共查询到16条相似文献,搜索用时 78 毫秒
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电子束和X射线双曝光制作大高宽比高分辨率的X射线波带片 总被引:1,自引:1,他引:0
介绍了利用电子束和 X射线束双曝光技术制作大高宽比高分辨率的 X射线聚焦或色散元件的新方法 (波长范围为 1~ 5 nm )。所制做的厚度为 10μm的 Au波带片具有 30个波带 ,最外环的宽度为 0 .5μm。实验表明 :对 8ke V的X射线来说 ,波带片的衬度大于 10 ,分辨率为 0 .5 5μm,焦距为 2 1.3cm。 相似文献
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高能电子束对抗蚀剂曝光的Monte Carlo模拟 总被引:1,自引:0,他引:1
利用分段散射模型, 借助Monte Carlo方法模拟了具有高斯分布特征的
高能入射电子束(50keV≤E0≤100keV)在抗蚀剂中的
散射过程, 分别得到了不同曝光条件下的电子背散射系数和能量沉积分布,
模拟结果与实验结果很好地符合. 在这一能量段, 当电子束能量越高、抗蚀剂
越薄、基片材料的原子序数越低时, 邻近效应越弱. 本文的模拟结果不仅能为高能电子束光刻工艺优化曝光条件、降低邻近效应提供理论指导, 而且能为进一步的邻近效应的校正提供更精确的数据. 相似文献
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超导纳米线单光子探测器是新型超导电子器件,因其具有高探测效率、低暗计数及低时间抖动等优势,在量子信息、激光雷达等方面已得到广泛的应用.目前主流超导纳米线单光子探测器主要工作在1.5μm以下的可见光和近红外波段.中红外波长的红外探测技术在基础科学、医学、日常生活以及军事等广泛领域发挥着重要作用,中红外单光子探测器可以使得中红外波段探测技术进入量子极限灵敏度.根据超导纳米线单光子探测器探测机理,超窄线宽的纳米线条可以提升超导纳米线单光子探测器在中红外波长的灵敏度.电子束曝光技术是目前实现超导纳米线单光子探测器纳米线线条加工的主流技术,电子束抗蚀剂种类繁多,面向超窄线宽超导纳米线单光子探测器器件的制备需求,对两款抗蚀剂进行性能测试表征,和窄纳米线制备尝试.根据负性电子束抗蚀剂MaN-2401在制备窄线宽时的显著优点,优化工艺,利用其成功制备出50 nm线宽超导纳米线单光子探测器并成功实现了2000 nm的单光子响应. 相似文献
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利用微芯片制备技术制备了带有电极的原位电学薄膜芯片,并结合自制的原位透射电镜样品台,实现了低温下透射电子显微镜聚焦电子束对InAs纳米线的精细刻蚀以及不同温度下的原位电学性能测量.研究发现,随着刻蚀区域截面积的减小,纳米线的电导率也随之减小.当纳米线的截面积从大于10000 nm2刻蚀至约800 nm2时,纳米线电导的减小速率与截面积的减小具有线性关系.同时利用低温聚焦电子束刻蚀,在InAs纳米线上原位制备了一个10 nm的纳米点,并在77与300 K下对该纳米点进行了电学性能测量.通过测量发现在77 K时出现库仑阻塞效应,发生了电子隧穿现象;而300 K时,热扰动提供的能量使这种现象消失. 相似文献
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In this work, we study the modification of hydrogenated diamond films deposited on silicon resulting from its exposure to DBr followed by an annealing above 600 K, using high resolution electron energy loss spectroscopy (HREELS). This procedure results in silicon carbide SiC formation within the diamond film, as evidenced by the observation of a loss peak at 117 meV and its first harmonic at 233 meV in HREEL spectra. This diamond surface modification is interpreted as resulting from the reaction of products of the silicon support thermally activated etching with hydrogenated diamond. 相似文献
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Focal depth and focal splitting of hyperbolic-cosine-Gaussian beams induced by a phase plate were investigated. The pure phase plate consists of three concentric zones: a center circle zone, an inner annular zone and an outer annular zone. The phase variance of the inner annular zone is adjustable. Simulation results show that the focal depth can be adjusted by changing the radii of zones. With the increase of the inner radius of the outer annular zone, the focal spot broadens along the optical axis and splits into two peaks. Then the two peaks combine back into one peak. There are two critical values for the inner radius of the outer annular zone, at which focal spot changes sharply. The tunable range of the focal depth varies considerably. The phase variance of the inner annular zone affects focal depth also; when the phase variance is π, the effect attains maximum. The parameters of cosh parts of the beam affect both focal splitting and focal depth evidently; focal splitting disappears with increasing parameters of cosh parts, and focal depth increases with increasing the parameters of cosh parts in both the low and the high numerical-aperture optical systems. 相似文献
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To theoretically explore the feasibility of neutron dose characterized by Cerenkov photons, the relationship between Cerenkov photons and neutron dose in a water phantom was quantified using the Monte Carlo toolkit Geant4. Results showed that the ratio of the neutron dose deposited by secondary electrons above Cerenkov threshold energy to the total neutron dose is approximately a constant for monoenergetic neutrons from 0.01 eV to 100 eV. With the initial neutron beam energy from 0.01 eV to 100 eV, the number of Cerenkov photons has a good correlation with the total neutron dose along the central axis of the water phantom. The changes of neutron energy spectrum and mechanism analysis also explored at different depths. And the ratio of total neutron dose to the intensity of Cerenkov photons is independent of neutron energy for neutrons from 0.01 eV to 100 eV. These findings indicate that Cerenkov radiation also has potential in the application of neutron dose measurement in some specific fields. 相似文献
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为了探究VO2薄膜受激光辐照的温度场分布,以及1 064 nm激光直接辐照100 s内至相变的激光功率密度阈值,并比较近红外和中红外波段透过率调制特性差异。首先基于COMSOL建立了薄膜受激光辐照的模型并进行了温度场仿真,然后分别测试了薄膜正反面被不同功率密度的1 064 nm激光辐照100 s内激光透过率随时间响应特性。实验中的VO2薄膜利用分子束外延法在Al2O3基底上制备得到。仿真结果表明,激光功率密度为25 W·mm-2时,50 nm厚薄膜在被辐照1 ms时间内即达到相变温度。经激光辐照实验发现:50 nm厚的VO2薄膜正反面受1 064 nm激光直接辐照100 s内至相变的功率密度阈值分别为4.1 W·mm-2和5.39 W·mm-2。30 nm厚VO2薄膜对1 064 nmn激光的透过率调制深度约为13%,对3 459 nm激光透过率调制深度约62%,说明VO2薄膜对近红外透过率调制特性不明显。 相似文献
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Nishant N. Patel K. B. Joshi 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,59(1):19-23
Using empirical pseudopotential method Γ-L crossover is found for
the Ga0.74Al0.26Sb. The conduction band minimum is observed to
switch at the (0.87, 0, 0) point for Ga0.51Al0.49Sb which shifts to
the X point for Ga0.21Al0.79Sb and remains at X leading finally to
indirect band gap in AlSb. Band structure calculations for a large number of
alloys are performed and bowing parameters bX and bL are proposed
for the EX and EL respectively. Our findings may serve as
directive to select the materials in a range of composition to examine the
bowing parameters and thereby effective mass experimentally for the
GaxAl1-xSb alloys. 相似文献