2001
DOI: 10.1016/s0920-5632(01)01518-3
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Domain walls in supersymmetric QCD

Abstract: In this talk we construct BPS-saturated domain walls in supersymmetric QCD, for any values of the masses of the chiral matter superfields. We compare our results to those already obtained in the literature and we also discuss their range of applicability, as well as future directions that would be desirable to explore in order to achieve a complete understanding of supersymmetric gluodynamics as a step in improving our knowledge of how QCD works.

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Cited by 10 publications
(8 citation statements)
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“…Perturbative analysis indicates that there are at most four trajectories emanating from each vacuum, and an analysis along the lines of [38] demonstrates that only two of these interpolate to the second vacuum providing true wall configurations. This conclusion is backed up by explicit numerical solutions found 7 in [17] which were confirmed in [19]. More generally, if we retain the dependence on the full 2 × 2 meson matrix, the flavor asymmetric ansatz will break the SU(2) symmetry down to U(1), inducing flavor moduli parametrizing a CP 1 sigma model on the worldvolume.…”
Section: Breaking the Flavor Symmetry And Nmentioning
confidence: 79%
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“…Perturbative analysis indicates that there are at most four trajectories emanating from each vacuum, and an analysis along the lines of [38] demonstrates that only two of these interpolate to the second vacuum providing true wall configurations. This conclusion is backed up by explicit numerical solutions found 7 in [17] which were confirmed in [19]. More generally, if we retain the dependence on the full 2 × 2 meson matrix, the flavor asymmetric ansatz will break the SU(2) symmetry down to U(1), inducing flavor moduli parametrizing a CP 1 sigma model on the worldvolume.…”
Section: Breaking the Flavor Symmetry And Nmentioning
confidence: 79%
“…If all remaining entries in the mass matrix m ′ are much less than Λ N −1 then the N vacua of the theory lie at weak coupling and one can reliably calculate the index ν k by counting solutions of the classical BPS equations. Thus, we conclude that to ensure the validity of weak coupling analysis the mass matrix should be of the hierarchical form (18) Nonetheless, the reason we have emphasized the N-flavor perspective is that we can restore the maximal SU(N) flavor symmetry of the superpotential, despite the presence of the hierarchical mass matrix (18), by a holomorphic field rescaling. In practice it is convenient to introduce the dimensionless fields X g f ,…”
Section: From Sym Theory To Sqcdmentioning
confidence: 97%
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“…The corresponding central charge is present in the superalgebra [9] and such solitons are 1/2-BPS saturated. In previous work [10], we studied the BPS wall spectrum in this theory, following earlier work on BPS walls in other variants of N= 1 SQCD [9,[11][12][13][14][15][16][17]. The vacuum structure is illustrated in the plane of the superpotential in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…• In some cases the CP walls are approximately BPS-saturated, with calculable tensions [12]. BPS domain walls in SQCD have been extensively studied in the literature [12][13][14][15][16][17][18][19][20][21]. SUSY-breaking effects on the tension may be computed perturbatively.…”
Section: Introductionmentioning
confidence: 99%