Model of magnetic heads audio characteristics

Dubrovin, V. T.; Subbotin, Sergey

doi:10.1109/cadsm.2001.975821

Cited by 1 publication

(2 citation statements)

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“…are canonical 1-differentials, A i dΩ j = δ ij . When the prepotential satisfies the WDVV equations this choice is equivalent to specifying a flat structure [20,21]. Further the second derivatives T ij of the prepotential ( 5) with respect to these coordinates then form the period matrix of C. An even simpler expression -the "residue formula" -exists for the variation of the period matrix, that is for the third derivatives of F (a) (see, e.g.…”

Section: Basics Of Sw Theorymentioning

confidence: 99%

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The Ruijsenaars-Schneider model in the context of Seiberg-Witten theory

et al. 1999

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The compactification of five dimensional N = 2 SUSY Yang-Mills (YM) theory onto a circle provides a four dimensional YM model with N = 4 SUSY. This supersymmetry can be broken down to N = 2 if non-trivial boundary conditions in the compact dimension, φ(x 5 + R) = e 2πiǫ φ(x 5 ), are imposed on half of the fields. This two-parameter (R, ǫ) family of compactifications includes as particular limits most of the previously studied four dimensional N = 2 SUSY YM models with supermultiplets in the adjoint representation of the gauge group. The finite-dimensional integrable system associated to these theories via the Seiberg-Witten construction is the generic elliptic Ruijsenaars-Schneider model. In particular the perturbative (weak coupling) limit is described by the trigonometric Ruijsenaars-Schneider model.

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Section: Basics Of Sw Theorymentioning

confidence: 99%

“…Observe that with our choice (20) this equation, which describes the Seiberg-Witten spectral curve, may be expressed in the form.…”

Section: Spectral Curvementioning

confidence: 99%