1985
DOI: 10.1088/0305-4470/18/17/026
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Harmonic superspaces of extended supersymmetry. I. The calculus of harmonic variables

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Cited by 37 publications
(60 citation statements)
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“…Therefore, we consider it as crucial to introduce USp(4) harmonic variables which are employed for the corresponding N =4 harmonic superspace. The various cosets of the USp(4) group were introduced and studied in [25], and the corresponding harmonic variables were further applied in [26,27] to d=5 and d=6 N =4 SYM models. In our work we find them useful also for d=4 N =4 SYM and superparticle models.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, we consider it as crucial to introduce USp(4) harmonic variables which are employed for the corresponding N =4 harmonic superspace. The various cosets of the USp(4) group were introduced and studied in [25], and the corresponding harmonic variables were further applied in [26,27] to d=5 and d=6 N =4 SYM models. In our work we find them useful also for d=4 N =4 SYM and superparticle models.…”
Section: Introductionmentioning
confidence: 99%
“…Since the R-symmetry group is SU(4), the harmonic coordinates that we introduce will form the coset manifold SU(4)/H, where H is a subgroup of SU(4). As has been discussed in [67], there are several possibilities for the choice of H, which are suitable for different physical contexts (see e.g. [11] for one particular application).…”
Section: B1 Harmonic Coordinatesmentioning
confidence: 99%
“…Using the covariant derivatives and solving the Bianchi identities, we can immediately write down the supersymmetry transformations (2) By analogy with the case of the N = 2 models with the intrinsic central charge [12]- [15], the equations (14,18,19) can be called the generalized Dirac equation, the Yang-Mills equation and the Klein-Gordon equation respectively. Thus the central charge plays the role of 'fifth coordinate'.…”
mentioning
confidence: 99%
“…As a consequence of (9)- (19), we can construct the complete power expansion of the 1) . The set of constraints (9)- (19) shows that the component fields in [1] are completely determined by the lowest orders in the expansion W ij (x, θ,θ, z) over z, θ,θ. Then it is clear that we can completely fix the dependence of all quantities under consideration on the central-charge coordinate z, as was done for the theories with N = 2 rigid supersymmetry with the central charge [12], [14], [15].…”
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confidence: 99%
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