铷原子频标中的微波功率频移

根据我们的测量，在铷原子频标中微波功率频移系数总是正的。已有的关于微波功率频移的解释无法解释此现象。本文从微波场引起交流Ｚｅｅｍａｎ效应的观点出发，解释了这一现象。     

铷原子频标中的微波动功率频移

根据的测量，在铷原子频标中微波功率频移系数总是正的。已有的关于微波功率频移的解释无法解释此现象。本文从微波场引起交流Ｚｅｅｍａｎ效应的观点出发，解释了这一现象。     

海面微波散射场多普勒谱特性研究

基于粗糙面电磁散射双尺度模型推导给出了海面微波散射场多普勒谱频移和谱宽的理论公式, 在该理论公式的推导过程中同时考虑了大尺度海浪的倾斜调制、遮蔽效应和曲率修正效应等因素的影响. 文中将理论公式计算结果与精确数值结果进行了比较, 并讨论了倾斜调制、遮蔽效应及曲率修正效应等因素对多普勒频移和谱宽的影响, 发现倾斜调制使水平极化散射回波多普勒频移显著增大, 从而导致水平极化回波多普勒频移比垂直极化回波多普勒频移大; 在中等入射角度区域, 遮蔽效应和曲率修正效应对多普勒谱并无显著影响, 而在掠射条件下, 遮蔽效应使得多普勒频移增大、谱宽变窄. 本研究对深入理解动态海面散射场频谱特性具有一定参考意义.     

二维粗糙海面散射回波多普勒谱频移及展宽特征

基于二维线性海面模型及粗糙面电磁散射的一阶小斜率近似公式,研究了海面回波各阶多普勒谱的频移特性,得到了多普勒谱频移所对应的理论公式,与经典多普勒频移公式相比考虑到了风速、大尺度波浪轨道运动等因素对多普勒谱频移的影响;同时根据粗糙面的双尺度模型,基于多普勒谱频移的物理机理,给出了求解散射场多普勒谱展宽的理论公式.最后将理论公式计算所得结果与模拟结果及实测数据进行了比较,讨论了风速、入射波频率及入射角等因素对多普勒频移及多普勒谱展宽的影响.通过比较可以发现,给出的理论公式可以对多普勒谱频移和展宽进行一定程度的预测. 关键词： 粗糙海面 电磁散射 多普勒谱     

基于多普勒效应的水波特性实验装置的设计

设计了一种基于多普勒效应的水波特性实验装置,在频闪光源照射下,通过毛玻璃屏,可直接观察多普勒效应的现象,通过设计的光电检测装置测量出水波的频率及频率的变化情况,实现水波多普勒频移的数字化测量.当波源位置固定,波源以一定频率振动,根据多普勒效应,通过实时测量多普勒频率,测量出探头的速度,进而推算出水波波速.该装置有利于多普勒效应的水波特性研究,直观演示了多普勒频移现象.     

从光量子性看多普勒频移

从光的粒子性出发，分析计算了运动原子和静止原子发射的光子的频率，得到了完全相同的多普勒频移公式．     

广义非线性薛定谔方程描述的波坍缩及其演变

介绍了广义非线性薛定谔方程, 并且运用分步傅里叶方法进行了数值求解. 在外部势场一定的情况下, 给定系统一个小的初始扰动, 讨论了广义非线性薛定谔方程中复系数p, q 对波场演变过程的影响. 通过数值研究发现波场会相继出现调制不稳定性、波坍缩、逆级联以及整个空间的湍流现象. 而当改变非线性频移系数的量级时, 数值研究发现在波坍缩之后出现了逆级联, 最终系统的能量主要凝聚在3个不同波矢终端的附近区域.     

时间频率基准装置的研制现状

时间频率基准装置——铯原子喷泉钟, 在标准时间产生和保持、基础物理研究中发挥了重要的作用. 介绍了铯原子喷泉钟的工作原理, 对影响其性能的各项噪声源和频移项给出了分析, 影响频率稳定度性能的主要因素为Dick 效应相关的原子团装载时间、微波激励源相位噪声和探测激光的频率噪声, 影响频率不确定性能主要频移项为: 黑体辐射频移、冷原子碰撞频移、腔相位分布频移和微波泄露频移; 总结和比较了当前具有先进性能的铯原子喷泉钟采用的技术; 介绍了铯原子喷泉钟的主要应用方向、空间冷原子铯钟的研制情况和光学频率原子钟进展.     

基于不同散射机制特征的海杂波时变多普勒谱模型

海杂波的多普勒谱建模对采用多普勒处理技术的雷达进行有效的海杂波抑制和目标检测具有重要的意义.本文分别考虑Bragg,白冠和破碎波三种散射机制对应的多普勒谱分量的特征,对三种谱分量的频移和展宽进行分离,并引入附加速度频移量,提出了基于不同散射机制特征的雷达海杂波时变多普勒谱模型.该模型假设谱强度为受观测时间区间影响的随机变量,能够同时适用于平均多普勒谱与短时多普勒谱建模.通过分别对黄海海域实测的岸基P,S波段海杂波平均多普勒谱与短时多普勒谱建模测试,结果表明该模型相对传统模型的建模精度更高,尤其体现在短时谱的观测时间较长和平均谱形式较为复杂的情况下,建模误差显著减小.     

基于里德伯原子天线的低频电场波形测量

里德伯原子的高极化率可以实现电磁场的多维度参数测量.本文利用室温里德伯原子构建原子天线,基于原子天线将低频电场幅度信息转化为强度信息,从而实现低频电场的参数测量.实验采用双光子激发制备铯原子里德伯态,通过阶梯型电磁感应透明(electromagnetically induced transparency, EIT)光谱实现里德伯原子量子态的检测,基于内置电极技术在室温原子气室导入k Hz频段低频电场.电场中里德伯原子的Stark频移会在EIT过程导致双光子失谐,从而引起EIT光谱频移和强度变化.在弱电场条件下, EIT光谱频移可以忽略, EIT透射强度与输入低频电场强度近似为线性关系,基于该效应可以实现低频电场的波形、幅度、频率等参数测量.     

低频调制场中钾原子的激发

本文用含时多态展开方法计算了里德堡钾原子在静电场、微波场和低射频场[a radio-frequency(rf)field]共同作用下方波振荡的激发特性.研究计算了通过改变微波场的频率、振幅和静电场的振幅以及用低射频锯齿波代替低射频余弦波后方波振荡的变化,获得了一些非常有趣的结果,并给出了理论解释.     

The Doppler effect in NMR spectroscopy

An NMR sample may be subject to motions, such as those due to sample spinning or to liquid flow. Is the spectrum of such a sample affected by the Doppler effect? The question arises because, instrumental dimensions being much shorter than the wavelength, it is the near-field of the precessing magnetic moment which couples to the receiver coil, rather than the radiated far-field. We expand the near-field into plane propagating waves. For each such wave there is another one with the same amplitude, propagating in the opposite direction. The Doppler shifts are therefore equal and opposite. In the model case of a small fluid sample moving with constant velocity, this leads to a distribution of Doppler shifts which is symmetrical with respect to the unshifted frequency: there is no net spectral shift. We examine the possibility of observing the Doppler distribution in this case. We also consider the case of thermal motion of a gas. We draw attention to the resolved Doppler splitting of molecular rotational transitions in a supersonic burst as observed in a microwave resonator. We also mention briefly the Doppler effect in molecular beam spectroscopy.     

Simultaneous detection of the acoustic-field aberration and Doppler shift in forward acoustic scattering

The aberration in the received acoustic field and the Doppler shift in the forward scattered field are simultaneously induced when a submerged target crosses the source–receiver line. Formulations for the two variations are developed upon an ideal forward scattering configuration. Both the field aberration and the Doppler shift are expressed as functions of the same argument — the target motion time. An experimental validation was carried out in a tank, in which the continuous wave was transmitted. The field aberration and the Doppler shift were extracted from the collected data by the simple Hilbert transform and a hybrid technique, respectively. The measured aberration and Doppler shift agree with the theoretical results.Simultaneous detection outputs are beneficial to enhance the reliability on target detection by providing both the aberrations in the received acoustic field and the Doppler shift in the forward scattered field.     

低磁场过模慢波结构型高功率毫米波发生器的改进

 利用粒子模拟的方法设计了一个高功率毫米波发生器,并对其进行了实验研究及改进。采用过模慢波结构以增大束波作用空间,从而提高功率容量;为实现过模慢波器件的单模、单频工作,选择TM01模的π模作为工作模式。采用过模慢波结构,结合合理的器件结构设计,可降低器件工作所需的导引磁场。实验在TORCH-01加速器平台进行,产生的微波频率由色散线法测量,其功率由远场积分法得到。最初的器件采用矩形波纹慢波结构,得到频率为33.56 GHz、功率约110 MW的微波输出,但功率难以进一步提高,脉宽仅为7~8 ns,且在慢波结构边沿发现击穿痕迹。对矩形慢波结构进行倒圆角处理后,借助数值模拟,发现其TM01模的π模频率变化不大。改进后的器件在0.8 T导引磁场下,当电压和电流分别为590 kV与5.2 kA时,实验得到频率33.56 GHz、功率320 MW的毫米波输出,微波模式为准TM01模,效率约10%,脉宽延长至约13 ns,器件内表面无明显击穿痕迹。     

The electromagnetic field in the plasma jet of a microwave plasmatron

A coaxial microwave plasmatron operating at a frequency of 10 GHz is investigated. The microwave field distribution in the plasma jet of the plasmatron is studied using a vibrating string as a small perturbation source. The phase structure of the microwave field inside the plasma is found to differ from that on the outer side of the plasma jet boundary. A slow surface electromagnetic wave propagating along the plasma jet is observed.     

Experimental observation of superradiance in the stimulated scattering of an intense microwave pump wave by a counterpropagating subnanosecond high-current relativistic electron bunch

The generation of ultrashort superradiant pulses in the stimulated scattering of an intense microwave (38 GHz) pump wave by a counterpropagating high-current relativistic electron bunch has been observed. Scattered radiation is a single ～200-ps pulse with a peak power of about 1 MW. Owing to the Doppler shift of the radiation frequency, frequencies up to 150 GHz are present in the spectrum of the scattered pulse.     

Slow-light solitons in three-level atomic systems modified by a microwave field

We study the modified effect of slow-light soliton in a resonant three-level atomic system via electromagnetically inducedtransparency (EIT) by utilizing a microwave field. We derive ahigh-order nonlinear Schrödinger equation by using a perturbation method of multiple-scales, and calculate the modification ofsoliton velocity and frequency shift. We find that in the presence of the microwave field an obvious decrease of propagating velocityof soliton can be realized, which provides an effective method to slow down optical solitons in EIT systems. We also find that thedown shift of oscillating frequency of soliton in such system can be largely suppressed by the microwave field.     

Observation of a motional Stark effect to determine the second-order Doppler effect

The high resolution two-photon spectroscopy of hydrogen is often limited by the second-order Doppler effect. To determine this effect, we apply a magnetic field perpendicular to the atomic beam. This field induces a quadratic motional Stark shift proportional, as the second-order Doppler effect, to v(2) (v atomic velocity). For some magnetic field, these two effects are opposite and the total shift due to the atomic velocity is reduced. We present the first observation of this effect for the 1S-3S transition in hydrogen.     

X波段永磁包装相对论返波管研制

设计了一个X波段相对论返波管,通过对器件结构的特殊设计,提高了器件的Q值,同时增大了电子束与慢波结构之间的耦合阻抗,从而实现器件的低磁场运行以便对其进行永磁包装;当引导磁场强度0.46 T、电子束束压750 kV、束流约5.5 kA时,得到频率9.1 GHz、功率1.24 GW的微波输出。根据模拟结果设计加工了一个磁场强度为0.46 T的小型化永磁磁体,该磁体长48 cm,最大外半径15 cm,总重量约116 kg。开展了永磁包装返波管的实验研究,得到以20 Hz的频率运行1 s时功率900 MW、单次运行时功率940 MW的X波段微波输出。