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On Generalised Discrete Torsion

Philip Boyle Smith, Yuji Tachikawa

Abstract

For a 2d gauged sigma model with target space $M$ and discrete gauge group $G$, we consider a generalisation of Vafa's discrete torsion $H^2(BG; U(1))$ that assigns different local discrete torsion phases to different singular loci of the orbifold $M/G$. Our generalised discrete torsion lives in $H^2_G(M; U(1))$, and gives a consistent implementation of Gaberdiel and Kaste's prescription for inserting such local discrete torsion phases by hand at higher genus. We revisit the original application to $T^6/\mathbb{Z}_2^2$ and $T^7/\mathbb{Z}_2^3$ orbifold CFTs, and determine what smooth Calabi-Yau and $G_2$ geometries result from different choices of the generalised discrete torsion. We find that the local discrete torsion phases can be different from each other, but are not completely independent either; in the $T^7/\mathbb{Z}_2^3$ case for example, the orbifold CFTs only realise 3 out of the 9 possible Betti numbers of $G_2$ resolutions constructed by Joyce.

On Generalised Discrete Torsion

Abstract

For a 2d gauged sigma model with target space and discrete gauge group , we consider a generalisation of Vafa's discrete torsion that assigns different local discrete torsion phases to different singular loci of the orbifold . Our generalised discrete torsion lives in , and gives a consistent implementation of Gaberdiel and Kaste's prescription for inserting such local discrete torsion phases by hand at higher genus. We revisit the original application to and orbifold CFTs, and determine what smooth Calabi-Yau and geometries result from different choices of the generalised discrete torsion. We find that the local discrete torsion phases can be different from each other, but are not completely independent either; in the case for example, the orbifold CFTs only realise 3 out of the 9 possible Betti numbers of resolutions constructed by Joyce.

Paper Structure

This paper contains 19 sections, 75 equations, 1 table.