2016
DOI: 10.1007/jhep03(2016)004
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Sequencing BPS spectra

Abstract: This paper provides both a detailed study of color-dependence of link homologies, as realized in physics as certain spaces of BPS states, and a broad study of the behavior of BPS states in general. We consider how the spectrum of BPS states varies as continuous parameters of a theory are perturbed. This question can be posed in a wide variety of physical contexts, and we answer it by proposing that the relationship between unperturbed and perturbed BPS spectra is described by a spectral sequence. These general… Show more

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Cited by 57 publications
(78 citation statements)
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References 186 publications
(688 reference statements)
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“…(Other B-twisted Landau-Ginzburg models have also been proposed to describe the same system, e.g. [96][97][98][99]; their relation with T 2d is still unclear. )…”
Section: Jhep10(2016)108mentioning
confidence: 99%
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“…(Other B-twisted Landau-Ginzburg models have also been proposed to describe the same system, e.g. [96][97][98][99]; their relation with T 2d is still unclear. )…”
Section: Jhep10(2016)108mentioning
confidence: 99%
“…In the presence of nonzero t R , it is natural to deform the boundary conditions by an infinite gradient flow with respect to h t , as first discussed in section 2.5.6 (and in parallel to the abelian Higgs-branch discussion of section 6.2.3). For right boundary conditions, the deformation is achieved by rescaling 97) and sending λ → ∞. (For left b.c., one should send λ → 0 instead.)…”
Section: Neumann Boundary Conditionsmentioning
confidence: 99%
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“…can be very effectively computed for various families of knots, using the formalism of differentials [24,25,27,28]. Note that generalizations of the LMOV conjecture to the case of superpolynomials have been considered in [11,29].…”
Section: Knot Invariants Knot Homologies and Lmov Conjecturementioning
confidence: 99%
“…This formalism is successfully developed in [31] and [33] and has already allowed us to find the inclusive Racah matrices for R = [2,2] and even R = [3,1]. In combination with the differential expansion method [142][143][144][145][146][147][148][149][150], this provides extensions to other rectangular representations. Further progress (for other nonrectangular representations) is expected after developing the ∆-technique briefly outlined in [33].…”
Section: Highest Weight Methodsmentioning
confidence: 99%