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1.
X-band Gunn diode amplifiers have been tested while exposed to pulsed ionizing radiation. Peak photo currents induced vary as the .65 power of the dose rate, as had been found for oscillator diodes. The principal effect is a transient loss of gain, with the recovery time less than 400 ns for dose rates up to 5×1010 rad (Si)/s. The dependence of gain on dose rate agrees very well with a calculation based on the change in electric field distribution caused by radiation-induced excess carriers. A permanent failure mode was also observed at the maximum operating voltage and dose rate. 相似文献
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M. Z. Khan S. Ahmad M. Zakaullah A. Waheed R. Ahmad G. Murtaza 《Journal of Fusion Energy》2002,21(3-4):211-215
A compact diode comprising a flat plate anode and a sharp-edged cathode (a piece of razor blade) energized by 0.5 F capacitor charged to 30 kV is investigated for optimization of X-rays emission vis-à-vis separation between electrodes and width of the cathode, which is responsible for electron emission by impact of electric field. It is a high-inductance system, the parasitic inductance is found to be 353 ± 5 nH, and the recorded peak discharge current is just 35 ± 02 kA. The maximum X-ray emission is observed for a 2-mm-wide cathode with an interelectrode separation of 3 mm. The X-ray yield in 4-geometry is found to be 34 ± 3 mJ with a wall-plug efficiency of 0.015 ± 0.001%. The X-ray emission occurs about 200 ns after the application of high voltage, synchronized with the dip in current wave form. The low efficiency of the system for X-ray generation is attributed to high parasitic inductance. 相似文献
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碳化硅结势垒肖特基二极管(SiC JBS)是新一代航天器电推进系统的关键部件,但高能粒子辐射严重威胁其可靠性与稳定性。为揭示其辐射损伤机理,为其抗辐射加固设计与考核评估储备数据,本研究基于加速器开展了先进商用SiC JBS 10~20 MeV中能质子地面辐照实验,并提取器件辐照前后的正向伏安特性、反向伏安特性、电容电压等电学参数及缺陷特性。系统分析器件关键特性随辐照条件的改变规律。结果显示,质子辐照引起了器件肖特基势垒升高、载流子浓度降低,且10 MeV较低能质子导致的位移损伤退化更严重。分析认为,PN结界面缺陷导致高性能商用SiC JBS反向电学性能对中能质子的辐照更加敏感,正向特性相对稳定,辐照生碳缺陷造成载流子去除效应是引起SiC JBS性能退化的主要机制。 相似文献
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陈盘训 《核电子学与探测技术》1987,(2)
在中子辐照环境下,变容二极管C—V特性发生变化,在给定偏置下,结电容随中子注量的增加而下降。它是因外延层中引入深俘获能级所致,在高中子注量下,漏电流和正向压降均变大,优值Q也发生变化。 相似文献
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《Journal of Nuclear Science and Technology》2013,50(6):433-437
Radiolysis of N2O adsorbed on silica gel degassed at 200, 450 and 600°C has been studied to investigate the behavior of electrons on the gel surface. The G-value of nitrogen as the major radiolytic product increases with an increase of N2O concentration adsorbed approaching a plateau value which depends on degassing temperature of the gel prior to irradiation. By the competitive electron scavenging of N2O with several electron scavengers, such as CCl4, SF6 and nitrobenzene, initial yield of electrons G (e ?), and relative rate constant for reaction of electrons with scavenger to that with N2O, k s /k N2O, have been obtained. The G (e ?) is 3.8 and 2.0 for the gel degassed at 200 and 600°C respectively. In the former gel, the value of k s /k N2O is comparable with that in aqueous system, while in the latter, with that in non-polar hydrocarbon such as neopentane. The observed difference may be attributed to the presence of silanol groups and residual water which facilitate some form of hydration of electrons on the gel degassed at low temperature. Despite of the complexity of the heterogeneous system, Hammett's relationship is observed among the reactions of electrons with monosubstituted derivatives of benzene, providing the reaction constant ρ as 2.8. 相似文献
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Buried channel CTD's must be designed to isolate their depleted channels from charge generated in the substrate by penetrating radiation to obtain optimum transient radiation hardness or radiation detector time response. This can be achieved by employing an NPN structure so that the electrons generated in the N substrate are confined by the reverse biased P-N junction from diffusing across the P layer to the N channel. Unfortunately, moderate doped P layers often do not have the necessary conductivity required experimentally to pin the junction bias during intense transient radiation. However, the use of P+ layers is shown to accomplish this purpose. Although buried channel CTD's are used as experimental examples, the principles are applicable to a wide range of MOS charge storage devices. One potential application is in the reduction of alpha particle induced soft errors associated with conventional packaging. This soft error problem is a significant issue in future small cell VLSI development. 相似文献
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There are many cathode electron emission mechanisms which have been discussed [1]. But in arc discharge ) the thermionic and the field emission playan important role. The electron emission has influence on the properties of cathode fall region, whichcan be divided into two subzonesf space charge zoneand ionization zone [21. In this paper, the spacecharge zone is called cathode sheath (CS). The cathode sheath, being nearest to the cathode surface, isaffected by the electron emission first. Th… 相似文献
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《中国原子能科学研究院年报(英文版)》2016,(0)
正In recent years,with the rapid development of space industry,the stability of the space equipment caught the attention of people.The semiconductor industry continues to scale CMOS technologies to smaller feature sizes with reduced operating voltages in pursuit of performance and density goals.Continuing decreases in device dimension 相似文献
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利用2×6 MV串列静电加速器提供的1~10 MeV质子,开展了线阵电荷耦合器件辐射损伤效应的模拟试验和测量,研制了加速器质子扩束扫描装置及电荷耦合器件辐射敏感参数测量系统,建立了电荷耦合器件质子辐射效应的模拟试验方法,分析了质子注量、质子能量、器件偏置等对器件电荷转移效率和暗电流的影响。模拟试验结果表明,电荷转移效率随辐照质子注量的增加而下降,暗电流随辐照质子注量的增加而增大,在1~10 MeV质子能量范围内,质子能量越低,电荷转移效率的降低与暗电流的增加越显著。 相似文献
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Narendra Kr. Singh Ranojoy Bhattacharya Hasina Khatun Udaybir Singh A. K. Sinha 《Journal of Fusion Energy》2012,31(3):205-210
This paper presents the design study of toroid shape filament heater for dispenser cathode.The filament heater will be used
in cathode assembly of 200 kW 42 GHz gyrotron. A 3 D model of cathode assembly is designed using electromagnetic and thermal
simulation software, ANSYS. The simulations are performed for optimizing the input filament heater power with respect to cathode
surface temperature. The parametric study shows that the input power and cathode surface temperature depends strongly on the
potting material, diameter of filament, number of turns, position and height of the filament heater with respect to cathode
pellet. The design analyses are also carried out for two different filament heater materials i.e. tungsten and molybdenum.
Further, the thermal, structural and transient analyses are also carried out to study the mechanical strength of the filament
heater. It is concluded that the input heater power should be greater than 200 W to achieve cathode surface temperature greater
than 1,000°C. 相似文献
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(20-300)kV X射线参考辐射装置的建立 总被引:1,自引:0,他引:1
为了推进X射线空气比释动能基准量值传递工作的开展,建立了(20-300)kV X射线参考辐射装置。距离X光管焦点1 m的均匀野处,建立了CCRI会议推荐的两组低能X射线参考辐射质50kV(a)和50 kV(b),采用拟合方法测量得到的半值层、同质系数与推荐值相差2%以内。通过蒙卡模拟软件EGSnrc研究两组参考辐射质的能谱分布情况,并计算了其平均能量,分别为33.3和28.1 keV。 相似文献
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Design considerations have been developed for a compact ignition test reactor (CITR). The objectives of this tokamak device are to achieve ignition, to study the characteristics of plasmas that are self-heated by alpha particles, and to investigate burn control. To achieve a compact design, the toroidal field magnet consists of copper-stainless steel plates to accommodate relatively high stresses; it is inertially cooled by liquid nitrogen. No neutron shielding is provided between the plasma and the toroidal field magnet. The flat-top of the toroidal field magnet is 10 s. Strong auxiliary heating is employed. In one design option, adiabatic compression in major radius is employed to reduce the neutral beam energy required for adequate penetration; thiscompression boosted design option has a horizontally elongated vacuum chamber; illustrative parameters are a compressed plasma witha=0.50 m, R=1.35 m,B
T
=9.1 T, and a neutral beam power of 15 MW of 160 keVD
0 beams. A design option has also been developed for alarge bore device, which utilizes a circular vacuum chamber. Thelarge bore design provides increased margin and flexibility; both direct heating with RF or neutral beam injection and compression boosted startup are possible. The large bore design also facilitates the investigation of high-Q driven operation. Illustrative plasma parameters for full use of the large bore area=0.85 m,R=1.90 m, andB
T
=7.5 T. 相似文献
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《等离子体科学和技术》2016,18(9):918-923
Plasma source is the most important part of the laboratory plasma platform for fundamental plasma experimental research. Barium oxide coated cathode plasma source is well recognized as an effective technique due to its high electron emission current. An indirectly heated oxide coated cathode plasma source has been constructed on a linear magnetized plasma device. The electron emission current density can reach 2 A/cm 2 to 6 A/cm 2 in pulsed mode within pulse length 5–20 ms. A 10 cm diameter, 2 m long plasma column with density 10 18 m −3 to 10 19 m 3 and electron temperature Te ≈ 3–7 eV is produced. The spatial uniformity of the emission ability is less than 4% and the discharge reproducibility is better than 97%. With a wide range of the plasma parameters, this kind of plasma source provides great flexibility for many basic plasma investigations. The detail of construction and initial characterization of oxide coated cathode are described in this paper. 相似文献
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Radiation testing was performed on a number of specific memory devices representative of the major LSI process technologies to address the problem of selection of suitable memories for hardened mircroprocessor based systems. Responses to dose-rate and total-dose irradiation were obtained using the Boeing Linac and Gammacell cobalt facilities. The devices chosen for testing were the Intel 2147 4K and 2125H 1K HMOS RAMs, the American Micro Systems 4017 4K VMOS RAM, the Fairchild 93471 4K TTL/ECL RAM, the Harris 6508 1K hard oxide CMOS RAM, the Harris 6611 256×4 CMOS PROM, the Intersil 6604 512×8 CMOS EPROM, and the Fairchild 93481 4K TTL/I2L dynamic RAM. Test methods are described and results are summarized for each. 相似文献
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241Am-Be中子源被广泛用于实验研究,为保护实验人员免受中子及γ射线照射,需要设计适当的屏蔽。利用蒙特卡罗方法计算中子透射不同材料后的能谱分布与剂量,优选各层屏蔽材料种类与厚度,设计一套241Am-Be中子源紧凑型屏蔽装置。装置由内而外采用钨+聚乙烯+含硼聚乙烯+不锈钢进行防护,外表面周围剂量当量率H*(10)低于10μSv/h,满足辐射防护要求。同时对装置内部热中子、超热中子和快中子注量分布进行研究,确定装置快中子和热中子输出通道最佳位置。在辐照装置同时开放快中子和热中子通道进行实验测试时,需要设置距离大于130 cm的控制区,以保障操作人员安全。 相似文献
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国际标准化组织核能标准化委员会辐射防护分委员会(ISO/TC 85/SC2)最近编制了几个有关辐射防护中子测量装置校准的标准,其中ISO8529规定了参考中子辐射的特性和产生方法、辐射场校准以及场所和个人中子剂量仪(计)校准和响应的确定;此外,ISO12789—2002规定了利用模拟中子辐射场对辐射防护中子测量装置的校准。本文介绍ISO8529系列标准的主要内容及一些相关问题。 相似文献