Ronald Workman , Bing-Song Zou

We evaluate the light, strange and charm scalar content of the nucleon using one lattice QCD ensemble generated with two degenerate light quarks with mass fixed to their physical value. We use improved techniques to evaluate the…

Within QCD, colourless states may be constructed corresponding to exotic matter outside of the traditional quark model. Experiments have recently observed tetraquark and pentaquark states, but no definitive hybrid meson signals have been…

High Energy Physics - Phenomenology · Physics 2022-09-21 Jason Ho , Derek Harnett , Tom Steele

Light-Front Quantization -- Dirac's "Front Form" -- provides a physical, frame-independent formalism for hadron dynamics and structure. Observables such as structure functions, transverse momentum distributions, and distribution amplitudes…

High Energy Physics - Phenomenology · Physics 2015-12-22 Stanley J. Brodsky

The study of $J/\psi$ photoproduction at low energies has consequences for the understanding of multiple aspects of nonperturbative QCD, ranging from mechanical properties of the proton, to the binding inside nuclei, and the existence of…

I discuss a number of novel phenomenological features of QCD in high transverse momentum reactions. The presence of direct higher-twist processes, where a proton is produced directly in the hard subprocess, can explain the "baryon anomaly"…

High Energy Physics - Phenomenology · Physics 2010-12-17 Stanley J. Brodsky

Constituting the largest subset of multiquark states so far observed by experiment, tetraquark mesons carrying overall quark flavour quantum numbers identical to those of the (conventional) quark-antiquark mesons necessitate their…

High Energy Physics - Phenomenology · Physics 2024-09-04 Wolfgang Lucha

Studies of the structure of excited baryons are key to the N* program at Jefferson Lab. Within the first year of data taking with the Hall B CLAS12 detector following the 12 GeV upgrade, a dedicated experiment will aim to extract the N*…

We present a calculation of the strangeness and charmness contents <N|\bar{s}s|N> and <N|\bar{c}c|N> of the nucleon from dynamical lattice QCD with 2+1 flavors. The calculation is performed with overlap valence quarks on 2+1-flavor…

High Energy Physics - Phenomenology · Physics 2013-08-20 M. Gong , A. Alexandru , Y. Chen , T. Doi , S. J. Dong , T. Draper , W. Freeman , M. Glatzmaier , A. Li , K. F. Liu , Z. Liu

Both charged hadrons and D mesons are considered to be excellent probes of QCD matter created in ultra relativistic heavy ion collisions. Surprisingly, recent experimental observations at LHC show the same jet suppression for these two…

Nuclear Theory · Physics 2014-02-05 Magdalena Djordjevic

The QCD light-front (LF) Hamiltonian equation H_{LF}|\Psi> = M^2 |\Psi> derived from quantization at fixed LF time \tau = t+z/c provides a causal, frame-independent, method for computing hadron spectroscopy as well as dynamical observables…

High Energy Physics - Phenomenology · Physics 2020-08-26 Stanley J. Brodsky , Alexandre Deur

Thermal shifts and fluctuations at finite temperature below the deconfinement crossover of QCD from hadronic matter to the Quark-Gluon Plasma provide a viable way to look for exotic and missing states with given quantum numbers in the…

High Energy Physics - Phenomenology · Physics 2025-01-10 Eugenio Megias , Enrique Ruiz Arriola , Lorenzo Luis Salcedo