Zhou Fu-zhao;Zhao Ren-ke.Least-square Solutions of Inverse Problem for Anti-symmetric and Ortho-antisymmetric Matirices.Journal of Hei long-jiang University.2004.79-84ZHOU Fu-zhao,ZHAO Ren-ke.Least-square solution of inverse problems for anti-symmetric ortho-antisymmetric matrices. Journal of ...
15a, illustrating an inversely customized metamaterial device [287], attached on the surface of a plate under inspection, to achieve high-efficiency antisymmetric-to-symmetric mode conversion, since the latter is more conducive to the generation of the cumulative second harmonics, used as the damage...
A feedback loop-based numerical optimi- zation algorithm is used to define the required states of the matrix elements automatically. Different linear optical devices have been proposed and realized using this method25–28. However, nonlinear phenomena, e.g., the dependence of the wavelength on ...
A feedback loop-based numerical optimi- zation algorithm is used to define the required states of the matrix elements automatically. Different linear optical devices have been proposed and realized using this method25–28. However, nonlinear phenomena, e.g., the dependence of the wavelength on ...
The mass matrix of the sneutrinos written in each 3\times 3 block is given by \begin{aligned} (M_{\tilde{\nu }})_{{\tilde{\nu }}_+ {\tilde{\nu }}_+}&= \frac{1}{2}I_3 M_z^2 \cos 2\beta + \frac{1}{2}\left( \tilde{m}_L^2 + \tilde{m}_L^{2T}\right) \no...
= diag( M11, A√simple M22, √paMra3m3)etemrˆiνzUatPi†oMnNSof[9m8D], which is completely different from the total antisymmetric m D given in Ref. [√76]. The ISS condition |mˆ ν| |m D| M0 gives μX mˆ ν M0 0. Then we have |μX | Mˆ N = Mˆ R O3...
In this paper, a class of constrained inverse eigenproblern and associated approximation problem for skew symmetric and centrosymmetric matrices are essentially decomposed into the same kind subproblems for real antisymmetric matrices with smaller dimensions. We present the general solution of the ...
We consider the multidimensional nonrelativistic Newton equation in a static electromagnetic field where V ∈ C 2(, ), B(x) is the n × n real antisymmetric matrix with elements Bi,k(x), Bi,k ∈ C 1(, ) (and B satisfies the closure condition), and ≤β |j 1|(1 + |x|)–(α...
We consider the multidimensional Newton-Einstein equation in static electromagnetic field p = F(x, x), F(x, x) = -▽V(x) + c/1B(x)x, where V ∈ C~2 (R~d , R), B(x) is the d x d real antisymmetric matrix with elements B_(i,k)(x) = ex/eAk(x) -ex_k/eA_i(x)...
2) matrix iteration 矩阵迭代法 1. In the paper, the effects of the selection of the initial vector and the controlling condition of the iterating cycles in the matrix iteration method are inquired into. 矩阵迭代法是求矩阵的第一阶特征值与特征向量的一种数值方法 。3) antisymmetric iterative ...