39,444 research outputs found

    Harder-Narasimhan filtration for rank 2 tensors and stable coverings

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    We construct a Harder-Narasimhan filtration for rank 22 tensors, where there does not exist any such notion a priori, as coming from a GIT notion of maximal unstability. The filtration associated to the 1-parameter subgroup of Kempf giving the maximal way to destabilize, in the GIT sense, a point in the parameter space of the construction of the moduli space of rank 22 tensors over a smooth projective complex variety, does not depend on certain integer used in the construction of the moduli space, for large values of the integer. Hence, this filtration is unique and we define the Harder-Narasimhan filtration for rank 22 tensors as this unique filtration coming from GIT. Symmetric rank 22 tensors over smooth projective complex curves define curve coverings lying on a ruled surface, hence we can translate the stability condition to define stable coverings and characterize the Harder-Narasimhan filtration in terms of intersection theory.Comment: 22 pages; Minor changes suggested by the referee; To appear on Proc. Indian Acad. Sci. (Math. Sci.

    On the Operator Product Expansion in Noncommutative Quantum Field Theory

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    Motivated by the mixing of UV and IR effects, we test the OPE formula in noncommutative field theory. First we look at the renormalization of local composite operators, identifying some of their characteristic IR/UV singularities. Then we find that the product of two fields in general cannot be described by a series expansion of single local operator insertions.Comment: 15 pages, six figures. LaTeX, JHEP class. Minor improvements, typos corrected. To be published in JHE

    Regulating the Global Banking Network -- What Role (if any) for the IMF?

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    Separation of analytic sets by rectangles of low complexity

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    We provide Hurewicz tests for the separation of disjoint analytic sets by rectangles of the form Γ×Γâ€Č\Gamma\times\Gamma' for Γ,Γâ€Č∈Σ10,Π10,Π20\Gamma,\Gamma'\in {\mathbf\Sigma^0_1 , \mathbf\Pi^0_1 , \mathbf\Pi^0_2 }
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