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71.
A. K. Chernyshov S. P. Kotova V. L. Velichanskii 《Journal of Russian Laser Research》2002,23(2):132-147
It is shown that the type of lateral waveguide of a laser diode cannot be determined uniquely based on just the measured magnitude of astigmatism. For a unique determination, the K-factor of Petermann, which characterizes the wavefront curvature at the laser output facet, must be measured as well. In order to determine the type of lateral waveguide, a setup for measuring astigmatic distances in the range 0–200 m with an error of ±2 m and a K-factor with an error of 20% was developed. Operational features of the setup were analyzed, and a technique that allows one to minimize the effect of beam ellipticity on the measurement results was found. Using the technique, the optimization of spatial matching of a laser diode with a ring interferometer of the butterfly type was accomplished. For transformation of the astigmatic elliptical beam into the axially symmetric mode of the interferometer, we have used an optical system that consists of two cylindrical and one spherical lenses. The algorithm for designing the matching system was developed, and the 85% injection of radiation of a AlGaAs laser diode into the principal mode of a ring interferometer was experimentally demonstrated. 相似文献
72.
A sharp almost sure bound is derived for limit points of average sum of weakly dependent random variables, which ensures strong laws of large numbers for and -mixing random variables, without assumptions on rate of tending to zero of and -mixing parameters n and n. 相似文献
73.
程业斌 《高校应用数学学报(A辑)》1999,14(2):169-177
本文研究异方差回归模型Yi^(n)=g(xi^(n))+εi^(n),i=1,…,n,其中g是右实函数,xi^(n)是非随机设计点列,εi^(n)是随机误差,文中定义了一类g(x)的近邻型估计gn(x)=(n)∑(i=1)Wm(x)Yi^(n),得到了r阶平均相全和渐近正态性,特别,在(∞)∑(n=1)(n)∑(i=1)E/εi^(n)/^s/(ni)^s/r〈∞,maxE(1≤i≤n)/εi(^ 相似文献
74.
G. Oniani 《Georgian Mathematical Journal》1999,6(2):149-168
For the frame in n, let B2()()( n) be a family of all n-dimensional rectangles containing x and having edges parallel to the straight lines of , and let MB
2() be a maximal operator corresponding to B
2(). The main result of the paper is the following
Theorem.
For any function fL(1+1n+
L)(
n
) (n2) there exists a measure preserving and invertible mapping
n
n
such that
.This theorem gives a general solution of M. de Guzmán's problem that was previously studied by various authors. 相似文献
(1) |
1\} } M_{B_2 (\theta )} (fo\omega ) < \infty .$$ " align="middle" vspace="20%" border="0"> | (2) |
75.
This paper reviews a microscopic model of basic electron-hole pair excitation processes in strongly confined semiconductor quantum dots (QD) and their influence on the optical QD properties. The effects of valence band mixing, Coulomb interaction, and surface polarization are taken into account. The exciton and biexciton wave functions and energies are obtained using a numerical diagonalization method. The computed optical spectra, such as absorption, gain, pump-probe, and two-photon absorption, agree well with experiments. 相似文献
76.
The phenomenon of elliptical polarization of the linearly polarized radiation reflected near the Brewster angle by the leaves of plants has been investigated. It has been shown that the appearance of ellipticity is associated with the complex structure of the cuticle.__________Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 72, No. 2, pp. 236–240, March–April, 2005. 相似文献
77.
Velan SS 《Journal of magnetic resonance (San Diego, Calif. : 1997)》2004,171(2):40-352
Longitudinal multispin orders provide an effective way for measurement of scalar couplings and also to probe molecular interactions and dynamics. Analysis of longitudinal orders has been made in strongly coupled AB and ABX spin systems to determine the dependence of strong coupling parameter on these orders. Experimental and simulated spectra of various longitudinal orders are illustrated for these spin systems. This general procedure can be extended to broad range of spin systems to understand the influence of strong coupling on longitudinal orders. 相似文献
78.
Fordyce A. Davidson Bryan P. Rynne 《Journal of Mathematical Analysis and Applications》2004,300(2):491-504
Let TR be a time-scale, with a=infT, b=supT. We consider the nonlinear boundary value problem (2) (4)
u(a)=u(b)=0,