线腔

本文主要针对基于Cooper对盒子与超导传输线腔耦合系统的量子信息传输进行了理论研究。

In this paper , we focus on the Cooper Pairs Box-Transmission Line Resonator coupling system of quantum information transfer , and some researches on the theoretical models are presented .

我们提出了用传输线腔（TLR）来耦合多个双量子点分子的模型，大大加强双量子点分子之间的耦合强度（直接的库仑相互作用强度较小）。

We propose to couple double quantum dot molecules with a transmission line resonator ( TLR ), and thus the coupling strength between two double quantum dot molecules can be much enlarged ( the direct coulomb interaction is not large enough ) .

理论分析表明在传输线腔中存在两类谐振模式，分别是传输模式下的谐振和截止模式的谐振。

Cavity performances were analyzed theoretically under the transmission and cut off mode based on equivalent circuit parameters of loaded antenna . It is proved that there were two resonant modes .

为了提高双量子点分子之间的耦合强度，我们提出了用超导传输线腔来耦合多个双量子点分子。

In order to increase the interaction strength between two double quantum dot molecules , we propose to use a superconducting transmission line resonator ( TLR ) to connect many double quantum dot molecules .

轴流泵叶轮内部流场大涡模拟及分析不同涡旋型线压缩腔流场的模拟分析

Large-eddy Simulation and Analysis of Turbulent Flow in Axial Pump Impeller A Simulation and Analysis of Different Scroll Profiles ′ Interior Flow Field

涡旋压缩机堵转测试台的设计与制作不同涡旋型线压缩腔流场的模拟分析

Design & establishment of locked rotor test bench for scroll compressor A Simulation and Analysis of Different Scroll Profiles ′ Interior Flow Field

提出了开路传输线谐振腔的概念，很好地解释了一类线散射中的广义谐振现象，并提出一种通过改变导线长度消除线散射中广义谐振影响的方案。

The generalized resonance occurring in wire scattering can be explained by open transmission line cavity . The effect of generalized resonance can be avoided by changing the length of wires .

通用涡旋型线中心压缩腔几何修正方法研究

A Study on Geometry Modification of the Central Portion of General Scroll Profiles

慢波结构是行波管的重要组成部分，是传播电磁波并使电磁波与电子注发生相互作用的部件。慢波结构有螺旋线、耦合腔、梯形线、折叠波导等多种结构形式。

A slow-wave structure is an important component of traveling-wave tubes , where electromagnetic wave interacts with electron beams .

铝包钢线包覆型腔金属流动特性的光塑性实验研究

Photoplastic study on the flow law governing the deformation of materials in the cladding chamber of aluminum clad steel wires

旋转超声电机定子超谐共振分析与非线性动力学实验磁绝缘线振荡器谐振腔的高频特性研究

Superharmonic Resonance of the Stator of a Rotary Ultrasonic Motor and Nonlinear Dynamical Experiments Numerical analysis on high frequency characteristics of MILO

外部电磁波通过小孔及线耦合到腔体内，并在导线上感应出瞬态电流，在端接部分感应出电压，由此形成的干扰对系统有破坏作用。

Through an aperture and wires external electromagnetic pulse couples to the cavity , in which the transient current is induced on the lines and the transient voltage is induced on the line ends , and the interference formed by the transient current and voltage has destructive effect .

结合实际谐振腔的参数值进行分析得出：导致反射系数相位法失效的最主要原因是传输线与谐振腔只通过部分电感耦合，并且耦合电感太小。

Finally , by analyzing all the possible values of the parameters of the practical cavities , a conclusion is got that the primary cause of the failure of the method is that the transmission line couples with the cavity by a too small part of inductance in the cavity .

基于通用型线的涡旋压缩腔几何模型

Geometrical model of scroll compressor chamber based on general profile

磁绝缘线振荡器的冷腔研究

Study Of Cooling Magnetically Insulated Line Oscillator

1.517μm附近水汽分子谱线加宽系数的腔衰荡光谱测量

Measurement of broadening coefficients of water vapor molecules near 1.517 μ m with continuous-wave cavity ring down spectroscopy

本文运用谱域法和传输线概念建立背腔式槽阵的本征方程，在窄槽情况下，与文〖3〗的本征方程相同。

The Characteristic equation of cavity-backed slot array is formulated , using the spectral domain approach and the concept of transmission line . Consider narrow slot , then , the formula is consistent with [ 3 ] .

而当半导体纳米线中的声子腔呈准周期序列排列时，透射谱线出现尖锐透射峰的特性，却又强烈的依赖于声子腔宽度的取值。

While the quasi-periodic sequence arrangement of the phononic cavities in the semiconductor nanowire , the transmission spectrum lines also appear the sharp transmission peaks , but the property depends greatly on the width of the phononic cavities .

微波是在传输线中传播的，因此我首先介绍了传输线的理论，而后介绍了将传输线转化为谐振腔的方法，最后将谐振腔中的电磁场量子化。

Due to microwave transport in transmission lines , the theory of transmission lines is intro-duced firstly . Then , I introduce the setups which transform a transmission line into a microwave cavity . At last , the microwave field in a cavity is quantized .