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121.
A. F. Sidorenko 《Random Structures and Algorithms》1991,2(1):73-99
The “best” inequalities of type P{(ζ, η)? E} ≧f(P{η? D1}P{η?Dm}) for independent and identically distributed random elements ζ and η can be reduced to Turán-type problems for graphs with colored vertices. In the present work we describe a finite algorithm for obtaining the asymptotical solution for an arbitrary problem of such type. In the case of two colors we obtain the final form of asymptotic solution without using the algorithm. 相似文献
122.
123.
Alexey V. VarlamovFedor I. Zubkov Ekaterina V. BoltukhinaNatalya V. Sidorenko Roman S. Borisov 《Tetrahedron letters》2003,44(18):3641-3643
An efficient two-step synthesis of new isoindolo[2,1-a]quinoline-10-carboxylic acids via [4+2] cycloaddition of the 4-α-furyl-4-N-arylaminobut-1-enes and maleic anhydride is described. 相似文献
124.
Yu. A. Babanov A. V. Ryazhkin A. F. Sidorenko L. A. Blaginina 《Journal of Structural Chemistry》1998,39(6):833-838
The problem of correcting EXAFS spectra by the core level width is discussed. A method of correcting experimental EXAFS spectra
is developed. An iteration algorithm for solving the integral equation is proposed. This method has a number of advantages
over other methods, namely, high stability against statistical error and fast convergence. Model numerical calculations are
performed. An example is the EXAFS spectrum of polycrystalline Pd for which the broadening effect is significant.
Translated fromZhumal Struktumoi Khimii, Vol. 39, No. 6, pp. 1018–1024, November–December, 1998. 相似文献
125.
A theory of μSR method is developed for uniaxial anisotropic high-T
c superconductors. In two extreme cases ofH
ext‖c
andH
ext⊥c
analytical formulas are obtained which makes it possible to determine from the position of van Hove singularities in the
Fourier-spectrum of muonium polarization, the type and parameters of the vortex lattice, such as λ
ab
(λ
c
). In caseH
ext≲H
c2 we obtained the shape of the Fourier-spectrum in analytical form and the simple method of determining the Ginsburg-Landau
parameter κ.
Convenient expressions for numerical calculations are obtained for the arbitrary orientation of the external field, and an
algorithm is provided to compute the mean fieldB, the vortex lattice parameters and the bulk field distribution in anisotropic superconductor. The Fourier spectrum of polarization
based on these calculations can be used to independently check the validity of the high-T
c parameters determination for “appropriate” orientations. 相似文献
126.
Alexander Sidorenko 《Graphs and Combinatorics》1995,11(2):179-199
The numbers which are traditionally named in honor of Paul Turán were introduced by him as a generalization of a problem he solved in 1941. The general problem of Turán having anextremely simple formulation but beingextremely hard to solve, has become one of the most fascinatingextremal problems in combinatorics. We describe the present situation and list conjectures which are not so hopeless. 相似文献
127.
V. A. Belyakov A. A. Konakov N. V. Kurova K. V. Sidorenko V. A. Burdov 《Bulletin of the Russian Academy of Sciences: Physics》2011,75(8):1070-1072
It is found that the radiative recombination rate rises when silicon nanocrystals are doped with donors. This rise turns out
to be stronger when a nanocrystal surface contains abundant defects capable of capturing electrons emitted by donors. 相似文献
128.
129.
I. V. Ukrainets R. G. Red’kin L. V. Sidorenko A. V. Turov 《Chemistry of Heterocyclic Compounds》2009,45(12):1478-1484
A three-component condensation of 1-allyl-4-hydroxy-2-oxo-1,2-dihydroquinoline, isatin, and malononitrile gave a satisfactory
yield of 4,3'-spiro[(6-allyl-2-amino-5-oxo-5,6-dihydro-4H-pyrano-[3,2-c]quinoline-3-carbonitrile)-2'-oxindole], which structure
was confirmed by X-ray analysis. 相似文献
130.
For the equation K(t)u
xx
+ u
tt
− b
2
K(t)u = 0 in the rectangular domain D = “(x, t)‖ 0 < x < 1, −α < t < β”, where K(t) = (sgnt)|t|
m
, m > 0, and b > 0, α > 0, and β > 0 are given real numbers, we use the spectral method to obtain necessary and sufficient conditions for the unique solvability
of the boundary value problem u(0, t) = u(1, t), u
x
(0, t) = u
x
(1, t), −α ≤ t ≤ β, u(x, β) = φ(x), u(x,−α) = ψ(x), 0 ≤ x ≤ 1. 相似文献