1989
DOI: 10.1143/ptp.82.153
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Quark Confinement through Dyonic Condensation

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Cited by 25 publications
(11 citation statements)
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“…As such, the dynamical breaking of the magnetic symmetry in this theory ultimately induces the generalized Meissner effect with its electric constituent as usual, the Meissner effect, and its magnetic constituent as usual, the dual Meissner effect. It dictates the mechanism for confinement of the electric and magnetic fluxes associated with dyonic quarks (12) in the present theory. Among others, an important property of the QCD Lagrangian is that it is ultraviolet finite, and infrared unstable.…”
Section: Dyonic Condensation and Quark Confinementmentioning
confidence: 91%
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“…As such, the dynamical breaking of the magnetic symmetry in this theory ultimately induces the generalized Meissner effect with its electric constituent as usual, the Meissner effect, and its magnetic constituent as usual, the dual Meissner effect. It dictates the mechanism for confinement of the electric and magnetic fluxes associated with dyonic quarks (12) in the present theory. Among others, an important property of the QCD Lagrangian is that it is ultraviolet finite, and infrared unstable.…”
Section: Dyonic Condensation and Quark Confinementmentioning
confidence: 91%
“…Furthermore, Mandelstam (8) has shown that condensation of the magnetic monopoles of a Q C D vacuum could produce the dual Meissner effect leading to the confinement of the color electric flux carried by the quarks. Based on this idea, we recently (9, 10) constructed, out of SU(2) QCD, a dual gauge theory called restricted chromodynamics (1 1) (RCD), which could produce a dynamical dyonic (electric as well as magnetic) condensation (12) and exhibit the desired dual dynamics (1 3-15) that guarantee the confinement of dyonic quarks through the generalized Meissner effect. This RCD is extracted from Q C D by imposing an additional internal symmetry, i.e., the magnetic symmetry (I 1) that reduces the dynamical degrees of freedom and hence there remains the unsettled questions regarding the physical spectrum of RCD and the confinement if one removes the magnetic symmetry and reactivates the suppressed dynamical degrees of freedom.…”
Section: Introductionmentioning
confidence: 99%
“…So the topological structure ofm may be identified with the topological pointlike objects of the underlying non-Abelian gauge symmetry. As such, when the second homotopy 2 (G/H ) defined bym is nontrivial, the gauge potential V µ becomes in a way dual so that the part of it that is completely fixed by magnetic symmetric requirement describes pointlike colored topological structures while the unrestricted part describes conventional dyonic objects (quarks) [14].…”
Section: Restricted Quantum Chromodynamics: An Overviewmentioning
confidence: 99%
“…Since the Lagrangian (15) does not have any additional degrees of freedom, there seems to be no other way than to introduce an extra degree of freedom in RCD in terms of a scalar field φ. Following Mandelstam [8] and 't Hooft [8], we describe [14] the dyonic source in RCD by a complex field operator φ, as a result the RCD Lagrangian (15) is modified to…”
Section: Restricted Quantum Chromodynamics: An Overviewmentioning
confidence: 99%
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