79 research outputs found

    Determinantal and eigenvalue inequalities for matrices with numerical ranges in a sector

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    Let A = \pmatrix A_{11} & A_{12} \cr A_{21} & A_{22}\cr\pmatrix \in M_n, where A11MmA_{11} \in M_m with mn/2m \le n/2, be such that the numerical range of AA lies in the set \{e^{i\varphi} z \in \IC: |\Im z| \le (\Re z) \tan \alpha\}, for some φ[0,2π)\varphi \in [0, 2\pi) and α[0,π/2)\alpha \in [0, \pi/2). We obtain the optimal containment region for the generalized eigenvalue λ\lambda satisfying \lambda \pmatrix A_{11} & 0 \cr 0 & A_{22}\cr\pmatrix x = \pmatrix 0 & A_{12} \cr A_{21} & 0\cr\pmatrix x \quad \hbox{for some nonzero} x \in \IC^n, and the optimal eigenvalue containment region of the matrix ImA111A12A221A21I_m - A_{11}^{-1}A_{12} A_{22}^{-1}A_{21} in case A11A_{11} and A22A_{22} are invertible. From this result, one can show det(A)sec2m(α)det(A11)det(A22)|\det(A)| \le \sec^{2m}(\alpha) |\det(A_{11})\det(A_{22})|. In particular, if AA is a accretive-dissipative matrix, then det(A)2mdet(A11)det(A22)|\det(A)| \le 2^m |\det(A_{11})\det(A_{22})|. These affirm some conjectures of Drury and Lin.Comment: 6 pages, to appear in Journal of Mathematical Analysi

    Canonical forms, higher rank numerical range, convexity, totally isotropic subspace, matrix equations

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    Results on matrix canonical forms are used to give a complete description of the higher rank numerical range of matrices arising from the study of quantum error correction. It is shown that the set can be obtained as the intersection of closed half planes (of complex numbers). As a result, it is always a convex set in C\mathcal C. Moreover, the higher rank numerical range of a normal matrix is a convex polygon determined by the eigenvalues. These two consequences confirm the conjectures of Choi et al. on the subject. In addition, the results are used to derive a formula for the optimal upper bound for the dimension of a totally isotropic subspace of a square matrix, and verify the solvability of certain matrix equations.Comment: 10 pages. To appear in Proceedings of the American Mathematical Societ

    Linear rank preservers of tensor products of rank one matrices

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    Let n1,,nkn_1,\ldots,n_k be integers larger than or equal to 2. We characterize linear maps ϕ:Mn1nkMn1nk\phi: M_{n_1\cdots n_k}\rightarrow M_{n_1\cdots n_k} such that rank(ϕ(A1Ak))=1wheneverrank(A1Ak)=1for allAiMni,i=1,,k.{\mathrm rank}\,(\phi(A_1\otimes \cdots \otimes A_k))=1\quad\hbox{whenever}\quad{\mathrm rank}\, (A_1\otimes \cdots \otimes A_k)=1 \quad \hbox{for all}\quad A_i \in M_{n_i},\, i = 1,\dots,k. Applying this result, we extend two recent results on linear maps that preserving the rank of special classes of matrices.Comment: 12 page

    A note on the perturbation of positive matrices by normal and unitary matrices

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    AbstractIn a recent paper, Neumann and Sze considered for an n×n nonnegative matrix A, the minimization and maximization of ρ(A+S), the spectral radius of (A+S), as S ranges over all the doubly stochastic matrices. They showed that both extremal values are always attained at an n×n permutation matrix. As a permutation matrix is a particular case of a normal matrix whose spectral radius is 1, we consider here, for positive matrices A such that (A+N) is a nonnegative matrix, for all normal matrices N whose spectral radius is 1, the minimization and maximization problems of ρ(A+N) as N ranges over all such matrices. We show that the extremal values always occur at an n×n real unitary matrix. We compare our results with a less recent work of Han, Neumann, and Tastsomeros in which the maximum value of ρ(A+X) over all n×n real matrices X of Frobenius norm n was sought

    Linear preservers and quantum information science

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    Let m,n2m,n\ge 2 be positive integers, MmM_m the set of m×mm\times m complex matrices and MnM_n the set of n×nn\times n complex matrices. Regard MmnM_{mn} as the tensor space MmMnM_m\otimes M_n. Suppose |\cdot| is the Ky Fan kk-norm with 1kmn1 \le k \le mn, or the Schatten pp-norm with 1p1 \le p \le \infty (p2p\ne 2) on MmnM_{mn}. It is shown that a linear map ϕ:MmnMmn\phi: M_{mn} \rightarrow M_{mn} satisfying AB=ϕ(AB)|A\otimes B| = |\phi(A\otimes B)| for all AMmA \in M_m and BMnB \in M_n if and only if there are unitary U,VMmnU, V \in M_{mn} such that ϕ\phi has the form ABU(φ1(A)φ2(B))VA\otimes B \mapsto U(\varphi_1(A) \otimes \varphi_2(B))V, where φi(X)\varphi_i(X) is either the identity map XXX \mapsto X or the transposition map XXtX \mapsto X^t. The results are extended to tensor space Mn1...MnmM_{n_1} \otimes ... \otimes M_{n_m} of higher level. The connection of the problem to quantum information science is mentioned.Comment: 13 page

    Characterizations of inverse M-matrices with special zero patterns

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    AbstractIn this paper, we provide some characterizations of inverse M-matrices with special zero patterns. In particular, we give necessary and sufficient conditions for k-diagonal matrices and symmetric k-diagonal matrices to be inverse M-matrices. In addition, results for triadic matrices, tridiagonal matrices and symmetric 5-diagonal matrices are presented as corollaries

    Maximal noiseless code rates for collective rotation channels on qudits

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    We study noiseless subsystems on collective rotation channels of qudits, i.e., quantum channels with operators in the set E(d,n)={Un:USU(d)}.{\mathcal E}(d,n) = \{ U^{\otimes n}: U \in {\mathrm{SU}}(d)\}. This is done by analyzing the decomposition of the algebra A(d,n){\mathcal A}(d,n) generated by E(d,n){\mathcal E}(d,n). We summarize the results for the channels on qubits (d=2d=2), and obtain the maximum dimension of the noiseless subsystem that can be used as the quantum error correction code for the channel. Then we extend our results to general dd. In particular, it is shown that the code rate, i.e., the number of protected qudits over the number of physical qudits, always approaches 1 for a suitable noiseless subsystem. Moreover, one can determine the maximum dimension of the noiseless subsystem by solving a non-trivial discrete optimization problem. The maximum dimension of the noiseless subsystem for d=3d = 3 (qutrits) is explicitly determined by a combination of mathematical analysis and the symbolic software Mathematica.Comment: 16 pages, proofs are put in Appendix for clearer presentation. Title has been changed and some related materials, such as quantum secret sharing and erasure errors, are mentione
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