1999
DOI: 10.1002/(sici)1521-3978(199906)47:6<643::aid-prop643>3.0.co;2-x
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Abstract: Exact solutions to the low‐energy effective action (LEEA) of the four‐dimensional N = 2 supersymmetric gauge theories are known to be obtained either by quantum field theory methods from S‐duality in the Seiberg‐Witten approach, or by the Type‐IIA superstring/M‐Theory methods of brane technology. After a brief review of the standard field‐theoretical results for the N = 2 gauge (Seiberg‐Witten) LEEA, we consider a field‐theoretical derivation of the exact hypermultiplet LEEA by using the N = 2 harmonic supers… Show more

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Cited by 10 publications
(24 citation statements)
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“…However, magnetically charged (massive) hypermultiplets can have a non-trivial self-interaction [27,28]. This observation is consistent with the brane technology [29]. The corresponding LEEA just describes the low-energy dynamics of the BPS monopoles representing nonperturbative degrees of freedom, in the Lorentz-invariant way (cf.…”
Section: Introductionsupporting
confidence: 65%
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“…However, magnetically charged (massive) hypermultiplets can have a non-trivial self-interaction [27,28]. This observation is consistent with the brane technology [29]. The corresponding LEEA just describes the low-energy dynamics of the BPS monopoles representing nonperturbative degrees of freedom, in the Lorentz-invariant way (cf.…”
Section: Introductionsupporting
confidence: 65%
“…Since the Seiberg-Witten curve Σ SW is known to have the simple geometrical interpretation in M-theory, where it can be considered as the part of a magnetically charged fivebrane worldvolume wrapped about Σ SW [65], it is conceivable that the hypermultiplet spectral curve Σ H may have, perhaps, a similar geometrical interpretation which is presumably related to (Dirichlet) 6-branes in ten-dimensional spacetime [29].…”
Section: Resultsmentioning
confidence: 99%
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“…(5.2), it is instructive to consider first a simpler case, by assuming the additional (translational) U(1) T symmetry that acts on the complex superfields (q + , * q + ) by phase rotations (with a constant parameter α), q + → e iα θ + , * q + → e −iα * q + , (5.5) but does not move the hyper-Kähler structure in the target space of the N=2 NLSM (3.19). It happens, e.g., in the N=2 supersymmetric QED with a single charged hypermultiplet, or in the Coulomb branch of the Seiberg-Witten model [30]. In geometrical terms, the U(1) T symmetry amounts to the existence of a tri-holomorphic (translational) isometry in the N=2 NLSM target space.…”
Section: Examplesmentioning
confidence: 99%
“…2 See [22] for earlier attempts to construct an N = 2 supersymmetric version of the Born-Infeld action.…”
Section: Introductionmentioning
confidence: 99%