223 research outputs found

    The necessary and sufficient conditions of copositive tensors

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    In this paper, it is proved that (strict) copositivity of a symmetric tensor A\mathcal{A} is equivalent to the fact that every principal sub-tensor of A\mathcal{A} has no a (non-positive) negative H++H^{++}-eigenvalue. The necessary and sufficient conditions are also given in terms of the Z++Z^{++}-eigenvalue of the principal sub-tensor of the given tensor. This presents a method of testing (strict) copositivity of a symmetric tensor by means of the lower dimensional tensors. Also the equivalent definition of strictly copositive tensors is given on entire space Rn\mathbb{R}^n.Comment: 13 pages. arXiv admin note: text overlap with arXiv:1302.608

    Infinite and finite dimensional Hilbert tensors

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    For an mm-order nn-dimensional Hilbert tensor (hypermatrix) Hn=(Hi1i2im)\mathcal{H}_n=(\mathcal{H}_{i_1i_2\cdots i_m}), Hi1i2im=1i1+i2++imm+1, i1,,im=1,2,,n\mathcal{H}_{i_1i_2\cdots i_m}=\frac1{i_1+i_2+\cdots+i_m-m+1},\ i_1,\cdots, i_m=1,2,\cdots,n its spectral radius is not larger than nm1sinπnn^{m-1}\sin\frac{\pi}{n}, and an upper bound of its EE-spectral radius is nm2sinπnn^{\frac{m}2}\sin\frac{\pi}{n}. Moreover, its spectral radius is strictly increasing and its EE-spectral radius is nondecreasing with respect to the dimension nn. When the order is even, both infinite and finite dimensional Hilbert tensors are positive definite. We also show that the mm-order infinite dimensional Hilbert tensor (hypermatrix) H=(Hi1i2im)\mathcal{H}_\infty=(\mathcal{H}_{i_1i_2\cdots i_m}) defines a bounded and positively (m1)(m-1)-homogeneous operator from l1l^1 into lpl^p (1<p<1<p<\infty), and the norm of corresponding positively homogeneous operator is smaller than or equal to π6\frac{\pi}{\sqrt6}

    Tensor Complementarity Problem and Semi-positive Tensors

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    The tensor complementarity problem (\q, \mathcal{A}) is to \mbox{ find } \x \in \mathbb{R}^n\mbox{ such that }\x \geq \0, \q + \mathcal{A}\x^{m-1} \geq \0, \mbox{ and }\x^\top (\q + \mathcal{A}\x^{m-1}) = 0. We prove that a real tensor A\mathcal{A} is a (strictly) semi-positive tensor if and only if the tensor complementarity problem (\q, \mathcal{A}) has a unique solution for \q>\0 (\q\geq\0), and a symmetric real tensor is a (strictly) semi-positive tensor if and only if it is (strictly) copositive. That is, for a strictly copositive symmetric tensor A\mathcal{A}, the tensor complementarity problem (\q, \mathcal{A}) has a solution for all \q \in \mathbb{R}^n

    Properties of Some Classes of Structured Tensors

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    In this paper, we extend some classes of structured matrices to higher order tensors. We discuss their relationships with positive semi-definite tensors and some other structured tensors. We show that every principal sub-tensor of such a structured tensor is still a structured tensor in the same class, with a lower dimension. The potential links of such structured tensors with optimization, nonlinear equations, nonlinear complementarity problems, variational inequalities and the nonnegative tensor theory are also discussed.Comment: arXiv admin note: text overlap with arXiv:1405.1288 by other author
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