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利用光线追迹法和四阶龙格-库塔法分析了光参量啁啾脉冲放大系统中实际展宽器和压缩器所带来的各阶色散,并将其代入放大过程数值模拟了脉冲变化的情况,讨论了压缩器光栅对表面不平行、刻线不平行、信号光强度、泵浦光强度等因素对输出脉冲宽度和时间波形的影响。结果表明,光栅对表面不平行将引起脉冲宽度变大,且光栅顺时针旋转对脉冲宽度和波形影响更大。而光栅刻线不平行时,当仅考虑二阶色散时,夹角为0.8°时脉宽最小,考虑到三阶色散时,夹角为1°脉宽最小,且光栅顺时针和逆时针旋转对脉冲的作用相同。对实际OPCPA系统,当放大晶体材料及长度一定时,尽量调整压缩器光栅平行,信号光强度和泵浦光强度有一最佳值能使输出脉冲宽度达到最小。 相似文献
54.
提出一种实现简并光学参量振荡器混沌反控制的方法,用正弦信号调制简并光学参量振荡器的基模衰减率,使简并光学参量振荡器从定态输出转化为混沌态.数值模拟结果表明,选择不同的调制幅度和调制角频率,只要满足系统的最大李雅谱诺夫指数大于零,即可实现不同的混沌轨道重构.通过比较最大李雅谱诺夫指数λmax随调制幅度和调制角频率变化曲线, 指出系统从周期态调制到混沌态比从无亚谐波输出的定态调制到混沌态更容易,有更宽的调制幅度和调制角频率选择范围.
关键词:
简并光学参量振荡器
混沌反控制
调制 相似文献
55.
E. Lazzaro R. Coelho 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,19(1):97-101
A major limit to steady state and advanced high operation of tokamaks of reactor class is due to the onset of tearing modes that develop magnetic and may cause loss of energy confinement or a major disruption. Here the structure of a classical problem
about the effects of external control helical fields is analysed and it is shown to offer a general paradigm of response of
low order classical and neoclassical tearing modes to a wide class of external perturbations. New results of principle on
the structural stability of the response model are obtained, leading to a clear interpretation of the role of “seed islands"
in the onset of neo-classical tearing modes and the role of finite ion larmor radius corrections to Ohm's law.
Received 12 November 2001 and Received in final form 4 January 2002 相似文献
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R. Fedele H. Schamel 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,27(3):313-320
An investigation to deepen the connection between the family of nonlinear Schr?dinger equations and the one of Korteweg-de
Vries equations is carried out within the context of the Madelung's fluid picture. In particular, under suitable hypothesis
for the current velocity, it is proven that the cubic nonlinear Schr?dinger equation, whose solution is a complex wave function,
can be put in correspondence with the standard Korteweg-de Vries equation, is such a way that the soliton solutions of the
latter are the squared modulus of the envelope soliton solution of the former. Under suitable physical hypothesis for the
current velocity, this correspondence allows us to find envelope soliton solutions of the cubic nonlinear Schr?dinger equation,
starting from the soliton solutions of the associated Korteweg-de Vries equation. In particular, in the case of constant current
velocities, the solitary waves have the amplitude independent of the envelope velocity (which coincides with the constant
current velocity). They are bright or dark envelope solitons and have a phase linearly depending both on space and on time coordinates. In the case of an arbitrarily
large stationary-profile perturbation of the current velocity, envelope solitons are grey or dark and they relate the velocity u0 with the amplitude; in fact, they exist for a limited range of velocities and have a phase nonlinearly depending on the combined
variable x-u0 s (s being a time-like variable). This novel method in solving the nonlinear Schr?dinger equation starting from the Korteweg-de
Vries equation give new insights and represents an alternative key of reading of the dark/grey envelope solitons based on the fluid language. Moreover, a comparison between the solutions found in the
present paper and the ones already known in literature is also presented.
Received 20 February 2002 and Received in final form 22 April 2002 Published online 6 June 2002 相似文献
59.
We study time dependence of various measures of entanglement (covariance entanglement coefficient, purity entanglement coefficient, normalized distance coefficient, entropy coefficients) between resonantly coupled modes of the electromagnetic field in ideal cavities with oscillating boundaries. Two types of cavities are considered — a three-dimensional cavity possessing eigenfrequencies 3 = 31, whose wall oscillates at the frequency w = 21, and a one-dimensional (Fabry–Perot) cavity with an equidistant spectrum n = n1 where the distance between perfect mirrors oscillates at the frequencies 1 and 21. The behavior of entanglement measures in these cases turns out to be completely different, although all three coefficients demonstrate qualitatively similar time dependences in each case (except some specific situations where the covariance entanglement coefficient based on traces of covariance submatrices seems to be essentially more sensitive to entanglement than other measures, which are based on determinants of covariance submatrices). Different initial states of the field, namely, vacuum, squeezed vacuum, thermal, Fock, and even/odd coherent states, are considered. 相似文献
60.
本文报道了AgGaS_2晶体Ⅱ类非共线相位匹配Q开关Nd:YAG激光泵浦CO_2激光参量上转换研究结果,用迭代法计算了相位失配因子△K=0时的最佳非共线夹角.当泵浦功率密度为6MW/cm~2和晶体长度为4.7mm时,功率转换效率达16.1%,并且首次采用硅雪崩光电二极管接收和频信号. 相似文献