KT—5C托卡马克离子伯恩斯坦波功率发射系统

本文概述了在ＫＴ－５Ｃ托卡马克上研究非线性离子伯恩斯坦波用的新型射频波功率发射系统，给出了工作频率选择和稳定、射频功率的传输调节、脉冲响应、耦合网络及其阻抗变换、移动式天线等实验结果，还给出了测量天线真空负载阻抗的一种简便方法，讨论了有关结果。     

标签密集环境下天线互偶效应研究

基于射频识别技术原理及Friis传输方程, 导出了无源超高频射频识别系统链路模型, 结合二端口网络分析方法, 导出了标签密集环境下的标签天线互阻抗计算表达式.利用单阅读器单标签时的标签阻抗匹配条件, 基于功率传输系数及调制因子, 分析了互偶效应对系统链路的影响.在开阔室内环境中, 测试了双标签及标签单、双平面布置情形下的阅读器天线最小发射功率及系统识别率.测试结果表明, 双标签及双平面情形下, 阅读器天线最小发射功率变化率分别为(-7%, 11.6%)及(-10%, 12.5%). 关键词： 射频识别 密集环境 互偶效应 互阻抗     

硅薄膜沉积中等离子体辉光功率和阻抗的测试分析

采用改进的电压和电流测试方法对衬底电极外加不同电压V_s的射频等离子体中的阻抗和功率消耗进行了测试分析.结果表明：在射频电极施加恒定的电压V_el时，随衬底电极外加电压V_s的增加，辉光的电流在增加，结果导致阻抗在减小；另外，通过计算分析发现：仅有一小部分功率用于辉光，大部分功率消耗在匹配器和电缆上.通过对等离子体电学特性的综合测试分析也说明：在保证有足够多的硅烷时，衬底电极外加电压V关键词： 等离子体 辉光功率 阻抗 诊断     

KT—5C托卡马克射频波加热实验用回路天线的负载阻抗测量

针对ＫＴ－５Ｃ托卡马克装置等离子体的射频离子回旋波加热实验，本文给出一种回路天线负载阻抗的简便测量方法和测量结果。该方法的特点是，只涉及射频电流相对比值的测量，不要求专用设备，因此使物理量的标定、数据记录和处理都变得简单易行。     

ICRH射频系统二次实验匹配法的分析

本文提出了在大功率射频发射系统中对一个未知的天线负载，可用二次实验数据来确定双Ｔ调配器的参数，以达到射频源和天线负载间的匹配。文中详细地讨论了这种高配法的理论并给出了用以实验的解析公式。     

无源射频识别系统中的雷达截面分析与计算

基于无源射频识别技术原理和天线散射理论,导出了不同负载情况下的雷达截面计算方法,并结合雷达截面和电磁传播环境分析了无源射频识别系统的识别距离.通过测量标签天线不同负载情况下的反向散射功率,再结合该计算方法,从而得出雷达截面.理论分析与实验测量结果保持一致.研究结果对优化无源射频识别系统的标签性能有益. 关键词： 射频识别 天线 雷达截面 识别距离     

碳纳米管光混频器产生太赫兹功率的理论分析

以光混频器电路模型为基础,理论分析了碳纳米管(CNT)材料光混频器产生太赫兹功率的大小.通过对光混频器电导、天线的阻抗和外加偏置电压的模拟结果表明:提高光混频器电导、天线阻抗和外加偏置电压都能够提高输出太赫兹波功率,在小信号输入条件下,输出功率理论上能够达到数十微瓦.     

射频电感性耦合等离子体调谐基片自偏压特性

采用调节射频电感性耦合等离子体中基片电极与地之间的外部电路阻抗的方法，控制基片电极的射频自偏压。研究了调谐基片自偏压随外部调谐电容值的变化特征，得到了调谐基片射频自偏压随射频放电功率、气压的变化曲线。在一定放电参数区域内，调谐基片射频自偏压随调谐电容的变化曲线呈现跳变、双稳、迟滞现象。     

2 MHz/80 kW离子源射频功率耦合系统的设计

介绍了一种用于大科学工程装置中国散裂中子源(CSNS) 功率升级的RF负氢离子源大功率射频功率耦合系统的研制。主要内容包括射频功率耦合系统的构造, 指标计算分配以及具体实现, 重点阐述了射频功率放大器、隔离变压器、阻抗变压调谐器以及配套的电源、控制和冷却系统的设计, 并对整个系统的结构和热设计提出了工程解决方法。针对离子源功率耦合系统的特点作了细致的分析, 并以此为基础, 研制出了一款输出功率达80kW的射频功率耦合系统产品。     

CSNS射频负氢离子源控制系统研制

为满足中国散裂中子源打靶功率提升需求，加速器采用外置天线射频负氢离子源替换此前使用的潘宁表面负氢离子源，为加速器提供高品质和高稳定的束流。文章主要介绍了基于EPICS软件系统和PLC硬件平台的射频负氢离子源控制系统设计方案和具体实现。针对射频功率源的电磁干扰和高压平台打火造成设备损坏，给出了相应的解决措施。此外，为提高离子源长期运行稳定性，设计了放电室高精度注铯控制程序及打靶功率稳定程序。控制系统自投入运行以来，运行稳定可靠，为离子源的高效运行提供了有力保障。     

Low frequency double electron muon resonance (Demur) in fused quartz

Double electron muon resonance was studied with comparable amplitudes of the static and rf magnetic fields. The experiments were carried out in fused quartz and employed a resonant linearly-polarized rf field and a small static field. For small amplitudes of the rf field a three-line frequency spectrum was obtained consisting of a central line at the rf frequency and two weaker lines of equal amplitude symmetrically positioned about the central line. A symmetrical three line spectrum is predicted for muonium using the rotating wave approximation (RWA). For large rf fields the amplitudes of the three lines were not symmetric and depended on whether positrons were observed parallel or perpendicular to the beam. For very large rf fields the total amplitude of all the lines was less than for lower rf fields. These results do not agree with the theory using the RWA and no satisfactory theory currently exists.     

Frequency dependence of the radio frequency collapse effect

A systematic study of the dependence of the radio frequency (rf) collapse effect on the frequency of the rf field which induces the fast relaxation of the hyperfine field was performed for Permalloy and amorphous Fe₄₅Ni₃₀Si₁₀B₁₅ alloy. The rf collapse was studied for the frequency range of 12 MHz to 64 MHz. The results show that the rf collapse appears gradually in both materials as the rf field frequency exceeds the Larmor frequency what is in agreement with the model predictions.     

Harmonic and subharmonic shapiro steps in orthorhombic Tas3

Observation of harmonic and subharmonic Shapiro steps in orthorhombic TaS₃ in the presence of combined rf and dc drive is reported, demonstrating that both the harmonic and subharmonic steps are a general characteristic of charge-density-wave response. Compared to NbSe₃, the noise spectrum is typically much broader in TaS₃, leading to poorly defined steps at small rf voltages. The steps sharpen with larger amplitudes of rf. Increased rf amplitude is also accompanied by an increase in the CDW current density at a given step, but this increase approaches a limiting value for large rf levels. The results are interpreted as evidence for increased coherence of the CDW response in the presence of large rf driving fields.     

The rf coil as a sensitive motion detector for magnetic resonance imaging

A new sensor principle for detection of patient movement in magnetic resonance imaging has been successfully applied for the reduction of motion artifacts. It uses a device that is already present in every MRI system, namely the rf coil. Patient movement within the coil causes changes in the rf impedance match of the coil, which can be measured as variations in the reflected rf power. The principle used for the detection of respiratory and cardiac motion is described, and experimental results measured with several coil arrangements are given. Images are presented which were acquired with respiratory gating derived from the rf body coil of a 2 Tesla whole body MRI system.     

Spectral hole burning for wideband, high-resolution radio-frequency spectrum analysis

We present experimental results for what is to our knowledge the first spectral-hole-burning based rf spectrum analyzer to cover 10 GHz of rf analysis bandwidth. The rf signal of interest is modulated onto an optical carrier, and the resultant optical sidebands are burned into the inhomogeneously broadened absorption band of a Tm3+:YAG crystal. At the same time a second, frequency-swept laser reads out the absorption profile, which is a double-sideband replica of the rf spectrum, and thus the rf spectrum can be deduced after spectral calibration of the nonlinear readout chirp. This initial demonstration shows spectral analysis covering 10 GHz of bandwidth with >5500 spectral channels and provides 43 dB of dynamic range.     

关于热阴极微波电子枪中电子反轰问题的研究

 提出了热阴极微波电子枪的设计中可以通过缩短腔长减小电子反轰功率，并通过模拟计算详细研究了腔长对电子反轰及枪出口束流品质的影响。     

N2��Ƶ�ŵ��������(e,N2+, N+)��PIC-MCģ��

采用PIC-MC自洽模型,模拟了氮气电容性耦合射频放电的微观等离子体过程及带电粒子(e,N2+,N+)的行为。结果表明,离子(N2+,N+)的运动状态滞后瞬时射频电场的变化;在两极附近,N2+具较高密度,但能量较低,N+具较低的密度但能量较高,两者的密度差6倍左右。两种离子轰击射频电极的能量分布变化规律类似,随放电参数变化,离子(N2+,N+)能量变化显著,其密度变化不明显。模拟的电子能量几率分布与测量结果一致。     

The collapse effect of Mössbauer spectra in radio frequency fields

The Collapse effect of amorphous alloys Fe38Ni38Mo4B20 and Fe48Ni31Si10B11 in the rf field was investigated by means of the measurement of the temperature of the samples in rf field and the observations of aftereffect of the strong rf field. The collapse observed is caused by rf induced magnetic fluctuation rather than thermal effects. The results agree well with the model based on a magnetic cluster picture.     

Velocity sensitivity of slice-selective excitation

The purpose of this study was to investigate how flow affects slice-selective excitation, particularly for radiofrequency (rf) pulses optimized for slice-selective excitation of stationary material. Simulation methods were used to calculate the slice profiles for material flowing at different velocities, using optimal flow compensation when appropriate. Four rf pulses of very different shapes were used in the simulation study: a 90° linear-phase Shinnar-LeRoux pulse; a 90° self-refocusing pulse; a minimum-phase Shinnar-LeRoux inversion pulse; and a SPINCALC inversion pulse. Slice profiles from simulations with a laminar flow model were compared with experimental studies for two different rf pulses using a clinical magnetic resonance imaging (MRI) system. We found that, for a given rf pulse, the effect of flow on slice-selective excitation depends on the product of the selection gradient amplitude, the component of velocity in the slice selection direction, and the square of the rf pulse duration. The shapes of the slice profiles from the Shinnar-LeRoux pulses were relatively insensitive to velocity. However, the slice profiles from the self-refocusing pulse and the SPINCALC pulse were significantly degraded by velocity. Experimental slice profiles showed excellent agreement with simulation. In conclusion, our study demonstrates that slice-selective excitation can be significantly degraded by flow depending on the velocity, the gradient amplitude, and characteristics of the rf excitation pulse used. The results can aid in the design of rf pulses for slice-selective excitation of flowing material.     

光泵磁共振信号幅度与射频场振幅的关系

在光泵磁共振实验中观测到单量子跃迁共振信号幅度随射频场振幅增加而迅速增加,并很快达到饱和,然后单调缓慢下降的关系.当射频场振幅更大时(约大于3.5V),观测到双量子跃迁共振信号,信号幅度与射频场振幅成二次函数关系.本文对实验结果进行了分析和解释.