输入腔高频场的矩阵分析

 应用模匹配理论推导和建立了单级突变的矩阵方程，并分析给出了具有多级突变和渐变结构级联情况下波导腔体的处理方法。在理论推导的基础上，通过编制程序计算出多级突变结构波导腔体模匹配系数级联矩阵，并由矩阵参数得到所需的腔体谐振频率和Q值等物理特性参量。实际计算结果表明，由程序模拟输入腔计算得到的数据结果与腔体的冷测实验结果基本一致，为进一步的注波互作用研究和回旋速调管的设计工作提供了参考依据。     

回旋速调管加载损耗介质群聚腔的研究

 用模式场匹配理论建立了散射矩阵,数值模拟并分析了加载损耗介质层对群聚腔Q值、谐振特性以及群聚腔两端漂移段半径的大小对谐振特性的影响。研究表明：加载损耗介质在高频率下使群聚腔主要寄生模式EH₂₁₂和EH₃₁₁得到极大的抑制,对工作模式H₀₁模更有利;衰减常数随损耗层厚度的增加而迅速增加,Q值随介质厚度的增加迅速减小,因此在设计腔体时必须严格控制损耗材料厚度。最后为正在研制的回旋速调管设计了满足要求的低Q群聚腔,该腔冷测实验结果与计算结果基本一致。     

非均匀传输线型谐振腔的研究

 分析了周期性电容盘片加载的同轴线的传输特性,并将其应用于四分之一波长线谐振腔,利用传输线理论和数值模拟两种方法分析了这种腔体的谐振特性,得到了谐振频率、Q值与盘片半径、盘片个数间的关系,并论证了这种方法在减小腔体尺寸方面的可行性及在一台质子回旋加速器腔体中的应用。     

铁氧体环的导磁率及其品质因数的测量

 初级绕有线圈的铁氧体环形成电感,如果同时在其次级绕有偏磁线圈并加一直流电流,当此电流改变时,铁氧体导磁率会随之改变,绕有线圈的铁氧体环的电感量也就相应改变。加载了铁氧体环谐振腔的谐振阻抗与铁氧体导磁率、品质因数及腔体谐振频率的乘积成正比,而腔体谐振阻抗直接决定其所需功率的大小。讨论了铁氧体环导磁率和品质因数的测量原理,给出了测试装置的具体电路和测量结果。     

回旋速调管放大器输出腔的特性研究

 利用变截面波导的耦合模理论，根据输出腔中电场幅值分布函数所满足的微分方程组，编写了具有自动优化功能的计算程序，分析研究了不同渐变角度、考虑腔体损耗前后和输出腔与外电路失配时，谐振频率、腔体品质因数和高频场幅值沿轴分布的变化情况，为进一步研究高频场与电子注的互作用和输出腔奠定了基础。     

新型小铷钟微波腔谐振特性的研究

采用模匹配法对一种陶瓷介质填充的圆柱谐振腔TE₀₁₁、TE₁₁₁模的谐振特性进行了理论分析和软件仿真. 计算了该种谐振腔的谐振频率,并与其他理论方法得到的仿真结果进行了比较,验证了理论方法的正确性. 在此基础上,分析了陶瓷介质尺寸对谐振频率的影响. 与目前铷钟广泛使用的微波腔相比,该种谐振腔腔体的体积在很大程度上得到减小,这对于铷原子钟小型化的实现具有重要的作用.     

六面顶压机立方压腔内压强的定量测量及受力分析

将六面顶压机立方压腔内置入电路,采用原位电阻测量确定Bi,Tl,Ba相变的方法,标定了压腔内不同位置的压力(强).通过标定立方压腔顶锤表面的压力并结合计算,分别得到了外部加载与压腔密封边受力以及合成腔体受力的对应关系.实验分析结果表明,随着外部加载的增加,当腔体压力达到5 GPa时,消耗在压腔密封边上的加载急剧上升,消耗在合成腔体的加载趋于不变,从而导致立方压腔压力达到上限.利用实验结果,分析了立方压腔在高压下的受力状态,解释了立方压腔的压力难以超过7 GPa的原因.结合立方压腔的几何结构,通过理论分析,提出了采用高体弹模量的物质作为传压介质,同时采用低体弹模量的物质作为密封边提高立方压腔压力上限的可行方案.通过定量标定叶腊石压腔轴向的压力梯度,给出了压腔内沿对称轴不同位置压力值的计算方法,此方法可为高压实验提供更精确的压力数据.     

Helmholtz水声换能器弹性壁液腔谐振频率研究

针对传统Helmholtz水声换能器设计中刚性壁假设的局限性,将Helmholtz腔体的弹性计入到液腔谐振频率计算中,实现低频弹性Helmholtz水声换能器液腔谐振频率精确设计.基于细长圆柱壳腔体的低频集中参数模型,导出了腔体弹性引入的附加声阻抗表达式,得到了弹性壁条件下Helmholtz水声换能器等效电路图,给出了考虑了末端修正的弹性壁Helmholtz共振腔液腔谐振频率计算公式.利用ANSYS软件建立了算例模型,仿真分析了不同材质、半径、长度时的Helmholtz共振腔液腔谐振频率.结果对比表明弹性理论值与仿真值符合得很好,相比起传统的刚性壁理论计算结果,本文的弹性壁理论得出的液腔谐振频率值有所降低,与真实情况更加接近.本文的结论可以为精确设计低频弹性Helmholtz水声换能器提供理论支持.     

双间隙输出腔开放腔的高频特性分析

 建立了S波段相对论速调管放大器双间隙输出腔开放腔的3维模型。采用时域有限差分法，通过监测激励电流源的响应计算了该双间隙输出腔的谐振频率、有载Q值、场分布以及特性阻抗，并分析了腔体结构尺寸对谐振频率、有载Q值和特性阻抗的影响。研究表明：腔体半径对开放腔的谐振频率影响很大，耦合孔尺寸对腔体谐振频率的影响较小；随着耦合孔张角增加，有载Q值逐渐减小；随着腔体半径增大、间隙的减小，腔体特性阻抗降低。研究结果可为S波段强流相对论速调管放大器双间隙输出腔的设计提供理论依据。     

0.3 THz TM10, 1, 0模同轴耦合腔链

通过本征方程研究了工作在太赫兹(THz)频段的高次模同轴谐振腔,讨论了TM_{m, 1, 0}模,TM_{m, 2.0}模与TM_{m, 1, 1}模的谐振频率与腔体的几何参数之间的关系,并给出了工作模式的选择依据。在此基础上,提出了一种新型的0.3 THz TM_{10, 1, 0}模同轴耦合腔链,使用等效电路模型和CST-MWS软件对耦合腔链的色散特性、特征阻抗和电场分布等冷腔特性进行了分析和仿真,并着重分析和总结了耦合腔链的几何参数对色散特性和特征阻抗的影响。研究结果表明:对于工作在THz频段的高次模同轴耦合腔链,采用TM_{10, 1, 0}模为工作模式是合理的选择; 工作于2π腔模的0.3 THz TM_{10, 1, 0}模同轴耦合腔链具有较大的特征阻抗,但模式间隔较小,因此可将其应用于窄带太赫兹扩展互作用器件; 增大高次模耦合腔链的耦合槽张角是增大模式间隔的最佳途径。     

反馈调制型同轴虚阴极振荡器

 对反馈调制型同轴虚阴极振荡器进行了理论分析和数值模拟研究,结果表明:该器件通过增加同轴谐振腔结构并引入反馈可以对入射电子束形成明显的调制效果,从而使得器件具有高束波转化效率和频率单一稳定的特性;同时输出微波的频率被器件结构中的同轴谐振腔锁定,调节腔参数可以在一定范围内对输出微波频率进行调谐;在二极管电压约为600 kV,电子束功率26.2 GW条件下,可以得到平均功率3.6 GW的微波输出,转换效率达到13.7%,主频为5.5 GHz,模式为TM₀₂模。     

HIRFL-CSR实验环高频同轴谐振腔设计原理

介绍了同步加速器高频铁氧体加载腔体的设计原理和设计计算过程。 详细说明了腔体加载铁氧体材料的作用和意义, 并对传统的传输线理论计算结果、 CST(Computer Simulation Technology)软件模拟计算结果和实际腔体测量结果进行了比较。 In this paper, the principle and the process of design and calculation based on RF ferrite loaded coaxial cavity in synchrotron are presented. The function and significance of cavity loaded by ferrite are elaborated in detail. Then the calculated results by traditional transmission line theory, software simulated results by Computer Simulation Technology(CST ) and the actual cavity measured results are compared.     

同轴虚阴极振荡器数值模拟

 给出了同轴型虚阴极振荡器的数值模拟和部分理论分析结果, 指出许多几何结构参数包括阴极宽度、二极管间隙等都对输出微波的频率、带宽和能量转换效率有较大的影响。给出了这些参量之间关系的数值模拟结果，在一定程度上为同轴虚阴极振荡器的实验研究提供了理论基础。     

基于异向传输线的亚波长谐振腔设计

 提出了一种新型的谐振腔，该谐振腔的谐振条件与普通谐振腔不同，其两个端面的总相移不必是180°的正整数倍。这种谐振腔由异向传输线和右手传输线两种不同性质的传输线级联构成，它利用耦合腔链作为异向传输线实现负相移，同轴波导作为右手传输线实现正相移，使谐振腔两个端面的总相移为零，满足谐振腔的谐振条件。由于它与传统谐振腔谐振条件不同，理论证明这种谐振腔的长度可远远小于传统谐振腔，设计实例的仿真结果表明这种新型谐振腔的长度最短仅为传统谐振腔的1/7。     

Stop band characteristics of a TESLA cavity coaxial-type HOM coupler

A TTF-type coaxial higher order modes (HOM) coupler has been used in a TESLA 9 cell cavity. It is impossible to measure the stop band characteristics of the HOM coupler with the cavity. A measurement device for the coaxial transmission line type for the HOM coupler has been designed at Peking University. Experimentally it was shown that the average voltage standing wave ratio of the coaxial transmission line is smaller than 1.08. The experimental results of the stop band characteristics of the TTF-type HOM coupler have been fitted for the simulation. This paper describes the design of the measurement device and discusses the experimental and simulation results of stop band characteristics of the HOM coupler.     

单谐振腔束团长度监测器的设计与仿真

提出了一种利用单个谐振腔测量直线加速器束团长度的新方法。不同于传统的双谐振腔束团长度监测器，该方法仅需要使用单个谐振腔，省去了用于辅助测量的参考腔，从而简化了装置结构，节省了空间。针对国家同步辐射实验室基于可调谐红外激光的能源化学研究大型实验装置进行了监测器的物理设计。通过设定同轴探针的插入位置，解决了双模信号互相干扰的问题，利用微扰金属改变调节工作频率，克服了双模难以同时谐振的困难。利用CST软件进行建模和仿真。仿真结果表明，该监测器可实现2～5 ps束团长度的诊断，测量误差小于5%。     

单谐振腔束团长度监测器耦合结构设计与仿真

单谐振腔束团长度监测器利用谐振腔内的两个本征模式测量ps量级的电子束团长度,它的关键是如何将两个不同频率的模式互不干扰地耦合提取出来。为解决这个问题,基于低通和带通滤波器的理论,提出了同轴滤波耦合结构和膜片加载波导滤波结构,借助CST微波工作室对滤波器进行建模并仿真得到其S参数。为测试耦合器的应用效果,设计了一套带有该耦合结构的单谐振腔束团长度监测器探头,根据国家同步辐射实验室基于可调谐红外激光的能源化学研究大型实验装置FELiChEM的束流特点,在CST内对所设计的探头进行束流模拟仿真。仿真结果表明,该耦合器可以实现对特定模式的耦合,并有效降低其它模式的干扰,采用同轴滤波耦合结构和膜片加载波导滤波结构的谐振腔监测器可以实现对FELiChEM装置束团长度的高精度测量,测量误差小于2 %。     

Stop band characteristics of a TESLA cavity coaxial-type HOM coupler

A TTF-type coaxial higher order modes (HOM) coupler has been used in a TESLA 9 cell cavity. It is impossible to measure the stop band characteristics of the HOM coupler with the cavity. A measurement device for the coaxial transmission line type for the HOM coupler has been designed at Peking University. Experimentally it was shown that the average voltage standing wave ratio of the coaxial transmission line is smaller than 1.08. The experimental results of the stop band characteristics of the TTF-type HOM coupler have been fitted for the simulation. This paper describes the design of the measurement device and discusses the experimental and simulation results of stop band characteristics of the HOM coupler.     

Multiple-sample probe for solid-state NMR studies of pharmaceuticals

Solid-state NMR spectroscopy (SSNMR) is an extremely powerful technique for the analysis of pharmaceutical dosage forms. A major limitation of SSNMR is the number of samples that can be analyzed in a given period of time. A solid-state magic-angle spinning (MAS) probe that can simultaneously acquire up to seven SSNMR spectra is being developed to increase throughput/signal-to-noise ratios. A prototype probe incorporating two MAS modules has been developed and spectra of ibuprofen and aspirin have been acquired simultaneously. This version is limited to being a two-module probe due to large amounts of space required for the tuning elements located next to the MAS modules. A new probe design incorporating coaxial transmission lines and smaller MAS modules has been constructed. This probe allows for close proximity of the MAS modules (within 3 cm), adequate proton decoupling power (>50 kHz), and the capability of remote tuning and sample changing. Spectra of hexamethylbenzene (HMB) have been acquired and show signal-to-noise ratios comparable to existing SSNMR probes. Adamantane line widths are also comparable to conventional probe technology. Decoupling powers of 70 kHz have been achieved using a MAS module suitable for 3 cm spacing between modules. Remote tuning has also been achieved with this new coaxial transmission line design. This probe design can be easily scaled to incorporate multiple MAS modules, which is a limitation of the previous design. The number of modules that can be incorporated is only limited by the number of transmission lines that will fit in a cross-sectional diameter of the bore and the axial field length of the magnet.     

Design and research of RF system for 10 MeV compact cyclotron

A 10 MeV compact cyclotron (CYCHU-10) has been developing in Huazhong University of Science and Technology (HUST). The RF system includes a 10 kW RF power generator and a resonance cavity. There is no automatic frequency tuning equipment in the cavity due to space limitations, so the generator must search and track the cavity resonant frequency. AD9850 synthesizer is used to generate RF signal in the experimental prototype, and a fine sinusoidal waveform around 99 MHz is obtained with the method of picking up a special aliased signal from the synthesizer’s output, and the output power level can be set by regulating the resistor connected to the Pin ‘R _set’. The final stage amplifier based on tetrode operates in the grounded cathode configuration, and the schematic of the tetrode circuit is illustrated. The method of searching the resonant frequency is discussed in detail. For the sake of a compact and robust structure, the resonance cavity will adopt non-uniform characteristic impedance coaxial structure, and the magnet surface electroplated with copper will be used as dummy Dees. The precise shapes and dimensions of the cavity are designed and simulation results are carried out in this paper. The distributions of electromagnetic field are illustrated by means of numerical calculation analysis, and the wooden model test is preformed as well.