Abstract

We study the behaviour of supersymmetric ground states in a class of one-dimensional N = 2 abelian gauged linear sigma models, including theories for which the target space is a complete intersection in projective space, and more generally, models with an interaction term introduced by Herbst, Hori and Page in which the vacua correspond to elements of hypercohomology groups of complexes of sheaves. Combining physical insights from recent work by Hori, Kim and Yi with the use of spectral sequences, we propose a way to reconcile the non-linear sigma model description, valid deep within a geometric phase, with the effective Coulomb branch description, valid near a phase boundary. This leads to a physical interpretation of the hypercohomology groups from the perspective of the Coulomb branch, as well as an interpretation for the spectral sequences used to compute them.

Highlights

  • This means that, by avoiding these singularities in the moduli space, one can pass smoothly from one phase to another

  • We study the behaviour of supersymmetric ground states in a class of onedimensional N = 2 abelian gauged linear sigma models, including theories for which the target space is a complete intersection in projective space, and more generally, models with an interaction term introduced by Herbst, Hori and Page in which the vacua correspond to elements of hypercohomology groups of complexes of sheaves

  • In the ζ → ∞ limit, the supersymmetric vacua in such models localise on a compact Higgs branch, and the theory is well described by a non-linear sigma model

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Summary

Supersymmetric vacua

Having analysed the spectrum of supersymmetric ground states in the limit ζ → ∞, we study the opposite regime, ζ → 0. In this limit, the Higgs branch of classical vacua shrinks to zero size, and the Coulomb branch emerges. The aim of this section is to characterise this effective action on the Coulomb branch, and to determine the fate of the individual supersymmetric ground states that we found in the Higgs branch picture, as we reduce ζ from infinity to zero. We expect the quantum wavefunctions of the supersymmetric vacua to spread along the Coulomb branch, becoming non-normalisable at infinity when ζ = 0 [20,21,22].

Fermi multiplets and complete intersections in projective space
Spectral sequences
Examples
Free theories
Theories with potentials: matter sector
Effective Coulomb branch action: complexes of arbitrary length
Statement of main proposal
Final example: the Koszul complex
Concluding remarks
Full Text
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