Wednesday, 9 September 2009

gr.group theory - Schur Multipliers

The group H2(G,mathbbCtimes) plays a rôle in orbifold conformal field theory and is usually known as the discrete torsion group. In fact, in this context one actually needs the explicit cocycle and for the case of a finite simple abelian group it is very easy to compute explicitly.



Let varepsilon:GtimesGtomathbbCtimes be the cocycle. Without loss of generality one can normalise it so that
varepsilon(0,g)=varepsilon(g,0)=1


for all ginG. With this normalisation the cocycle conditions become, in addition, the following:
varepsilon(g,g)=1quadvarepsilon(g,g)=varepsilon(g,g)1

and
varepsilon(g1+g2,g)=varepsilon(g1,g)varepsilon(g2,g)

from where it follows that if G has order N, then for all g,ginG,
varepsilon(g,g)N=1



Let G=mathbbZ/N1timescdotstimesmathbbZ/Nk be a finite simple abelian group and let alphai be a generator of mathbbZ/Ni, so that we can write any element of G as a sum suminialphai where ni=0,1,ldots,Ni1.



Then one finds that all cocycles are given in terms of Bij=Bji taking the possible values 0,1,ldots,mathrmgcd(Ni,Nj)1, by the formula
varepsilon(suminialphai,sumjmjalphaj)=exp2pisqrt1sumi,jfracBijnimjmathrmgcd(Ni,Nj)



It is the bilinear Bij/mathrmgcd(Ni,Nj) which is called the discrete torsion. It should be emphasised that torsion here is by analogy with the torsion of a connection in differential geometry and not with torsion as in group theory.



If you google "discrete torsion" and "orbifold" you might find suitable references, just like this paper of Vafa and Witten.

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