第 2 図 X 2. X 線応力計測法について q ( a ) X 線回折モデル q X X X X Bragg 第 3 図 Bragg X X q X ( E ) ( v ) X 2 5 mm X (1) (2) (3) (4) 計測可能領域表面表面下, 断面 ( b ) 無負荷 (5) (6)

Assume that F maps positive definite matrices either into positive definite matrices or into negative definite matrices, the general nonlinear matrix equation X A ∗ FXA Q was

Then by applying specialization maps of admissible fundamental groups and Nakajima’s result concerning ordinariness of cyclic ´ etale coverings of generic curves, we may prove that

In this section, we establish a purity theorem for Zariski and etale weight-two motivic cohomology, generalizing results of [23]... In the general case, we dene the

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We provide an accurate upper bound of the maximum number of limit cycles that this class of systems can have bifurcating from the periodic orbits of the linear center ˙ x = y, y ˙ =

In the second section, we study the continuity of the functions f p (for the definition of this function see the abstract) when (X, f ) is a dynamical system in which X is a

More general problem of evaluation of higher derivatives of Bessel and Macdonald functions of arbitrary order has been solved by Brychkov in [7].. However, much more

Algebraic curvature tensor satisfying the condition of type (1.2) If ∇J ̸= 0, the anti-K¨ ahler condition (1.2) does not hold.. Yet, for any almost anti-Hermitian manifold there