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71.
Theoretically, the solution of all linear ordinary differential equation problems, whether initial-value or two-point boundary-value problems, can be expressed in terms of the fundamental matrix. The examination of well-known two-point boundary-value methods discloses, however, the absence of the fundamental matrix in the development of the techniques and in their applications. This paper reveals that the fundamental matrix is indeed present in these techniques, although its presence is latent and appears in various guises. 相似文献
72.
A one-sweep method for the numerical solution of finite-element equations is presented. This procedure is especially efficient in computing time and storage when the solution is required at only a few nodes of the finite-element mesh. Furthermore, the method is particularly useful in dealing with problems on infinite or semi-infinite domains. Artificial boundaries must be introduced in such cases, and the one-sweep method affords an extremely efficient algorithm by which the dependence of the solution on the location of these boundaries can be assessed. An application of the method to the vibration of a half-submerged circular cylinder in a heavy fluid is presented.The second author wishes to express his thanks to Professor J. L. Sackman for reviewing this work.(deceased). 相似文献
73.
74.
In this paper, we discuss an approximate method for the numerical integration of a class of linear, singularly perturbed two-point boundary-value problems in ordinary differential equations with a boundary layer on the left end of the underlying interval. This method requires a minimum of problem preparation and can be implemented easily on a computer. We replace the original singular perturbation problem by an approximate first-order differential equation with a small deviating argument. Then, we use the trapezoidal formula to obtain the three-term recurrence relationship. Discrete invariant imbedding algorithm is used to solve a tridiagonal algebraic system. The stability of this algorithm is investigated. The proposed method is iterative on the deviating argument. Several numerical experiments have been included to demonstrate the efficiency of the method.The authors wish to express their sincere thanks to Dr. S. M. Roberts for his comments and valuable suggestions. 相似文献
75.
76.
James C. Fu 《Annals of the Institute of Statistical Mathematics》1995,47(3):435-446
Traditionally the distributions of the number of patterns and successions in a random permutation ofn integers 1,2, ..., andn were studied by combinatorial analysis. In this short article, a simple way based on finite Markov chain imbedding technique is used to obtain the exact distribution of successions on a permutation. This approach also gives a direct proof that the limiting distribution of successions is a Poisson distribution with parameter =1. Furthermore, a direct application of the main result, it also yields the waiting time distribution of a succession.This work was supported in part by the Natural Sciences and Engineering Research Council of Canada under Grant NSERC A-9216, and National Science Council of Republic of China under Grant 85-2121-M-259-003. 相似文献
77.
78.
Anatoliy K. Prykarpatsky Nikolai N. BogoliubovJr. Jolanta Golenia Ufuk Taneri 《International Journal of Theoretical Physics》2008,47(11):2882-2897
Introductive backgrounds to a new mathematical physics discipline—Quantum Mathematics—are discussed and analyzed both from
historical and from analytical points of view. The magic properties of the second quantization method, invented by V. Fock
in 1932, are demonstrated, and an impressive application to the nonlinear dynamical systems theory is considered.
The Authors devote their article to their Friend and Teacher academician Prof. Anatoliy M. Samoilenko on occasion of his 70
years-Birthday with great compliments and gratitude to his brilliant talent and impressive impact to modern theory of nonlinear
dynamical systems of mathematical physics and nonlinear analysis 相似文献
79.
It is now well known that in the extreme quantum limit, dominated by the elastic impurity scattering and the concomitant quantum
interference, the zero-temperature d.c. resistance of a strictly one-dimensional disordered system is non-additive and non-self-averaging.
While these statistical fluctuations may persist in the case of a physically thin wire, they are implicitly and questionably
ignored in higher dimensions. In this work, we have re-examined this question. Following an invariant imbedding formulation,
we first derive a stochastic differential equation for the complex amplitude reflection coefficient and hence obtain a Fokker-Planck
equation for the full probability distribution of resistance for a one-dimensional continuum with a gaussian white-noise random
potential. We then employ the Migdal-Kadanoff type bond moving procedure and derive thed-dimensional generalization of the above probability distribution, or rather the associated cumulant function—‘the free energy’.
Ford=3, our analysis shows that the dispersion dominates the mobility edge phenomena in that (i) a one-parameterβ-function depending on the mean conductance only does not exist, (ii) one has a line of fixed-points in the space of the first
two cumulants of conductance, (iii) an approximate treatment gives a diffusion-correction involving the second cumulant. It
is, however, not clear whether the fluctuations can render the transition at the mobility edge ‘first-order’. We also report
some analytical results for the case of the one-dimensional system in the presence of a finite electric field. We find a cross-over
from the exponential to the power-law length dependence of resistance as the field increases from zero. Also, the distribution
of resistance saturates asymptotically to a Poissonian form. Most of our analytical results are supported by the recent numerical
simulation work reported by some authors.
The author felicitates Prof. D S Kothari on his eightieth birthday and dedicates this paper to him on this occasion. 相似文献
80.
We consider the distribution of the number of successes in success runs of length at least k in a binary sequence. One important application of this statistic is in the detection of tandem repeats among DNA sequence
segments. In the literature, its distribution has been computed for independent sequences and Markovian sequences of order
one. We extend these results to Markovian sequences of a general order. We also show that the statistic can be represented
as a function of the number of overlapping success runs of lengths k and k + 1 in the sequence, and give immediate consequences of this representation.
AMS 2000 Subject Classification 60E05, 60J05 相似文献