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SIAM Journal on Matrix Analysis and Applications

A Lower Bound on the C-Numerical Radius of Nilpotent Matrices Appearing in Coherent Spectroscopy

Chi-Kwong Li, Hugo J. Woerdeman

Published Jan 1, 2005• 9 citations
Publisher

Abstract

We provide a lower bound for the efficiency of polarization or coherence transfer between quantized states under unitary transformations. Mathematically the problem is the determination of the C-numerical radius of A for certain nilpotent matrices C and A. The presented lower bound is conjectured to be exact as it coincides with numerical data provided in [U. Helmke et al., J. Global Optim., 23 (2002), pp. 283-308].

DOI
10.1137/040613330

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We provide a lower bound for the efficiency of polarization or coherence transfer between quantized states under unitary transformations. Mathematically the problem is the determination of the C-numerical radius of A for certain nilpotent matrices C and A. The presented lower bound is conjectured to be exact as it coincides with numerical data provided in [U. Helmke et al., J. Global Optim., 23 (2002), pp. 283-308].
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We investigate the geometric structure of the set of spectra of bipartite absolute separable states (ASEPm,n\mathrm{ASEP}_{m,n}ASEPm,n​) and absolute positive partial transpose states (APPTm,n\mathrm{APPT}_{m,n}APPTm,n​), \emph{i.e.}, bipartite quantum states that remain separable or PPT, respectively, under all global unitary transformations. First, we establish general geometric properties of absolute convex sets of matrices, their spectra and extreme points. Regarding absolute separability, we present a permutation-symmetric reformulation of the absolute PPT criterion and use it to demonstrate that APPTm,n\mathrm{APPT}_{m,n}APPTm,n​ is a spectrahedron for all m≤nm\leq nm≤n: in particular, all its faces are exposed. While ASEP2,n\mathrm{ASEP}_{2,n}ASEP2,n​ is a spectrahedron, too, for ASEPm,n\mathrm{ASEP}_{m,n}ASEPm,n​ we can in general only show that it is a semialgebraic set for all m,n≥3m,n\geq 3m,n≥3. Furthermore, we provide a complete characterization of the faces and extreme points of APPTm,n\mathrm{APPT}_{m,n}APPTm,n​ and demonstrate that the dimension of a face is determined by the rank of a certain matrix, with maximal proper faces having dimension mn−m−1mn-m-1mn−m−1. In the quantitative setting, we provide a rigorous lower bound on the maximal attainable purity of APPTm,n\mathrm{APPT}_{m,n}APPTm,n​ via an inscribed polytope Pm,n\mathcal{P}_{m,n}Pm,n​ and conjecture that the maximal purity of APPTm,n\mathrm{APPT}_{m,n}APPTm,n​ (along with its spectra) coincides with the polytope for arbitrary dimensions except when m=n=2m=n=2m=n=2. Additionally, we also provide a rigorous upper bound on the minimal von Neumann entropy of APPTm,n\mathrm{APPT}_{m,n}APPTm,n​ and demonstrate numerically that the minimum entropy eventually coincides with the polytope Pm,n\mathcal{P}_{m,n}Pm,n​ as the local system dimension nnn increases. Finally, we show that the relative spectral volume of APPTm,n\mathrm{APPT}_{m,n}APPTm,n​ decays exponentially in nnn by a constant multiplicative factor of the relative volume of the inscribed polytope Pm,n\mathcal{P}_{m,n}Pm,n​.
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