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Physics Letters B

Modular invariants from simple currents. An explicit proof

A.N. Schellekens, Shimon Yankielowicz B

Published Aug 1, 1989• 80 citations
Publisher
DOI
10.1016/0370-2693(89)90948-9

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The twisted convolution identity and ghost rrr-SICs from finite quantum dilogarithms
Radchenko and Wheeler (RW) recently proved a finite pentagon relation for real quadratic special values of the modular quantum dilogarithm and used it to establish the rank-111 twisted convolution identity conjectured by the current authors. RW gave an explicit argument in the principal case and remarked that their proof holds for all rank-111 admissible tuples. We extend their proof to all rank-rrr admissible tuples and provide an explicit dictionary between the modular quantum dilogarithm and the Shintani-Faddeev modular cocycle conventions in the respective papers. Thus, we establish that, if d,rd,rd,r are positive integers such that r<d−12r<\frac{d-1}{2}r<2d−1​ and d2−1r(d−r)∈Z\frac{d^2-1}{r(d-r)} \in \mathbb{Z}r(d−r)d2−1​∈Z, then there exist ghost rrr-SICs: i.e., configurations of d2d^2d2 rank-rrr subspaces in Cd\mathbb{C}^dCd that satisfy a non-Hermitian equichordal condition. Under the Stark conjecture, these configurations are Galois conjugate to Hermitian equichordal configurations called rrr-SICs (or rank-rrr SIC-POVMs).
Modular invariance imposes rigid constraints on the partition functions of two-dimensional conformal field theories (CFTs). Many fundamental results follow strictly from modular invariance and unitarity, giving rise to the numerical modular bootstrap program. Here we report on a way to relate a particular family of quantum error correcting codes to a family of "code CFTs," which forms a subset of the space of Narain CFTs. This correspondence reduces modular invariance of the 2D CFT partition function to a few simple algebraic relations obeyed by a multivariate polynomial characterizing the corresponding code. Using this correspondence, we construct many explicit examples of physically distinct isospectral theories, as well as many examples of nonholomorphic functions, which satisfy all the basic properties of a 2D CFT partition function, yet are not associated with any known CFT.