共查询到19条相似文献,搜索用时 62 毫秒
1.
聚酰亚胺LB膜MIS结构C—V特性 总被引:1,自引:0,他引:1
本文报道了Al/LB聚酰亚胺膜/P-Si(100)MIS结构的C-V特性研究结果。67层LB膜样品C-V特性近乎理想,具有负的固定电荷密度约10^1^1cm^-^2量级,平带时滞后小于0.3V,对于MIS隧道结,除了在-0.5-1.5V间具有反型层箝位产生的电容峰外,在-1.5-4V间还出现了另一电容峰值,假设在强电场下隧穿能力剧增,从而结构由隧穿限制区重新进入半导体限制区,可以解释这一峰值的出现 相似文献
2.
DBM-g-PE与PVC的相互作用研究EI 总被引:5,自引:1,他引:4
采用固相接枝法制备了DBM-g-PE,用红外光谱分析证明了接枝物确实存在。PVC/CPE=100/5合金性能测定结果表明,添加5份接枝物的合金(A),缺口冲击强度、拉伸强度分别为18.2kJ/m2和53.0MPa;而添加5份PE的合金(B),其相应性能为5.1kJ/m2和33.8MPa。不加接枝物的合金(C),虽有高韧性,但拉伸强度却由53.0MPa降至50.2MPa。DSC、SEM的结果均表明,PE接枝DBM后与PVC的相互作用增强,与CPE协同作用能增韧、增强PVC,并探讨了其机理。 相似文献
3.
HL—1M装置硼化膜的研究 总被引:2,自引:0,他引:2
HL-1M装置采用C2B10H12蒸汽等离子体增强沉积技术对第一壁进行了原位硼化,在第一壁表面上形成一层半透明、非晶a-B/C:H膜。在单电极、1.2A/750V放电参数下,平均沉积速率为110nm/h,膜厚不均匀度为84%,B/C=0.6-2.0,B-C的结合能为97-99eV,与B/C值有关。膜层中有20-30%的硼是以B-C的形式存在,70-80%碳是以a-C:H形式存在,这是HL-1M装置 相似文献
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报导了采用全MOCVD生长的1.55μm的单片集成DFB=LD/EA组件的 在DWDM系统上的传输测试结果,出纤功率Pf≥2.5mW@If=75mA,边模抑制比SMSR〉35dB,调制器反向偏压为2.5V时的消光比为14dB,该发射模块在2.5Gb/sDWDM系统上进行了传输试验,传输240Km后无误码,其通道代价≤1dB@BER=10^-12。 相似文献
6.
张湘义 《理化检验(物理分册)》1995,31(2):28-29,44
对Fe73.5Cu1Mo3Si13.5B9微晶软磁合金的结构及其对合金磁性的影响了研究,结果表明,在最佳磁性能下,晶相点阵常数a=0.2843nm,相当于Fe(Si)固溶体中含Si%(mol/mol):18-20,体积百分数V=74.8%,晶粒尺寸D=14.6nm;残余非晶层厚度δ=1.23nm;当T退火≥560℃时明显有Fe-B化合物析出。Fe73.5Cu1Mo3Si13.5B9合金的磁性不仅与 相似文献
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立方A^4+M^5+2O7型化合物与新型负热膨胀材料 总被引:1,自引:0,他引:1
概述了立方A^4+M^5+2O7型化合物的结构特点,讨论了AV2-xPxO7型(A=Zr或Hf;x=0.1~1.2)及其部分取代的A^4+1-yB^4+yV2-xPxO7型(B=Ti,Ce,Th,U,Mo,Pt,Pb,Sn,Ge或Si;y=0.1~0.4)和A^4+1-yC^1+yD^3+yV2-xPxO7型(C为碱金属元素,D为稀土金属元素)材料的负热膨胀性能。 相似文献
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旋转CVI制备C/SiC复合材料 总被引:2,自引:0,他引:2
旋转 CVI是在 CVI原理基础上发展的一种制备 C/SiC复合材料的新工艺,通过石墨衬底的旋转,使预制体的制备与基体的沉积同步进行,能有效消除一般CVI工艺过程中存在的“瓶颈”效应.在自制的旋转 CVI设备上实验,探索了旋转 CVI工艺参数中 CH3SiCl3(MTS)的流量与浓度、沉积温度和C布缠绕线速度对SiC基体沉积速度,以及沉积温度对基体结构的影响.并在低压(5kPa)、高温 (1100℃)、 400 mL·min-1 H2、 200 mL·min-1Ar、 MTS40℃与C布以1.1~3.5mm·min-1的线速度连续旋转的沉积条件下,实现了单丝纤维间微观孔隙、纤维束之间以及C布层间宏观孔隙的致密化同步完成. 相似文献
11.
Pawan Tyagi 《Thin solid films》2011,519(7):2355-2361
Application of the economical metal oxide thin-film photovoltaic devices is hindered by the poor energy efficiency. This paper investigates the photovoltaic effect with an ultrathin tantalum oxide (TaOx) tunnel barrier, formed by the plasma oxidation of a pre-deposited tantalum (Ta) film. These ~ 3 nm TaOx tunnel barriers showed approximately 160 mV open circuit voltage and 3-5% energy efficiency, for varying light intensity. The ultrathin TaOx (~ 3 nm) could absorb approximately 12% of the incident light radiation in 400-1000 nm wavelength range; this strong light absorbing capability was found to be associated with the dramatically large extinction coefficient. Spectroscopic ellipsometry revealed that the extinction coefficient of 3 nm TaOx was ~ 0.2, two orders higher than that of tantalum penta oxide (Ta2O5). Interestingly, refractive index of this 3 nm thick TaOx was comparable with that of stochiometeric Ta2O5. However, heating and prolonged high-intensity light exposure deteriorated the photovoltaic effect in TaOx junctions. This study provides the basis to explore the photovoltaic effect in a highly economical and easily processable ultrathin metal oxide tunnel barrier or analogous systems. 相似文献
12.
V K Jain Amita Gupta C R Jalwania Adarsh Kumar G K Singhal O P Arora D S Ahuja P P Puri R Singh M Pal 《Bulletin of Materials Science》1994,17(5):551-561
Efforts have been made to see the effect of some standard microelectronic processing steps on porous silicon. Our diffusion
experiments for making p-n junctions confirm that this material can withstand high temperatures of the order of 800°C to 1000°C.
A new technique for photolithography has been suggested to obtain porous silicon in selected areas. Etch stop method to control
the thickness of the porous layer and an organic protective layer for porous silicon have also been suggested. Models proposed
by other workers to explain luminescence in porous silicon are not sufficient to explain many experimental observations. A
hybrid model is suggested. 相似文献
13.
The behavior of a superconducting tunnel junction detector (STJ) in the regime of low excitation is described, and the characteristic times of the dynamical response are discussed. The effect of a proximity layer in the STJ is analyzed in terms of the McMillan model. A set of phenomenological equations for the proximized STJ driven out of equilibrium is obtained, showing the importance of the role of the proximity effect in the dynamics of the device. 相似文献
14.
Leonid Kuzmin 《Journal of Low Temperature Physics》2008,151(1-2):292-297
A novel concept of a Superconducting Cold-Electron Bolometer (SCEB) with Superconductor-Insulator-Weak Superconductor (SIS’)
Tunnel Junction and Josephson Junction has been proposed. The main innovation of this concept is utilizing the Josephson Junction
for DC and HF contacts, and for thermal isolation. The SIS’ junction is used also for electron cooling and dc readout of the
signal. The SIS’ junction is designed in loop geometry for suppression of the critical current by a weak magnetic field. The
key moment of this concept is that the critical current of the Josephson junction is not suppressed by this weak magnetic
field and can be used for dc contact. Due to this innovation, a robust two layer technology can be used for fabrication of
reliable structures. A direct connection of SCEBs to a 4-probe antenna has been proposed for effective RF coupling.
相似文献
15.
Collective pinning phenomena of vortices in Josephson junction networks (JJN) in magnetic fields are studied using numerical simulations. We consider two kinds of structure of JJN: a ladder (Josephson junction ladder, JJL) and a two-dimensional square array (Josephson junction array, JJA). For the JJL and JJA with distribution of the strengths of junction critical currents, we investigate the critical current of vortex depinning in the presence of bias currents. On the basis of a theory of collective vortex pinning, it is found that the critical currents for both JJL and JJA show a universal scaling behavior. 相似文献
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We investigated static magnetic flux dynamical properties of one-dimensional lattices of Josephson junctions. The discretized wave equations of the Josephson junction lattice were solved using a generalized relaxation iteration algorithm. Numerical simulations indicated that transitions between periodic state and chaotic state will occur as the physical parameters and geometric parameters such as external current y
n, magnetic field h
0, h, and the length of Josephson junction
n
and d
n
, varied. A shot length of the Josephson junction favors stable periodic states. 相似文献
18.
We have investigated electrical conductance of the single C60 and benzene molecules bridging between metal electrodes. The single C60 and benzene molecular junctions were prepared in ultra high vacuum. The single molecular junctions showed the high conductance values (around 0.1–1 G0: G0 = 2e2/h), which were comparable to that of the metal atomic contact. The highly conductive single molecular junctions could be prepared by direct binding of the π-conjugated organic molecule to the metal electrodes without the use of anchoring groups. For comparison, the single 1,4-benzenediamine molecular junction was investigated in solution. The benzene molecule was bound to the Au electrodes via amine (anchoring group) for the single 1,4-benzenediamine molecular junction. The conductance of the single 1,4-benzenediamine molecular junction was 8 × 10−3G0. It was suggested that the anchoring groups acted as resistive spacers between the molecule and metal. 相似文献
19.
The numerical analysis of the excitation of the Josephson junction (Jj) by an external electromagnetic field has been reported. The fully nonlinear approach requires using the quasiperiodic solutions of the sine-Gordon equation (sGe) which are expressed by the Riemann theta functions. Their local soliton approximation of the nondissipative Jj is presented. Using the self-consistent phenomenological model of a long Jj, the influence of the external electromagnetic field on the volt-ampere characteristics is considered. 相似文献