Single Photon Scattering in a Pair of Waveguides Coupled by a Whispering-Gallery Resonator Interacting with a Semiconductor Quantum Dot

The single photon scattering properties in a pair of waveguides coupled by a whispering-gallery resonator interacting with a semiconductor quantum dot are investigated theoretically.The two waveguides support four possible ports for an incident single photon.The quantum dot is considered a V-type system.The incident direction-dependent single photon scattering properties are studied and equal-output probability from the four ports for a single photon incident is discussed.The influences of backscattering between the two modes of the whispering-gallery resonator for incident direction-dependent single photon scattering properties are also presented.     

Controlling single-photon Fock-state propagation through opaque scattering media

The control of light scattering is essential in many quantum optical experiments. Wavefront shaping is a technique used for ultimate control over wave propagation through multiple-scattering media by adaptive manipulation of incident waves. We control the propagation of single-photon Fock states through opaque scattering media by spatial phase modulation of the incident wavefront. We enhance the probability that a single photon arrives in a target output mode with a factor 30. Our proof-of-principle experiment shows that the propagation of quantum light through multiple-scattering media can be controlled, with prospective applications in quantum communication and quantum cryptography.     

未被俘获电子对多光子非线性Compton散射能量转换效率的影响

 应用单粒子理论和电子与光子非弹性碰撞模型，研究了未被俘获电子对多光子非线性Compton散射能量转换效率的影响。结果表明，未被俘获电子使该散射的频谱展宽随入射电子速度和与电子同时作用的光子数的增大而增大，随电子与光子非弹性碰撞成分的增大而减小，从而使能量转换效率近乎与电子入射速度正比降低。用低能电子入射，能有效地减小这种损失。     

未被俘获电子对多光子非线性Compton散射能量转换效率的影响

应用单粒子理论和电子与光子非弹性碰撞模型,研究了未被俘获电子对多光子非线性Compton散射能量转换效率的影响。结果表明,未被俘获电子使该散射的频谱展宽随入射电子速度和与电子同时作用的光子数的增大而增大,随电子与光子非弹性碰撞成分的增大而减小,从而使能量转换效率近乎与电子入射速度正比降低。用低能电子入射,能有效地减小这种损失。     

A new technique for calculating virtual photon spectra

A first-order matrix differential equation in energy is used to propagate radial matrix elements arising in DWBA of relativistic electron scattering from nuclei. Given an initial set of matrix elements at some value of the energy, this equation permits the evaluation of the radial matrix elements over the complete energy transfer range. A computer code has been written for this new procedure and the virtual photon spectra accompanying electron scattering from a point nucleus is calculated as a function of photon energy for various multipoles, nuclear charges, and incident electron energies.     

Resonant enhancement of inelastic light scattering in strongly correlated materials

We use dynamical mean field theory to find an exact solution for inelastic light scattering in strongly correlated materials such as those near a quantum-critical metal-insulator transition. We evaluate the results for q=0 (Raman) scattering and find that resonant effects can be quite large, and yield a double resonance, a significant enhancement of nonresonant scattering peaks, a joint resonance of both peaks when the incident photon frequency is on the order of U, and the appearance of an isosbestic point in all symmetry channels for an intermediate range of incident photon frequencies.     

Modeling of photon density waves in the frequency domain

We have described the transfer of modulated radiation in a random medium in terms of the Bethe-Salpeter equation. Based on the obtained expression for the scattering intensity, we have developed an original technique of modeling the photon density waves in terms of the Monte Carlo method. Expressions for measurable parameters in the frequency domain have been derived, and, based on them, the amplitude and phase of the photon density waves have been calculated. We have studied how the parameters of the photon density waves depend on the scattering anisotropy for model states with the Henyey-Greenstein phase function. The range of applicability of the diffusion approximation for the interpretation of signals of photon density waves has been investigated.     

Resonant inelastic scattering of an X-ray photon by a linear molecule

The double differential cross section of resonant inelastic scattering of a linearly polarized X-ray photon by a spatially oriented HF molecule in a gas phase is theoretically described in the energy range of the ionization threshold of the deep molecular orbital 1σ. The effects of radial relaxation of the wave functions of the core and excited scattering states in fields of the formed core vacancies, the vibronic effects, and the effects of Auger and radiative decays of the vacancies are taken into account in the nonrelativistic Hartree-Fock approximation. The results of the calculations are predictive and agree well with the results of the experimental measurements of the Kα emission spectrum of the HF molecule at an incident photon energy of 2 keV, which considerably exceeds the energy of the 1σ ionization threshold.     

表面等离子激元非线性表面增强拉曼散射效应

本文采用热蒸发法制备得到纳米Ag颗粒作为增强拉曼衬底, 利用入射光子与纳米颗粒表面价电子的相互作用机理, 激发出高能表面等离子激元, 其表面等离子形成的高能"热点"起到表面增强拉曼散射效果. 通过比较不同入射光强下的拉曼峰强, 指出纳米Ag颗粒的增强拉曼散射效果可以实现低探测光强下的高散射强度, 即纳米Ag颗粒的表面等离子激元具有非线性的表面增强拉曼散射效果, 可降低对样品的光、热损伤, 以利于拓展拉曼散射光谱的应用范围. 同时比较不同纳米Ag颗粒衬底的表面增强拉曼散射效果表明, 采用的热蒸发工艺具有较大的工艺域度, 具有较强的工艺兼容性.     

高斯光束在双层云中传输的蒙特卡罗模拟

基于辐射传输理论, 利用蒙特卡罗方法模拟了无限窄(冲击函数)准直光束入射到典型水云以及冰水双层云时的后向散射特性, 进而将得到的冲击响应与高斯光束卷积, 得到高斯光束在云层中传输的多次散射特性. 文中给出了两种波束入射时水云以及冰水双层云的反射函数随径向r和天顶角α的变化关系, 并给出了光强在云层内部的二维分布图. 计算结果表明, 高斯光束入射时, 云层反射函数的特点与无限窄准直光束入射时有较大区别. 因此在利用激光雷达进行云层探测时需要考虑激光的散斑, 文中的方法可以为此提供理论依据.     

光子与相对论麦克斯韦分布电子散射的能谱角度谱研究

光子与相对论麦克斯韦分布电子散射的描述及能谱角度谱计算非常复杂且费时.本文提出了一种光子与相对论麦克斯韦速度分布电子散射的蒙特卡罗(MC)模拟方法,该方法能够细致模拟高温等离子体中任意能量光子与任意温度电子的Compton和逆Compton散射问题.对于散射后光子的能谱和角度谱参数,可以根据电子温度抽样若干不同状态的电子,分别模拟其与光子发生散射,可以得到各次散射后的光子能量和偏转角度,取统计平均后的结果即可获得该光子与该温度电子散射的能谱和角度谱分布.根据该方法编写了光子与相对论电子散射MC模拟程序,开展了高温全电离等离子体中光子与相对论电子散射的能谱角度谱计算和分析,分析结果显示:热运动电子将展宽出射光子能谱,且低能光子与高温电子散射后的蓝移现象明显;出射光子的角度谱很复杂,其决定于入射光子能量、出射光子能量及电子温度.基于该方法计算并以数表形式给出的光子-相对论电子散射能谱角度谱数据,可以供辐射输运数值模拟程序使用.     

Phonon-assisted normal incidence intersubband absorption in semiconductor quantum wells

In the presence of a normally incident mid-IR pulsed laser field, phonon-assisted photon absorption by both intrasubband and intersubband phonon scattering of conduction electrons in GaAs/AlGaAs quantum wells are predicted. The novel non-resonant and non-linear intersubband absorption is found by including the photon-induced phonon scattering process in a Boltzmann equation for phonon energies smaller than the energy separation between two electron subbands in the quantum well. The predicted phonon-assisted photon absorption by intersubband transitions of electrons from the first to the second subband is a unique feature in quantum-well systems and is expected to have a significant effect on the electron populations in both subbands.     

Simultaneous solution of Kompaneets equation and radiative transfer equation in the photon energy range 1-125 keV

Radiative transfer equation in plane parallel geometry and Kompaneets equation is solved simultaneously to obtain theoretical spectrum of 1-125 keV photon energy range. Diffuse radiation field are calculated using time-independent radiative transfer equation in plane parallel geometry, which is developed using discrete space theory (DST) of radiative transfer in a homogeneous medium for different optical depths. We assumed free-free emission and absorption and emission due to electron gas to be operating in the medium. The three terms n, n² and (∂n/∂x_k) where n is photon phase density and x_k=(hν/kT_e), in Kompaneets equation and those due to free-free emission are utilized to calculate the change in the photon phase density in a hot electron gas. Two types of incident radiation are considered: (1) isotropic radiation with the modified black body radiation I^MB[1] and (2) anisotropic radiation which is angle dependent. The emergent radiation at τ=0 and reflected radiation τ=τ_max are calculated by using the diffuse radiation from the medium. The emergent and reflected radiation contain the free-free emission and emission from the hot electron gas. Kompaneets equation gives the changes in photon phase densities in different types of media. Although the initial spectrum is angle dependent, the Kompaneets equation gives a spectrum which is angle independent after several Compton scattering times.     

Measurement of the proton spin polarizabilities at MAMI

The spin polarizabilities of the nucleon are fundamental structure constants which describe the response of the nucleon spin to an incident polarized photon. The most model-independent way to measure the nucleon spin polarizabilities is the Compton scattering with polarization degrees of freedom. Three Compton scattering asymmetries on the proton were measured in the Δ(1232) region using a polarized incident photon beam and a polarized (or unpolarized) proton target at the Mainz Microtron (MAMI). These asymmetries are sensitive to values of the spin polarizabilities. Fits to asymmetry data were performed using a dispersion model calculation, and a separation of all four proton spin-polarizabilities in the multipole basis was achieved. The values of the proton spin polarizabilities are presented.     

Physical characteristics of X-ray scattering in fat and blood

A Monte Carlo simulation program is constructed in order to trace the histories of photon interactions inside fat and blood under tissue-characterization conditions (energies from 7 to 60 keV and samples from 0.5 to 20 cm). The effect of incident photon energy on the number of coherent and incoherent interactions up to the 3rd order scattering is studied for three different sample sizes. The ratio of scattering to total interactions (including photoelectric absorption) is also studied for fat and blood under the same scattering conditions. Results show considerable differences in the scattering properties of fat and blood over a wide range of energies. This may explain the experimental differences reported by Evans et al. and Kosanetzky et al. The percentage of photons making three incoherent interactions recorded a maximum of 10% which implies the need to correct for multiple scattering in incoherent scattering measurements intended for tissue characterization.     

X射线与非晶硒作用中的散射光子重吸收研究

本文对光电吸收占优的条件下,X射线与非晶硒作用中产生的散射光子重吸收作了较为详细的研究.结果显示,有相当一部分散射光子被非晶硒重吸收;随着入射光子能量的升高和非晶硒膜层厚度的加大,因散射重吸收而增加的能量吸收与初级作用中能量吸收的比值增大.这表明对于能量较高的入射X射线光子和厚的非晶硒膜层,散射重吸收将对X射线成象过程产生一定的影响.     

Multiple‐element spectrometer for non‐resonant inelastic X‐ray spectroscopy of electronic excitations

A multiple‐analyser‐crystal spectrometer for non‐resonant inelastic X‐ray scattering spectroscopy installed at beamline ID16 of the European Synchrotron Radiation Facility is presented. Nine analyser crystals with bending radii R = 1 m measure spectra for five different momentum transfer values simultaneously. Using a two‐dimensional detector, the spectra given by all analysers can be treated individually. The spectrometer is based on a Rowland circle design with fixed Bragg angles of about 88°. The energy resolution can be chosen between 30–2000 meV with typical incident‐photon energies of 6–13 keV. The spectrometer is optimized for studies of valence and core electron excitations resolving both energy and momentum transfer.     

Photon momentum in a surface plasmon

It is shown that the photon momentum in a surface plasmon is ? k, where k is the plasmon wave vector. In a significantly delayed plasmon on a thin metal film or filament, the photon momentum is several hundred times larger than the momentum of a photon of the same frequency in a plane wave in free space. The plasmon-plasmon and free-space plane wave-plasmon scattering by a free electron is considered. It is shown that, in contrast to the plane wave-plane wave scattering, the electron acquires a significant momentum, while the scattered plasmon frequency significantly changes. The former process is similar to the Compton effect: scattering of X-ray and γ quanta (having a significant momentum) by an electron. In the latter process, the system composed on an incident photon and an electron at rest, which has a small total momentum, generates a photon and an electron, each having a large momentum. A device for detecting electrons from plasmons excited in nearby metal nanofilms and nanowires can be developed on the basis of this principle.     

Photon emission induced by elastic exciton-carrier scattering in semiconductor quantum wells

We present a study of the elastic exciton-electron (X-e⁻) and exciton-hole (X-h) scattering processes in semiconductor quantum wells, including fermion exchange effects. The balance between the exciton and the free carrier populations within the electron-hole plasma is discussed in terms of ionization degree in the nondegenerate regime. Assuming a two-dimensional Coulomb potential statically screened by the free carrier gas, we apply the variable phase method to obtain the excitonic wavefunctions, which we use to calculate the 1s exciton-free carrier matrix elements that describe the scattering of excitons into the light cone where they can radiatively recombine. The photon emission rates due to the carrierassisted exciton recombination in semiconductor quantum-wells (QWs) at room temperature and in a low density regime are obtained from Fermi’s golden rule, and studied for mid-gap and wide-gap materials. The quantitative comparison of the direct and exchange terms of the scattering matrix elements shows that fermion exchange is the dominant mechanism of the exciton-carrier scattering process. This is confirmed by our analysis of the rates of photon emission induced by electron-assisted and hole-assisted exciton recombinations.     

Anisotropic charge transfer rates in the scattering of oriented atoms or molecules from surfaces

Atoms or molecules scattered from surfaces can undergo charge transfer to or from the surface during the scattering event. It is proposed that when the incident particle is “prepared” in an excited or ionic state which is oriented with respect to the surface, observable anisotropies in charge transfer rates involving the oriented state should occur. The effect is illustrated with two examples.