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911.
尚小明  汤国庆  张桂兰  陈文驹 《光学学报》1996,16(10):1371-1378
报道了以N2激光为泵浦光源,获得激发态分子内质子转移(ESIPT)分子HBO的激光输出现象。其激光转换效率约为17%,调谐范围为495~540nm,最强的输出波长在510nm。以HBO的激发态分子内质子转移的光物理和光化学过程为基础,建立了HBO产生激光的动态模型,数值模拟了在宽带和窄带情况下激光输出的光谱特性和时间特性,理论计算值与实验观测值很好相符,同时证实了激发态分子内质子转移分子的激光脉冲宽度依赖于激发态分子内质子转移分子的酮式异构体的基态S′0的寿命  相似文献   
912.
NovelAlDigitalSchemeforOpenLoopFiberOpticGyroscopesYANGYuanhong(The5thResearchDivisionofBeijingUniversityofAeronauts&Astronau...  相似文献   
913.
Summary. The dimensional reduction method for solving boundary value problems of Helmholtz's equation in domain by replacing them with systems of equations in dimensional space are investigated. It is proved that the existence and uniqueness for the exact solution and the dimensionally reduced solution of the boundary value problem if the input data on the faces are in some class of functions. In addition, the difference between and in is estimated as and are fixed. Finally, some numerical experiments in a domain are given in order to compare theretical results. Received April 2, 1996 / Revised version received July 30, 1990  相似文献   
914.
915.
916.
An evolutionary method for optimization of plate buckling resistance   总被引:9,自引:0,他引:9  
Optimization of plate buckling resistance is very complicated, because the in-plane stress resultants in the prebuckled state of a plate are functions of thickness distribution. This paper discusses the problem of finding the optimum thickness distribution of isotropic plate structures, with a given volume and layout, that would maximise the buckling load. A simple numerical method using the finite-element analysis is presented to obtain the optimum thickness distribution. Optimum designs of compression-loaded rectangular plates with different boundary conditions and plate aspect ratios are obtained by using the proposed method. Optimum designs from earlier studies and the methods of buckling analysis used to attain these results are discussed and compared with the designs from the proposed method. This paper also examines the reliability of the optimality criterion generally used for plate buckling optimization, which is based on the uniform strain energy density.  相似文献   
917.
We study the large-time behavior and rate of convergence to the invariant measures of the processes dX (t)=b(X) (t)) dt + (X (t)) dB(t). A crucial constant appears naturally in our study. Heuristically, when the time is of the order exp( – )/2 , the transition density has a good lower bound and when the process has run for about exp( – )/2, it is very close to the invariant measure. LetL =(2/2) – U · be a second-order differential operator on d. Under suitable conditions,L z has the discrete spectrum
- \lambda _2^\varepsilon ...and lim \varepsilon ^2 log \lambda _2^\varepsilon = - \Lambda \hfill \\ \varepsilon \to 0 \hfill \\ \end{gathered} $$ " align="middle" vspace="20%" border="0">  相似文献   
918.
Summary In the present work we extent the results in [RS] on CHIP, i.e. Cardinal Hermite Interpolation by the span of translates of directional derivatives of a box spline. These directional derivatives are that ones which define the type of the Hermite Interpolation. We admit here several (linearly independent) directions with multiplicities instead of one direction as in [RS]. Under the same assumptions on the smoothness of the box spline and its defining matrixT we can prove as in [RS]: CHIP has a system of fundamental solutions which are inL L 2 together with its directional derivatives mentioned above. Moreover, for data sequences inl p ( d ), 1p2, there is a spline function inL p, 1/p+1/p=1, which solves CHIP.Research supported in part by NSERC Canada under Grant # A7687. This research was completed while this author was supported by a grant from the Deutscher Akademischer Austauschdienst  相似文献   
919.
In this paper, assuming a certain set-theoretic hypothesis, a positive answer is given to a question of H. Kraljevi, namely it is shown that there exists a Lebesgue measurable subsetA of the real line such that the set {c R: A + cA contains an interval} is nonmeasurable. Here the setA + cA = {a + ca: a, a A}. Two other results about sets of the formA + cA are presented.  相似文献   
920.
IfK is a field of characteristic 0 then the following is shown. Iff, g, h: M n (K) K are non-constant solutions of the Binet—Pexider functional equation
  相似文献   
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