Veen, H. Akindinov, S. Kiselev, D. Mikhaylov, A. Nedosekin, R. Sultanov, K. Colella, J. Jadlovsky, P. Kalinak, I. Krivda, J. Musinsky, L. Baral, T.
Mishra, S. Sahoo, P. Danu, A. Dobrin, M. Gheata, M. Haiduc, C. Mitu, M. Niculescu, C. Ristea, A. Sevcenco, I. Cuautle, I. Maldonado Cervantes, L. Nellen, A. Alfaro Molina, E. Belmont-Moreno, D. Grabski, H. Menchaca-Rocha, A. Buthelezi, S. Foertsch, M. Marchisone, S. Murray, K. Batyunya, S. Grigoryan, L. Malinina, K. Mikhaylov, P. Nomokonov, E. Rogochaya, A. Karasu Uysal, A. Barret, N. Bastid, A. Batista Camejo, P. Crochet, P. Dupieux, V. Feuillard, S. Li, X. Lopez, F. Manso, S. Porteboeuf-Houssais, P. Rosnet, L. Conesa Balbastre, J. Faivre, C. Furget, R. Guernane, C. Bianchi, L.
Case Study: Quarks and other Sub-Nucleon Particles
Calero Diaz, P. Di Nezza, A. Fantoni, P. Gianotti, V. Muccifora, A. Reolon, F. Ronchetti, S. Bock, A. Collu, M. Fasel, D. Gangadharan, B. Jacak, P. Jacobs, C. Loizides, L. Milano, M. Porter, J. Belyaev, A. Bogdanov, V. Grigoriev, M. Ippolitov, V. Kaplin, N. Kondratyeva, V. Loginov, Y. Melikyan, D. Deloff, O. Kovalenko, P. Kurashvili, R. Nair, K. Redlich, T.
Andrei, I. Berceanu, A. Bercuci, A. Herghelegiu, M. Petrovici, A. Pop, C. Biswas, A. Dash, B. Mohanty, K. Aleksandrov, D. Blau, S. Fokin, M. Manko, S. Nikolaev, S. Nikulin, A. Nyanin, D. Peresunko, E. Ryabinkin, Y.
Sibiriak, A. Bearden, A. Bilandzic, H. Bourjau, M. Chojnacki, C. Christensen, J. Gajdosova, K. Gulbrandsen, B. Nielsen, L. Pimentel, V. Christakoglou, C. Deplano, A. Dobrin, P. Kuijer, F. Ferencei, F. Krizek, V. Pospisil, M. Cormier, M. Poghosyan, K. Berdnikov, V. Khanzadeev, E. Kryshen, M.
Malaev, V. Nikulin, V. Riabov, Y. Ryabov, V. Aggarwal, A. Bhati, L. Ganoti, F. Roukoutakis, M. Cleymans, T. Dietel, S. Bala, A. Bhasin, I. Bhat, A. Gupta, R. Gupta, M. Kour, A. Mahajan, S. Rajput, S. Sambyal, A. Gasik, R. Anguelov, H. Beck, F. Bock, M. Danisch, A. Deisting, P. Karayan, J. Kim, S. Klewin, M. Knichel, L. Leardini, J. Oeschler, K. Oyama, Y. Pachmayer, F. Reidt, K. Reygers, R. Schicker, S. Schuchmann, J. Stachel, J. Stiller, M. Weiser, J. Wilkinson, B. Windelband, M. Borissov, K. Choi, S. Chung, J. Eum, J. Andronic, R. Averbeck, P. Braun-Munzinger, A.
Foka, U. Frankenfeld, C. Garabatos, J. Gronefeld, R. Grosso, M. Ivanov, R. Jimenez Bustamante, L.
Quarks | IOPSpark
Karayan, T. Kollegger, C. Lippmann, P. Malzacher, A. Martin, S. Masciocchi, D. Nicassio, J. Onderwaater, W. Park, C. Schmidt, K. Schwarz, K. Schweda, I. Selyuzhenkov, F.
Sozzi, D. Vranic, J. Budnikov, S. Filchagin, R. Ilkaev, A. Kuryakin, A. Mamonov, S. Nazarenko, V. Punin, A. Chattopadhyay, D. Das, I. Das, P. Khan, P. Alexandre, H. Andrews, L. Barnby, D. Evans, K. Graham, P. Jones, A. Jusko, M. Krivda, R. Lietava, O. Calvo Villar, E. Elia, V. Lenti, V. Manzari, E. Alici, P. Antonioli, F.
Cindolo, D. Hatzifotiadou, A. Margotti, R. Nania, F. Noferini, O. Preghenella, E. Scapparone, M. Cicalo, A. Antinori, A. Dainese, B. Di Ruzza, D. Fragiacomo, N. Grion, S. Agnello, B. Alessandro, R. Arnaldi, S. Bagnasco, C. Bedda, E. Bruna, P. Cerello, Y. Corrales Morales, N. De Marco, A. Feliciello, P. Giubellino, S. La Pointe, C. Oppedisano, B. Paul, F. Evdokimov, V. Izucheev, Y. Kharlov, E. Kondratyuk, V. Petrov, B. Polichtchouk, S.
Gruber, S. Lehner, J. Aphecetche, B. Audurier, G. Batigne, B.
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Jadlovsky, M. Gotovac, E. Bartke, J. Bhom, J. Figiel, E. Gladysz-Dziadus, L. Kowalski, A. Matyja, C. Mayer, J. Otwinowski, A. Blair, E. Gauger, A. Knospe, C. Beltran, C. Galvan, I. Bregant, M. Cosentino, S. De, C. Domenicis Gimenez, M. Figueredo, C. Jahnke, C. Lagana Fernandes, A. Mas, M. Munhoz, H. Natal da Luz, A.
Oliveira Da Silva, A. Albuquerque, D. Chinellato, R. Bellwied, L.
Bianchi, P. Jayarathna, S. Jena, A. Knospe, D. Mcdonald, F. Ng, L. Pinsky, D. Chang, D. Kim, J. Rak, M. Slupecki, T. Snellman, W. Trzaska, M. Borri, M. Chartier, M. Castro, C. Hughes, J. Mazer, C. Nattrass, K. Read, R. Scott, N. Gunji, H. Hamagaki, S. Hayashi, H. Murakami, Y. Sekiguchi, K. Terasaki, T. Busch, T. Chujo, S. Esumi, R. Hosokawa, M. Inaba, Y. The broad categories into which the material has been placed, reflect the diverse studies of quark-gluon plasma and its manifestation.
They are: phase-space models of particle production, perturbative QCD plasma, lattice gauge theory, fluid dynamics and flow, strangeness, heavy flavor charm , electromagnetic signals, parton cascade and minijets, parton energy loss and jet quenching, Hanbury Brown--Twiss HBT interferometry, disoriented chiral condensates, phase transition dynamics and cosmology, and color superconductivity. Each chapter is prefaced by an introduction, which contains a list of significant papers which is more complete than the reprinted papers, though by no means exhaustive.
It also contains citations to most relevant papers published up to the date of completion of this volume fall It is hoped that the short reviews will help bring the reader up to date on the latest developments. The selection of papers cited in each chapter, and in particular the ones selected for reprinting, is solely the responsibility of the Editors. It is based on their best judgement and experience in this field dating back to the mids. In order to be reprinted a paper must have been pioneering in the sense of originality and impact on the field.
Generally they have been cited over a hundred times by other papers published in refereed journals. The final selection was reviewed and discussed among the Editors repeatedly. Just because a paper is not included does not mean they do not know of it or do not have a high regard for it. All of the papers cited or reprinted are original research contributions. There are three other types of publications listed. The first is a compilation of books. The second is a list of reviews, many of which contain a significant amount of original material.
The third is a list of the proceedings of the series of Quark Matter meetings, the primary series of international conferences in this field that is attended by both theorists and experimentalists. We are always looking for ways to improve customer experience on Elsevier. We would like to ask you for a moment of your time to fill in a short questionnaire, at the end of your visit. If you decide to participate, a new browser tab will open so you can complete the survey after you have completed your visit to this website. Thanks in advance for your time. Skip to content.
Search for books, journals or webpages All Pages Books Journals. Authors: J. Kapusta B. Hardcover ISBN: Imprint: Elsevier Science. Published Date: 25th November Page Count: For regional delivery times, please check When will I receive my book? Sorry, this product is currently out of stock. Institutional Subscription. Free Shipping Free global shipping No minimum order. Fermi, Prog. Hagedorn, Suppl. Nuovo Cimento On the hadronic mass spectrum, R.
Hagedorn, Nuovo Cimento Strange anti-baryons from quark-gluon plasma, J. Rafelski, Phys. Collins and M. Perry, Phys. The ground-state energy of a relativistic quark gas, B. Freedman and L. McLerran, Phys. Shuryak, Zh. Kapusta, Nucl. B Infrared problem in the thermodynamics of the Yang-Mills gas, A. Linde, Phys. B Covariant calculations at finite temperature: the relativistic plasma, H. Weldon, Phys. D Spectrum of elementary Fermi excitations in quark-gluon plasma, V.
Klimov, Yad. Braaten and R. Pisarski, Nucl. Susskind, Phys. McLerran and B. Svetitsky, Phys. Kuti, J. Engels and H. Satz, Phys. Brown, F. Butler, H. Chen, N. Christ, Z. Dong, W. Schaffer, L. This is called the antiparticle. For example, the antiparticle of an electron is a particle of positive electric charge called the positron. Bosons also have antiparticles, except for those that have zero value for all charges, for example, a photon or a composite boson made from a quark and its corresponding antiquark. In this case there is no distinction between the particle and the antiparticle, they are the same object.
An antiquark is denoted by putting a bar over the corresponding quark , , , etc. It will explore the fundamental nature of matter and the basic forces that shape our Universe. The proton uud and the neutron udd are both baryons. They may also contain additional quark-antiquark pairs.
All particles are either fermions or bosons. The particles associated with all the fundamental interactions forces are bosons. Composite particles with even numbers of fermion constituents quarks are also bosons. It sits astride the French-Swiss border near Geneva. CERN is a laboratory where scientists unite to study the building blocks of matter and the forces that hold them together. CERN exists primarily to provide them with the necessary tools. These are accelerators, which accelerate particles to almost the speed of light and detectors to make the particles visible.
Founded in , the laboratory was one of Europe's first joint ventures and includes now 20 Member States. Determines whether the particle can participate in an interaction process. A particle with electric charge has electrical interactions; one with strong charge has strong interactions, etc.
For composites made of color charged particles the rules of neutralization are complex. Three quarks baryon or a quark plus an antiquark meson can both form color-neutral combinations. The sum of the masses of the produced particles is always less than the mass of the original particle. Also a collection of such devices designed so that each serves a particular purpose in allowing physicists to reconstruct particle events. It is the most common lepton, with electric charge Particle theories predict the probabilities of various possible events occurring when many similar collisions or decays are studied.
They cannot predict the outcome for any single event. Named for particle physics pioneer Enrico Fermi. As a consequence of this peculiar angular momentum, fermions obey a rule called the Pauli Exclusion Principle, which states that no two fermions can exist in the same state at the same place and time.
Related Quark Model and High Energy Collisions, Second Edition
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