利用光学渡越辐射进行强流束诊断

当匀速运动的带电粒子通过介质交界面时，在库仑场重建的过程中，会产生渡越辐射，位于可见光波段的渡越辐射被称为光学渡越辐射（OTR）。它作为一种束流诊断工具，具有空间分辨率高、时间响应快、多参数同时测量、对束流影响小、装置简单等特点，能够测量束剖面、发散角、发射度、能量、束流的宏脉冲长度和微脉冲长度等多个参数，因此在国外加速器领域得到了比较广泛的应用。     

产生于介质箔组的渡越辐射微分谱的理论计算

在产生于单一介质箔渡越辐射的基础上,利用辐射场相加和辐射强度相加的方法导出了产生于介质箔组的相干和非相干渡越辐射量子微分谱公式,利用非相干渡辐射微分谱公式,对54MeV的电子分别穿越铍箔组(18片箔),镁箔组(12片箔)和铝箔组(12片箔)时产生的渡越辐射微分谱做了计算,计算结果与实验相符合.     

X波段渡越辐射振荡器的理论和实验

研究了电子束在任意驻波场中的渡越辐射，并结合课题的需要探索了基于渡越辐射在X波段产生高功率微波的可行性。研究工作包括以下部分。     

带电粒子与超晶格相互作用及其超高能粒子识别

讨论了非沟道粒子与晶体的相互作用及其渡越辐射, 并将渡越辐射同沟道辐射进行了比较, 结果表明, 渡越辐射对沟道辐射的贡献主要是在长波区域使沟道辐射的本底增强; 由于超晶格是由两种不同介电性能的材料交替生长而成的多层薄膜结构, 它的渡越辐射比较强. 正是这个特点, 可望利用超晶格的渡越辐射来识别超高能粒子.     

渡越辐射在强流电子束诊断中的应用

文中描述了渡越辐射用于束流诊断的理论依据,介绍了利用渡越辐射对18MeV,2.7kA的强流脉冲电子束进行诊断的实验方案,介绍了在强流束测量中遇到的困难和解决方法.实验中获得了渡越辐射的特征图案,并对特征图案进行了分析,得到了测量时应该使用偏振片的结论.据此,利用渡越辐射测量了强流脉冲束的剖面、能量、发散角.并采用渡越辐射与切伦科夫辐射相结合的方法，用切伦科夫辐射测量束剖面,用渡越辐射测量能量和发散角,在同一次实验中获得了强流脉冲束的归一化发射度.     

X波段五腔渡越管振荡器的理论与实验

随着脉冲功率技术和等离子体物理的不断发展，出现了一类基于电子束在谐振腔中的渡越时间效应的渡越辐射机制来产生高功率微波的器件。该类微波器件的起源是单腔管(TTO)，近年来，美国科学家提出了分离腔振荡器(SCO)，后来又研制出超级后加速振荡器（Super-Reltron)（通过对这些器件的研究，提出并仔细研究了基于渡越时间效应的渡越管振荡器。     

渡越辐射的研究

本文对渡越辐射的理论、实验及其应用等方面的情况做了较详细的综述;分析了影响渡越辐射强度的一些不利因素;对进一步改善渡越辐射的质量,提高渡越辐射强度等问题进行了讨论。     

渡越辐射的研究

本文对渡越辐射的理论、实验及其应用等方面的情况做了较详细的综述;分析了影响渡越辐射强度的一些不利因素;对进一步改善渡越辐射的质量,提高渡越辐射强度等问题进行了讨论。     

超短超强激光与固体靶相互作用中背表面光发射的实验研究

从金属箔背表面测量了超热电子穿越固体靶产生的光发射.光发射积分成像图案呈圆环状，在圆环边缘附近出现局部化明亮光信号确定为光学渡越辐射；光发射光谱在300—500nm之间出现一系列非周期锐利尖峰，在400nm（2ω）附近的尖峰较明显，这个光发射取决于v×B加 热机制产生的超热电子束的微束团引起的相干渡越辐射，(v为电子电度，B为磁场强度)，光 强随靶厚度的增加而减小. 关键词： 超热电子 光发射 光学渡越辐射 v×B加热机制 相干渡越辐射     

超短脉冲激光辐照固体靶背向光发射的测量

利用光学CCD相机和OMA光学多道分析仪,分别在金属箔背表面法线方向测量了光发射的积分成像光谱和散射光光谱.积分成像光谱测量结果显示,光谱呈圆环状,在圆环边缘附近出现局部化明亮光信号确定为超热电子输运穿越固体靶引起的光学渡越辐射(OTR);散射光光谱测量结果显示,光谱在300～500 nm之间出现一系列非周期锐利尖峰,在400 nm(2ω)附近出现的尖峰归结于v×B加热机制产生的超热电子束中的聚束引起的相干渡越辐射(CTR).渡越辐射光强随靶厚度的增加而减小.     

Transition radiation,Cerenkov radiation and energy losses of relativistic charged particles traversing thin foils at oblique incidence

Semiclassical relativistic energy losses and the transition radiation are calculated for fast charged particles (e.g. electrons) traversing a thin dielectric foil at oblique incidence. The transition radiation formula is generalized for foils with spatial dispersion. This formula for oblique electron incidence is of particular interest for the observation of Cerenkov radiation, emitted from a dielectric foil. The emission of Cerenkov radiation is discussed for varying electron incidence angle and foil thickness by the aid of numerical computations.     

Features of transition and Cherenkov radiations and the correlation between them

It is shown that transition radiation arising at the boundary of two media is being emitted as a Cherenkov one, if the phase velocity of transition radiation waves in the medium of transition radiation propagation becomes equal to the velocity of the moving radiating particle (the necessary condition for the Cherenkov radiation). The proof of this statement is based on the analysis of the transition radiation formation zone, which may become large enough and provide interference between the field of transition radiation and the own Coulomb field of the moving particle, in case when the Cherenkov radiation condition is fulfilled. As a result, the transition radiation field transforms into the Cherenkov field. The problem is considered for cases of both a waveguide and free space.     

X-ray transition radiation of electrons with energy of 300 to 900 MeV in periodic multifoil radiators

Results of experiments conducted at the Tomsk synchrotron to study resonant X-ray transition radiation generated by relativistic electrons in periodic multifoil radiators are reviewed. Both the internal synchrotron beam and the external secondary electron beam from the pair magnetic γ-spectrometer with energies ranging from 300 to 900 MeV were used in the experiments. The radiators consisted of many thin amorphous foils of various materials. The generation of X-ray radiation in a compound radiator consisting of a multifoil radiator and a crystal is also studied. In this case, the resonant X-ray transition radiation generated in the multifoil radiator is diffracted in the crystal and emitted at Bragg angles, together with the parametric X-ray radiation generated in the crystal. Spectral and angular properties of the resonant X-ray transition radiation and diffracted resonant X-ray transition radiation are investigated. The ratio between the contributions from the diffracted resonant X-ray transition radiation and other types of radiation to the total coherent X-ray radiation flux generated by electrons in periodic structures and crystals is estimated.     

On the eikonal approximation in the theory of transition radiation

The transition radiation of relativistic electrons in nonuniform media is considered. Based on the equivalent photon method and the eikonal approximation in wave mechanics, a method for describing this process is proposed. For the case in which the permittivity depends on several coordinates, equations for the spectral-angular density of transition radiation are obtained. The main results obtained in the Born and eikonal approximations of the theory of transition radiation are compared. The equations obtained are used to analyze the transition radiation process for a fiberlike target.     

Emission spectra following radiation trapping switching off: coherent effects detected up to resonance and signal enhancement

This paper reports strong-field modified emission spectra of a dipole allowed transition to the ground state, detected in an optically thick vapour subject to radiation trapping. The strong field coupled the higher level of the atomic transition to an upper level of the same atomic species (strontium). The coherence effects were outlined up to resonance in rather dilute vapour conditions. Enhancement of the fluorescent signal after radiation trapping switching off depends on the overlapping of the coupling laser beam with the radiation trapping region.     

Application of transition radiation in a small dihedral angle to detection of relativistic particles

The features of transition radiation excited by a relativistic particle in a dihedral angle with an opening comparable to the angular divergence of transition radiation are considered. It is shown that the radiation distribution in the dihedral angle is more sensitive to the direction of emitting particle motion and to the position of the surface intersection by the particle, than the radiation excited when a plane surface is intersected. It is indicated that the spectral radiation density in the small dihedral angle is higher than the density of radiation excited when a plane surface is intersected. These features offer additional opportunities to use transition radiation in systems for measuring particle parameters.     

Resonant transition radiation in plamsa with magnetic inhomogeneities

We calculate the spectrum of the resonant transition radiation generated by a fast charged particle moving in plasma with small-scale random magnetic inhomogeneities. We determine the conditions under which this type of transition radiation dominates over the transition radiation on plasma density inhomogeneities. We discuss possible applications of the resonant transition radiation in astrophysical and geophysical conditions.     

Radiation of charged particles interacting with interface of two different transparent media

It is shown that the Vavilov-Cherenkov radiation has an essential contribution in experiments on optical transition radiation. The properties of the Vavilov-Cherenkov radiation, such as direction, threshold condition, and polarization, are considered. Peculiarities appearing at sliding incidence of electrons at the target in experiments on optical transition radiation are discussed.     

Coherent radiation under conditions of the propagation of heavy charged particles through the dielectric in an external electric field

The process of electromagnetic radiation arising during the propagation of heavy charged particles through a dielectric layer situated in an external electric field is investigated. This radiation is due to the degradation of polarization medium induced by the field. The local maximum within the centimeter frequency range of the energy spectrum is analyzed under varying external parameters of the model. Conditions that might allow for the intensity of the radiation to be comparable to the transition radiation are found.