Weyl–Heisenberg-covariant SICs in every dimension
- Field
- Topic
Problem
Does every finite dimension admit a symmetric informationally complete measurement that is a single Weyl–Heisenberg orbit? For an integer \(d\geq2\), let \(\omega_d=e^{2\pi i/d}\) and define shift, phase, and displacement operators on the computational basis by
Equation (1) fixes a phase convention that does not affect the orbit of rank-one projectors. The question is whether, for every \(d\geq2\), there is a unit vector \(\lvert\phi\rangle\in\mathbb C^d\) satisfying
If Eq. (2) holds, the \(d^2\) projectors in the Weyl–Heisenberg orbit of \(\lvert\phi\rangle\) form a SIC.
Source
Renes, Blume-Kohout, Scott, and Caves explicitly conjecture the existence of a Weyl–Heisenberg-covariant SIC in every finite dimension [RBS+04].
Progress
Renes, Blume-Kohout, Scott, and Caves stated Eq. (2) in every dimension as Conjecture 1 and found numerical solutions through \(d=45\) [RBS+04].
Appleby, Bengtsson, Flammia, and Goyeneche reported numerical Weyl–Heisenberg SICs in every dimension through \(d=181\) and in many larger dimensions. These computations establish individual finite cases, not the all-dimensional assertion [ABFG19].
Appleby, Flammia, and Kopp give a construction for all \(d>3\) conditional on the order-one abelian Stark conjecture and a special-value identity for the Shintani–Faddeev modular cocycle. The hypotheses remain unproved, so the construction is not unconditional [AFK25].
Comment
The unresolved step is an unconditional construction, or existence proof, for Eq. (2) in every \(d\). Problem 19 imposes the additional requirement that the fiducial be Zauner symmetric.