Pauli graphs when the Hilbert space dimension contains a square: why the Dedekind psi function ?
arXiv:1009.3858 · doi:10.1088/1751-8113/44/4/045301
Abstract
We study the commutation relations within the Pauli groups built on all decompositions of a given Hilbert space dimension , containing a square, into its factors. Illustrative low dimensional examples are the quartit () and two-qubit () systems, the octit (), qubit/quartit () and three-qubit () systems, and so on. In the single qudit case, e.g. , one defines a bijection between the maximal commuting sets [with the sum of divisors of ] of Pauli observables and the maximal submodules of the modular ring , that arrange into the projective line and a independent set of size [with the Dedekind psi function]. In the multiple qudit case, e.g. , the Pauli graphs rely on symplectic polar spaces such as the generalized quadrangles GQ(2,2) (if ) and GQ(3,3) (if ). More precisely, in dimension ( a prime) of the Hilbert space, the observables of the Pauli group (modulo the center) are seen as the elements of the -dimensional vector space over the field . In this space, one makes use of the commutator to define a symplectic polar space of cardinality , that encodes the maximal commuting sets of the Pauli group by its totally isotropic subspaces. Building blocks of are punctured polar spaces (i.e. a observable and all maximum cliques passing to it are removed) of size given by the Dedekind psi function . For multiple qudit mixtures (e.g. qubit/quartit, qubit/octit and so on), one finds multiple copies of polar spaces, ponctured polar spaces, hypercube geometries and other intricate structures. Such structures play a role in the science of quantum information.
18 pages, version submiited to J. Phys. A: Math. Theor
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