全文获取类型
收费全文 | 8146篇 |
免费 | 368篇 |
国内免费 | 661篇 |
专业分类
化学 | 758篇 |
晶体学 | 7篇 |
力学 | 373篇 |
综合类 | 55篇 |
数学 | 6852篇 |
物理学 | 1130篇 |
出版年
2023年 | 81篇 |
2022年 | 74篇 |
2021年 | 91篇 |
2020年 | 154篇 |
2019年 | 168篇 |
2018年 | 194篇 |
2017年 | 197篇 |
2016年 | 228篇 |
2015年 | 149篇 |
2014年 | 319篇 |
2013年 | 554篇 |
2012年 | 332篇 |
2011年 | 342篇 |
2010年 | 329篇 |
2009年 | 500篇 |
2008年 | 586篇 |
2007年 | 530篇 |
2006年 | 484篇 |
2005年 | 427篇 |
2004年 | 303篇 |
2003年 | 378篇 |
2002年 | 339篇 |
2001年 | 249篇 |
2000年 | 261篇 |
1999年 | 264篇 |
1998年 | 213篇 |
1997年 | 233篇 |
1996年 | 125篇 |
1995年 | 120篇 |
1994年 | 100篇 |
1993年 | 70篇 |
1992年 | 58篇 |
1991年 | 60篇 |
1990年 | 66篇 |
1989年 | 50篇 |
1988年 | 53篇 |
1987年 | 39篇 |
1986年 | 38篇 |
1985年 | 50篇 |
1984年 | 56篇 |
1983年 | 18篇 |
1982年 | 36篇 |
1981年 | 32篇 |
1980年 | 33篇 |
1979年 | 26篇 |
1978年 | 31篇 |
1977年 | 38篇 |
1976年 | 25篇 |
1974年 | 16篇 |
1973年 | 16篇 |
排序方式: 共有9175条查询结果,搜索用时 0 毫秒
51.
对经典一维受迫谐振子量子化,求解量子化后体系的时间演化算符.应用相空间准概率分布函数,研究了体系的量子特性.研究结果表明,初始为真空态,经过时间演化,系统波函数是一个二维高斯波包;波包中心的振幅和相位受到作用力的调制,成为调幅、调相波,波包中心的运动与经典受迫谐振子的运动形式相同. 相似文献
52.
本文利用提取直射波并结合自适应数字滤波等技术提出一种计算水平层状介质中电磁场并矢Green函数的快速算法. 首先将谱域Green函数中表征均匀介质作用的直射波提取出来并对其积分进行解析计算,这种处理降低了谱域Green函数的奇异性,可在很大程度上缩短其积分收敛区间. 然后在将谱域Green函数剩余部分对应积分转化为三个快速下降积分的基础上,引入一种自适应数字滤波算法对其进行快速求解. 最后通过具体算例验证了本文所述算法的有效性.
关键词:
并矢Green函数
快速算法
水平层状介质 相似文献
53.
We associate a family of Hilbert spaces H
q
2;(D) of analytic functions on the unit disk D=z
:|z|<1 the q-continuous Gegenbauer polynomials C
n
(x;q) on the interval]–1;1[ and give a q-analogue of the unitary integral transform that Watanabe constructed from the Hilbert space L
2(]–1;1[;(1–x
2)–
dx onto the weighted Hilbert space H
2;(D). 相似文献
54.
Oleg Lisovyy 《Letters in Mathematical Physics》2006,77(1):63-81
We introduce and study a family of quantum fields, associated to δ-interactions in one dimension. These fields are analogous to holonomic quantum fields of Sato et al. in Holonomic quantum fields I–V (Publ. RIMS, Kyoto University, 14: 223–267, 1978; 15: 201–278, 1979; 15: 577–629, 1979; 15: 871-972, 1979; 16: 531–584, 1979). Corresponding field operators belong to an infinite-dimensional representation of the group
in the Fock space of ordinary harmonic oscillator. We compute form factors of such fields and their correlation functions, which are related to the determinants of Schroedinger operators with a finite number of point interactions. It is also shown that these determinants coincide with tau functions, obtained through the trivialization of the det*-bundle over a Grassmannian associated to a family of Schroedinger operators. 相似文献
55.
Liping Liu Kevin B. Davies Michal Kří žek & Guan Li 《advances in applied mathematics and mechanics.》2011,3(2):131-140
In this paper we first prove a theorem on the
nonexistence of pyramidal polynomial basis functions. Then we
present a new symmetric composite pyramidal finite element which
yields a better convergence than the nonsymmetric one. It has
fourteen degrees of freedom and its basis functions are incomplete
piecewise triquadratic polynomials. The space of ansatz functions
contains all quadratic functions on each of four sub-tetrahedra that
form a given pyramidal element. 相似文献
56.
Usually, numerical self-consistent calculations predict a much larger intrinsic bistability region than actually is measured in resonant tunneling diodes (RTDs). In addition, numerical calculations have shown that scattering in the well reduces bistability. We used a unified treatment of current flowing from continuum states and emitter quasi-bound states to show numerically and analytically that not only the scattering in the quantum well but also the scattering in the emitter reduces bistability. Moreover, within the Hartree approximation, bistability occurs by tunneling resonantly between emitter quasi-bound state and well quasi-bound state as a pitchfork bifurcation. 相似文献
57.
Narendra Singh 《Optics & Laser Technology》2010,42(5):724-588
We propose a new method for multiple image encryption using linear canonical transforms and chaotic maps. Three linear canonical transforms and three chaotic maps are used in the proposed technique. The three linear canonical transforms that have been used are the fractional Fourier transform, the extended fractional Fourier transform and the Fresnel transform. The three chaotic maps that have been used are the tent map, the Kaplan-Yorke map and the Ikeda map. These chaotic maps are used to generate the random phase masks and these random phase masks are known as chaotic random phase masks. The mean square error and the signal to noise ratio have been calculated. Robustness of the proposed technique to blind decryption has been evaluated. Optical implementation of the technique has been proposed. Experimental and simulations results are presented to verify the validity of the proposed technique. 相似文献
58.
59.
Differential equations and maps are the most frequently studied examples of dynamical systems and may be considered as continuous
and discrete time-evolution processes respectively. The processes in which time evolution takes place on Cantor-like fractal
subsets of the real line may be termed as fractal-time dynamical systems. Formulation of these systems requires an appropriate
framework. A new calculus calledF
α-calculus, is a natural calculus on subsetsF⊂ R of dimension α,0 < α ≤ 1. It involves integral and derivative of order α, calledF
α-integral andF
α-derivative respectively. TheF
α-integral is suitable for integrating functions with fractal support of dimension α, while theF
α-derivative enables us to differentiate functions like the Cantor staircase. The functions like the Cantor staircase function
occur naturally as solutions ofF
α-differential equations. Hence the latter can be used to model fractal-time processes or sublinear dynamical systems.
We discuss construction and solutions of some fractal differential equations of the form
whereh is a vector field andD
F,t
α
is a fractal differential operator of order α in timet. We also consider some equations of the form
whereL is an ordinary differential operator in the real variablex, and(t,x) ∈F × Rn whereF is a Cantor-like set of dimension α.
Further, we discuss a method of finding solutions toF
α-differential equations: They can be mapped to ordinary differential equations, and the solutions of the latter can be transformed
back to get those of the former. This is illustrated with a couple of examples. 相似文献
60.