利用法布里-珀罗腔抑制电光相位调制中的剩余幅度调制

激光经电光相位调制后,由于剩余幅度调制的存在造成调制边带幅度不相等。利用法布里-珀罗腔的透射特性和Pound-Drever-Hall技术对通过法布里-珀罗腔的调制光正、负一级边带的幅度产生不同的衰减,使得调制边带的幅度相等,从而实现对电光相位调制中剩余幅度调制的抑制。采用该方法,理论上计算了调制光经法布里-珀罗腔后的光外差光谱信号,获得锁定法布里-珀罗腔后调制边带幅度的不对称度较腔锁定前减小四个数量级。实验研究了调制光经法布里-珀罗腔透射的光外差光谱,结果表明将法布里-珀罗腔锁定于该透射光外差光谱中心零位时,对剩余幅度调制的抑制程度可达45 dB。     

微型化光纤法布里-珀罗传感器腔长一致性的控制研究

研究了光纤法布里-珀罗腔传感器的腔长一致性的控制技术.通过三维调整架组成微调装置来控制全光纤法布里-珀罗腔的腔长;结合法布里-珀罗腔的工作原理,利用光谱分析仪实时检测加工过程中法布里-珀罗腔的腔长并用装置予以修正;以热熔接的方法将毛细玻璃管与光纤加工成法布里-珀罗腔;利用超景深光学显微系统检查加工的法布里-珀罗腔的关键部位的结构,并对熔接点的牢固性进行了检测.实验结果和数据分析显示:法布里-珀罗腔的腔长得到了较好的控制及一致性,熔接部位的变形和对法布里-珀罗腔的性能的影响也很小.该工艺可用于制备全光纤法布里-珀罗腔传感器.     

光纤光栅法布里-珀罗腔的腔、栅边缘特性分析

把组成光纤光栅法布里-珀罗腔的两个光纤光栅的初相位纳入了讨论范围,用耦合波方程推导了任意初相位下光纤光栅法布里-珀罗腔的透射和反射率的表达式.其中的相位因子包含了由光传播常数调制的腔长、光纤光栅的相位突变、光纤光栅仞相位和由光纤光栅空间频率涮制的光栅长度等四部分.分析了光纤光栅初相、由光栅空间频率调制的光栅长度两个因子对反射谱的影响,并提出了一种把光纤光栅法布里-珀罗腔等效为理想法布里-珀罗腔的方法.     

一种同时测量电流和温度的光纤光栅传感器

提出了一种基于光纤光栅法布里-珀罗干涉仪且可以同时测量交变电流和温度的传感器,并对其进行了理论分析和实验研究.该传感器采用单频激光入射,作为反射镜的一对光纤布喇格光栅自由放置,其间的法布里-珀罗腔粘贴在磁致伸缩材料上,通电导线周围的磁场通过磁致伸缩材料作用于光纤光栅法布里-珀罗腔,引起腔长周期性变化.同时,由于热膨胀和热光效应,环境温度的变化会引起光纤长度和折射率的改变,从而改变光纤光栅法布里-珀罗腔的反射光谱特性.通过检测输出光信号的频率和峰值可实现电流和温度的同时测量.对通电线圈的电流及环境温度进行测量的实验结果与理论分析相吻合.     

一种同时测量电流和温度的光纤光栅传感器

提出了一种基于光纤光栅法布里-珀罗干涉仪且可以同时测量交变电流和温度的传感器,并对其进行了理论分析和实验研究.该传感器采用单频激光入射,作为反射镜的一对光纤布喇格光栅自由放置,其间的法布里-珀罗腔粘贴在磁致伸缩材料上,通电导线周围的磁场通过磁致伸缩材料作用于光纤光栅法布里-珀罗腔,引起腔长周期性变化.同时,由于热膨胀和热光效应,环境温度的变化会引起光纤长度和折射率的改变,从而改变光纤光栅法布里-珀罗腔的反射光谱特性.通过检测输出光信号的频率和峰值可实现电流和温度的同时测量.对通电线圈的电流及环境温度进行测量的实验结果与理论分析相吻合.     

短腔长复合式光纤法布里-珀罗压力传感器椭圆拟合腔长解调算法

建立了一种短腔长复合式光纤法布里-珀罗压力传感器反射光谱的模型,提出了一种双参数椭圆拟合腔长解调算法,并对腔长为26～30μm的复合式法布里-珀罗腔的解调进行了仿真。结果表明,采用双参数椭圆拟合算法进行腔长解调的最大误差仅为0.05μm。搭建了光纤法布里-珀罗传感器解调系统,在加压条件下对复合式光纤法布里-珀罗压力传感器进行了解调实验,实现了20 kHz的解调速率,验证了所提算法在解调短腔长复合式光纤法布里-珀罗压力传感器方面的可行性与实时性。     

本征不对称光纤法布里-珀罗干涉仪的理论模型

应用光学和数学理论导出本征不对称光纤法布里－珀罗干涉仪中反射光与透射光的数学模型及低反射率法布里－珀罗干涉腔长度的变化与干涉光光强的数学模型,半指出当ｒ１１＝ｔ１ｔ１ｒ２＝ｒ,且ｔ１ｔ１＝１－ｒ１＾２≈２。则法布里－珀罗腔反射光间的干涉近似为两束等幅光的干涉;文章还给出了光电转换器输出与法布里－珠罗干涉腔长度变化的数学模型。这些模型为不对称光纤法布里－珀罗干涉仪的使用提供理论依据。     

高精细度微透镜光纤法布里-珀罗干涉仪

通过在镀膜单模光纤端面制作微透镜,构造了微透镜光纤法布里-珀罗干涉仪.利用ABCD矩阵方法分析厂微透镜法布单-珀罗腔的模场.由于微透镜的会聚作用,法布里-珀罗腔模场可以和单模光纤模场良好的匹配,从而达到高精细度和低插入损耗.实验制作的微透镜光纤法布里-珀罗干涉仪,自由光谱区范围32.28 nm,精细度为78,峰值透射比为73%;在法布里-珀罗腔的光学腔长增加到100um的情况下,峰值透射比仍然大于50%.该微透镜光纤法布里-珀罗十涉仪制作容易、对设备要求低,可以封装成光纤法布里-珀罗滤波器和传感器,具有广泛的应用前景.     

双法布里—珀罗干涉仪传感模型的理论分析

本文提出了一种用发光二极管作为光源、用自聚焦透镜构成法布里-珀罗腔的双法布里-珀罗干涉仪光纤位移传感模型.根据部分相干光的干涉理论,得到了这个传感模型输出光强与两个法布里一珀罗干涉仪腔长之差的函数曲线.     

光纤光栅法布里-珀罗腔中受激布里渊散射的理论研究

对光纤光栅法布里-珀罗腔中稳态受激布里渊散射模型进行了理论分析,在其耦合强度方程组基础上,推导出仅产生一阶斯托克斯波时,耦合强度方程组的解析表达式,由此计算出光纤光栅法布里-珀罗腔中抽运波与斯托克斯波透射功率和反射功率。对于光纤光栅法布里-珀罗腔中二阶斯托克斯波的产生,推导出光纤光栅法布里-珀罗腔入射端抽运波的解析表达式和忽略光纤损耗时能量守恒方程,利用Shooting和L-M算法数值求解出耦合强度方程组。分析讨论了抽运波,一阶斯托克斯波和二阶斯托克斯波的反射与透射功率随着入射波功率变化的情况。最后,仿真出光纤光栅法布里-珀罗腔中,抽运波与斯托克斯波沿腔长分布的情况。     

Inelastic light scattering by a two-dimensional electron system with Rashba spin-orbit coupling

Inelastic light scattering by a two-dimensional system of electrons in a conduction band with Rashba spinorbit coupling is studied theoretically for the resonance case where the frequencies of the incident and scattered light are close to the effective distance between the conduction band and spin-split band in a III–V semiconductor. It is shown that, in contrast to the case of no spin-orbit coupling, the spectrum of the scattered light exhibits a plasmon peak even for strictly perpendicular polarizations of the incident and scattered light. There exists a configuration where the scattering spectrum exhibits features originating from single-particle transitions only. Furthermore, it is shown that, for the general case of elliptic polarizations of the incident and scattered light, the amplitude of the plasmon peak depends on the sign of the effective Rashba spinorbit coupling constant and the signs of the phases of the polarization vectors. This fact can be used to determine the sign of the Rashba constant.     

Active light noise filter by a differential operation

A method for an active light noise filter is proposed by using two identical light receivers. They work as a differential electrometer by a common mode connection. Therefore, only an output of a laser light incident upon one receiver can be obtained as a signal. It was found from the experiment that the light noise was reduced to about 0.6% in the usual light room and further the signal to noise ratio was improved up to 30 times at least as compared to a usual light shielding method. The method can then be effectively used under a well-lighted room such as a factory without noise light shielding cover.     

Depolarization of backscattered linearly polarized light from ZnO thin film

The depolarization behavior of backscattered linearly polarized light from ZnO thin film was investigated experimentally. The results show that the characteristics are related to both the polarization orientation and wavelength of linearly polarized incident light. When the incident light is s-polarized, the depolarization behaviors are different for different wavelengths. When the incident light is p-polarized, the depolarization behaviors, on the contrary, are similar for different wavelengths. In addition, there is an optimal incident angle for depolarization of linearly polarized light with different wavelengths, which is equal to their effective Brewster angles, respectively.     

Polarization characteristics and magneto-optic diffraction efficiency at oblique light incidence

In a great number of papers that deal with the study of the magneto-optic diffraction (MOD), theoretical analysis and interpretation of experimental data are performed without regard for reflection effects of the incident and diffracted light beams on the entrance and exit surfaces of the transparent film. In consequence the MOD parameters are not connected with the angle of light incidence and the orientation of the incident light polarization plane. In the present work the reflection effects are taken into account. For the Raman-Nat diffraction region the general expressions involving the relationships of diffracted light polarization and intensity with the symmetry of the grating, angle of incidence and polarization of the incident light are obtained. In particular it is shown that even for a symmetrical grating the polarization of the zeroth-order diffracted beam differs from that of the incident light, and the polarization of higher-order beams differs from the orthogonal one providing that the incident light is not s- or p-polarized. A maximum in the angular dependence of diffraction efficiency is predicted being observed experimentally.     

Experimental investigation of magnetically induced unusual emission of light from a ferrodispersion

An unusual emission of light is observed when a coherent light beam is passed through a mixture of a magnetorheological suspension and a ferrofluid that is subjected to a critical magnetic field. When first the incident light is removed and then the field is switched off, a flash of light is observed. In this Letter certain characteristics of this unusual emission are reported. Our findings suggest that a part of the incident light energy is magnetically trapped within the medium. Upon removal of the field, the same is released. Several physical phenomena that may give rise to such emission are discussed. The magnetically tunable emission will be useful to develop photonic devices.     

Height distribution on a rough plane and specularly diffracted light amplitude are Fourier transform pair

In this report we show that the amplitude of specularly diffracted light from a plane rough surface as a function of incident angle cosine is Fourier transform of the height distribution on the surface. Therefore, an even height distribution function, which is the case for many rough surfaces, can be obtained by measuring the specularly diffracted light intensities. Also, it is observed that for polychromatic illumination the spectrum of the specularly diffracted light is modified and the modification depends on roughness, incident angle, and wavelength. It is also shown that, for a fixed incident angle, the height distribution on the rough plane is Fourier transform of the spectral modifying function. Experimental studies on some surfaces of different roughnesses, prepared by grinding sheet-glasses by powders of different grain sizes, show that the corresponding height distributions are Gaussian and the rms heights obtained by the two approaches are quite consistent.     

High-efficiency frequency-modulation non-redundant scanning of a light beam in a half space

It is shown that a large fraction of the energy of the impinging light beam on a parallel plate grating can be injected into only one transmitted order, which is not the zeroth transmitted order, when the incident angle of the beam and the refractive indices of the lossless dielectric bounding media satisfy the condition of total reflection. This signififies that non-redundant scanning of the radiation transmitted through the grafting can be obtained by varying the frequency of the incident radiation with little of the incident energy being scattered into the reflected orders.     

Influence of incident light polarization on photonic nanojet

Dielectric microspheres can confine light in a three-dimensional (3D) region called photonic nanojet is shown when they are illuminated by different polarized beams. The influence of incident light polarization on photonic nanojet using the finite-difference time-domain (FDTD) method is demostrated. The axial field intensity profiles of photonic nanojets for both the linear and circular polarization incident beams are very similar. Azimuthal polarization incident beam induces a doughnut beam along the optical axis, while the radial polarization incident beam permits one to reach an effective volume as small as 0.7(λ/n) 3 .     

部分相干椭球光笼

 从理论上研究部分相干光束经透镜聚焦的三维光强分布。研究结果表明，在几何焦点附近的光强分布不仅依赖于入射部分相干光束的光强分布，而且还依赖于入射光束的空间相干度。基于这一点，提出了一种控制部分相干光束的空间相干度，在几何焦点附近获得了类似椭球光笼形状的光强分布的新方法。通过控制入射部分相干光的空间相干度，来改变聚焦在几何焦点附近的三维光强分布，从而获得希望得到的光强分布。     

Forward light reflection from a moving inhomogeneity

The reflection of monochromatic and quasi-monochromatic pulsed light incident on a moving inhomogeneity in the optical characteristics of a medium having plasma-type dispersion has been analyzed. The velocity V of the inhomogeneity, induced in the medium by an intense laser pulse, has been changed by varying its carrier frequency. It has been shown that the usual back-reflection mode, when the reflected radiation pulse moves in the direction opposite the direction of incident radiation, is implemented only if the velocity V is less than the critical value V _min, which depends on the carrier frequency of the incident radiation pulse. It has been found that reflected radiation moves in the same direction as the incident radiation in a certain range of the velocity V _min < V < V _max (forward reflection). In this case, the reflected radiation pulse begins to lag behind a fast-moving inhomogeneity. When V _max < V < c, where c is the speed of light in vacuum, the group velocity of the incident radiation pulse is less than the speed of inhomogeneity, and there is no reflection. Analytical treatment is supported by numerical simulation.