A modular invariant for a chiral conformal field theory is physical if there is a full conformal field theory with the given chiral halves realising the modular invariant. The easiest modular invariants are the charge conjugation and the diagonal modular invariants. While the charge conjugation modular invariant is always physical there are examples of chiral CFTs for which the diagonal modular invariant is not physical. Here we give (in
group theoretical terms) a necessary and sufficient condition for diagonal modular invariants of
G-orbifolds of holomorphic conformal field theories to be physical.
Mathematically a physical modular invariant is an invariant of a Lagrangian algebra in the product of (chiral) modular categories. The chiral modular category of a G -orbifold of a holomorphic conformal field theory is the so-called (twisted) Drinfeld centre Z(G,α) of the finite group G . We show that the diagonal modular invariant for e00f88e263bbfe" title="Click to view the MathML source">Z(G) is physical if and only if the group G has a double class inverting automorphism, that is an automorphism ϕ:G→G with the property that for any commuting x,y∈G there is g∈G such that ϕ(x)=gx−1g−1, ϕ(y)=gy−1g−1.
Groups without double class inverting automorphisms are abundant and provide examples of chiral conformal field theories for which the diagonal modular invariant is unphysical.
