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901.
The cross sections for the production of nuclides of element 108 via
hot fusion evaporation reactions are studied using a two-parameter
Smoluchowski equation. The optimal reactions for the synthesis of
new nuclides of element 108 with mass numbers from 266 to 271 are
suggested. The macroscopic-microscopic approach predicts a strong
deformed shell closure at Z \approx 108 and N=162. The synthesis
of more nuclides of element 108 is meaningful to the confirmation of
the existence of this deformed shell closure. 相似文献
902.
903.
可调谐二极管激光吸收光谱法测量气体温度 总被引:2,自引:1,他引:2
研究了一种新型的非接触式测温技术——可调谐二极管激光吸收光谱(TDLAS)测温技术。介绍了温度测量及调制吸收光谱技术原理,分析了调制幅度对气体温度测量的影响。优选了氧气吸收谱线对13163.78 cm-1和13164.18 cm-1,在搭建的高温实验系统上,实现了气体温度和浓度的同时测量。通过分析实测波形获得了谱线13164.18 cm-1在823~1323 K温度范围内的碰撞展宽系数和温度指数。实验结果表明,在823~1323 K温度范围内,系统温度测量的线性误差为0.65%,最大波动为±15 K。 相似文献
904.
905.
Z.Q. Li D.X. Zhang X.H. Zhang Y.Q. Gao X.J. Liu E.Y. Jiang 《Physics letters. A》2007,370(5-6):512-516
The charge ordering characteristics in Y0.5Ca0.5MnO3 manganite, prepared by sol–gel process, have been investigated experimentally. It is found that the superlattice diffractions appear in the electron diffraction patterns recorded at low temperatures, while only basic Brag diffraction spots can be observed when temperature is higher than 300 K. This provides direct evidence for the existence of charge ordering in Y0.5Ca0.5MnO3. The magnetization and specific heat measurements indicate the charge ordering temperature of Y0.5Ca0.5MnO3 is 290 K, around which both the magnetization and specific heat reveal anomalous behaviors. We also observed that the MnO bond length changed remarkably and the effective number of carriers reduced prominently with decreasing temperature around charge ordering temperature through transform infrared spectra measurements. 相似文献
906.
J.-B. Liu J.-H. Li X.-Y. Lü A. Zheng 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,44(3):601-606
In this paper, we investigate the geometric phase of a composite system which is composed of two spin-
particles driven by a
time-varying magnetic field. Firstly, we consider the special case that only one subsystem driven by time-varying magnetic
field. Using the quantum jump
approach, we calculate the geometric phase associated with the adiabatic evolution of the system subjected to decoherence.
The results show that the lowest
order corrections to the phase in the no-jump trajectory is only quadratic in decoherence coefficient. Then, both subsystem
driven by time-varying magnetic
field is considered, we show that the geometric phase is related to the exchange-interaction coefficient and polar angle of
the magnetic field. 相似文献
907.
H.A. Michelsen F. Liu B.F. Kock H. Bladh A. Boiarciuc M. Charwath T. Dreier R. Hadef M. Hofmann J. Reimann S. Will P.-E. Bengtsson H. Bockhorn F. Foucher K.-P. Geigle C. Mounaïm-Rousselle C. Schulz R. Stirn B. Tribalet R. Suntz 《Applied physics. B, Lasers and optics》2007,87(3):503-521
We have performed a comparison of ten models that predict the temporal behavior of laser-induced incandescence (LII) of soot.
In this paper we present a summary of the models and comparisons of calculated temperatures, diameters, signals, and energy-balance
terms. The models were run assuming laser heating at 532 nm at fluences of 0.05 and 0.70 J/cm2 with a laser temporal profile provided. Calculations were performed for a single primary particle with a diameter of 30 nm
at an ambient temperature of 1800 K and a pressure of 1 bar. Preliminary calculations were performed with a fully constrained
model. The comparison of unconstrained models demonstrates a wide spread in calculated LII signals. Many of the differences
can be attributed to the values of a few important parameters, such as the refractive-index function E(m) and thermal and
mass accommodation coefficients. Constraining these parameters brings most of the models into much better agreement with each
other, particularly for the low-fluence case. Agreement among models is not as good for the high-fluence case, even when selected
parameters are constrained. The reason for greater variability in model results at high fluence appears to be related to solution
approaches to mass and heat loss by sublimation.
PACS 65.80.+n; 78.20.Nv; 42.62.-b; 44.05.+e 相似文献
908.
909.
A planar chiral nanostructure with asymmetric transmission of linearly polarized wave and huge optical activity in near-infrared band 下载免费PDF全文
Just like an electronic diode that allows the electrical current to flow in one direction only, a kind of chiral metamaterial structure with a similar functionality for the electromagnetic wave is proposed. The designed nanostructure that consists of twisted metallic split-ring resonators on both sides of a dielectric substrate achieves asymmetric transmission for a forward and backward propagating linearly polarized wave by numerical simulation in near-infrared band. Difference in transmission efficiency of the optimized structure between the same polarized waves incident from opposite directions can reach a maximum at the communication wavelength (1.55 μm). Moreover, the simulation results of this structure also exhibit strong optical activity and circular dichroism. 相似文献
910.
基于等离子体激励器工作过程中气体放电的焦耳加热作用, 并结合局部热力学平衡等离子体物理假设, 开展了等离子体合成射流三维唯象数值研究, 获得了完整工作周期内等离子体合成射流流场发展演变过程. 研究结果表明, 单次能量沉积建立的自维持周期性射流中存在有实现激励器腔体"充分" 回填的最大脉冲工作频率––饱和频率. 大的能量沉积、小的激励器出口直径和相同腔体体积下大的径高比都可以产生速度更高的射流, 而射流速度的提高会伴随有饱和频率的降低. 一个饱和周期内, 最多约有16%的初始腔内气体喷出, 吸气复原仅能实现初始腔体质量90%左右的回填.一个大气压条件下, 容性电源供能的等离子体合成射流激励器电能向气体热能和射流动能的转化效率分别约为5%和1.6%.
关键词:
等离子体激励器
合成射流
能量效率
饱和频率 相似文献