电子束注入简单磁镜中被电子迴旋共振加热捕获的实验研究

在简单磁镜MM-2中,在采用15GHz大功率迴旋管进行电子迴旋共振加热(ECRH)的同时,以不同的方式向磁镜中注入电子束,进行了ECRH捕获电子束的实验研究。结果表明:由于电子束的提前注入,等离子体的预电离时间被大大地缩短。由上ECRH对电子束的捕获,使得热电子环参数得到很大的改善,热电子环的反磁β值约增加62%,对应反磁增加的捕获效率约为(30—40)%。在迴旋管输出约30kW的条件下,适应建立热电环的气体压力窗为(4.67—21.3)×10^-4Pa。 关键词：     

用碘化钠探测器研究简单磁镜装置MM—2中热电子环特性

使用碘化钠(NaI)探测器,对MM-2简单磁镜装置中热电子环参数进行了测量,得到热电子温度为140—170keV,热电子环的半径为7cm,其径向厚度为4cm,轴向尺寸边缘区域从±10cm延伸至±20cm,同时也观测到了热电子密度沿径向分布,环的位置与磁场强度的关系以及硬X射线发射的时间特性。     

异亮氨酸的真空紫外光电离和光离解

利用同步辐射光电离质谱结合理论计算, 研究了异亮氨酸的真空紫外光诱导电离解离．在光子能量为13 eV的质谱中探测到了m/z=86、75、74、69、57、46、45、44、41、30、28、18的碎片离子．对于异亮氨酸的主要碎片离子为：C₅H₁₂N⁺ (m/z=86)、C₂H₅NO₄⁺ (m/z=75)、C₅H₉⁺ (m/z=69)、C₄H₉⁺(m/z=57)和CH₄N⁺(m/z=30)．由光电离效率曲线得到出现势分别为：8.84±0.07、9.25±0.06、10.20±0.12、9.25±0.10、11.05±0.07 eV．结合量化理论计算(B3LYP/6-31++G(d,p)),详细给出了它们可能的生成路径．这些解离通道包括简单的键断裂反应和涉及中间体、过渡态的反应,实验值和理论计算的离子出现能或势垒一致．     

热电子、双离子成分对离子漂移迴旋不稳定性的影响

分析了热电子、温(热)离子成分对离子漂移迴旋不稳定性的影响。给出了临界稳定热电子成分值α与温(热)离子成分值、离子温度比和离子抗磁漂移速度的关系;讨论了热电子、温(热),冷离子成分对不稳定性各谐频分支的影响;分析了热电子成分稳定作用的物理机制。     

热电子环结构对阱深和贮能影响的分析

简单磁镜MM-2ECH实验产生的热电子环未能在磁镜中形成磁阱。反磁信号△V为15cmV时,热电子环垂直方向贮能W。为0.317J,最大β_(⊥,max)为1.6％,热电子环在中平面径向平均β⊥为0.9％。局域使增量△B为零,或使增量△∮dl/B为零所需热电子环的贮能W和β_(⊥,max)与热电子环结构(厚度、宽度和位置)有关。     

硅的低温电学性质

本文在20°—300°K研究了室温载流子浓度2×10¹²—1×10²⁰cm^-3含硼或磷(砷)Si的电学性质。对一些p-Si样品用弱场横向磁阻法及杂质激活能法进行了补偿度的测定,并进行了比较。从霍尔系数与温度关系的分析指出,对于较纯样品,硼受主能级的电离能为0.045eV,磷施主能级为0.045eV,在载流子浓度为10¹⁸—10¹⁹cm^-3时发现了费米简并,对载流子浓度为2×10¹⁷—1×10¹⁸cm^-3的p-Si及5×10¹⁷—4×10¹⁸cm^-3的n-Si观察到了杂质电导行为。从霍尔系数与电导率计算了非本征的霍尔迁移率。在100°—300°K间,晶格散射迁移率μ满足关系式AT^-a,其中A=2.1×10⁹,α=2.7(对空穴);或A=1.2×10⁸,α=2.0(对电子)。另外,根据我们的材料(载流子浓度在5×10¹¹—5×10²⁰cm^-3间),分别建立了一条电阻率与载流子浓度及电阻率与迁移率的关系曲线,以提供制备材料时参考之用。     

对69Krβ延迟质子衰变的观察

通过对³²S+Ca反应中衰变质子谱的观测,发现了一组新的质子谱线,其能量为(4.07±0.05)MeV,对应的衰期为(32±10)ms,经反应道分析及与理论预言比较,确定该质子活性来源于⁴⁰Ca(³²S,3n)反应产生的⁶⁹Kr的β延迟质子衰变,它相应于由⁶⁹Br中的T=3/2同位旋相似态到⁶⁸Se基态的质子跃迁.基于测量结果与库仑位移能计算,得到⁶⁹Kr的质量剩余为(－32.15±0.30)MeV,并提出了⁶⁹Kr的部分衰变纲图.     

14MeV钕的同位素反应截面的测量

报道了在13.5—14.6MeV中子能区用活化法以⁹³Nb(n,2n)^92mNb反应截面为中子注量标准测得的¹⁵⁰Nd(n,2n)¹⁴⁹Nd,¹⁴⁸Nd(n,2n)¹⁴⁷Nd和¹⁴²Nd(n,2n)¹⁴¹Nd的反应截面值.由13.5±0.2,14.1±0.1和14.6±0.2MeV中子引起的¹⁵⁰Nd(n,2n)¹⁴⁹Nd反应截面值分别为2037±85,1737±68,1657±65mb,¹⁴⁸Nd(n,2n)¹⁴⁷Nd反应截面值分别为1394±58,1416±54,1956±76mb,^{142Nd(n,2n)141Nd反应截面值分别为1501±59,1623±62,1764±111mb.单能中子由T(d,n)4He反应获得.文中还收集了已发表的数据以作比较.}     

160Gd(n,2n)159Gd和158Gd(n,p)158Eu反应截面测量

报道了在13.5—14.6MeV中子能区用活化法测得的¹⁶⁰Gd(n,2n)¹⁵⁹Gd和¹⁵⁸Gd(n,p)¹⁵⁸Eu的 反应截面值. 中子注量用⁹³Nb(n, 2n)⁹²m Nb反应截面得到. 由(13.5±0.2)MeV,(14.1±0.1)MeV和(14.6±0.2)MeV中子引起的¹⁶⁰Gd(n, 2n) ¹⁵⁹Gd反应截面值分别为(1940±83)mb, (2324±92)mb和(1983±77)mb, ¹⁵⁸Gd(n, p) ¹⁵⁸Eu反应截面值分别为(1.9±0.1)mb, (2.1±0.1)mb和(3.5±0.1)mb. 单能中子由T(d, n)⁴He反应获得.文中还列举了已收集到的数据以作比较.     

13.5—14.6MeV中子能区镓的同位素反应截面的测量

报道了在13.5—14.6MeV中子能区用活化法以⁹³Nb(n,2n)^92mNb反应截面为中子注量标准测得的⁶⁹Ga(n,2n)⁶⁸Ga,⁶⁹Ga(n,p)^69mZn,⁷¹Ga(n,p)^71mZn和⁷¹Ga(n,n′α)⁶⁷Cu的反应截面值.由(13.5±0.2),(14.1±0.1)和(14.6±0.2)MeV中子引起的⁶⁹Ga(n,2n)68Ga反应截面值分别为(794±31),(869±35)和(986±39)mb,⁷¹Ga(n,n′α)⁶⁷Cu反应截面值分别为(1.3±0.1),(1.7±0.1)和(2.5±0.1)mb.在中子能量为(14.1±0.1)MeV能量点,⁶⁹Ga(n,p)^69mZn反应截面值为(21.5±1.0)mb,⁷¹Ga(n,p)^71mZn反应截面值为(12.4±0.7)mb.单能中子由T(d,n)⁴He反应获得.文中还列举了尽可能收集到的数据以作比较.     

托卡马克微波预电离等离子体

使用回旋管系统产生的电子回旋波段的大功率微波在托卡马克中得到无电流等离子体。其电子密度达8×10¹²cm^-3,电子温度达50eV,粒子约束时间约为0.5ms,加热效率达25％以上。研究了对环向击穿的影响及加热机制。     

Spectroscopic diagnostics of carbon and aluminum laser-produced plasmas

VUV emission spectra of plasmas produced by focusing laser radiation with intensity of 10¹⁰–10¹¹ W/cm² on carbon and aluminum targets were studied. Using the partial local thermodynamic equilibrium model for an electron density exceeding 10¹⁷ cm^?3, the spectroscopic diagnostics and the analysis of ion composition of plasmas were carried out. The electron temperatures determined for carbon and aluminum plasmas from the ratio of intensities of ionic lines were found to be 8±3 eV and 11±4 eV, respectively. Stark broadening of aluminum lines was measured and parameters of electron broadening were determined. Using the spatially resolved measurement of Stark line broadening, the spatial density distribution and the law of electron gas expansion were found. The electron gas in the hot region of size 5 mm with an average density of (5±2) 10₁₇cm ^?3 experienced one-dimensional expansion according to the law 1/z ^1.1 with increasing distance z from the target.     

Spatial variation of the electron energy in a H. F. ring discharge

The electron temperature has been measured in inductively coupled high frequency gas discharges in Ar, Kr and Xe with the aid of Langmuir probes. The measured temperature shows a rather low radial space dependence up to values ofpR ≈ 30 Torr cm (p=gas pressure,R=radius of the discharge vessel). This behaviour is explained on the basis of the local energy balance of the electrons as a consequence of the energy transport by thermal conduction in the electron gas.     

Über Elektronendriftbeweglichkeit und Stoßionisierung in KBr-Kristallen bei hohen elektrischen Feldstärken

A swarm of electrons passing a KBr-crystal has been investigated by fast oscilloscopic techniques at high electric fields (3×10⁴ to 4×10⁵ V/cm). From the temporal current shape we determined the electron drift mobilityμ=15±2 cm²/Vsec, the electron life timeτ=2±0.3 × 10^?7 sec and the multiplication factor. From this measurement the ionization coefficientα for electrons was calculated as a function of the applied electric field.     

Axisymmetric quasi-optical gyrotron oscillator

An axisymmetric quasi-optical gyrotron (ASQUOTRON) is considered to realize a 10 MW, 150 GHz, CW oscillator required for an electron cyclotron resonance heating of a fusion plasma. The gyrotron has an axisymmetric mirror to be used as its optical cavity. It is shown that the axisymmetric mirror of relatively small radius (20 cm) can be used in producing the 10 MW continuous wave with a tolerable mirror heat load (0.5 kW/cm²). Considerations are also made on wave transmissions through the mirror and to a target.     

On plasma parameters of a self-organized plasma jet at atmospheric pressure

Electron temperature and electron concentration in the active zone of a miniaturized radio frequency (RF) non-thermal atmospheric pressure plasma jet in argon have been determined using two independent approaches: the spectroscopic measurement of the broadening of Balmer H_b_\beta and H_g_\gamma lines and a time-dependent, spatially two-dimensional fluid model of a single discharge filament. The plasma source has been configured as a capacitively coupled RF jet (27.12 MHz, 8 W generator output power) with two outer ring electrodes around a quartz capillary with diameter of 4.0 mm between which Ar flows at typical rates of 0.3 slm. The discharge has been operated in a self-organized mode, where equidistant, stationary filaments rotate regularly with a constant frequency at the inner wall of the outer capillary. For the purpose of calculating the spectral line broadening different models applicable at higher electron concentration have been evaluated. Resulting electron concentrations are between 2.2 and 3.3 × 1014 cm^-3. The calculation according to the line broadening model provides electron temperatures between 20 000 and 30 000 K which is in agreement with the results of the fluid model calculations. Here, a broad radial profile with a maximal value of about 22 000 K in the centre of the column and an electron concentration of about 7 × 10¹³ cm^-3 have been obtained. Moreover, the results of the model calculations reveal a structural change of the filament from the dielectric surface through the sheath to the column. The axially inhomogeneous region has an extension of about 0.5 mm. In the column a concentration of about 10¹³ cm^-3 has been found for the excited argon atoms, whose collisions with electrons represent the most important ionization channel there.     

X射线探测器的脉冲标定技术

利用强流电子束技术产生通量密度为10¹⁸—10¹⁹X-ray photon/sr·s的脉冲CuKX射线源,标定PIN型硅二极管半导体探测器对X光子的脉冲灵敏度。用绝对X射线监测器——P10气体脉冲电离室作为脉冲X射线通量密度的标准。脉冲电荷自动测量仪由微处理机进行程序控制,并予以实时校准。该电离室测量通量密度的精度为±5％,适用的能通量率范围可达4×10^-9—2×10²W/cm²,适用的光子能量范围为1.5—10keV,标定探测器的精度为±7.0％,并发现PIN型硅二极管的脉冲灵敏度比稳态X射线束标定的灵敏度高30％左右。 关键词：     

Influence of pressure on the relative population of the two lowest vibrational levels of the C <Superscript>3</Superscript> Π<Subscript>u</Subscript> state of nitrogen for electron beam excitation

Continuous and pulsed 12 keV electron beams were used to excite nitrogen within a gas cell at pressures ranging from 10 to 1400 hPa. The pressure dependence of the ratio of photon fluxes for emission from vibrational levels v'=0 and 1 of the C ³Π _u state has been studied. The results confirm the presence of a collisional excitation mechanism populating v'=0, 1 in addition to electron impact excitation. Rate constants of (1.27 ±0.04)×10^-11 cm³s^-1 [ v'=0] and (2.68 ±0.08)×10^-11 cm³s^-1 [ v'=1] were measured for C ³Π _u quenching by ground state nitrogen. For electron beam conditions relative excitation efficiencies of 1:0.59:0.22 for vibrational levels 0, 1 and 2 were calculated. The recorded flux ratios are compared with the predictions given by a vibrational relaxation model.     

A new approach for a multistage depressed collector for gyrotrons

A feasibility study for a two-stage depressed gyrotron collector has been performed. A new approach for an adiabatic magnetic decompression of the hollow electron beam has been used. It permits control of the radius of the constant magnetic flux surface, which determines the radial extension of the electron beam. Independent of the value of the magnetic field around the beam. For this purpose, either solenoidal coils or a ferromagnetic insert can be placed inside the hollow electron beam. Thus, the radial dimensions of a multistage depressed collector of a high-power high-frequency gyrotron can be kept within limits given by technological constraints. The energy sorting of the electron beam is improved by using electrodes inside the hollow electron beam for controlling the potential distribution. The additional control electrodes make it possible to eliminate almost all of the effect of secondary electrons on the operation of the collector. In order to demonstrate the proposed approach, a compact two-stage depressed collector has been designed for a 1.5-MW coaxial cavity gyrotron operating at 165 GHz in the transverse electric (TE)_31,17 mode, which is under development at FZK, Karlsruhe, Germany. Including the effect due to secondary electrons, a collector efficiency of 73% has been calculated with an average and peak heat dissipation density of about 240 W/cm² and 500 W/cm², respectively. This results in an increase of the output gyrotron efficiency from 36.5% to 62.6% when internal radio frequency (RF)-losses inside the gyrotron tube of 15% are taken into account