Affine A^{(1)}_{3} N=2 monopole as the D module and affine ADHMN sheaf

Details Affine A^{(1)}_{3} N=2 monopole as the D module and affine ADHMN sheaf Affine A^{(1)}_{3} N=2 monopole as the D module and affine ADHMN sheaf

2006-12-19

arxiv.org/abs/hep-th/0612198v3

Commun.Theor.Phys.49:439-450,2008

Physics

High Energy Physics

High Energy Physics - Theory

Identical to the version 2 and only the acknowledgement is replaced

Scientific paper

10.1088/0253-6102/49/2/40

A Higgs-Yang Mills monopole scattering spherical symmetrically along light cones is given. The left incoming anti-self-dual \alpha plane fields are holomorphic, but the right outgoing SD \beta plane fields are antiholomorphic, meanwhile the diffeomorphism symmetry is preserved with mutual inverse affine rapidity parameters \mu and \mu^{-1}. The Dirac wave function scattering in this background also factorized respectively into the (anti)holomorphic amplitudes. The holomorphic anomaly is realized by the center term of a quasi Hopf algebra corresponding to an integrable conform affine massive field. We find explicit Nahm transformation matrix(Fourier-Mukai transformation) between the Higgs YM BPS (flat) bundles (D modules) and the affinized blow up ADHMN twistors (perverse sheafs). Thus establish the algebra for the Hecke-'t Hooft operators in the Hecke correspondence of the geometric Langlands Program.

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