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31.
本文首先简要介绍了停止损失序在风险期望值相等时的一些推论 ,然后借助停止损失序详尽地讨论了仅取有限个值的随机变量的格点化 ,并以此作为出发点在多重衰减模型的框架下 ,给出了以 Poisson复合模型近似个体风险模型的一般步骤 ,同时导出了评价这一近似优劣程度的一个数量指标的解析表达式。  相似文献   
32.
为获取双峰分布超细颗粒的动态光散射模拟信号,通过建立动态光散射随机过程的AR模型,利用修正的Levison Durbin递推算法确定模型参数和阶数的方法模拟光散射信号.分别对10 nm与90 nm,200 nm与1 000 nm双峰分布颗粒的动态光散射信号进行模拟,得到的模拟信号光强自相关函数与理论值吻合,用双指数法对颗粒粒径反演,相对误差小于3.55%.通过分析模型阶数、采样时间、采样频率、模拟数据长度等参数对模拟精度的影响,得出双峰分布颗粒光散射信号的模拟精度与各参数的关系:在低于阈值阶数时,模型阶数选择对精度影响大,模型阶数越高,信号模拟的精度越高,高于阈值阶数时,模型阶数选择对精度影响不大,可选阈值阶数模型模拟信号.选定一定的采样时间,采样频率越高,模拟数据长度越长,模拟精度越高.  相似文献   
33.
The three-dimensional(3D) Dirac semimetals have linearly dispersive 3D Dirac nodes where the conduction band and valence band are connected. They have isolated 3D Dirac nodes in the whole Brillouin zone and can be viewed as a 3D counterpart of graphene. Recent theoretical calculations and experimental results indicate that the 3D Dirac semimetal state can be realized in a simple stoichiometric compound A_3Bi(A = Na, K, Rb). Here we report comprehensive high-resolution angle-resolved photoemission(ARPES) measurements on the two cleaved surfaces,(001) and(100), of Na_3Bi. On the(001) surface, by comparison with theoretical calculations, we provide a proper assignment of the observed bands, and in particular, pinpoint the band that is responsible for the formation of the three-dimensional Dirac cones. We observe clear evidence of 3D Dirac cones in the three-dimensional momentum space by directly measuring on the k_x–k_y plane and by varying the photon energy to get access to different out-of-plane k_zs. In addition, we reveal new features around the Brillouin zone corners that may be related with surface reconstruction. On the(100) surface, our ARPES measurements over a large momentum space raise an issue on the selection of the basic Brillouin zone in the(100) plane. We directly observe two isolated 3D Dirac nodes on the(100) surface. We observe the signature of the Fermi-arc surface states connecting the two 3D Dirac nodes that extend to a binding energy of ~150 me V before merging into the bulk band. Our observations constitute strong evidence on the existence of the Dirac semimetal state in Na_3Bi that are consistent with previous theoretical and experimental work. In addition, our results provide new information to clarify on the nature of the band that forms the3 D Dirac cones, on the possible formation of surface reconstruction of the(001) surface, and on the issue of basic Brillouin zone selection for the(100) surface.  相似文献   
34.
Ta2O5 films axe deposited on fused silica substrates by conventional electron beam evaporation method. By annealing at different temperatures, Ta2 O5 films of amorphous, hexagonal and orthorhombic phases are obtained and confirmed by x-ray diffractometer (XRD) results. X-ray photoelectron spectroscopy (XPS) analysis shows that chemical composition of all the films is stoichiometry. It is found that the amorphous Ta2 O5 film achieves the highest laser induced damage threshold (LIDT) either at 355 or 1064nm, followed by hexagonal phase and finally orthorhombic phase. The damage morphologies at 355 and 1064nm are different as the former shows a uniform fused area while the latter is centred on one or more defect points, which is induced by different damage mechanisms. The decrease of the LIDT at 1064nm is attributed to the increasing structural defect, while at 355nm is due to the combination effect of the increasing structural defect and decreasing band gap energy.  相似文献   
35.
TiO2 and ZrO2 films are deposited by electron-beam (EB) evaporation and by sol-gel process. The film properties are characterized by visible and Fourier-transform infrared spectrometry, x-ray diffraction analysis, surface roughness measure, absorption and laser-induced damage threshold (LIDT) test. It is found that the sol-gel films have lower refractive index, packing density and roughness than EB deposited films due to their amorphous structure and high OH group concentration in the film. The high LIDT of sol-gel films is mainly due to their amorphous and porous structure, and low absorption. LIDT of EB deposited film is considerably affected by defects in the film, and LIDT of sol-gel deposited film is mainly effected by residual organic impurities and solvent trapped in the film.  相似文献   
36.
基于密度泛函(DFT)理论,采用CAM-B3LYP方法,以C32分子为多极矩构建骨架,设计了两类替位式共掺杂的富勒烯衍生物C28B2N2和C28B2P2,共16种同分异构体,并对它们的电子性质、线性极化率α和一阶超极化率β进行研究。结果表明,掺杂后分子的HOMO-LUMO能隙变小,C28B2P2的α和β值均大于C28B2N2系列。其中偶极分子具有大的β值,八极分子则有较小的β值,筛选出具有优异的二阶非线性光学(NLO)响应特性的结构。含时密度泛函理论(TD-DFT)的结果表明,与C32相比,掺杂后所有结构的吸收光谱的响应范围变宽,最大吸收强度减弱,且最大吸收波长的位置发生红移或蓝移。基于完全态求和(SOS)方法,分别用二能级或三能级公式解释了两类共掺杂结构中β值最大的来源,并且证明了与之有关的电子激发类型为π→π*激发。  相似文献   
37.
为了解铜氧化物高温超导体的正常态输运特性对其超导电性的影响,我们对不同温度烧结样品正常态电阻率和超导电性之关联进行了系统的研究,实验结果显示:室温电阻率随烧结温度的增加而明显减小,而在920℃以上温度烧结的样品,变化趋于平稳,利用四引线法测量了不同温度烧结样品的电阻温度关系,结果显示:所有榈的超导转变温度均在92K左右,而且超导转变温度及其转变宽度均与烧结温度有一定的关联,实验结果反映了烧结温度在920~940℃范围内的样品,样品具有稳定的正常态特性,而其超导电物理性能亦具有良好的稳定性和可靠性。  相似文献   
38.
W片的双折射     
董大明  晋伟 《光学学报》1996,16(10):451-1455
具有维格特效应的W片所显示的光学各向生中同时具备二向色性和双折射两个因素,两者均与波长有关,通常在双折射很微弱时予以忽略。本文提供了二向色性很强时双折射相当显著的实验结果,获得了一系列实验数据及曲线。本文还提供了一种同时测定一块W片的二向色性与双折射的原理及实验方法。  相似文献   
39.
根据推广的惠更斯-菲涅耳原理和Rytov相位结构函数二次近似,推导出高斯-谢尔模型光束在湍流大气传输中交叉谱密度矩阵的表达式,研究了湍流对椭圆偏振高斯-谢尔模型光束传输中的偏振特性影响,并与部分偏振高斯-谢尔模型光束进行了对比分析.结果表明,相对于部分偏振高斯-谢尔模型光束,椭圆偏振高斯-谢尔模型光束在湍流大气传输中偏振度、方位角以及椭圆度的变化受湍流的影响较小.同时得到椭圆偏振高斯-谢尔模型光束在湍流大气斜程传输中偏振度的变化幅度比部分偏振高斯-谢尔模型光束的小,而方位角和椭圆度的变化幅度比部分偏振高斯-谢尔模型光束的大.  相似文献   
40.
<正>The DNA conformational transition depends on both the DNA sequences and environment such as solvent as well as electrolyte in the solution.This paper uses the AMBER8 package to investigate the electrolyte concentration influence on the dynamics of the A→B conformational transition of DNA duplex d(CGCGAATTCGCG)_2.The results from the restrained molecular dynamics(MD) simulations indicate that the total energies of the systems for A-DNA are always higher than those for B-DNA,and that the A→B conformational transition in aqueous NaCl solution is a downhill process.The results from the unrestrained MD simulations,as judged by the average distance between the C5' atoms(average helical rise per ten base pair),show that the concentrated NaCl solution slows down the A→B conformational transition.This observation can be well understood by analyses of the difference between the counterion distributions around A-DNA and B-DNA.  相似文献   
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