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正温度系数的热敏电阻(PTC)作为一种新型过流保护元件,近几年来已在程控交换机的用户接口电路防高压雷击、交流电搭接等方面得到了广泛应用。热敏电阻(PTC)按制造材料可分为有机聚合物PTC和陶瓷PTC两大类。有机PTC由高分子聚合物掺入碳粉经挤压成形。... 相似文献
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通过工艺试验,研究了BaTiO3陶瓷PTC材料在烧成过程中的冷却速度及烧成气氛对其PTC特性之影响。试验结果表明:采用适当的缓冷速度及氧气氛烧成可大大提高材料的PTC特性,αT、R(200)/R(min)明显增大,室温电阻达45Ω左右。所制元件与日本样品性能相近,完全能满足开关型元件的要求。 相似文献
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研究了不同烧结气氛对正温度系数热敏电阻(PTCR)性能的影响,在CO2气氛下烧结的PTCR室温电阻率(ρ0)比在空气中烧结的低将近50%,而其他各种电性能几乎没有明显的变化,因而在CO2气氛下的烧结是获得低电阻率PTCR的一种有效的工艺途径。 相似文献
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表面等离子体可调谐滤色器(Surface Plasmon Tunable filter,简作SPTF),是喷气推进到正在开发的新技术。将SPTF用于LCD投影机,可简化系统结构并提高效率。由三个SPTF组成的卷进式(scrolling)SPTF,可卷进地产生红(R)、绿(G)、蓝(B)三色,并能将单板LCD投影机的效率提高到与三板LCD投影机相同的水平。由6个SPTF组成的卷进式SPTF可以产生两 相似文献
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本文介绍了一种快速测量正温度系数热敏电阻(PTCR)的重要参数(居里温度Tc和电阻温度系数αt)的测量方法,并根据这种方法设计了PTCR特性参数Tc,αt快速测试仪,该仪器的使用改变了传统测试方法时间长,工作量大的状况。通过测量PTCR在室温和两个特征温度下的电阻值,该仪器能很快计算并显示出Tc和αt的结果,大大提高了测试效率,该仪器以8031单片机系统为核心,简单实用,使用方便,成本低,文中介绍 相似文献
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钛酸钡基陶瓷材料晶界掺杂与PTCR效应 总被引:1,自引:1,他引:0
“晶界掺杂”是一个全新的概念,它针对的是陶瓷晶界。在钛酸钡材料中,晶界掺杂能明显地改变PTCR效应。在晶界上,施主杂质同某些受主杂质一样,也可以明显提高材料的PTCR效应。通过晶界掺杂引入的Pb2+则对PTCR效应有明显的损害。 相似文献
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采用溶胶包裹再凝胶工艺制备了C-2CH复合型PTCR薄膜。实验表明,这种材料的PTC效应是由2CH的相变体膨胀引起的,C的粒径大小对复合薄膜PTC特性有十分显著的影响。较高的热循环温度和较多的热循环老化次数使PTCR薄膜电性能重现性得以改善。 相似文献
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一台离子注入机的改进及其在BaTiO3陶瓷改性中的应用 总被引:1,自引:0,他引:1
本文介绍了武汉大学200keV离子注入机的改进情况,用贝纳斯离子源替换了原有的高频离子源,使输出流强由几十微安提高到毫安级,离子种类由原来单电荷的气体离子扩展到多电荷离子和金属离子。用该机对半导体BaTiO3陶瓷注入Cu离子,使材料的PTCR突跳幅度增加,室温电阻率提高,证实Cu(2+)离子在PTCR材料晶界起着电子陷阱作用。 相似文献
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自由电子与周围电磁环境互作用时可以通过不同的形式辐射电磁波.超材料是一种人工复合材料,可实现传统自然材料所不具备的电磁特性.基于超材料与自由电子之间的相互作用可以打破传统电磁辐射系统的限制,实现对辐射电磁波的极化、相位、波前等特性的灵活操控,这为发展新型的自由电子辐射器件提供了新思路.本文简单介绍了切伦科夫辐射、史密斯... 相似文献
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红外目标多光谱图像为目标红外辐射特性的研究提供了有效的手段,在目标材质识别、伪装目标辨识和复杂背景抑制等目标探测技术领域有着极为重要的应用。以黑体辐射理论为基础,提出了一种基于波段拓展的红外多光谱成像的方法。首先,利用中波红外热像仪(3~5 μm)采集红外图像,通过目标表面的真实红外辐射反推出热图像中不同像素点的温度值,然后利用普朗克公式可以获得不同像素点在预拓展波段处的辐射出射度数值,最后根据这些数值进行红外多光谱成像。 相似文献
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The charge collection efficiency of CdZnTe radiation detectors with two different configurations: aSchottky diode detector and aresistive detector are compared. The average charge collection efficiencies for three different directions of irradiation (negative electrode,
positive electrode and perpendicular to the electric field) are calculated. The mobility-lifetime product of the CdZnTe substrates
is evaluated from the dependence of the measured spectra upon detector bias voltage. The measurement of the average charge
collection efficiency is based on monitoring the shift of the peak channel with bias voltage in an experimental setup which
is well calibrated. Two types of radiation are used:gamma photons from several radioactive sources andalpha particles from an241Am source. The models for the evaluation of mobility-lifetime product from the measured data for the two types of detector
configurations as well as for the two types of radiation sources, are compared and discussed. The CdZnTe (Zn = 10%) substrates
under study are obtained commercially and are grown by the high pressure Bridgeman method. The mobility-lifetime products
and specific resistivity of the two types of detectors are evaluated and compared. A lower resistivity material has a narrower
depletion region and behaves like a thinner detector thus exhibiting better collection efficiencies. Therefore, medium resistivity
material which is completely inadequate for resistive detectors can still yield high performance Schottky detectors. The preferred
direction of irradiation, i.e. from the negative electrode, is possible only in the case of n-type material which is reverse
biased by negative voltages applied to the Schottky gate. The mobility-lifetime products that are derived on both the resistive
detector (with specific resistivity of ≈1.1010 ω.cm) and the Schottky diode (with specific resistivity of ≈1.106 Ω.cm) are μnτn ≈-4.10−4 cm2V−1 and μpτp≅ 8.10−5 cm2V−1. 相似文献
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D. P. Webb Y. C. Chan C. K. H. Wong Y. W. Lam K. M. Leung D. S. Chrp 《Journal of Electronic Materials》1997,26(5):470-473
Thermally stimulated current (TSC) measurements have been performed on a xerographic photoreceptor which has been treated
with ultraviolet (UV) radiation. The charge transport layer of the photoreceptor consists of a polyester molecularly doped
with an arylamine substituted hydrazone which was observed to undergo UV induced rearrangement to an indazole derivative.
The indazole derivative is transparent to the wavelength component inducing the photo-reaction so that the depth of converted
material gradually extends farther into the CTL with UV exposure time. The xerographic residual potential variation with irradiation
time is attributed to the formation of a potential barrier to transfer of charge from hydrazone hopping states to indazole
hopping states. The mobility activation energy obtained from TSC measurements is 0.22 eV for unirradiated material, which
decreases to 0.12 eV after 1200 s of irradiation. The latter energy is identified as a signature of the potential barrier.
This identification is corroborated by the correlation between the decrease of the residual potential and the increase of
the TSC activation energy after 3600 s of irradiation. 相似文献
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介绍了采用全剂量SIMOX SOI材料制备的0.8μm SOI CMOS器件的抗总剂量辐射特性,该特性用器件的阈值电压、漏电流和专用集成电路的静态电流与高达500krad(Si)的总剂量的关系来表征.实验结果表明pMOS器件在关态下1Mrad(Si)辐射后最大阈值电压漂移小于320mV,nMOS器件在开态下1Mrad(Si)辐射后最大阈值电压漂移小于120mV,器件在总剂量1Mrad(Si)辐射后没有观察到明显漏电,在总剂量500krad(Si)辐射下专用集成电路的静态电流小于5μA. 相似文献
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Facile Single‐Precursor Synthesis and Surface Modification of Hafnium Oxide Nanoparticles for Nanocomposite γ‐Ray Scintillators
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Chao Liu Tibor Jacob Hajagos David Kishpaugh Yunxia Jin Wei Hu Qi Chen Qibing Pei 《Advanced functional materials》2015,25(29):4607-4616
Inorganic nanoparticles/polymer nanocomposites provide a low cost, high performance alternative for gamma scintillation. However, inorganic nanoparticles used thus far suffer from either moderate atomic numbers or low band gaps, limiting the gamma stopping power and photoelectron production in these systems. Here, a highly efficient, facile single‐precursor synthesis protocol is reported for hafnium oxide nanoparticles with an average diameter of 5 nm. The nanoparticle surface is further functionalized for the fabrication of highly transparent bulk‐size nanocomposite monoliths (2 mm thick, transmittance at 550 nm >75%) with nanoparticle loadings up to 40 wt% (net hafnium wt% up to 28.5%). Using poly(vinyltoluene) as the matrix, 2‐(4‐tert‐butylphenyl)‐5‐(4‐biphenylyl)‐1,3,4‐oxadiazole and 1,4‐bis(5‐phenyl‐2‐oxazolyl)benzene as the cascade fluors, and hafnium oxide nanoparticles as the gamma sensitizer, the nanocomposite monolith of 1 cm diameter and 2 mm thickness is fabricated capable of producing a full energy photopeak for 662 keV gamma rays, with the best deconvoluted photopeak energy resolution <8%. 相似文献