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Journal articles on the topic 'QCD topology'

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Author: Grafiati
Published: 10 December 2022
Last updated: 28 January 2023

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1

Teper, M. "Topology in QCD." Nuclear Physics B - Proceedings Supplements 83-84, no. 1-3 (March 2000): 146–50. http://dx.doi.org/10.1016/s0920-5632(00)00212-7.

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2

Teper, M. "Topology in QCD." Nuclear Physics B - Proceedings Supplements 83-84 (April 2000): 146–50. http://dx.doi.org/10.1016/s0920-5632(00)91608-6.

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3

Shuryak, Edward. "QCD with many fermions and QCD topology." Journal of Physics: Conference Series 432 (April 30, 2013): 012022. http://dx.doi.org/10.1088/1742-6596/432/1/012022.

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4

Lombardo, Maria Paola, and Anton Trunin. "Topology and axions in QCD." International Journal of Modern Physics A 35, no. 20 (July 15, 2020): 2030010. http://dx.doi.org/10.1142/s0217751x20300100.

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QCD axions are at the crossroads of QCD topology and Dark Matter searches. We present here the current status of topological studies on the lattice, and their implication on axion physics. We outline the specific challenges posed by lattice topology, the different proposals for handling them, the observable effects of topology on the QCD spectrum and its interrelation with chiral and axial symmetries. We review the transition to the quark–gluon plasma, the fate of topology at the transition, and the approach to the high temperature limit. We discuss the extrapolations needed to reach the regime of cosmological relevance, and the resulting constraints on the QCD axion.
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5

Zou, L. P., P. M. Zhang, and D. G. Pak. "Knot topology in QCD." Physics Letters B 726, no. 1-3 (October 2013): 436–43. http://dx.doi.org/10.1016/j.physletb.2013.08.037.

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6

de Forcrand, Philippe, Margarita García Pérez, James E. Hetrick, and Ion-Olimpu Stamatescu. "Topology of full QCD." Nuclear Physics B - Proceedings Supplements 63, no. 1-3 (April 1998): 549–51. http://dx.doi.org/10.1016/s0920-5632(97)00830-x.

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7

Brower, R., S. Chandrasekharan, J. W. Negele, and U. J. Wiese. "QCD at fixed topology." Physics Letters B 560, no. 1-2 (May 2003): 64–74. http://dx.doi.org/10.1016/s0370-2693(03)00369-1.

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8

Zubkov, M. A. "Momentum space topology of QCD." Annals of Physics 393 (June 2018): 264–87. http://dx.doi.org/10.1016/j.aop.2018.04.016.

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9

Kharzeev, Dmitri E. "Color confinement from fluctuating topology." International Journal of Modern Physics A 31, no. 28n29 (October 19, 2016): 1645023. http://dx.doi.org/10.1142/s0217751x16450238.

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QCD possesses a compact gauge group, and this implies a non-trivial topological structure of the vacuum. In this contribution to the Gribov-85 Memorial volume, we first discuss the origin of Gribov copies and their interpretation in terms of fluctuating topology in the QCD vacuum. We then describe the recent work with E. Levin that links the confinement of gluons and color screening to the fluctuating topology, and discuss implications for spin physics, high energy scattering, and the physics of quark-gluon plasma.
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10

Gogohia, V., and H. Toki. "Topology of the chiral QCD vacuum." Physics Letters B 466, no. 2-4 (November 1999): 305–12. http://dx.doi.org/10.1016/s0370-2693(99)01106-5.

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11

Cho, Y. M. "Knot topology of classical QCD vacuum." Physics Letters B 644, no. 2-3 (January 2007): 208–11. http://dx.doi.org/10.1016/j.physletb.2006.11.040.

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12

Boyd, G., B. Allés, M. D'Elia, A. Di Giacomo, and E. Vicari. "Decorrelating the topology in full QCD." Nuclear Physics B - Proceedings Supplements 53, no. 1-3 (February 1997): 544–46. http://dx.doi.org/10.1016/s0920-5632(96)00713-x.

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13

Chandola, H. C., H. C. Pandey, and H. Nandan. "Topology of QCD vacuum and color confinement." Canadian Journal of Physics 80, no. 7 (July 1, 2002): 745–54. http://dx.doi.org/10.1139/p02-023.

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Using the magnetic symmetry structure of non-Abelian gauge theories of the Yang–Mills type, the mathematical foundation of dual chromodynamics in fiber-bundle form is discussed. The dual gauge potential in its restricted form is constructed in terms of magnetic vectors on global sections, which has been shown to lead the dual dynamics between topological charges and color isocharges. Constructing the Lagrangian for such dual theory, the dynamical breaking of magnetic symmetry by an effective potential is shown to push the QCD vacuum in a confining phase. The dynamical structure of the theory is investigated by deriving the field equations associated with the confining phase. The associated flux-tube structure responsible for the confinement is analyzed by computing the asymptotic string solutions of the field equations under cylindrical symmetry. Using the confining part of the dual restricted Lagrangian, the finite string energy per unit length is calculated and its implications on color confinement are discussed. PACS Nos.: 11.38Aw, 14.80Hv, 11.30Jw
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14

D'Elia, Massimo. "Topology and θ dependence in lattice QCD." Nuclear Physics B - Proceedings Supplements 133 (July 2004): 285–90. http://dx.doi.org/10.1016/j.nuclphysbps.2004.04.180.

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15

KHOZE, V. A., A. I. LEBEDEV, and J. A. VAZDIK. "QCD COHERENCE IN DIRECT COMPTON SCATTERING." Modern Physics Letters A 09, no. 18 (June 14, 1994): 1665–71. http://dx.doi.org/10.1142/s0217732394001507.

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The color coherence effects are studied for direct processes of γp interactions at high energies using PYTHIA Monte-Carlo simulation and perturbative QCD approach. Sub-processes of QED and QCD Compton scattering on quarks leading to jet topology of photoproduction events are considered. It is shown that the coherence leads to drag phenomenon in the interjet region.
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16

Roy, Pinaki, and Rajkumar Roychoudhury. "Notizen: On Chiral Symmetry Breaking in a Non-Simply Connected Space-Time." Zeitschrift für Naturforschung A 40, no. 9 (September 1, 1985): 957–58. http://dx.doi.org/10.1515/zna-1985-0918.

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17

Bietenholz, Wolfgang, Karl Jansen, Kei-Ichi Nagai, Silvia Necco, Luigi Scorzato, and Stanislav Shcheredin. "Exploring topology conserving gauge actions for lattice QCD." Journal of High Energy Physics 2006, no. 03 (March 2, 2006): 017. http://dx.doi.org/10.1088/1126-6708/2006/03/017.

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18

Edwards, Robert G., Urs M. Heller, and Rajamani Narayanan. "Spectral flow, condensate and topology in lattice QCD." Nuclear Physics B 535, no. 1-2 (December 1998): 403–22. http://dx.doi.org/10.1016/s0550-3213(98)00588-4.

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19

Edwards, R. "Topology and chiral symmetry in finite temperature QCD." Nuclear Physics B - Proceedings Supplements 83-84, no. 1-3 (March 2000): 479–81. http://dx.doi.org/10.1016/s0920-5632(00)00265-6.

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20

Edwards, Robert G., Urs M. Heller, Joe Kiskis, and Rajamani Narayanan. "Topology and chiral symmetry in finite temperature QCD." Nuclear Physics B - Proceedings Supplements 83-84 (April 2000): 479–81. http://dx.doi.org/10.1016/s0920-5632(00)91711-0.

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21

Hart, A. "Glueballs and topology with (a)-improved lattice QCD." Nuclear Physics B - Proceedings Supplements 106-107 (March 2002): 575–77. http://dx.doi.org/10.1016/s0920-5632(01)01782-0.

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22

Brower, R., S. Chandrasekharan, J. W. Negele, and U. J. Wiese. "Physical observables from lattice QCD at fixed topology." Nuclear Physics B - Proceedings Supplements 106-107 (March 2002): 581–83. http://dx.doi.org/10.1016/s0920-5632(01)01784-4.

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23

Gogohia, V., and H. Toki. "Erratum to: “Topology of the chiral QCD vacuum”." Physics Letters B 499, no. 3-4 (February 2001): 328–29. http://dx.doi.org/10.1016/s0370-2693(01)00047-8.

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24

WARNER, ROLAND C., and G. C. JOSHI. "INTERACTION BETWEEN COLOUR-SINGLET HADRONS FROM NONPERTURBATIVE QCD." International Journal of Modern Physics A 05, no. 19 (October 10, 1990): 3787–99. http://dx.doi.org/10.1142/s0217751x90001616.

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We present a nonperturbative QCD contribution to interactions between separated coloursinglet hadrons, arising from the nontrivial topology of the QCD vacuum. We have calculated the effect of the structure of the vacuum (modelled here as a dilute gas of instantons) on hadron propagation, as a way of studying at least some nonperturbative effects. We find that a nonperturbative interaction arises which is familiar to us from our earlier studies of many-body potentials in multiquark systems. This interaction is distinct from those earlier perturbative QCD calculations which bear a direct analogy to the van der Waals interaction of atomic physics.
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25

Dromard, A., W. Bietenholz, K. Cichy, and M. Wagner. "Computing the Topological Susceptibility from Fixed Topology QCD Simulations." Acta Physica Polonica B Proceedings Supplement 9, no. 3 (2016): 635. http://dx.doi.org/10.5506/aphyspolbsupp.9.635.

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26

Shcheredin, S., W. Bietenholz, K. Jansen, K. I. Nagai, S. Necco, and L. Scorzato. "Testing a Topology Conserving Gauge Action in Lattice QCD." Nuclear Physics B - Proceedings Supplements 140 (March 2005): 779–81. http://dx.doi.org/10.1016/j.nuclphysbps.2004.11.122.

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27

Chen, P., N. Christ, G. Fleming, A. Kaehler, C. Malureanu, R. Mawhinney, G. Siegert, C. Sui, P. Vranas, and Y. Zhestkov. "The anomaly and topology in quenched QCD above Tc." Nuclear Physics B - Proceedings Supplements 73, no. 1-3 (March 1999): 405–7. http://dx.doi.org/10.1016/s0920-5632(99)85087-7.

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28

Allés, B. "Topology in QCD with 4 flavours of dynamical fermions." Nuclear Physics B - Proceedings Supplements 83-84, no. 1-3 (March 2000): 431–33. http://dx.doi.org/10.1016/s0920-5632(00)00347-9.

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29

Allés, B., M. D'Elia, and A. Di Giacomo. "Topology in QCD with 4 flavours of dynamical fermions." Nuclear Physics B - Proceedings Supplements 83-84 (April 2000): 431–33. http://dx.doi.org/10.1016/s0920-5632(00)91696-7.

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30

Azcoiti, Vicente. "Topology in the SU(Nf) chiral symmetry restored phase of unquenched QCD and axion cosmology." EPJ Web of Conferences 175 (2018): 04007. http://dx.doi.org/10.1051/epjconf/201817504007.

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The axion is one of the more interesting candidates to make the dark matter of the universe, and the axion potential plays a fundamental role in the determination of the dynamics of the axion field. Moreover, the way in which the U(1)A anomaly manifests itself in the chiral symmetry restored phase of QCD at high temperature could be tested when probing the QCD phase transition in relativistic heavy ion collisions. With these motivations, we investigate the physical consequences of the survival of the effects of the U(1)A anomaly in the chiral symmetric phase of QCD, and show that the free energy density is a singular function of the quark mass m, in the chiral limit, and that the σ and π susceptibilities diverge in this limit at any T ≥ Tc. We also show that the difference between the π and δ susceptibilities diverges in the chiral limit at any T ≥ Tc, a result that can be contrasted with the existing lattice calculations; and discuss on the generalization of these results to the Nf ≥ 3 model.
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31

Khan, Shahid, Viktor Klochkov, Olha Lavoryk, Oleksii Lubynets, Ali Imdad Khan, Andrea Dubla, and Ilya Selyuzhenkov. "Machine Learning Application for Λ Hyperon Reconstruction in CBM at FAIR." EPJ Web of Conferences 259 (2022): 13008. http://dx.doi.org/10.1051/epjconf/202225913008.

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The Compressed Baryonic Matter experiment at FAIR will investigate the QCD phase diagram in the region of high net-baryon densities. Enhanced production of strange baryons, such as the most abundantly produced Λ hyperons, can signal transition to a new phase of the QCD matter. In this work, the CBM performance for reconstruction of the Λ hyperon via its decay to proton and π− is presented. Decay topology reconstruction is implemented in the Particle-Finder Simple (PFSimple) package with Machine Learning algorithms providing effcient selection of the decays and high signal to background ratio.
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32

Kovács, Tamás G., E. T. Tomboulis, and Zsolt Schram. "Topology on the lattice; 2d QCD with a theta term." Nuclear Physics B 454, no. 1-2 (November 1995): 45–58. http://dx.doi.org/10.1016/0550-3213(95)00440-4.

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33

Grandy, J., and G. Kilcup. "Effect of improving the lattice gauge action on QCD topology." Nuclear Physics B - Proceedings Supplements 53, no. 1-3 (February 1997): 560–63. http://dx.doi.org/10.1016/s0920-5632(96)00718-9.

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34

Bitar, Khalil M., R. Edwards, U. M. Heller, A. D. Kennedy, Thomas A. DeGrand, Steven Gottlieb, A. Krasnitz, et al. "Glueballs and topology in lattice QCD with two light flavors." Physical Review D 44, no. 7 (October 1, 1991): 2090–109. http://dx.doi.org/10.1103/physrevd.44.2090.

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35

Kuramashi, Y., M. Fukugita, H. Mino, M. Okawa, and A. Ukawa. "Dynamical quark effects on glueballs and topology in lattice QCD." Nuclear Physics B - Proceedings Supplements 26 (January 1992): 275–77. http://dx.doi.org/10.1016/0920-5632(92)90251-m.

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36

FIELD, J. H. "TESTS OF PERTURBATIVE QCD USING R, $\Gamma _h^Z $ AND EVENT TOPOLOGY MEASUREMENTS IN HADRONIC Z-DECAYS." Modern Physics Letters A 07, no. 02 (January 20, 1992): 161–74. http://dx.doi.org/10.1142/s0217732392000094.

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The world data on R and [Formula: see text] is used to derive a value of the QCD scale parameter, free of hadronization and renormalization scale uncertainties, of [Formula: see text]. This value is then used to investigate the convergence of the QCD perturbation expansions for several different jet topology measures, with the choice [Formula: see text] of the renormalization scale. In most cases satisfactory convergence is observed. The overall consistency of all measurements of [Formula: see text] is also discussed. Although [Formula: see text] seems high, present data is consistent (17% C.L.) with a global world average value of [Formula: see text], [Formula: see text].
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37

Lucha, Wolfgang, Dmitri Melikhov, and Hagop Sazdjian. "Zooming in on Multiquark Hadrons within QCD Sum-Rule Approaches." EPJ Web of Conferences 274 (2022): 03004. http://dx.doi.org/10.1051/epjconf/202227403004.

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Aiming at self-consistent descriptions of multiquark hadrons (such as tetraquarks, pentaquarks, hexaquarks) by means of QCD sum rules, we note that the totality of contributions to two-point or three-point correlation functions that involve, respectively, either two or just a single operator capable of interpolating the particular multiquark under study can be straightforwardly disentangled into two disjoint classes defined by unambiguously identifiable members. The first is formed by so-called multiquark-phile contributions which indeed might support multiquarks. In the case of flavour-exotic tetraquarks, by definition composed of four (anti–) quarks of mutually different flavours, a tetraquark-phile contribution has to exhibit two or more gluon exchanges of appropriate topology. The second consists of contributions evidently not bearing any relation to multiquarks; these must be discarded when studying multiquarks by QCD sum rules. The first class only should enter the “multiquark-adequate” QCD sum rules for exotic hadrons.
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38

Schierholz, Gerrit. "Dynamical solution of the strong CP problem within QCD?" EPJ Web of Conferences 274 (2022): 01009. http://dx.doi.org/10.1051/epjconf/202227401009.

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The strong CP problem is inseparably connected with the topology of gauge fields and the mechanism of color confinement, which requires nonperturbative tools to solve it. In this talk I present results of a recent lattice investigation of QCD with the θ term in collaboration with Yoshifumi Nakamura [1, 2]. The tool we are using to address the nonperturbative properties of the theory is the gradient flow, which is a particular realization of momentum space RG transformations. The novel result is that within QCD the vacuum angle θ is renormalized, together with the strong coupling constant, and flows to θ = 0 in the infrared limit. This means that CP is conserved by the strong interactions.
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39

Bloch, Jacques, and Tilo Wettig. "Random matrix analysis of the QCD sign problem for general topology." Journal of High Energy Physics 2009, no. 03 (March 17, 2009): 100. http://dx.doi.org/10.1088/1126-6708/2009/03/100.

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40

Burger, Florian, Ernst-Michael Ilgenfritz, Maria Paola Lombardo, Michael Müller-Preussker, and Anton Trunin. "Topology (and axion's properties) from lattice QCD with a dynamical charm." Nuclear Physics A 967 (November 2017): 880–83. http://dx.doi.org/10.1016/j.nuclphysa.2017.07.006.

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41

AliKhan, A. "Eta meson mass and topology in QCD with two light flavors." Nuclear Physics B - Proceedings Supplements 83-84, no. 1-3 (March 2000): 162–64. http://dx.doi.org/10.1016/s0920-5632(00)00215-2.

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42

Ali Khan, A., S. Aoki, R. Burkhalter, S. Ejiri, M. Fukugita, S. Hashimoto, N. Ishizuka, et al. "Eta meson mass and topology in QCD with two light flavors." Nuclear Physics B - Proceedings Supplements 83-84 (April 2000): 162–64. http://dx.doi.org/10.1016/s0920-5632(00)91611-6.

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43

Stamatescu, Ion-Olimpiu, and Christian Weiss. "QCD topology using scale controlled cooling: densities and cooling invariant observables." Nuclear Physics B - Proceedings Supplements 94, no. 1-3 (March 2001): 532–36. http://dx.doi.org/10.1016/s0920-5632(01)00860-x.

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44

CHANDOLA, H. C., and H. C. PANDEY. "CURRENT CORRELATORS AND DUAL DESCRIPTION OF LONG DISTANCE QCD." Modern Physics Letters A 17, no. 10 (March 28, 2002): 599–607. http://dx.doi.org/10.1142/s0217732302006771.

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An attempt has been made to analyze the magnetic symmetry of the non-Abelian gauge theory associated with the strong interactions using the fibre bundle formulation. Utilizing the gauge field topology, the analysis of dual dynamics associated with the non-Abelian fields is shown to have important bearings on the nonperturbative hadronic effects like confinement of colored quarks and gluons inside hadrons. The state of dual superconductivity for the magnetically condensed vacuum has been analyzed to understand the bulk QCD magnetic properties by evaluating the current correlators in magnetic gauge in terms of the dielectric parameters. The dielectric behavior has been shown to lead to the p-4 confining nature to the dual gluon propagators and to provide an effective macroscopic description of the complicated nonperturbative microscopic interactions of charged particles in dual QCD. The p-4 behavior of dual gluon propagator has also been shown to confirm the linearly rising inter-quark confining potential with an explicit dual gluon mass dependency in dual QCD.
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45

Allés, B., M. D'Elia, and M. P. Lombardo. "Topology, chiral and screening transitions at finite density in two colour QCD." Nuclear Physics B - Proceedings Supplements 174 (December 2007): 225–28. http://dx.doi.org/10.1016/j.nuclphysbps.2007.08.130.

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46

Kogut, J. B., J. F. Lagaë, and D. K. Sinclair. "Topology, fermionic zero modes and flavor singlet correlators in finite temperature QCD." Nuclear Physics B - Proceedings Supplements 63, no. 1-3 (April 1998): 433–35. http://dx.doi.org/10.1016/s0920-5632(97)00793-7.

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47

Allés, B., M. D'Elia, M. P. Lombardo, and M. Pepe. "Topology in full QCD with 2 colours at finite temperature and density." Nuclear Physics B - Proceedings Supplements 94, no. 1-3 (March 2001): 441–44. http://dx.doi.org/10.1016/s0920-5632(01)00999-9.

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48

Charzyński, S., G. Rudolph, and M. Schmidt. "On the topology of the reduced classical configuration space of lattice QCD." Journal of Geometry and Physics 58, no. 11 (November 2008): 1607–23. http://dx.doi.org/10.1016/j.geomphys.2008.07.005.

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49

Phat, Tran Huu, Nguyen Tuan Anh, and Phung Thi Thu Ha. "Topological phase transition in effective model of QCD with chiral nonrestoration." International Journal of Modern Physics E 24, no. 03 (March 2015): 1550021. http://dx.doi.org/10.1142/s0218301315500214.

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The topological phase transition is studied systematically within an effective model of Quantum Chromodynamics (QCD) where the chiral symmetry, broken at zero temperature, is not restored at high temperature and/or baryon chemical potential. It is found that during phase transition the system undergoes a first-order transition from the nonFermi liquid state to the Fermi liquid state which is protected by topology of the Fermi sphere. The phase diagram of the transition in the plane of temperature and baryon chemical potential is established. The critical behaviors of various equations of state are determined.
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50

Collins, Graham P. "Supersymmetric QCD Sheds Light on Quark Confinement and the Topology of 4‐Manifolds." Physics Today 48, no. 3 (March 1995): 17–20. http://dx.doi.org/10.1063/1.2807935.

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