Relevant bibliographies by topics / Finite temperature QCD

Academic literature on the topic 'Finite temperature QCD'

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Published: 6 September 2023

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Journal articles on the topic "Finite temperature QCD"

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Christ, Norman H. "Finite temperature QCD." Nuclear Physics A 544, no. 1-2 (July 1992): 81–93. http://dx.doi.org/10.1016/0375-9474(92)90566-3.

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PANDEY, H. C., H. C. CHANDOLA, and H. DEHNEN. "COLOR CONFINEMENT AND FINITE TEMPERATURE QCD PHASE TRANSITION." International Journal of Modern Physics A 19, no. 02 (January 20, 2004): 271–85. http://dx.doi.org/10.1142/s0217751x04017471.

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We study an effective theory of QCD in which the fundamental variables are dual magnetic potentials coupled to the monopole field. Dual dynamics are then used to explain the properties of QCD vacuum at zero temperature as well as at finite temperatures. At zero temperature, the color confinement is realized through the dynamical breaking of magnetic symmetry, which leads to the magnetic condensation of QCD vacuum. The flux tube structure of SU(2) QCD vacuum is investigated by solving the field equations in the low energy regimes of the theory, which guarantees dual superconducting nature of the QCD vacuum. The QCD phase transition at finite temperature is studied by the functional diagrammatic evaluation of the effective potential on the one-loop level. We then obtained analytical expressions for the vacuum expectation value of the condensed monopoles as well as the masses of glueballs from the temperature dependent effective potential. These nonperturbative parameters are also evaluated numerically and used to determine the critical temperature of the QCD phase transition. Finally, it is shown that near the critical temperature (Tc≃0.195 GeV ), continuous reduction of vacuum expectation value (VEV) of the condensed monopoles caused the disappearance of vector and scalar glueball masses, which brings a second order phase transition in pure SU(2) gauge QCD.
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Lawlor, Dale, Simon Hands, Seyong Kim, and Jon-Ivar Skullerud. "Thermal Transitions in Dense Two-Colour QCD." EPJ Web of Conferences 274 (2022): 07012. http://dx.doi.org/10.1051/epjconf/202227407012.

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The infamous sign problem makes it impossible to probe dense (baryon density μB > 0) QCD at temperatures near or below the deconfinement threshold. As a workaround, one can explore QCD-like theories such as twocolour QCD (QC2D) which don’t suffer from this sign problem but are qualitively similar to real QCD. Previous studies on smaller lattice volumes have investigated deconfinement and colour superfluid to normal matter transitions. In this study we look at a larger lattice volume Ns = 24 in an attempt to disentangle finite volume and finite temperature effects. We also fit to a larger number of diquark sources to better allow for extrapolation to zero diquark source.
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Laermann, E., and O. Philipsen. "LATTICE QCD AT FINITE TEMPERATURE." Annual Review of Nuclear and Particle Science 53, no. 1 (December 2003): 163–98. http://dx.doi.org/10.1146/annurev.nucl.53.041002.110609.

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Petersson, B., and E. Laermann. "Finite Temperature QCD on Quadrics." Progress of Theoretical Physics Supplement 122 (1996): 85–96. http://dx.doi.org/10.1143/ptps.122.85.

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Ejiri, Shinji. "Lattice QCD at finite temperature." Nuclear Physics B - Proceedings Supplements 94, no. 1-3 (March 2001): 19–26. http://dx.doi.org/10.1016/s0920-5632(01)00922-7.

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Petreczky, P. "Lattice QCD at finite temperature." Nuclear Physics A 785, no. 1-2 (March 2007): 10–17. http://dx.doi.org/10.1016/j.nuclphysa.2006.11.129.

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Reinhardt, Hugo, Davide Campagnari, and Markus Quandt. "Hamiltonian Approach to QCD at Finite Temperature." Universe 5, no. 2 (January 22, 2019): 40. http://dx.doi.org/10.3390/universe5020040.

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A novel approach to the Hamiltonian formulation of quantum field theory at finite temperature is presented. The temperature is introduced by compactification of a spatial dimension. The whole finite-temperature theory is encoded in the ground state on the spatial manifold S 1 ( L ) × R 2 where L is the length of the compactified dimension which defines the inverse temperature. The approach is then applied to the Hamiltonian formulation of QCD in Coulomb gauge to study the chiral phase transition at finite temperatures.
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Ayala, Alejandro, C. A. Dominguez, and M. Loewe. "Finite Temperature QCD Sum Rules: A Review." Advances in High Energy Physics 2017 (2017): 1–24. http://dx.doi.org/10.1155/2017/9291623.

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The method of QCD sum rules at finite temperature is reviewed, with emphasis on recent results. These include predictions for the survival of charmonium and bottonium states, at and beyond the critical temperature for deconfinement, as later confirmed by lattice QCD simulations. Also included are determinations in the light-quark vector and axial-vector channels, allowing analysing the Weinberg sum rules and predicting the dimuon spectrum in heavy-ion collisions in the region of the rho-meson. Also, in this sector, the determination of the temperature behaviour of the up-down quark mass, together with the pion decay constant, will be described. Finally, an extension of the QCD sum rule method to incorporate finite baryon chemical potential is reviewed.
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XIANGJUN, CHEN, and YASUSHI FUJIMOTO. "FINITE TEMPERATURE QCD AT THREE-LOOP." Modern Physics Letters A 11, no. 13 (April 30, 1996): 1033–36. http://dx.doi.org/10.1142/s0217732396001065.

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QCD three-loop vacuum graphs are calculated in Feynman gauge. All the temperature-dependent divergences are extracted by using dimensional regularization. Ultraviolet divergences are shown to cancel with each other and the ir divergences remain uncanceled.
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Dissertations / Theses on the topic "Finite temperature QCD"

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Cossu, Guido. "Deconfinement transition in QCD at finite temperature." Doctoral thesis, Scuola Normale Superiore, 2009. http://hdl.handle.net/11384/85831.

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The main subject of this thesis is the problem of confinement in QCD. Since the discovery of quarks in high energy experiments, their absence as free particles in nature became one of the hot topics in modern physics. The non abelian gauge field theories developed in the 50s by Yang and Mills and successively generalized in the Standard Model have proved successful in describing the real world. Electroweak and short distance interactions are well explained by perturbative expansions in gauge coupling powers. Perturbative calculations, however, cannot account for the confinement problem which is inherently non perturbative in nature. The non perturbative region of strongly coupled theories was out of reach for any analytical calculation since the proposal by Wilson of a regularization on the lattice of gauge field theories. Soon, in early works of lattice field theory it was realized that Yang Mills theories could also account for confinement of quarks by a potential linearly rising with distance. In finite temperature calculations it was also shown that this linear behavior disappears as some temperature Tc , called deconfinement temperature, above which quarks are not bounded inside hadrons. At present time there are no widely accepted explanations from first principles of the dynamics of confinement. Several mechanisms were proposed to describe confinement at low temperatures by means of the topological properties of Yang Mills theories. We shall concentrate on the so called Dual Superconductor Picture which conjectures that confinement is related to condensation of magnetic charges in analogy with common superconductors where condensation of electric charges “confines” magnetic monopoles. We shall propose and test a way to prove its correctness in several gauge theories (see chapter 3). Although no definitive conclusions can be drawn, we shall show, by using an operator that detects the condensation of magnetic charges in the vacuum, that the Dual Superconductor Picture is indeed a proper candidate for the description of the confinement dynamics. The problem was deeply studied in the last years by the Pisa group. The confinement by condensation of monopoles was demonstrated in an U(1) abelian theory both analytically (Frölich and Marchetti) and numerically (Pisa group). During my PhD we discovered that some of our previous data on non abelian gauge theories were misinterpreted. In pure non abelian gauge theories, the presence of unphysical bulk transitions spoils the relation of the operator singularities to a confinement-deconfinement transition. Conversely, similar calculations in theories with fermions in different representations do not show any signal of bulk transitions and results are consistent with the Dual Superconductor Picture. We are dedicating our efforts to clarify this unwelcome behavior of the operator. I will present the first attempts to redefine the operator in pure gauge theories to circumvent these issues. The problem of a suitable definition of the operator on the lattice is still open and a detailed discussion on the subject will be proposed in chapter 3. If the confinement-deconfinement transition is related to the breaking of some symmetry of the theory we then expect that a true phase transition takes place. Strictly speaking, we have explicit symmetries only in the two opposite regions of zero and infinite quark masses (respectively chiral and center symmetries). We aim at establishing if, even at finite quark masses, the path from the low temperature region (confined) to the high temperature region where quarks are free, encounters singularities. A positive answer demonstrates the non trivial fact this two phases have different symmetries, otherwise confinement is ambiguously defined. In this respect, the problem of determining the order of the chiral transition in QCD with two degenerate quarks, a case close to the physical one, becomes a relevant point (chapter 4). In few words, if the transition is second order for massless quarks we then expect that it turns into a crossover for light masses, while if the transition is first order then the non analyticity could survive in a region of small masses (or beyond). The later possibility could explain naturally the experimental evidence of free quark suppression in nature. In chapter 4 we shall address the problem with Finite Size Scaling techniques (chapter 2). By isolating the dependence on one of the two variables (temperature and bare quark mass) we shall analyze the volume scaling of thermodynamical quantities like specific heat and chiral condensate susceptibility. The task of unambiguously determining the order is hard to accomplish but we shall give some evidences that, despite the common lore, the transition could be first order, and that surely is not second order in the class predicted by effective theories. Summarizing the objectives of this thesis is twofold: • address the confinement problem by probing the vacuum with a magnetically charged operator to establish if the dual superconductor picture is a valid picture; • address the confinement problem by studying the related issue of the order of the transition in two flavors quantum chromodynamics.
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Zhang, Yingwen. "Applications of QCD sum rules at finite temperature." Doctoral thesis, University of Cape Town, 2013. http://hdl.handle.net/11427/30179.

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QCD Sum Rules is one of the most successful quantum field theory frameworks to extract hadronic information from QCD analytically. This technique is based on the Operator Product Expansion (OPE) and Cauchy's Theorem in the complex energy plane. OPE factorizes the short and long distance interactions where the former are calculated using perturbative theory, and the latter are parameterized in terms of the quark and gluon vacuum condensates. By using Cauchy's theorem, the results from QCD calculations can be matched to the hadronic channel, this is known as 'quark-hadron duality'. My Project involves using QCD Sum Rules to determine the behaviour of hadronic parameters of charmonium in the scalar and pseudoscalar channel and also light-light quark mesons in the vector and axial-vector channel at finite temperature. From our results of the behaviour of the width and the hadronic coupling at finite temperature, both channels of charmonium shows signs of survival beyond the deconfinement temperature Tc whereas the light-light quark mesons disappears at Tc. An extension of the method to finite density in. the axial-vector channel of light-light quark mesons also shows signs of disappearance at the deconfinement density μc.
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Hatta, Yoshitaka. "The QCD phase transition at finite temperature and density." 京都大学 (Kyoto University), 2004. http://hdl.handle.net/2433/147809.

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Aouane, Rafik. "Gluon and ghost propagator studies in lattice QCD at finite temperature." Doctoral thesis, Humboldt-Universität zu Berlin, Mathematisch-Naturwissenschaftliche Fakultät I, 2013. http://dx.doi.org/10.18452/16735.

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Die im infraroten Impulsbereich der Quantenchromodynamik (QCD) berechneten Gluon- und Ghost-Propagatoren spielen eine große Rolle für das sogenannte Confinement der Quarks und Gluonen. Sie sind Gegenstand intensiver Foschungen dank nicht-perturbativer Methoden basierend auf Dyson-Schwinger- (DS) und funktionalen Renormierungsgruppen-Gleichungen (FRG). Darüber hinaus sollte es deren Verhalten bei endlichen Temperaturen erlauben, den chiralen und Deconfinement-Phasenübergang bzw. das Crossover in der QCD besser aufzuklären. Unser Zugang beruht auf der gitter-diskretisierten QCD (LQCD), die es als ab-initio-Methode gestattet, verschiedenste störungstheoretisch nicht zugängliche QCD-Observablen der hadronischen Welt zu berechnen. Wir untersuchen das Temperaturverhalten der Gluon- und Ghost-Propagatoren in der Landau-Eichung für die reine Gluodynamik und die volle QCD. Für den Gluon-Propagator berechnen wir deren longitudinale (DL) sowie transversale (DT) Komponenten. Ziel ist es, Datensätze in Form von Fit-Formeln zu liefern, welche als Input für die DS- (oder FRG-) Gleichungen verwendet werden können. Wir beschäftigen uns mit der vollen (Nf=2) LQCD unter Verwendung der sogenannten twisted mass Fermiondiskretisierung. Von der tmfT-Kollaboration wurden uns dafür Eichfeldkonfigurationen für Temperaturen im Crossover-Bereich sowie jeweils für drei fixierte Pion-Massenwerte im Intervall [300, 500] MeV bereitgestellt. Schließlich berechnen wir innerhalb der reinen SU(3) Eichtheorie (bei T=0) den Landau Gluon-Propagator unter Verwendung verschiedener Eichfixierungskriterien. Unser Ziel ist es, den Einfluss von Eich-Kopien mit minimalen (nicht-trivialen) Eigenwerten des Faddeev-Popov-Operators zu verstehen. Eine solche Studie soll klären, wie Gribov-Kopien das Verhalten der Gluon- und Ghost-Propagatoren im infraroten Bereich prinzipiell beeinflussen.
Gluon and ghost propagators in quantum chromodynamics (QCD) computed in the infrared momentum region play an important role to understand quark and gluon confinement. They are the subject of intensive research thanks to non-perturbative methods based on Dyson-Schwinger (DS) and functional renormalization group (FRG) equations. Moreover, their temperature behavior might also help to explore the chiral and deconfinement phase transition or crossover within QCD at non-zero temperature. Our prime tool is the lattice discretized QCD (LQCD) providing a unique ab-initio non-perturbative approach to deal with the computation of various observables of the hadronic world. We investigate the temperature dependence of Landau gauge gluon and ghost propagators in pure gluodynamics and in full QCD. Regarding the gluon propagator, we compute its longitudinal DL as well its transversal DT components. The aim is to provide a data set in terms of fitting formulae which can be used as input for DS (or FRG) equations. We deal with full (Nf=2) LQCD with the twisted mass fermion discretization. We employ gauge field configurations provided by the tmfT collaboration for temperatures in the crossover region and for three fixed pion mass values in the range [300,500] MeV. Finally, within SU(3) pure gauge theory (at T=0) we compute the Landau gauge gluon propagator according to different gauge fixing criteria. Our goal is to understand the influence of gauge copies with minimal (non-trivial) eigenvalues of the Faddeev-Popov operator.
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Fetea, Mirela Simona. "Pions and vector mesons at finite temperature from QCD sum rules." Doctoral thesis, University of Cape Town, 1998. http://hdl.handle.net/11427/9694.

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Bibliography: p. 89-92.
The temperature corrections to the current algebra Gell-Mann, Oakes and Renner(GMOR) relation in SU(2) X SU(2), the temperature behaviour of the pion mass and the q2 and T dependence of the ρππ vertex function in the space-like region are investigated.
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Vuorinen, Aleksi. "The pressure of QCD at finite temperature and quark number density." Helsinki : University of Helsinki, 2003. http://ethesis.helsinki.fi/julkaisut/mat/fysik/vk/vuorinen/.

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Burger, Florian. "The finite temperature QCD phase transition and the thermodynamic equation of state." Doctoral thesis, Humboldt-Universität zu Berlin, Mathematisch-Naturwissenschaftliche Fakultät I, 2013. http://dx.doi.org/10.18452/16679.

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In dieser Arbeit wird mit Hilfe der Gitter-Methode der Phasenübergang/Crossover bei nicht verschwindender Temperatur der Quantenchromodynamik mit zwei Quark Flavour untersucht sowie die thermodynamische Zustandsgleichung berechnet. Es wird dabei die Wilson twisted-mass Formulierung der Quark-Wirkung verwendet, welche hinsichtlich des Kontinuum-Limes eine automatische Verbesserung birgt. Erste belastbare Resultate mit dieser Wirkung bei endlicher Temperatur werden in dieser Arbeit gezeigt. Mehrere kleine Werte der Pion-Masse werden betrachtet mit dem Ziel, Aufschluss über die Ordnung des Phasenüberganges im chiralen Limes zu erhalten. Im Bereich der von uns simulierten Pion-Massen zwischen 300 und 700 MeV wird hierbei lediglich ein Crossover-Übergang beobachtet. Die Abhängigkeit der gemessenen Crossover-Temperatur von der Masse wird für eine Extrapolation zu verschwindender Masse hin verwendet unter der Annahme verschiedener Szenarien für den chiralen Limes. Dazu komplementär wird das chirale Kondensat, der Ordnungsparameter der spontanen Brechung der chiralen Symmetrie, vor dem Hintergrund der so genannten magnetischen Zustandsgleichung untersucht, welche das universelle Verhalten in der Nähe des Phasenüberganges für die Universalitätsklasse des O(4) Modells angibt. Hinsichtlich der Thermodynamik wird ausgehend von der Spur-Anomalie und unter Benutzung der Temperatur-Integral Methode der Druck und die Energiedichte im Crossover-Gebiet berechnet. Der Kontinuum-Limes der Spur-Anomalie wird mit mehreren Gitterdiskretisierungen der Temperatur Nt sowie unter Zuhilfenahme einer tree-level Korrektur untersucht.
In this thesis we report about an investigation of the finite temperature crossover/phase transition of quantum chromodynamics and the evaluation of the thermodynamic equation of state. To this end the lattice method and the Wilson twisted mass discretisation of the quark action are used. This formulation is known to have an automatic improvement of lattice artifacts and thus an improved continuum limit behaviour. This work presents first robust results using this action for the non-vanishing temperature case. We investigate the chiral limit of the two flavour phase transition with several small values of the pion mass in order to address the open question of the order of the transition in the limit of vanishing quark mass. For the currently simulated pion masses in the range of 300 to 700 MeV we present evidence that the finite temperature transition is a crossover transition rather than a genuine phase transition. The chiral limit is investigated by comparing the scaling of the observed crossover temperature with the mass including several possible scenarios. Complementary to this approach the chiral condensate as the order parameter for the spontaneous breaking of chiral symmetry is analysed in comparison with the O(4) universal scaling function which characterises a second order transition. With respect to thermodynamics the equation of state is obtained from the trace anomaly employing the temperature integral method which provides the pressure and energy density in the crossover region. The continuum limit of the trace anomaly is studied by considering several values of Nt and the tree-level correction technique.
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Robaina, Fernandez Daniel [Verfasser]. "Static and dynamic properties of QCD at finite temperature / Daniel Robaina Fernandez." Mainz : Universitätsbibliothek Mainz, 2016. http://d-nb.info/1106573382/34.

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Oevers, Manfred [Verfasser]. "The finite temperature phase diagram of 2-flavour QCD with improved Wilson fermions / Manfred Oevers." Bielefeld : Universitätsbibliothek Bielefeld, 1999. http://d-nb.info/1034401254/34.

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Heide, Johannes van der. "The pion form factor from lattice QCD a non-perturbative study at zero and finite temperature /." [S.l. : Amsterdam : s.n.] ; Universiteit van Amsterdam [Host], 2004. http://dare.uva.nl/document/76697.

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Books on the topic "Finite temperature QCD"

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A, Patkós, United States. National Aeronautics and Space Administration., and Fermi National Accelerator Laboratory, eds. Chiral interface at the finite temperature transition point of QCD. [Batavia, Ill.]: Fermi National Accelerator Laboratory, 1990.

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Zinn-Justin, Jean. Quantum Field Theory and Critical Phenomena. 5th ed. Oxford University Press, 2021. http://dx.doi.org/10.1093/oso/9780198834625.001.0001.

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Introduced as a quantum extension of Maxwell's classical theory, quantum electrodynamic (QED) has been the first example of a quantum field theory (QFT). Eventually, QFT has become the framework for the discussion of all fundamental interactions at the microscopic scale except, possibly, gravity. More surprisingly, it has also provided a framework for the understanding of second order phase transitions in statistical mechanics. In fact, as hopefully this work illustrates, QFT is the natural framework for the discussion of most systems involving an infinite number of degrees of freedom with local couplings. These systems range from cold Bose gases at the condensation temperature (about ten nanokelvin) to conventional phase transitions (from a few degrees to several hundred) and high energy particle physics up to a TeV, altogether more than twenty orders of magnitude in the energy scale. Therefore, although excellent textbooks about QFT had already been published, I thought, many years ago, that it might not be completely worthless to present a work in which the strong formal relations between particle physics and the theory of critical phenomena are systematically emphasized. This option explains some of the choices made in the presentation. A formulation in terms of field integrals has been adopted to study the properties of QFT. The language of partition and correlation functions has been used throughout, even in applications of QFT to particle physics. Renormalization and renormalization group (RG) properties are systematically discussed. The notion of effective field theory (EFT) and the emergence of renormalizable theories are described. The consequences for fine-tuning and triviality issue are emphasized. This fifth edition has been updated and fully revised.
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Book chapters on the topic "Finite temperature QCD"

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Karsch, Frithjof. "Lattice QCD at Finite Temperature." In QCD Perspectives on Hot and Dense Matter, 385–417. Dordrecht: Springer Netherlands, 2002. http://dx.doi.org/10.1007/978-94-010-0267-7_12.

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Karsch, Frithjof. "Critical Behaviour in Finite Temperature QCD." In Nuclear Matter in Different Phases and Transitions, 131–46. Dordrecht: Springer Netherlands, 1999. http://dx.doi.org/10.1007/978-94-011-4556-5_11.

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Dominguez, Cesareo A. "QCD Sum Rules at Finite Temperature." In SpringerBriefs in Physics, 81–85. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-97722-5_12.

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Leonidov, A. "On Power Corrections in Finite Temperature QCD." In Vacuum Structure in Intense Fields, 373–76. Boston, MA: Springer US, 1991. http://dx.doi.org/10.1007/978-1-4757-0441-9_25.

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Blaizot, J. P. "Quantum Fields at Finite Temperature: A Brief Introduction." In QCD Perspectives on Hot and Dense Matter, 305–26. Dordrecht: Springer Netherlands, 2002. http://dx.doi.org/10.1007/978-94-010-0267-7_9.

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DeGrand, Thomas. "Lattice Monte carlo calculations of finite temperature QCD." In Quark Matter '84, 17–38. Berlin, Heidelberg: Springer Berlin Heidelberg, 1985. http://dx.doi.org/10.1007/3-540-15183-4_23.

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Karsch, F. "Lattice QCD at finite temperature: a status report." In Quark Matter, 147–55. Berlin, Heidelberg: Springer Berlin Heidelberg, 1988. http://dx.doi.org/10.1007/978-3-642-83524-7_21.

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Karsch, Frithjof. "QCD at Finite Temperature and Baryon Number Density." In NATO ASI Series, 1–14. Boston, MA: Springer US, 1986. http://dx.doi.org/10.1007/978-1-4613-2231-3_1.

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Chandola, H. C., and H. C. Pandey. "Infrared Effective Dual QCD at Finite Temperature and Densities." In Springer Proceedings in Physics, 569–78. Singapore: Springer Singapore, 2021. http://dx.doi.org/10.1007/978-981-33-4408-2_79.

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Gubler, Philipp. "Quarkonium Spectra at Finite Temperature from QCD Sum Rules and MEM." In A Bayesian Analysis of QCD Sum Rules, 123–47. Tokyo: Springer Japan, 2013. http://dx.doi.org/10.1007/978-4-431-54318-3_7.

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Conference papers on the topic "Finite temperature QCD"

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Laine, Mikko. "Finite-temperature QCD." In The XXVII International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2010. http://dx.doi.org/10.22323/1.091.0006.

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Karsch, Frithjof. "Lattice QCD at Finite Temperature." In NEW STATES OF MATTER IN HADRONIC INTERACTIONS:Pan American Advanced Study Institute. AIP, 2002. http://dx.doi.org/10.1063/1.1513678.

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Fodor, Zoltan. "The finite temperature QCD transition." In The XXVIII International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2011. http://dx.doi.org/10.22323/1.105.0185.

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Zeidlewicz, Lars, Ernst-Michael Ilgenfritz, Karl Jansen, Maria-Paola Lombardo, Michael Muller-Preussker, Marcus Petschlies, Owe Philipsen, and Andre Sternbeck. "Twisted mass QCD at finite temperature." In The XXV International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2008. http://dx.doi.org/10.22323/1.042.0238.

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Ejiri, Shinji. "Monopole Dynamics in Finite Temperature QCD." In Proceedings of the International RCNP Workshop. WORLD SCIENTIFIC, 1996. http://dx.doi.org/10.1142/9789814447140_0036.

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Larsen, Rasmus, Sayantan Sharma, and Edward Shuryak. "Topological structures in finite temperature QCD." In The 36th Annual International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2019. http://dx.doi.org/10.22323/1.334.0156.

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Giannuzzi, Floriana, Leonardo Angelini, Pietro Colangelo, Fulvia De Fazio, G. E. Bruno, Donato Creanza, and E. Nappi. "Finite temperature hadrons from holographic QCD." In QCD@WORK 2010: International Workshop on Quantum Chromodynamics: Theory and Experiment Beppe Nardulli Memorial Workshop. AIP, 2010. http://dx.doi.org/10.1063/1.3536582.

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TYTGAT, MICHEL H. G. "SOME ASPECTS OF LARGE NC AT FINITE TEMPERATURE." In Phenomenology of Large NC QCD. WORLD SCIENTIFIC, 2002. http://dx.doi.org/10.1142/9789812776914_0003.

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Pasztor, Attila, R. Bellotti, Sz Borsanyi, Z. Fodor, J. Gunther, C. Ratti, S. Katz, and K. K. Szabo. "Fluctuations and correlations in finite temperature QCD." In 38th International Conference on High Energy Physics. Trieste, Italy: Sissa Medialab, 2017. http://dx.doi.org/10.22323/1.282.0369.

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Stephens, C. R. "Environmentally friendly renormalization in finite temperature QCD." In First Latin American symposium on high energy physics and The VII Mexican School of Particles and Fields. AIP, 1997. http://dx.doi.org/10.1063/1.53238.

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Reports on the topic "Finite temperature QCD"

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BLUM, T., M. CREUTZ, and P. PETRECZKY. LATTICE QCD AT FINITE TEMPERATURE AND DENSITY. Office of Scientific and Technical Information (OSTI), February 2004. http://dx.doi.org/10.2172/15006985.

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2

Hidaka, Yoshimasa, and Peter Petreczky. Proceedings of RIKEN BNL Research Center Workshop: QCD in Finite Temperature and Heavy-Io Collisions. Office of Scientific and Technical Information (OSTI), March 2017. http://dx.doi.org/10.2172/1425142.

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