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111.
XUE Qingsheng;BAI Haoxuan;LU Fengqin;YANG Jingyao;LI Hui 《光子学报》2023,52(5):301-314
With the development of the hyperspectral imaging technology, it has been widely used and convinced as a useful detecting tool in many areas such as medical area, food safety and mineral exploration. But most of the hyperspectral imagers used nowadays are based on push-broom spectral imaging technology, which achieve spectral imaging through moving the spectral imager by scanning structure. The time resolution is sacrificed to obtain rather good spectral and spatial resolution in this kind of spectral imaging way. And that means the dynamic target and process can not be detected by this kind of hyperspectral imagers, so the application range of this kind technology is limited largely. Due to the defects mentioned above, a snapshot hyperspectral imager based on microlens array is developed in this paper. The principle of the instrument developed is introduced in this paper. Then the imaging principle of the microlens is introduced based on geometrical optics. The signal-to-noise calculation model of the hyperspectral imaging system based on microlens is then derived according to the imaging characteristics of this kind of system. Based on these theories derived above, the optical system is designed. The detector and the microlens were first determined before the optical design job begin. The detector has 2 048×2 048 pixels with a pixel size of 5.5 μm×5.5 μm . And the microlens array is composed of 100×100 microlens. The size of each microlens is 100 μm, and the focal length of the microlens is 0.5 mm. According to the microlens size and the detector size, the wavelength range of the whole system is determined as 500~700 nm. An objective lens is first designed, the F number of the objective is determined as 60 according to the calculation result, and the field of view of the objective lens is 36°.The objective lens has a telecentric feature on image side. Then the spectral imaging system is designed. The F number of the spectral imaging system is determined as 5 according to the F number of the microlens. A double amici prism is designed and used as the dispersion element in the spectral imaging system. The collimating lens and imaging lens in the spectral imaging system are symmetrical to eliminate the vertical aberration in the system and make the fabrication of the lens simpler. A simulation is taken after the design work has been finished. A prototype is set up in the laboratory according to the simulation result, and several performance verification experiments are taken to test the imaging and spectral performance of the system. The spatial and spectral calibration of the system are first taken. According to the calibration result, the monochromatic images of different bands can be extracted. To test the spectral resolution of the whole system, a mercury lamp is used to illuminate the system. And according to the test result, the spectral resolution of the system is 2.034 nm at 546.08 nm and 7.052 69 nm at 696.54 nm. A special target is used to test the spatial resolution of the whole system. According to the test result, the resolution of the whole system is 2.2 mm when the object distance is 1.1 m. Then a board with different color blocks and a standard white board are used as the target and detected by the whole system. Then the reflectance curves of different color blocks are calculated, which match the reflectance curves obtained by a commercial spectrometer. The test results show that the system has a good spectral and relatively good spatial detection capability. Comparing to the traditional push-broom spectral imager, the built system can improve the detecting efficiency of the spectral imaging detection, reduce the volume of the whole hyperspectral imaging system, and expand the application range of hyperspectral imaging technology. 相似文献
112.
研发能够精确、实时、原位获取热液甲烷数据的深海甲烷传感器对深海研究具有非常重要的意义。前期研制的两款深海甲烷光学成像干涉系统,均利用甲烷辐射光谱开展甲烷状态参数探测和反演。首先,以分子光谱辐射理论为基础,建立了分子辐射光谱与浓度、温度、压强的理论关系式,结合深海高压环境特点,建立了基于Lorentz线型的深海分子辐射模型,该模型为利用光谱法定量反演分子浓度、温度、压强等状态参数提供理论依据,同时为深海分子光谱仿真提供有力工具。接着,借助HITRAN分子光谱数据库提供的分子基本谱线参数,挑选出甲烷成像干涉系统的光源谱线。对比CH4分子与CO2, H2S, H2O等分子的特征吸收谱线,在5 990~6 150 cm-1波段范围内,CH4谱线强度比CO2, H2S, H2O等三种干扰分子的谱线强度约高2~3个数量级,且此波段内甲烷六条有效谱线分布均匀,谱线间距皆约为2~3 nm,非常适合采用光谱法进行分子状态参数探测,因此选择谱线干扰较弱、谱线分布均匀、谱线间距适中的甲烷六条谱线(1 640.37, 1 642.91, 1 645.56, 1 648.23, 1 650.96和1 653.72 nm)作为甲烷成像干涉探测系统的目标光源谱线。最后,基于深海分子辐射模型和HITRAN数据库的甲烷分子基本谱线参数,人工合成了甲烷任意浓度,任意温度和任意压强的辐射光谱数据,并分析了甲烷辐射光谱随浓度、温度和压强的变化特征。对于单一中心谱线,甲烷分子辐亮度随着浓度的升高而线性增大,随着温度的升高而非线性增大,随着压强的升高而非线性减小。对于全波段谱线,甲烷辐射光谱的全线宽随着浓度、温度的升高而变宽,随着压强的升高而变窄。建立的深海甲烷辐射光谱理论和仿真分析结果,可以为基于光谱法的海洋原位甲烷传感器的研制和数据反演提供数据支撑和理论依据。 相似文献
113.
DU Xiaorui;XU Huangrong;LI Wenlong;HE Zhengquan;KONG Depeng 《光子学报》2022,51(9):169-178
Imaging fiber plays an important role in medicine, industry, aerospace and other fields because of its excellent flexibility, especially in the application of optical fiber endoscope in medicine. Optical fiber image transmission system is usually composed of imaging objective, imaging fiber and image sensor.At present, the number of pixels in cameras can reach millions or even tens of millions, but the number of pixels in optical fibers is usually only a few hundred thousand.Therefore, the resolution of the system is limited by the resolution of the imaging fiber itself, and the imaging resolution of the whole system basically depends on the number of pixels that the imaging fiber can transmit. At present, the imaging fiber bundles on the market have either high resolution but small total cross-sectional area, or large cross sectional size but fiber diameter up to ten microns. This phenomenon results in insufficient pixels and small image area of high resolution image fiber, while large cross section can not reach high resolution due to technological limitations. To solve the problems, this paper proposes a multi-aperture high-resolution imaging technology based on imaging fiber array, which uses the imaging fiber array and image Mosaic technology to break through the bottleneck of improving pixel number. The number of pixels in the system can be increased by using high resolution and small cross section imaging fiber arrays. Combined with the characteristics of overlapping imaging of microlens array, the problem of information loss caused by direct imaging of imaging fiber array can be solved and the integrity of optical fiber array imaging can be realized.This method is expected to increase the number of pixels in optical fiber image transmission system to millions of order of magnitude and improve the resolution of the system. The imaging fiber is designed to be arranged 6×8, and the microlens array is designed based on the imaging fiber array. There are two groups of aspherical lenses made of PMMA material, and the imaging fiber array and the two groups of microlens arrays have uniform positions. Add a telecentric objective lens in front of the microlens array as the main lens of the image transmission system to solve the problem of complete overlap of adjacent subgraphs caused by direct imaging of the microlens array. The focal length of the lens is 10.1 mm, the aperture coefficient is 6.3, and the field Angle is 88°. The simulation results show that both the main lens and the microlens array can meet the performance requirements of the imaging fiber, and the object information can be successfully transmitted to the imaging fiber. The modulation transfer function value of the system can reach more than 0.5 at 50 lp/mm, without weakening the quality of the primary image, and meet the resolution requirements of the imaging fiber. Experimental results show that the system contains 400 000 effective pixels and the system resolution is 40 lp/mm.The image is clear and complete, which proves that the design of the imaging system has a good feasibility, and has an important practical reference significance for improving the resolution of the optical fiber image transmission system. 相似文献
114.
CHENG Zhiyuan;JI Zhou;GAO Yansheng;SU Hua;YAN Peipei;XIA Aili 《光子学报》2022,51(12):24-35
Laser optical field imaging system transmits multiple laser beams to scan the target for imaging. When the new optical field imaging theory is applied in practical engineering, the inevitable multi beam intensity jitter effect will cause fluctuation in intensity amplitude. In the subsequent reconstruction of spectrum components based on the spectrum iteration theory, the fluctuation in light intensity amplitude will cause the reconstruction spectrum error, which will lead to degradation of imaging quality in further. Aiming at the problem of image quality degradation of optical field imaging caused by laser beam intensity disturbance, an approximate calculation method based on the demodulation ratio of light field echo signal is proposed in this study. First, the interference light field signals with different frequencies in optical field echo signal are demodulated. The demodulated optical field echo signal is affected by random fluctuations of the beam intensity amplitude. The phase closure coefficient is calculated based on the multi beam phase closure theory and an isospectral sampling array is constructed. Then, according to the principle of isospectral iterative reconstruction, the high-order spectral components can be obtained by iteratively solving the lower order spectral components in turn. In this study, the influence model of the light intensity perturbation factor on reconstructed spectrum component error is established, and the influence mechanism of light intensity perturbation on image quality is revealed. Due to the amplitude fluctuation effect of beam intensity, the disturbance factor of beam intensity fluctuates randomly, which affects the accuracy of spectral signal reconstruction and reduces the imaging quality. In order to eliminate the influence of light intensity disturbance on image quality, the influence of light intensity disturbance factor on reconstructed spectral signal should be suppressed. In the weak turbulence scene, the scale coefficient of the disturbance factor of multi-beam intensity can be approximated by the demodulation component of laser echo signal. The light intensity perturbation factor is calculated by the scale coefficient of demodulation echo signal. The value of laser beam intensity perturbation factor is substituted into the spectrum reconstruction model. Finally, the spectrum of eliminating light intensity disturbance factor is obtained. The target image is obtained by performing an inverse Fourier transform of signal spectrum component, and the image index of target is calculated to evaluate the reconstructed image quality. The demodulation ratio of optical field imaging method is analyzed and verified based on the simulation experiment. The simulation experiment results show that the demodulation ratio method suppresses the light intensity disturbance and improves the reconstruction image quality. The demodulation ratio method can effectively suppress the degradation effect of light intensity disturbance and improve the image quality. The validity of the demodulation ratio method is verified based on the desktop experimental platform. The experimental results show that the image sharpness is significantly improved, and the three image quality evaluation indexes of the reconstructed image Strehl ratio, peak signal-to-noise ratio and structural similarity are all improved, which further proves the effectiveness of the demodulation ratio method. The imaging error correction model of light intensity perturbation factor is proposed and the corresponding demulation ratio solution is proposed in optical field imaging system. This study provides an effective theoretical guidance for the suppression of light intensity perturbation factor and the improvement of image quality in actual optical field imaging. The research shows that the proposed demodulation ratio method can effectively suppress the influence of beam intensity disturbance on image quality, and effectively reduce the requirements of beam intensity stability and multi-beam intensity consistency for optical field imaging, thus reducing the difficulty of optical field imaging engineering. The research can provide technical support for experimental research and application transformation of optical field imaging technology. 相似文献
115.
FAN Xinghao;LIU Chunyu;XU Minglin;LIU Shuai;ZHAO Yingming;CUI Yazhen 《光子学报》2022,51(12):179-194
Hyperspectral remote sensing technology is an optical remote sensing technology developed on the basis of imaging spectroscopy, which can realize comprehensive observation of spatial information, spectral information and radiation information. The imaging spectrometer adopting the Prism-Grating-Prism (PGP) spectroscopic element avoids the off-axis problem of traditional prism-type and grating-type imaging spectrometers, and is conducive to the miniaturization and compactness of imaging spectrometers. Aiming at the problem that the spectral smile of coaxial PGP imaging spectrometer is difficult to correct, this paper proposes a method to rectify the curvature of spectral line by using curved slit and distortion of the collimator lens and focusing lens. On the basis of retaining the advantages of PGP such as high diffraction efficiency and coaxial optical path, this method can correct spectral smile and keystone of the instrument. In this paper, the prism-grating-prism vector dispersion model is established by focusing on the influence of lens distortion, the number of grating lines and prism angle on spectral smile and keystone. By tracing the light vector and analyzing the intersection between the light vector and the image plane after the light vector passes through the PGP element with different parameters, the influence of different parameters on the smile was analyzed. It is worth noting that when the shape of the slit changes, the direction of the initial light vector also changes. Therefore, this model can also analyze the effect of the slit shape on the spectral smile and keystone. Further, the prism-grating-prism vector dispersion model is used to analyze the spectral line bending characteristics of coaxial PGP spectroscopic elements: when the coaxial condition is met, the PGP imaging spectrometer will inevitably have a large smile, and the spectrum is bent in the short-wave direction. After adjusting the prism Angle, the number of grating lines and the lens distortion, we analyzed the smile size of the combination of the above parameters, and came to an optimistic conclusion: the smile problem of the imaging spectrometer could not be eliminated only by changing the prism, grating and lens. However, the smile can be corrected well by the method of bending the slit and matching the appropriate lens distortion. In order to improve the versatility of this method, this paper gives an objective function for correcting spectral curvature and spectral line curvature by using the PGP vector dispersion model, and uses genetic algorithm to optimize the objective function and calculate the best combination of slit shape and lens parameters quickly. In order to verify the feasibility of this method, this paper uses the calculation results of this method to design a curved slit PGP imaging spectrometer with a slit length of 22 mm, an operating wavelength of 400~800 nm, a spectral resolution of 3 nm, and an F number of 3.5 which has a spectral curvature of less than 2 μm and a spectral line curvature of less than 2 μm. The optical system has a diffuse spot radius of less than 5.4 μm in the wavelength range of 400~800 nm, and can distinguish slit images with a spectral interval of 2 nm. The energy concentration of all fields of view can reach 90% in the 2×2 pixel scale. The design results show that the use of curved slit and distortion of the collimator lens and focusing lens can effectively correct the curve of the spectral line, which has important guiding significance for the design of the coaxial PGP imaging spectrometers. In this article, we calculated the optimal slit shape and lens parameters for different slit lengths and different grating parameters, which proved that the method had universal applicability. 相似文献
116.
磁粒子成像是基于功能和断层影像技术检测磁性纳米粒子空间分布的示踪方法, 具有正向的对比信号、 较低的组织背景、 无限的组织穿透深度、 非侵入性成像以及无电离辐射等优点, 是近年来一种很有前途的生物医学成像技术. 磁粒子成像信号是通过在无场点切换磁性纳米粒子的磁自旋矢量来产生的. 磁粒子成像的灵敏度和空间分辨率都高度依赖于作为磁粒子成像示踪剂的磁性纳米粒子本身的磁性能, 因此目前的研究主要集中在磁性纳米粒子的设计和合成上. 本文重点介绍了磁粒子成像示踪剂的最新研究进展, 总结了可作为磁粒子成像示踪剂的磁性纳米粒子的种类、 合成方法、 性能以及生物医学应用, 以期为磁粒子成像的未来研究提供参考. 相似文献
117.
The past few years have shown rapid growth of NMR imaging in both image quality and diagnostic usefulness. It has become apparent, as the images have been published, that both inter- and intra-group imaging of the same underlying pathology produces images which can have vastly differing appearance. This effect is mainly due to imaging techniques which use different pulse sequence types and timings thus varying the relative contribution of the protpn density, T1, and T2 properties of the tissues. In this paper we investigate the contrast manipulation effects and methods for SNR optimization for the saturation recovery, inversion recovery, spin echo, and inversion recovery spin echo pulse sequences when applied to three clinically relevant imaging tasks. 相似文献
118.
Gd2O3 particles (less than 2 microns) in suspension were evaluated as a potential contrast agent for liver-spleen imaging with magnetic resonance. The agent was administered IV to rabbits in doses ranging from 10 to 120 mumol/kg and the tissues removed after sacrifice for in vitro T1 and T2 analysis. The temporal response was determined in liver and spleen samples of rabbits given a fixed dose (60 mumol/kg) and sacrificed at intervals from 15 min to 60 hr later. Documentation of the subanatomic location of Gd2O3 particles in tissue was accomplished by electron microscopy and x-ray dispersion microanalysis. T1 weighted images were obtained at 0.12T on a prototype resistive scanner. The liver, spleen, and lung relaxation times are very responsive to Gd2O3 IV and the effect is dose related. A peak effect is observed between 3-7 hr after injection and relaxation times may normalize by 60 hr. By electron microscopic and x-ray analysis, Gd2O3 is most prominently found in the hepatic and splenic sinusoids. The images show marked enhancement of liver and splenic tissues, aiding in the clear delineation of these tissues from neighboring structures. 相似文献
119.
正向成像技术是正向计算与反演相结合的密度重建技术的基础。为了正确获取闪光照相面光源下复杂客体的正向计算数值图像,提出了面光源点源化的思想,并用窗口化的探测系统模糊、径迹法等技术得到了更加准确的、含系统模糊的正向投影矩阵以及方程。利用含系统模糊的正向投影方程计算实验客体的正向投影,获得了与实验结果一致的边界信息。含系统模糊的正向投影方程和逆问题求解的约束共轭梯度法合成了整体密度重建方法。整体密度重建方法应用于FTO客体的模拟图像和实验图像,都能够将模糊控制在1~2个像素。 相似文献
120.
This review paper reports near-infrared (NIR) imaging studies using a newly-developed NIR camera, Compovision. Compovision can measure a significantly wide area of 150 mm×250 mm at high speed of between 2 and 5 s. It enables a wide spectral region measurement in the 1 000~2 350 nm range at 6 nm intervals. We investigated the potential of Compovision in the applications to industrial problems such as the evaluation of pharmaceutical tablets and polymers. Our studies have demonstrated that NIR imaging based on Compovision can solve several issues such as long acquisition times and relatively low sensitivity of detection. NIR imaging with Compovision is strongly expected to be applied not only to pharmaceutical tablet monitoring and polymer characterization but also to various applications such as those to food products, biomedical substances and organic and inorganic materials. 相似文献