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81.
CCD成像电子学单元光电参量测试系统   总被引:2,自引:0,他引:2       下载免费PDF全文
针对空间光学相机重要组成部分的CCD成像电子学单元的光电参量测试需求,介绍了CCD成像电子学单元光电参量测试必要性,提出了对CCD成像电子学单元光电参量进行系统测试的试验方案,并设计、研制了测试装置。对于该装置进行了系统调试与标定,得到单色仪波长定标系数为1.003 29,并对CCD成像电子学单元辐射性能测试中积分球的稳定性及均匀性进行了测试,测试结果满足要求。通过标准探测器标定待测探测器,得到待测探测器的相对光谱响应度。整套装置满足测试要求。  相似文献   
82.
In this paper, we have demonstrated a high performance waveguide photodiode integrated diluted waveguide serving as a fibre-to-waveguide coupler to achieve high coupling efficiency. High responsivity (> 1 A/W), high saturation power (> 45 mA) in the static state and extremely low dark current density (0.04 pA/μm2) with 3 dB bandwidth at 13.4 GHz have been achieved.  相似文献   
83.
84.
李健军  郑小兵  卢云君  张伟  谢萍  邹鹏 《物理学报》2009,58(9):6273-6278
介绍了利用钛宝石可调谐激光器、倍频器和单波长激光器作为光源,在24个波长分立点定标了三个硅陷阱探测器的绝对光谱响应度,解决了红外激光的精确定位与调整、窗口透过率模拟定标等关键技术.结果显示:在激光波长为412—800nm时,三个陷阱探测器定标的不确定度约低于0.05%;当激光波长大于800nm以及低于355nm时,获得的陷阱探测器的定标不确定度约低于0.065%.硅陷阱探测器可以作为空间各类遥感器在350—1064nm波段定标的传递标准探测器. 关键词: 陷阱探测器 低温辐射计 光谱响应度 辐射定标  相似文献   
85.
The recently proposed boundary condition-enforced immersed boundary-lattice Boltzmann method (IB-LBM) [14] is improved in this work to simulate three-dimensional incompressible viscous flows. In the conventional IB-LBM, the restoring force is pre-calculated, and the non-slip boundary condition is not enforced as compared to body-fitted solvers. As a result, there is a flow penetration to the solid boundary. This drawback was removed by the new version of IB-LBM [14], in which the restoring force is considered as unknown and is determined in such a way that the non-slip boundary condition is enforced. Since Eulerian points are also defined inside the solid boundary, the computational domain is usually regular and the Cartesian mesh is used. On the other hand, to well capture the boundary layer and in the meantime, to save the computational effort, we often use non-uniform mesh in IB-LBM applications. In our previous two-dimensional simulations [14], the Taylor series expansion and least squares-based lattice Boltzmann method (TLLBM) was used on the non-uniform Cartesian mesh to get the flow field. The final expression of TLLBM is an algebraic formulation with some weighting coefficients. These coefficients could be computed in advance and stored for the following computations. However, this way may become impractical for 3D cases as the memory requirement often exceeds the machine capacity. The other way is to calculate the coefficients at every time step. As a result, extra time is consumed significantly. To overcome this drawback, in this study, we propose a more efficient approach to solve lattice Boltzmann equation on the non-uniform Cartesian mesh. As compared to TLLBM, the proposed approach needs much less computational time and virtual storage. Its good accuracy and efficiency are well demonstrated by its application to simulate the 3D lid-driven cubic cavity flow. To valid the combination of proposed approach with the new version of IBM [14] for 3D flows with curved boundaries, the flows over a sphere and torus are simulated. The obtained numerical results compare very well with available data in the literature.  相似文献   
86.
Au nanoparticle (AuNP) core particles coated with a poly(N‐isopropylacrylamide) (pNIPAm) shell (Au@pNIPAm) are synthesized by seed mediated free radical polymerization. Subsequently, a temperature–light‐responsive photonic device is fabricated by sandwiching the Au@pNIPAm particles between two thin layers of Au. The optical device exhibits visual color and characteristic multipeak reflectance spectra, where peak position is primarily determined by the distance between two Au layers. Dual responsivities of the photonic device are achieved by combining the photothermal effect of AuNPs core (localized surface plasmon resonance (LSPR) effect) and the temperature responsivity of the pNIPAm shell. That is, the pNIPAm shell collapses as the temperature is increased above pNIPAm's lower critical solution temperature, either by direct heat input or heat generated by AuNPs' LSPR effect. To investigate the effect of AuNPs distribution in the microgels on the devices' photothermal responsivity, the Au@pNIPAm microgel‐based etalon devices are compared with that fabricated by AuNP‐doped pNIPAm‐based microgels; in terms of response kinetics and optical spectrum homogeneity. The uniform Au@pNIPAm microgel‐based devices show a fast response and exhibit a comparatively homogeneous spectrum over the whole slide. These materials can potentially find use in drug delivery systems, active optics, and soft robotics.  相似文献   
87.
基于人眼视觉非均匀特性的实时Mean Shift跟踪方法   总被引:3,自引:2,他引:1  
孙小炜  李言俊  陈义 《光子学报》2009,38(3):719-724
由于在成像制导过程中需要实时处理大量的信息,为了在尽可能保留有效信息情况下降低计算量,采用了一种人眼视觉非均匀采样模型——对数极坐标模型,来压缩信息量以提高计算速度;另外,由于对数极坐标变换对目标形状具有旋转和缩放不变性,在跟踪非刚性变形目标时该模型能表现出很好的稳健性;考虑到在成像跟踪末段,质心、角点之类的跟踪方法会产生匹配点漂移,为了抑制匹配点漂移,采用基于目标强度特征的Mean Shift跟踪方法,并对采用Gauss核函数的Mean Shift方法进行了优化来加快计算速度;实验结果表明,该方法能够有效抑制匹配点漂移,是一个稳健的目标跟踪方法.  相似文献   
88.
In this paper, we study the effect of the drain current on terahertz detection for Si metal-oxide semiconductor fieldeffect transistors(MOSFETs) both theoretically and experimentally. The analytical model, which is based on the smallsignal equivalent circuit of MOSFETs, predicts the significant improvement of the voltage responsivity Rv with the bias current. The experiment on antennas integrated with MOSFETs agrees with the analytical model, but the Rv improvement is accompanied first by a decrease, then an increase of the low-noise equivalent power(NEP) with the applied current. We determine the tradeoff between the low-NEP and high-Rv for the current-biased detectors. As the best-case scenario, we obtained an improvement of about six times in Rv without the cost of a higher NEP. We conclude that the current supply scheme can provide high-quality signal amplification in practical CMOS terahertz detection.  相似文献   
89.
白琳琅  葛辉良 《应用声学》2008,27(5):391-394
对用于水声探测的光纤水听器,加速度相移灵敏度是一个重要的参数。本文采用有限元法对空气背衬芯轴型光纤水听器的加速度相移灵敏度进行了理论分析,并通过实验验证,得到了空气背衬芯轴型光纤水听器加速度相移灵敏度的优化规律,提高芯轴壳体的硬度可有效降低光纤水听器的加速度相移灵敏度,而改变芯轴壳体的厚度对水听器加速度灵敏度影响不大。  相似文献   
90.
The paper considers the flow of a power-law fluid past a vertical stretching sheet. Effects of variable thermal conductivity and non-uniform heat source/sink on the heat transfer are addressed. The thermal conductivity is assumed to vary linearly with temperature. Similarity transformation is used to convert the governing partial differential equations into a set of coupled, non-linear ordinary differential equations. Two different types of boundary heating are considered, namely Prescribed power-law Surface Temperature (PST) and Prescribed power-law Heat Flux (PHF). Shooting method is used to obtain the numerical solution for the resulting boundary value problems. The effects of Chandrasekhar number, Grashof number, Prandtl number, non-uniform heat source/sink parameters, wall temperature parameter and variable thermal conductivity parameter on the dynamics are shown graphically in several plots. The skin friction and heat transfer coefficients are tabulated for a range of values of the parameters. Present study reveals that in a gravity affected flow buoyancy effect has a significant say in the control of flow and heat transfer.  相似文献   
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