2014
DOI: 10.1007/s00023-014-0385-6
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Spectral Properties of Non-Unitary Band Matrices

Abstract: We consider families of random non-unitary contraction operators defined as deformations of CMV matrices which appear naturally in the study of random quantum walks on trees or lattices. We establish several deterministic and almost sure results about the location and nature of the spectrum of such non-normal operators as a function of their parameters. We relate these results to the analysis of certain random quantum walks, the dynamics of which can be studied by means of iterates of such random non-unitary c… Show more

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Cited by 2 publications
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“…By Balanced Random Quantum Walk, BRQW for short, we mean a quantum walk defined either on the cubic lattice Z d or on the homogeneous tree T 2d , where d ∈ N is half the coordination number in the latter case, such that the quantum mechanical transition amplitude between neighbouring sites has uniform modulus and random argument uniformly distributed on the torus. We briefly recall the basics about RQWs below; for more details, see [HJ1,HJ2] 2.1 Random quantum walks on T 2d Let T 2d denote the homogeneous tree of degree 2d of the free group F {a 1 ,...,a d } generated by the alphabet…”
Section: Balanced Random Quantum Walkmentioning
confidence: 99%
“…By Balanced Random Quantum Walk, BRQW for short, we mean a quantum walk defined either on the cubic lattice Z d or on the homogeneous tree T 2d , where d ∈ N is half the coordination number in the latter case, such that the quantum mechanical transition amplitude between neighbouring sites has uniform modulus and random argument uniformly distributed on the torus. We briefly recall the basics about RQWs below; for more details, see [HJ1,HJ2] 2.1 Random quantum walks on T 2d Let T 2d denote the homogeneous tree of degree 2d of the free group F {a 1 ,...,a d } generated by the alphabet…”
Section: Balanced Random Quantum Walkmentioning
confidence: 99%