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31.
软X光多层镜反射率在同步辐射源上的标定   总被引:2,自引:0,他引:2       下载免费PDF全文
 软X光多层镜反射率标定实验在北京同步辐射装置 上进行,利用BSRF-3W1B 束线及其反射率计靶室(主靶室)标定不同材料的多层镜样品的反射率。多层镜的标定采用波长扫描法,以得到样品反射率随波长变化的曲线。给出了21°-B4C/Si,21°-B4C/Mo,10°-Cr/Ti,15°- B4C/W,10°- B4C/W以及6.86°-B4C/W等6块多层镜在50~1 500 eV能段上的反射率标定曲线,并将其与理论计算结果进行比较。结果表明:标定曲线与理论曲线很好地符合。影响标定结果的总不确定度的主要因素是光子能量不确定度,其次是角度不确定度,测量不确定度的影响很小。  相似文献   
32.
50~110 nm波段高反射率多层膜的设计与制备   总被引:1,自引:0,他引:1  
阐述了50~110 nm强吸收波段亚四分之一波长多层膜的设计方法.这种膜系是由强吸收材料叠加而成,每层膜光学厚度小于四分之一个波长.与常规周期多层膜相比,这种膜系更适用于提高强吸收波段的反射率.利用该方法设计了50 nm处高反射多层膜,并以此为初始条件通过Levenberg-Marquart优化方法完成了50~110 nm强吸收波段宽带高反射率Si/W/Co多层膜的设计,其平均反射率达到45%.采用直流磁控溅射方法制备了Si/W/Co多层膜,用X射线衍射仪(XRD)对膜层结构进行了测试,测试结果表明制作出的多层膜结构与设计结构基本相符.  相似文献   
33.
波长30.4 nm的He-II谱线是极紫外天文观测中最重要的谱线之一,空间极紫外太阳观测光学系统需要采用多层膜作为反射元件。为此研究了SiC/Mg、B4C/Mg、C/Mg、C/Al、Mo/Si、B4C/Si、SiC/Si、C/Si、Sc/Si等材料组合的多层膜在该波长处的反射性能。基于反射率最大与多层膜带宽最小的设计优化原则,选取了SiC/Mg作为膜系材料。采用直流磁控溅射技术制备了SiC/Mg多层膜,用X射线衍射仪测量了多层膜的周期厚度,用国家同步辐射计量站的反射率计测量了多层膜的反射率,在入射角12°时,实测30.4 nm处的反射率为38.0%。  相似文献   
34.
Design and Fabrication of Ni/Ti Multilayer for Neutron Supermirror   总被引:1,自引:0,他引:1       下载免费PDF全文
In the applications of neutron guides and focusing devices, by using the Ni/Ti multilayer supermirrors (SM), the neutron flux is significantly enhanced, because the critical reflective angle of supermirrors increases m times compared to the one of natural bulk Ni. We design and fabricate the Ni/Ti multilayer supermirrors by considering the effect of the interfacial imperfection, such as interface roughness and diffusion, and by using the direct current magnetron sputtering technology. The reflective performances of these supermirrors are measured on a V14 neutron beam line at the Berlin Neutron Scattering Centre (BENSC), Germany. The measurement data suggest that the critical angles of the supermirrors are 1.5 and 2.2 times that of bulk Ni, respectively.  相似文献   
35.
非周期多层膜Kirkpatrick-Baez显微镜成像   总被引:3,自引:3,他引:0       下载免费PDF全文
从光线传播的角度分析了非周期多层膜Kirkpatrick-Baez(KB)显微镜的成像性能,并与单层膜KB显微镜、周期多层膜KB显微镜进行了对比。与单层膜KB显微镜相比,多层膜KB显微镜提高了工作掠入射角度,在同样分辨力和集光效率要求下具有更大的视场。周期多层膜KB显微镜的反射率和能量分辨本领高于非周期多层膜KB显微镜,但非周期多层膜元件具有较大的角度带宽和均一的反射率,克服了周期多层膜KB显微镜视场范围和像场均匀性的不足。在此基础上,制备了中心角度1.133 0°的非周期多层膜反射镜元件,以8 keV能量的X射线光管为背光源进行了KB显微镜成像实验,实验结果与理论分析一致。  相似文献   
36.
为提高Mo/Si多层膜的稳定性与使用寿命,通过分析多层膜驻波电场的分布,对表面保护层及多层膜最上层材料的厚度进行优化设计,使优化后的反射率最高.计算表明,一定厚度的表面保护层总对应一个最优的最上层材料厚度.在13.36 nm波长,膜对数为50的Mo/Si多层膜10度入射的理论反射率为74.47%;当添加厚度为2.3 nm的Ru作为表面保护层,对应多层膜最上层Si的优化厚度为3.93 nm,其理论反射率为75.20%.设计结果表明,通过优化设计表面保护层,可以提高多层膜稳定性,改善多层膜性能.  相似文献   
37.
Infuence of interface roughness on the reflectivity of Tungsten/boron-carbide (W/B4C) multilayers varying with bi-layer number, N, is investigated. For W/B4C multilayers with the same design period thickness of 2.5 nm, a real-structure model is used to calculate the variation of reflectivities with N = 50, 100, 150, and 200, respectively. Then, these multilayers are fabricated by a direct current (DC) magnetron sputtering system. Their reflectivity and scattering intensity are measured by an X-ray diffractometer (XRD) working at Cu Kα line. The X-ray reflectivity measurement indicates that the reflectivity is a function of its bi-layer number. The X-ray scattering measured results show that the interface roughness of W/B4C multilayers increases slightly from layer to layer during multilayer growing. The variation of the reflectivity and interface roughness with bi-layer number is accurately explained by the presented realstructure model.  相似文献   
38.
30.4 nm波长处Mg基多层膜反射镜   总被引:1,自引:0,他引:1  
太阳光谱中重要的He-Ⅱ谱线(波长30.4 nm)的观测对于研究太阳活动和日地空间环境具有重要意义,实现空间极紫外太阳观测需要采用多层膜作为反射元件.研究了工作在30.4 nm的Mg基多层膜.以反射率最高为评价函数设计了多层膜,采用直流磁控溅射技术制备了SiC/Mg,B4C/Mg和C/Mg多层膜,用X射线衍射仪测量了多层膜的结构.研究表明虽然B4C/Mg多层膜理论反射率最高,但实际制备结果显示,SiC/Mg多层膜的成膜质量最好,反射率最高.同步辐射反射率测量表明:在入射角10°时实测的SiC/Mg多层膜反射率为44.6%.  相似文献   
39.
A linear zone plate named multilayer laue lens (MLL) is fabricated using a depth-graded multilayer structure. The lens shows considerable potential in focusing an X-ray beam into a nanometer scale with high efficiency. In this letter, a depth-graded multilayer consisting of 324 alternating WSi 2 and Si layers with a total thickness of 7.9 μm is deposited based on the thickness sequence according to the demands of the zone plate law. Subsequently, the multilayer sample is sliced and thinned to an ideal depth along the cross-section direction using raw abrasives and diamond lapping. Finally, the cross-section is polished by a chemical mechanical polishing (CMP) technique to remove the damages and improve the surface smoothness. The final depth of the MLL is approximately 7 μm with an achieved aspect ratio greater than 400. Results of scanning electron microscopy (SEM) and atomic force microscopy (AFM) indicate that interfaces are sharp, and the multilayer structure remains undamaged after the thinning and polishing processes. The surface roughness achieved is 0.33 nm.  相似文献   
40.
To develop high quality dispersion optics in the X-ray region, the sliced multilayer transmission grating is examined. Dynamical diffraction theory is used to calculate the diffraction property of this volume grating. A WSi 2 /Si multilayer with a d-spacing of 14.3 nm and bi-layer number of 300 is deposited on a superpolished silicon substrate by direct current magnetron sputtering technology. To make the transmission grating, the multilayer is sliced and thinned in the cross-section direction to a depth of 23-25 μm. The diffraction efficiency of the grating is measured at E = 8.05 keV, and the 1st-order efficiency is 19%. The sliced multilayer grating with large aspect ratio and nanometer period can be used for high efficiency and high dispersion optics in the X-ray region.  相似文献   
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