矩阵的稀释和特性

IF 0.8 Q2 MATHEMATICS Advances in Operator Theory Pub Date : 2024-06-21 DOI:10.1007/s43036-024-00360-7
Anju Rani, Yogesh Kapil, Bhavna Garg, Mandeep Singh
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引用次数: 0

摘要

让 A, B 是任意两个正定矩阵,Y 是任意一个矩阵。矩阵 \(M_Y(A,B)=\left[ \begin{array}{cc}A &{}A^{\frac{1}{2}}YB^{\frac{1}{2}}\\ B^{\frac{1}{2}}Y^{\star }A^{\frac{1}{2}} &{} B (end{array}\right] )。\)为 Y 的收缩矩阵、扩张矩阵或单元矩阵,实际上都是由矩阵/运算符手段产生的。我们的目标是建立 \(M_Y(A,B).\) 类型的两个矩阵之和的特征值的特征。我们通过 \({\mathcal {P}}_3(A)=\begin{bmatrix} 给出的扩张来描述任何 \(n\times n\) 矩阵 A。O &{}A &{}A^2\ A^* &{}O &{}A\ {A^*}^2 &{}A^* &{}O \end{bmatrix}\) 和 ( {\mathcal {M}}_3(A)=\begin{bmatrix}I &{}A &{}A^2\ A^* &{} I &{}A\ {A^*}^2 &{}A^* &{} I end{bmatrix},\) by means of inertia of dilations.
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Dilations and characterisations of matrices

Let AB be any two positive definite \(n\times n\) matrices and Y be any \(n\times n\) matrix. The matrices \(M_Y(A,B)=\left[ \begin{array}{cc} A &{} A^{\frac{1}{2}}YB^{\frac{1}{2}} \\ B^{\frac{1}{2}}Y^{\star }A^{\frac{1}{2}} &{} B \end{array}\right] \) for Y to be contractive, expansive or unitary matrix, are in fact arising from matrix/operator means. We aim to establish the signatures of the eigenvalues of the sum of two matrices of the type \(M_Y(A,B).\) We characterise any \(n\times n\) matrix A through its dilations given by \({\mathcal {P}}_3(A)=\begin{bmatrix} O &{} A &{} A^2\\ A^* &{} O &{} A\\ {A^*}^2 &{} A^* &{} O \end{bmatrix}\) and \({\mathcal {M}}_3(A)=\begin{bmatrix} I &{} A &{} A^2\\ A^* &{} I &{} A\\ {A^*}^2 &{} A^* &{} I \end{bmatrix},\) by means of inertia of dilations.

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CiteScore
1.60
自引率
0.00%
发文量
55
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