The MAGMA algebra system I: the user language
Journal of Symbolic Computation - Special issue on computational algebra and number theory: proceedings of the first MAGMA conference
The finite Heisenberg-Weyl groups in radar and communications
EURASIP Journal on Applied Signal Processing
On Weyl-Heisenberg orbits of equiangular lines
Journal of Algebraic Combinatorics: An International Journal
Equiangular lines, mutually unbiased bases, and spin models
European Journal of Combinatorics
Computing Equiangular Lines in Complex Space
Mathematical Methods in Computer Science
High-resolution radar via compressed sensing
IEEE Transactions on Signal Processing
Ideals, Varieties, and Algorithms: An Introduction to Computational Algebraic Geometry and Commutative Algebra
Quantum Information & Computation
On the quantumness of a hilbert space
Quantum Information & Computation
Equiangular spherical codes in quantum cryptography
Quantum Information & Computation
Quantumness, generalized 2-desing and symmetric informationally complete POVM
Quantum Information & Computation
The monomial representations of the Clifford group
Quantum Information & Computation
Decoherence-Insensitive Quantum Communication by Optimal -Encoding
IEEE Transactions on Information Theory
Galois automorphisms of a symmetric measurement
Quantum Information & Computation
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It is known that if the dimension is a perfect square the Clifford group can be represented by monomial matrices. Another way of expressing this result is to say that when the dimension is a perfect square the standard representation of the Clifford group has a system of imprimitivity consisting of one dimensional subspaces. We generalize this result to the case of an arbitrary dimension. Let k be the square-free part of the dimension. Then we show that the standard representation of the Clifford group has a system of imprimitivity consisting of k-dimensional subspaces. To illustrate the use of this result we apply it to the calculation of SIC-POVMs (symmetric informationally complete positive operator valued measures), constructing exact solutions in dimensions 8 (hand-calculation) as well as 12 and 28 (machine-calculation).