Plasmon beams interaction at interface between metal and dielectric with saturable Kerr nonlinearity

We present a novel theory of surface plasmon polariton interaction on the surface of dielectric with saturable Kerr nonlinearity. The effect of the total internal reflection of a weak signal plasmon beam from a high-power reference beam is discussed. Both ray and wave theories are used to describe signal propagation. The effect of the signal tunneling through the narrow inhomogeneity induced by the reference beam is considered.     

On observability of the ac Stark effect line splitting in case of beams of finite size

The small signal gain distortions in the field of a Gaussian pump beam were investigated theoretically and experimentally in a Λ-type quantum system depending on the size and power of the pump beam. The strong pump beam induces a change of refraction index of a methanol model material, depending on the frequency of the signal. It leads to a nonlinear active waveguiding effect causing distortion (narrowing and shift) of the signal line shape. In case of Stark splitting, the induced nonlinear active waveguiding effect manifests itself in the disappearance of the line split, for narrow pump beams. Collision induced frequency shift of the signal line depending on the pressure of the methanol gas was observed.     

Two-dimensional diffraction on a cylinder induced by a laser beam in a nonlinear gradient medium

A wave theory was developed and a numerical simulation performed of the diffractive flow of a signal wave around a negative inhomogeneity induced by a cylindrical pump beam in nonlinear medium while keeping both waves in the potential well. It was shown that a broad pump beam reflects a narrow signal beam. A nonlinear waveguide (a dark soliton) is described as well. These phenomena can be observed in Bose-Einstein condensate (BEC) and in a gradient waveguide.     

Lateral shift and tunneling of optical beam reflected from gradient-induced inhomogeneity

Two effects have been analytically and numerically studied: Goos-Hänchen shift, which is acquired by an optical beam reflected from a gradient inhomogeneity, and tunneling of radiation through a narrow induced inhomogeneity. A possibility of increasing the lateral beam shift in comparison with total internal reflection from a homogeneous medium is revealed. The dependence of the tunneling coefficient on the inhomogeneity parameters is determined and the critical inhomogeneity width at which the tunneling effect arises is found.     

三维自散焦介质中的暗光束诱导亮光束聚焦

为了获得一种对称压缩圆光束的方法,系统研究了三维自散焦介质中亮暗光束对的共同传输。数值结果表明:当两光束中心重合时,若抽运光(暗光束)初始振幅远大于信号光(亮光束)初始振幅,抽运光将通过交叉相位调制(XPM)诱导信号光聚焦,使得信号光的圆形光斑被对称压缩。讨论了光束参量对信号光聚焦效果的影响,发现抽运光初始振幅越大,信号光聚焦越强。当抽运光初始振幅一定时,暗光束的初始束宽存在最佳值使得信号光压缩最强。当抽运光与信号光的波长比取值为0.5~1.5时,信号光聚焦程度随着波长比的增大而有所降低。还设计了验证理论结果的实验方案。     

椭圆高斯光束在自散焦介质中的诱导聚焦

研究了在自散焦介质中诱导光束聚焦过程中椭圆高斯光束对光束聚焦的影响。通过数值计算讨论了在不同初始抽运光束振幅、初始光束间距和波长比情况下椭圆高斯光束对信号光束聚焦的影响。影响光束聚焦过程的方程参量和初始条件共有6个,即两光束波长比(方程参量)、抽运光束和信号光束的初始振幅、两光束初始中心间距和两光束X、Y初始束宽比。采用此理论模型验证了Hickmann在1992年得出的实验结果,数值计算结果表明理论结果能够和实验结果定量地吻合。     

光束束宽对自散焦介质中诱导光束聚焦的影响

影响自散焦介质中诱导光束聚焦过程的方程参量和初始条件共有5个，即两光束波长比(方程参量)、抽运光和信号光的初始振幅、两光束初始束宽比和两光束中心初始间距。通过数值计算讨论了初始束宽比在不同初始光束间距和波长比情况下对信号光聚焦过程的影响，得到了信号光聚焦效果的最佳初始参量条件。从而实现了对影响自散焦介质中诱导光束聚焦过程5个参量的完整详细研究。     

利用双色激光感生光栅光谱法测定^127I的核自旋

本文利用ＮｄＹＡＧ激光倍频光５３２ｎｍ激光分成强度大致相等的两束激光作为泵浦光以２．７３°交叉于碘分子样品室中，两束泵浦光发生干涉在碘分子中选择激发形成了空间正弦分布的激光态分子光栅和基态耗尽型光栅。另一束窄线宽染料激光作为探索光射入到激光感生光栅上，沿着布拉格衍射的方向接收信号光。利用泵浦共振为３２－０Ｒ（５５），探索共振为１３－０Ｐ（５５），Ｒ（５５）和泵浦共振为３２－０Ｐ（５２），探索共振为１３－０Ｐ（５２），Ｒ（５２）的碘分子双色激光感生光栅光谱谱线强度测定了１２７Ｉ的核自旋，测定值为５／２。     

抽运光波前畸变对拍瓦激光器前端OPA光束质量的影响

数值模拟了拍瓦激光器前端非共线光参变放大(OPA)过程中存在波前畸变的抽运光对信号光光束质量的影响.结果表明,当抽运光光束波前存在严重畸变时,衍射效应和走离效应通过不同的物理机制导致了信号光光束质量的急剧下降.在导致信号光光束质量下降的过程中,走离效应在OPA未饱和放大时起着主导作用,当OPA工作在过饱和状态时,过饱和导致的信号光近场空间分布中心凹陷成为光束质量下降的主要因素.     

Laser location and manipulation of a single quantum tunneling channel in an InAs quantum dot

We use a femtowatt focused laser beam to locate and manipulate a single quantum tunneling channel associated with an individual InAs quantum dot within an ensemble of dots. The intensity of the directed laser beam tunes the tunneling current through the targeted dot with an effective optical gain of 10(7) and modifies the curvature of the dot's confining potential and the spatial extent of its ground state electron eigenfunction. These observations are explained by the effect of photocreated hole charges which become bound close to the targeted dot, thus acting as an optically induced gate electrode.     

Coherent beam amplification with a photorefractive liquid crystal

Coherent amplification of a signal beam by a strong pump beam is observed in thin films of fullerene-doped nematic liquid crystal. Exponential gain constants as high as 2890 cm(-1) with no phase cross talk are achieved at low applied dc bias voltage and pump beam intensity. The underlying mechanism is the electro-optically induced spatially reorientation of the liquid-crystal axis and the resultant phase-shifted index grating required for two-beam coupling.     

Tunneling of two interacting electrons in a quantum wire

A model calculation is reported for the tunneling probability of one as well as two interacting electrons from a quantum well within a narrow channel. We discuss the cases when the two electrons are spin polarized or unpolarized by transforming the system to a noninteracting one with the use of quantal density functional theory to obtain an effective single-particle confining potential. A semiclassical approach is used to obtain the tunneling probability from this effective potential. The calculation is motivated by recent measurements of the conductance of an electron gas in a narrow channel but is not meant to explain the anomalous behavior that has been reported since, for example, we deal with a simplified two-level system. Numerical results for the tunneling probability are presented.     

Optically tunable superprism effect in nonlinear photonic crystals

An analysis of the tunable superprism effect in a two-dimensional nonlinear photonic crystal is presented. We show that, by shifting the photonic bands of the crystal through the Kerr effect induced by a pump beam, one can tune the refraction angle of a transmitted signal beam over tens of degrees. We also demonstrate that the optical power required to tune the refracted angle is dramatically reduced if the frequency of the pump beam is close to a bandgap edge.     

Doppler-free spectroscopy of neon atoms dressed by optical photons in nearly-degenerate four-wave mixing

We have investigated nearly degenerate four-wave mixing in neon on the 607 nm line. We have considered the case where one pump beam saturates the medium while the two other incident beams have a much weaker intensity. The frequency of the most intense pump beam is equal to the frequency of the probe beam. When the frequency of the second pump beam is scanned, narrow resonances are observed. These resonances correspond to transitions between the energy levels of the atom dressed by the photons of the intense pump beam.     

Dependency of injection seeding and spectral purity of a single resonant KTP optical parametric oscillator on the phase matching condition

For spectroscopic and remote sensing applications injection seeded optical parametric oscillators (OPOs) are well established. In this paper we study the dependencies of signal resonant injection seeding of an OPO on its resonator length, phase matching angle and pump power in detail. The quality of the seeding process is assessed by stabilising the seed laser on a molecular absorption line of water vapour and using a water vapour absorption cell as a narrow bandwidth filter for the injection seeded radiation. A reduction of the acceptance of injection seeding is observed with increasing pump power. For small phase mismatch injection seeding with a spectral purity of 99.7% was observed at 13-fold OPO threshold. A signal pulse energy of 38 mJ with 50% pump depletion was achieved with a beam parameter M² of about 6. PACS 42.65.Yj; 42.79.Nv; 42.79.Qx     

Spatial chirp in Ti:sapphire multipass amplifier

The spatial chirp generated in the Ti:sapphire multipass amplifier is numerically investigated based on the onedimensional(1D) and two-dimensional(2D) Frantz–Nodvik equations. The simulation indicates that the spatial chirp is induced by the spatially inhomogeneous gain, and it can be almost eliminated by utilization of proper beam profiles and spot sizes of the signal and pump pulses, for example, the pump pulse has a top-hatted beam profile and the signal pulse has a super-Gaussian beam profile with a relatively larger spot size. In this way, a clear understanding of spatial chirp mechanisms in the Ti:sapphire multipass amplifier is proposed, therefore we can effectively almost eliminate the spatial chirp and improve the beam quality of a high-power Ti:sapphire chirped pulse amplifier system.     

Competition between subharmonic and signal beams for photorefractive gain in BSO with two pump beams

It is shown that two pump beams incident upon a bismuth silicon oxide crystal give rise to a subharmonic beam bisecting the pump beam. Simultaneously a signal beam injected between the pump beams may be strongly amplified at the expense of the pump beams. It is shown that the amplified signal beam grows with a faster time constant than the subharmonic beam and that there is competition for gain in the steady state regime.     

光纤移频分布式布里渊光纤传感技术

提出了一种利用布里渊光纤环形腔移频技术实现分布式光纤布里渊传感的方法.该方法基于布里渊光时域分析法原理,将一束单纵模运转激光器输出的激光分为两束|一束光入射布里渊光纤环形腔中产生窄线宽的受激布里渊散射光作为斯托克斯光,另一束光经过低频相位调制后作为泵浦光|斯托克斯光和泵浦光分别相向入射进入传感光纤,通过测量布里渊谱得到光纤温度或应变.利用该方法可将十几GHz的微波频率转化为兆赫信号频率进行探测处理,仅需一台激光器,因此系统结构简单、成本低,还可减小激光器频率波动对测量准确度的影响.实验验证了该方法的可行性.     

Forward four-wave interactions in bismuth silicon oxide-theory and experiment

The interaction between two strong pump beams and two signal beams is investigated both theoretically and experimentally. It is shown that the frequencies of the beams need to satisfy the relation that the sum of the pump beam frequencies should be equal to the sum of the signal beam frequencies. The gain is shown to depend on the detuning of the pump beams relative to the incident signal beam and on the direction of the signal beam. Maximum gain is obtained when the signal beams bisect the pump beams.     

Nonlinear optical effects in an inhomogeneous Bose—Einstein condensate

A variety of nonlinear optical effects arising upon the interaction of a signal beam with a strong pump beam at the second harmonic frequency in a nonlinear Bose-Einstein condensate is studied. Along with the ratio of signal and pump beam widths, the influence of the mutual geometry of the trap and the pump beam profile on the studied processes is investigated.