knowledge absorption in the Optical Technology (OT) industry in Shanghai A slender string design for
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光谱分形状英文名Fractal SpectraThe captivating world of fractals has long been a source of fascination for scientists, mathematicians, and artists alike. One particularly intriguing aspect of this intricate geometric realm is the exploration of fractal spectra. These remarkable patterns, rooted in the fundamental principles of light and energy, have the power to unveil the hidden complexities of our natural world.Fractals, by their very nature, are self-similar structures that exhibit patterns at every scale, from the microscopic to the cosmic. When applied to the study of light and electromagnetic radiation, these fractal structures reveal a depth of understanding that transcends the boundaries of traditional scientific inquiry. The fractal spectra, a manifestation of this interplay between light and geometry, offer a unique window into the underlying rhythms and harmonies that govern the universe.At the core of fractal spectra lies the concept of self-similarity, where patterns repeat across different scales. This principle is exemplified in the renowned Mandelbrot set, a striking fractal shape that hascaptured the imagination of countless individuals. When this fractal is subjected to spectral analysis, the resulting patterns often exhibit a remarkable level of complexity and beauty, mirroring the intricate structure of the original form.One of the key aspects of fractal spectra is their ability to reveal the hidden harmonies within the electromagnetic spectrum. By decomposing light into its constituent wavelengths, the fractal patterns that emerge often display intricate and mesmerizing designs. These patterns can be seen in the vibrant hues of a rainbow, the shimmering iridescence of butterfly wings, and the shimmering patterns of light on the surface of a pond.Delving deeper into the realm of fractal spectra, we begin to uncover the profound connections between the microscopic and the macroscopic. The self-similar patterns observed in the spectra of individual atoms and molecules are echoed in the larger-scale structures of galaxies and cosmic phenomena. This realization has led to groundbreaking discoveries in fields such as quantum physics, astrophysics, and materials science, as researchers strive to unravel the underlying principles that govern the behavior of light and energy.The exploration of fractal spectra has also had a profound impact on our understanding of the natural world. By studying the fractalpatterns in the absorption and emission spectra of various materials, scientists have been able to gain insights into the molecular and atomic structures of these substances. This knowledge has enabled advancements in fields ranging from chemistry and materials science to biology and medical research.Furthermore, the fractal nature of light has inspired a wealth of artistic expression and technological innovation. Visual artists have long been captivated by the mesmerizing patterns of fractal spectra, incorporating them into mesmerizing works of art that blur the boundaries between science and aesthetics. Similarly, the principles of fractal optics have revolutionized the design of optical devices, from high-resolution imaging systems to advanced communication technologies.In conclusion, the exploration of fractal spectra represents a profound and ongoing journey of scientific discovery, artistic expression, and technological advancement. By delving into the intricate patterns and harmonies that govern the behavior of light and energy, we unlock a deeper understanding of the fundamental principles that shape our universe. The study of fractal spectra promises to continue yielding transformative insights, as we strive to unravel the mysteries of the natural world and push the boundaries of human knowledge and creativity.。
《光电技术》专业英语词汇1.Absorption coefficient 吸收系数2.Acceptance angle 接收角3.fibers 光纤4.Acceptors in semiconductors 半导体接收器5.Acousto-optic modulator 声光调制6.Bragg diffraction 布拉格衍射7.Air disk 艾里斑8.angular radius 角半径9.Airy rings 艾里环10.anisotropy 各向异性11.optical 光学的12.refractive index 各向异性13.Antireflection coating 抗反膜14.Argon-ion laser 氩离子激光器15.Attenuation coefficient 衰减系数16.Avalanche 雪崩17.breakdown voltage 击穿电压18.multiplication factor 倍增因子19.noise 燥声20.Avalanche photodiode(APD) 雪崩二极管21.absorption region in APD APD 吸收区域22.characteristics-table 特性表格23.guard ring 保护环24.internal gain 内增益25.noise 噪声26.photogeneration 光子再生27.primary photocurrent 起始光电流28.principle 原理29.responsivity of InGaAs InGaAs 响应度30.separate absorption and multiplication(SAM) 分离吸收和倍增31.separate absorption grading and multiplication(SAGM) 分离吸收等级和倍增32.silicon 硅33.Average irradiance 平均照度34.Bandgap 带隙35.energy gap 能级带隙36.bandgap diagram 带隙图37.Bandwidth 带宽38.Beam 光束39.Beam splitter cube立方分束器40.Biaxial crystals 双轴晶体41.Birefringent 双折射42.Bit rate 位率43.Black body radiation law 黑体辐射法则44.Bloch wave in a crystal 晶体中布洛赫波45.Boundary conditions 边界条件46.Bragg angle 布拉格角度47.Bragg diffraction condition 布拉格衍射条件48.Bragg wavelength 布拉格波长49.Brewster angle 布鲁斯特角50.Brewster window 布鲁斯特窗51.Calcite霰石52.Carrier confinement 载流子限制53.Centrosymmetric crystals 中心对称晶体54.Chirping 啁啾55.Cladding覆层56.Coefficient of index grating 指数光栅系数57.Coherence 连贯性pensation doping 掺杂补偿59.Conduction band 导带60.Conductivity 导电性61.Confining layers 限制层62.Conjugate image 共轭像63.Cut-off wavelength 截止波长64.Degenerate semiconductor简并半导体65.Density of states 态密度66.Depletion layer 耗尽层67.Detectivity 探测率68.Dielectric mirrors 介电质镜像69.Diffraction 衍射70.Diffraction grating 衍射光栅71.Diffraction grating equation 衍射光栅等式72.Diffusion current 扩散电流73.Diffusion flux 扩散流量74.Diffusion Length 扩散长度75.Diode equation 二极管公式76.Diode ideality factor 二极管理想因子77.Direct recombination 直接复合78.Dispersion 散射79.Dispersive medium 散射介质80.Distributed Bragg reflector 分布布拉格反射器81.Donors in semiconductors 施主离子82.Doppler broadened linewidth 多普勒扩展线宽83.Doppler effect 多普勒效应84.Doppler shift 多普勒位移85.Doppler-heterostructure 多普勒同质结构86.Drift mobility漂移迁移率87.Drift Velocity 漂移速度88.Effective density of states 有效态密度89.Effective mass 有效质量90.Efficiency 效率91.Einstein coefficients 爱因斯坦系数92.Electrical bandwidth of fibers 光纤电子带宽93.Electromagnetic wave 电磁波94.Electron affinity 电子亲和势95.Electron potential energy in a crystal 晶体电子阱能量96.Electro-optic effects 光电子效应97.Energy band 能量带宽98.Energy band diagram 能量带宽图99.Energy level 能级100.Epitaxial growth外延生长101.Erbium doped fiber amplifier 掺饵光纤放大器102.Excess carrier distribution 过剩载流子扩散103.External photocurrent 外部光电流104.Extrinsic semiconductors 本征半导体105.Fabry-Perot laser amplifier 法布里-珀罗激光放大器106.Fabry-Perot optical resonator 法布里-珀罗光谐振器107.Faraday effect 法拉第效应108.Fermi-Dirac function 费米狄拉克结109.Fermi energy 费米能级110.Fill factor 填充因子111.Free spectral range 自由谱范围112.Fresnel’s equations菲涅耳方程113.Fresnel’s optical indicatrix 菲涅耳椭圆球114.Full width at half maximum半峰宽115.Full width at half power半功率带宽116.Gaussian beam 高斯光束117.Gaussian dispersion 高斯散射118.Gaussian pulse 高斯脉冲119.Glass perform玻璃预制棒120.Goos Haenchen phase shift Goos Haenchen相位移121.Graded index rod lens 梯度折射率棒透镜122.Group delay 群延迟123.Group velocity 群参数124.Half-wave plate retarder 半波延迟器125.Helium-Neon laser氦氖激光器126.Heterojunction 异质结127.Heterostructure 异质结构128.Hole 空穴129.Hologram 全息图130.Holography 全息照相131.Homojunction 同质结132.Huygens-Fresnel principle惠更斯-菲涅耳原理133.Impact-ionization 碰撞电离134.Index matching 指数匹配135.Injection 注射136.Instantaneous irradiance 自发辐射137.Integrated optics 集成光路138.Intensity of light 光强139.Intersymbol interference 符号间干扰140.Intrinsic concentration本征浓度141.Intrinsic semiconductors 本征半导体142.Irradiance 辐射SER 激光144.active medium 活动介质145.active region 活动区域146.amplifiers 放大器147.cleaved-coupled-cavity解理耦合腔148.distributed Bragg reflection 分布布拉格反射149.distributed feedback 分布反馈150.efficiency of the He-Ne 氦氖效率151.multiple quantum well 多量子阱152.oscillation condition 振荡条件ser diode 激光二极管sing emission 激光发射155.LED 发光二极管156.Lineshape function 线形结157.Linewidth 线宽158.Lithium niobate铌酸锂159.Load line 负载线160.Loss coefficient 损耗系数161.Mazh-Zehnder modulator Mazh-Zehnder型调制器162.Macrobending loss 宏弯损耗163.Magneto-optic effects 磁光效应164.Magneto-optic isolator 磁光隔离165.Magneto-optic modulator 磁光调制166.Majority carriers 多数载流子167.Matrix emitter 矩阵发射168.Maximum acceptance angle 最优接收角169.Maxwell’s wave equation 麦克斯维方程170.Microbending loss 微弯损耗171.Microlaser 微型激光172.Minority carriers 少数载流子173.Modulated directional coupler 调制定向偶合器174.Modulation of light 光调制175.Monochromatic wave 单色光176.Multiplication region 倍增区177.Negative absolute temperature 负温度系数 round-trip optical gain 环路净光增益179.Noise 噪声180.Noncentrosymmetric crystals 非中心对称晶体181.Nondegenerate semiconductors 非简并半异体182.Non-linear optic 非线性光学183.Non-thermal equilibrium 非热平衡184.Normalized frequency 归一化频率185.Normalized index difference 归一化指数差异186.Normalized propagation constant 归一化传播常数187.Normalized thickness 归一化厚度188.Numerical aperture 孔径189.Optic axis 光轴190.Optical activity 光活性191.Optical anisotropy 光各向异性192.Optical bandwidth 光带宽193.Optical cavity 光腔194.Optical divergence 光发散195.Optic fibers 光纤196.Optical fiber amplifier 光纤放大器197.Optical field 光场198.Optical gain 光增益199.Optical indicatrix 光随圆球200.Optical isolater 光隔离器201.Optical Laser amplifiers 激光放大器202.Optical modulators 光调制器203.Optical pumping 光泵浦204.Optical resonator 光谐振器205.Optical tunneling光学通道206.Optical isotropic光学各向同性的207.Outside vapor deposition管外气相淀积208.Penetration depth 渗透深度209.Phase change 相位改变210.Phase condition in lasers 激光相条件211.Phase matching 相位匹配212.Phase matching angle 相位匹配角213.Phase mismatch 相位失配214.Phase modulation 相位调制215.Phase modulator 相位调制器216.Phase of a wave 波相217.Phase velocity 相速218.Phonon 光子219.Photoconductive detector 光导探测器220.Photoconductive gain 光导增益221.Photoconductivity 光导性222.Photocurrent 光电流223.Photodetector 光探测器224.Photodiode 光电二极管225.Photoelastic effect 光弹效应226.Photogeneration 光子再生227.Photon amplification 光子放大228.Photon confinement 光子限制229.Photortansistor 光电三极管230.Photovoltaic devices 光伏器件231.Piezoelectric effect 压电效应232.Planck’s radiation distribution law 普朗克辐射法则233.Pockels cell modulator 普克尔斯调制器234.Pockel coefficients 普克尔斯系数235.Pockels phase modulator 普克尔斯相位调制器236.Polarization 极化237.Polarization transmission matrix 极化传输矩阵238.Population inversion 粒子数反转239.Poynting vector能流密度向量240.Preform 预制棒241.Propagation constant 传播常数242.Pumping 泵浦243.Pyroelectric detectors 热释电探测器244.Quantum efficiency 量子效应245.Quantum noise 量子噪声246.Quantum well 量子阱247.Quarter-wave plate retarder 四分之一波长延迟248.Radiant sensitivity 辐射敏感性249.Ramo’s theorem拉莫定理250.Rate equations速率方程251.Rayleigh criterion 瑞利条件252.Rayleigh scattering limit 瑞利散射极限253.Real image 实像254.Recombination 复合255.Recombination lifetime 复合寿命256.Reflectance 反射257.Reflection 反射258.Refracted light 折射光259.Refractive index 折射系数260.Resolving power分辩力261.Response time 响应时间262.Return-to-zero data rate 归零码263.Rise time 上升时间264.Saturation drift velocity 饱和漂移速度265.Scattering 散射266.Second harmonic generation 二阶谐波267.Self-phase modulation 自相位调制268.Sellmeier dispersion equation色列米尔波散方程式269.Shockley equation肖克利公式270.Shot noise肖特基噪声271.Signal to noise ratio 信噪比272.Single frequency lasers 单波长噪声273.Single quantum well 单量子阱274.Snell’s law斯涅尔定律275.Solar cell 光电池276.Solid state photomultiplier 固态光复用器277.Spectral intensity 谱强度278.Spectral responsivity 光谱响应279.Spontaneous emission 自发辐射280.stimulated emission 受激辐射281.Terrestrial light 陆地光282.Theraml equilibrium热平衡283.Thermal generation 热再生284.Thermal velocity 热速度285.Thershold concentration 光强阈值286.Threshold current 阈值电流287.Threshold wavelength 阈值波长288.Total acceptance angle 全接受角289.Totla internal reflection 全反射290.Transfer distance 转移距离291.Transit time 渡越时间292.Transmission coefficient 传输系数293.Tramsmittance 传输294.Transverse electric field 电横波场295.Tranverse magnetic field 磁横波场296.Traveling vave lase 行波激光器297.Uniaxial crystals 单轴晶体298.UnPolarized light 非极化光299.Wave 波300.Wave equation 波公式301.Wavefront 波前302.Waveguide 波导303.Wave number 波数304.Wave packet 波包络305.Wavevector 波矢量306.Dark current 暗电流307.Saturation signal 饱和信号量308.Fringing field drift 边缘电场漂移plementary color 补色310.Image lag 残像311.Charge handling capability 操作电荷量312.Luminous quantity 测光量313.Pixel signal interpolating 插值处理314.Field integration 场读出方式315.Vertical CCD 垂直CCD316.Vertical overflow drain 垂直溢出漏极317.Conduction band 导带318.Charge coupled device 电荷耦合组件319.Electronic shutter 电子快门320.Dynamic range 动态范围321.Temporal resolution 动态分辨率322.Majority carrier 多数载流子323.Amorphous silicon photoconversion layer 非晶硅存储型324.Floating diffusion amplifier 浮置扩散放大器325.Floating gate amplifier 浮置栅极放大器326.Radiant quantity 辐射剂量327.Blooming 高光溢出328.High frame rate readout mode 高速读出模式329.Interlace scan 隔行扫描330.Fixed pattern noise 固定图形噪声331.Photodiode 光电二极管332.Iconoscope 光电摄像管333.Photolelctric effect 光电效应334.Spectral response 光谱响应335.Interline transfer CCD 行间转移型CCD336.Depletion layer 耗尽层plementary metal oxide semi-conductor 互补金属氧化物半导体338.Fundamental absorption edge 基本吸收带339.Valence band 价带340.Transistor 晶体管341.Visible light 可见光342.Spatial filter 空间滤波器343.Block access 块存取344.Pupil compensation 快门校正345.Diffusion current 扩散电流346.Discrete cosine transform 离散余弦变换347.Luminance signal 高度信号348.Quantum efficiency 量子效率349.Smear 漏光350.Edge enhancement 轮廓校正351.Nyquist frequency 奈奎斯特频率352.Energy band 能带353.Bias 偏压354.Drift current 漂移电流355.Clamp 钳位356.Global exposure 全面曝光357.Progressive scan 全像素读出方式358.Full frame CCD 全帧CCD359.Defect correction 缺陷补偿360.Thermal noise 热噪声361.Weak inversion 弱反转362.Shot noise 散粒噪声363.Chrominance difference signal 色差信号364.Color temperature 色温365.Minority carrier 少数载流子366.Image stabilizer 手振校正367.Horizontal CCD 水平CCD368.Random noise 随机噪声369.Tunneling effect 隧道效应370.Image sensor 图像传感器371.Aliasing 伪信号372.Passive 无源373.Passive pixel sensor 无源像素传感器374.Line transfer 线转移375.Correlated double sampling 相关双采样376.Pinned photodiode 掩埋型光电二极管377.Overflow 溢出378.Effective pixel 有效像素379.Active pixel sensor 有源像素传感器380.Threshold voltage 阈值电压381.Source follower 源极跟随器382.Illuminance 照度383.Refraction index 折射率384.Frame integration 帧读出方式385.Frame interline transfer CCD 帧行间转移CCD 386.Frame transfer 帧转移387.Frame transfer CCD 帧转移CCD388.Non interlace 逐行扫描389.Conversion efficiency 转换效率390.Automatic gain control 自动增益控制391.Self-induced drift 自激漂移392.Minimum illumination 最低照度393.CMOS image sensor COMS图像传感器394.MOS diode MOS二极管395.MOS image sensor MOS型图像传感器396.ISO sensitivity ISO感光度。
光学模型介绍英文作文英文:Optical model is a mathematical model that describesthe behavior of light in various media, such as air, water, and glass. It is widely used in the field of optics to predict and analyze the propagation, reflection, refraction, and absorption of light.The optical model is based on the principles of geometrical optics and wave optics. Geometrical optics assumes that light travels in straight lines and obeys the laws of reflection and refraction at the interface between two media. Wave optics, on the other hand, considers light as a wave that can diffract, interfere, and undergo polarization.One of the most important parameters in the optical model is the refractive index, which is a measure of how much a material slows down the speed of light. Therefractive index is different for different materials and can be used to calculate the angle of refraction when light passes through a medium.Another important parameter is the absorption coefficient, which measures how much light is absorbed by a material per unit distance. This is important for designing optical devices such as filters and lenses.In addition to these parameters, the optical model also considers factors such as the thickness of the medium, the angle of incidence, and the polarization state of light. By combining all these factors, the optical model can accurately predict the behavior of light in various scenarios.中文:光学模型是一种描述光在各种介质中行为的数学模型,例如空气、水和玻璃。
一 Make a choice 1) In graded-index optical fiber, the numerical aperture NA can be expressed as C.A. 21n n -B. ∆2aC. ∆2n 1D. 21n n a -2) In practical SMFs, the core diameter is just below the cutoff of the first higher-order mode; that is, for V slightly A.A. <2.4B. > 2.4C. =3D. =3.53) When the phase difference is an integral multiple of _2π_, the two modes will beat and the input polarization state will be reproduced.A. 2πB. πC. 1800D. π/24) It is well known that the total dispersion in the single-mode regime is composed of two components: C.A. mode-partition noise, inter- symbol InterferenceB. frequency chirp , modal dispersionC. material dispersion , waveguide dispersionD. modal dispersion , waveguide dispersion5) Which of the following codes cannot be transmitted in fibers B. A. CMI B. HDB3 C. 5B6B D. 8B1H6) Dispersion-shifted fiber (DSF) is a type of single-mode fiber designed to have zero dispersion near A nm. A. 1550 B. 850 C. 1310 D. 15107) To make sure that the APD photo detector works properly, a sufficiently D is applied across the p-n junction.A. high forward-bias voltageB. low forward-bias voltageC. low reverse-bias voltageD. high reverse-bias voltage8) A single mode fiber usually has a core diameter of A.A. 10mB. 62.5nmC. 125nmD. 50mm二Blank filling1) Each SDH frame comprising three areas: a section overhead area (SOH ), a pointer area, a payload area including the data to be transmitted.2) List three applications of FBG(fiber Bragg grating): filter 、Optical Add Drop Multiplexer(OADM) and dispersion compensator. 3) According to whether there is electric or magnetic field in the direction of propagation or not, transverse modes of light waves are classified into different types: TEM modes, TE modes, TM modes and hybrid modes.4) Transmission of information in an optical format is carried out not by frequency modulation of the carrier, but by varying the intensity of the optical power.5) Largely due to attenuation and dispersion, the optical signals undergo waveform distortion and decreased amplitude.6) Material dispersion occurs because the index of refraction varies as a function of the optical wavelength.7) ZDSF is a dispersion shifted single mode fiber that has the zero dispersion wavelength near the 1550 nm window, but outside the window actually used to transmit signals.8)A laser is constructed from three principal parts: a pump source, a gain medium, and an optical resonator.9)An optical fiber comprises at least two layers, a core and a cladding.10)Optical transmitter consists of optical source, a modulator and a channel coupler.11)Fiber refractive index profiles classify fibers as step-index fibers and graded-index fibers.12)BER (The bit error rate) performance and jitter are two important indicators in a opticaldigital communication system.13)LASER is a mechanism for emitting light within the electromagnetic radiation region of thespectrum, via the process of stimulated emission.14)There are two kinds of SOA:Fabry-Perot Amplifier (FPA) and Traveling-Wave Amplifier(TWA) .15)The principal noises associated with photo detectors that have no internal gain are quantumnoise, dark-current noise generated in the bulk material of the photodiode, and surface leakage current noise.16)In a step-index fiber, the refractive index of the core is uniform and undergoes an abruptchange at the core-cladding boundary. In graded-index fibers, the refractive index of the core varies gradually as a function of radial distance from the fiber center.17)If the input pulse excites both polarization components, it becomes broader as the twocomponents disperse along the fiber because of their different group velocities. This phenomenon is called the PMD.18)The most common semiconductor photo detector is the pin photodiode.19)The main cause of intrinsic absorption in the infrared region is the characteristic vibrationfrequency of atomic bonds.20)In SDH transmission structures, a TU (Tributary Unit) includes a low level VC and a TUPTR.21)Extrinsic absorption is caused by impurities introduced into the fiber material.22)Intramodal dispersion is a result of the group velocity being a function of the wavelength.23)The optical amplifiers is divided into 3 groups: semiconductor optical amplifier (SOA),optical fiber amplifier (OPA) and Raman amplifier (FRA).24)There are two kinds of directional couplers: a prism-fibre and a fibre-fibre lapped coupler.25)EDFA has three pumping structures: ①the forward pumping structure; ②the backwardpumping structure; ③ the double pumping structure.26) A laser consists of a gain medium inside a highly reflective optical cavity, as well as a meansto supply energy to the gain medium.27)Attenuation in an optical fiber is caused by absorption losses, scattering losses, and bendinglosses.28)STM-1 frames provide a transmission bit rate of 155 Mbit/s.29)From the point of view of the wave theory, light wave could be described as anelectromagnetic wave.30)Intermodal dispersion is a result of each mode having a different value of the group velocityat a single frequency.31) A typical optical digital communication system usually comprises three parts: transmitter,optical fiber channel, and receiver.32)The pin Photo detector structure consists of p and n regions separated by a very lightlyn-doped intrinsic (i) region.33)Please list three steps of SDH Multiplexing: mapping,aligning ,multiplexing.34)There are three variations of WDM that are commonly used: Broad WDM, Coarse WDM, and Dense WDM. 35)The STM-1 frame is the basic transmission format for SDH. The frame lasts for 125 microseconds; therefore there are 8000 frames per second. 36)In SDH frame structure, the SOH is made up of a regenerator section overhead (RSOH) and a multiplexing section overhead (MSOH). 37)The sensitivity of a photo detector in an optical fiber communication system is describable in terms of the minimum detectable optical power. 38)Please list three applications of EDFA in optical fiber communication system: as preamplifier of receiver 、as power amplifier of transmitter and as the optical repeater. 39) An optical isolator (optical diode), is an optical component which allows the transmission oflight in only one direction.三Interpretation of terms and phrases1) AON (all-optical network) 2) DBR (distributed Bragg reflector)3)FDDI (fiber distributed data interface) 4)HFC (hybrid fiber-coaxial)5)ISDN (integrated services digital network) 6)RA (raman amplifier)7)OC (optical carrier) 8)OTDM (optical time-division multiplexing)9)PON (passive optical network) 10)SCM (subcarrier multiplexing)11)SDH (synchronous digital hierarchy) 12)SPM (self-phase modulation)13)STS (synchronous transpor signal) 14)TW (traveling wave)15)WGA (waveguide-grating router) 16)IMD (intermodulation disortion)17)AWG (arrayed-waveguide grating) 18)AOTF (acousto-optic tunable filter)四 画图题1) Draw the element block of a Distributed forward Raman amplifier2) Draw an element diagram of a Double pump EDFA3) Draw a block diagram of a typical optical digital communication system and briefly describe the functions of each part.OutputInput EDF WDM IsolatorPump Laser Isolator Pump Laser WDMPump Laser outputfiber inputAn optical communication system consists of a transmitter, which encodes a message into an optical signal, a channel, which carries the signal to its destination, and a receiver, which reproduces the message from the received optical signal. The optical repeater is to extend the transmission distance of optical signal.4) Draw the element diagram of the application of optical amplifier.四 简答题1) Dispersion: Any phenomenon in which the velocity of propagation of any electromagnetic wave is wavelength dependent.2) Stimulated EmissionsIf a photon of energy hv 12 impinges on the system while the electron is still in its excited state, the electron is immediately stimulated to drop to the ground state and give off a photon of energy hv 12.3) There are 3 dispersion types in the optical fibers in general:1- Material Dispersion2- Waveguide Dispersion3- Polarization-Mode Dispersion4) Polarization mode dispersion (PMD) is due to slightly different velocity for each polarization mode because of the lack of perfectly symmetric & anisotropic of the fiber5) Laser is an optical oscillator. It comprises a resonant optical amplifier whose output is fed back into its input with matching phase. Any oscillator contains:1. An amplifier with a gain-saturated mechanism2. A feedback system3. A frequency selection mechanism4. An output coupling scheme Optical transmitter Repeater Opticalreceiverfiber fiber6) In thermal equilibrium the stimulated emission is essentially negligible, since the density of electrons in the excited state is very small, and optical emission is mainly because of the spontaneous emission. Stimulated emission will exceed absorption only if the population of the excited states is greater than that of the ground state. This condition is known as Population Inversion. Population inversion is achieved by various pumping techniques.7) Turn on DelayWhen the driving current suddenly jumps from low (I1 < Ith) to high (I2 > Ith) , (step input), there is a finite time before the laser will turn on8) The Quantum LimitFor an ideal photo-detector having unity quantum efficiency and producing no dark current, it is possible to find the minimum received optical power required for a specific BER performance in a digital system. This minimum received power level is known as the quantum limit.9) Gain flatness: The difference between the biggest gain and the smallest gain of the different frequency signal.10) The advantage of Raman amplifier: Simple fabricationLow noise, because amplifying action take place inside the ordinarily fiber.The wavelength can be selected in the low loss waveband.Very wide gain bandwidth.11) Micro bending Loss: microscopic bends of the fiber axis that can arise when the fibers are incorporated into cables. The power is dissipated through the micro bended fiber, because of the repetitive coupling of energy between guided modes & the leaky or radiation modes in the fiber.12) Gain saturation: when near saturation, the gain is nonlinear; saturation, the signal cannot be amplified.13) The disadvantage of Raman amplifier:Need large output power pump laser. As Raman Scattering, the energy is transferred from high frequency to low frequency. Cross talk will affect signal.14) The principal noises associated with photo detectors are:1- Quantum (Shot) noise: arises from statistical nature of the production and collection of photo-generated electrons upon optical illumination. It has been shown that the statistics follow a Poisson process.2- Dark current noise: is the current that continues to flow through the bias circuit in the absence of the light. This is the combination of bulk dark current, which is due to thermally generated e and h in the pn junction, and the surface dark current, due to surface defects, bias voltage and surface area.15) List the advantages of fiber-optic communications over other types of communication technologies.The advantage of optical fiber communication:1. Weight and Size2. Material cost (SiO2 is plentiful)3. Information Capacity4. No electromagnetic interference5. No electrical connection6. Distance between repeaters7. Better security8. Low crosstalk16) The fabrication of amplifierOptical isolator ,Optical multiplexer, EDF, Pump laser17) What are the advantages and disadvantages of SDH system as compared to PDH system? The main limitations of PDH are:Inability to identify individual channels in a higher-order bit stream;Insufficient capacity for network management;Most PDH network management is proprietary;There is no standardized definition of PDH bit rates greater than 140 Mbit/s; and,There are different hierarchies in use around the world. Specialized interface equipment is required to interwork the two hierarchies.18) List the types of fiber attenuation and dispersion.Absorbing\scattering and bending lossMaterial/ mode/ waveguide dispersion.19) The avalanche effect.The created carriers are accelerated by the high electric field, gaining enough energy to cause further impact ionization.20) Dynamic range:System dynamic range is the maximum optical power range to which any detector must be able to respond.21) Differentiate between step index and graded index optical fiber.Step index fiber has a core of one index of refraction; graded index fiber has a core in which the outside edge starts with a low index of refraction that gradually increases towards the center. 五 计算题1) Suppose two graded index fibers are misaligned with an axial offset of d=0.3a. Try to calculate the fraction of optical power coupled from the first fiber into the second fiber. (Parameter a is the core radius )The fraction of optical power coupled in the fiber :122222arccos()152262T P d d d d P a a a a π⎧⎫⎡⎤⎛⎫⎪⎪⎛⎫=---⎢⎥⎨⎬ ⎪ ⎪⎝⎭⎢⎥⎝⎭⎪⎪⎣⎦⎩⎭()()21220.320.15arccos(0.15)10.15532π⎧⎫⎛⎫⎪⎪⎡⎤=--- ⎪⎨⎬⎣⎦ ⎪⎪⎪⎝⎭⎩⎭0.748=Turn it into dB , obtain 10log 1.27T P dB P=- 1) A double-heterojunction InGaAsP LED emitting at a peak wavelength of 1310 nm has radiative and nonradiative recombination times of 30 and 100 ns, respectively. The drive current is 40 mA. Compute internal quantum efficiency and internal optical power. Then the internalquantum efficiency isthe internal power level is :2) A GaAs laser operating at800nm has a 500-µm length and a refractive index n=3.7.What are the frequency and wavelength spacing? From 2c Ln ν∆=,22Lnλλ∆= obtain: 86310812250010 3.7c GHz Ln ν-⨯∆===⨯⨯⨯,3) In a 100-ns pulse, 6×106 photons at a wavelength of 1300nm fall on an In GaAs photo detector. On the average, 5.4×106 electron-hole (e-h) pairs are generated.Please calculate the quantum efficiency.The quantum efficiencyNumber of e-h pairs generated= -----------------------------------------Number of incident photons=665.410610⨯⨯0.90= 4) Consider a graded-index optical fiber, core index n1=1.50 and the core cladding index difference Δ=0.01.Try to calculate:1. The cladding index n22. The numerical aperture NA解:已知:n 1 =1.50,∆=0.01,根据(1)77.0100/130/130/1111int =+=+=---nr r r τττηmW 92.21031.110602.1/103106256.604.077.0619834int int =⨯⨯⨯⨯⨯⋅⨯⨯⨯==---s m s J q Ihc P λη(2)由(1)式,可知2 n 12∆= n 12- n 22n 22= n 12(1-2∆)n 2= n 1∆-21将n 1、∆代入上式,可得n 2==1.5002.01-=1.5098.0⨯=1.50⨯0.98995=1.48491将n 1、∆代入(2)式,可得NA = n 1∆2=1.5002.0=1.50⨯0.14142=0.21213The numerical aperture NA isNA=∆21n =22.001.02560.1=⨯⨯The normalized frequency V=∆221λπn a =01.0231.15056.11416.3⨯⨯⨯=26.454>V C =2.4057) Consider a 30-km long optical fiber that has an attenuation of 0.8dB/km at 1300 nm. If 200µW of optical power is launched into the fiber, try to calculate the optical output power P out .First we turn the input signal power unit from mW into dBm63()20010()10log 10log 7.01110in in P W W P dBm dBm mW W --⎡⎤⨯⎡⎤===-⎢⎥⎢⎥⨯⎣⎦⎣⎦From ()10(0)l g ()P dB o km z P z α=, as z=30k, the output power is : ()()()10log 10log 11out in P W P W P dBm z out mW mW α⎡⎤⎡⎤==-⎢⎥⎢⎥⎣⎦⎣⎦7.0(0.8/)(30)31.0dBm dB km km dBm =--=- Also31.0/103(30)10(1)0.79100.79P km mW mW W μ--==⨯=8) A photodiode is constructed of GaAs, which has a band-gap energy of 1.43eV at 300K.What is the cutoff wavelength? The cutoff wavelength is ()()()()348196.62510310/8691.43 1.610/c g J s m s hc nm E eV J eV λ--⨯⋅⨯===⨯2) 一个折射率为3.6的GaAs 光源耦合进折射率为1.48的石英光纤中,如果光纤端面和光源在物理上紧密相接,于是分界面上发生菲涅尔反射:A GaAs optical source with a refractive index of 3.6 is coupled to a silica fiber that has a refractive index of 1.48 . If the fiber end and the source are in close physical contact , then , the Fresnel reflection at the interface is这相当于17.4%的发射功率反射回光源,与这一R 值相对应的耦合功率由下式给定:This value of R corresponds to a reflection of 17.4 percent of the emitted optical power back into the source . Given that由反射造成的功率损耗为:The power loss L in decibels is found from3) 有一个InGaAs 光电二极管,在100ns 内共入射了波长为1300 nm 的光子6×106 个,产生了 5.4×106 个电子空隙对,则其量子效率可以等于:In a 100-ns pulse, 6×106 photons at a wavelength of 1300 nm fall on an InGaAs photodetector. On the average, 5.4x106 electron-hole pairs are generated, quantum efficiency is .4) 能量为1.53 × 10-19 J 的光子入射到光电二极管上,此二极管的响应度为0.65 A/W ,如果入射光功率为10 mW ,则产生的光电流为:Photons of energy 1.53 × 10-19 J are incident on a photodiode which has a responsivity of 0.65 A/W. If the optical power level is 10 μW, the photocurrent is174.048.160.348.160.32211=⎪⎭⎫ ⎝⎛+-=⎪⎪⎭⎫ ⎝⎛+-=n n n n R ()em ittedcoupled P R P -=110log 10log(1)0.83dB coupled emitted P L R P ⎛⎫=-=--= ⎪⎝⎭%90106104.566=⨯⨯=ημA 5.6)μW 10()A/W 65.0(=⨯=ℜ=in p P I5) 如上图所示,波长范围为1300 nm - 1600 nm 的InGaAs pin ,量子效率约为90%,因此响应度为:As shown in above figure, for the wavelength range 1300 nm < λ < 1600 nm, the quantum efficiency for InGaAs is around 90%. So responsivity is当波长为1300 nm 时:Responsivity at 1300 nm is :6) 一种硅APD 在波长900 nm 时的量子效率为65%,假定0.5 mW 的光功率产生的倍增电流为10 mA ,试求倍增因子M 。
光学工程的英语文献English:For English literature on optical engineering, one can delve into various aspects of the field ranging from fundamental principles to advanced applications. A good starting point might be textbooks like "Optical Engineering Fundamentals" by Bruce H. Walker, which covers the basic principles of optics, including geometrical optics, wave optics, and optical system design. For those interested in more specialized topics, journals like the "Journal of the Optical Society of America A" and "Optics Express" offer a plethora of research papers on cutting-edge advancements in optical science and engineering. Topics covered in these journals include but are not limited to optical imaging, photonics, laser technology, optical materials, and computational optics. Additionally, conference proceedings from events like the "SPIE Optical Engineering + Applications" conference provide insights into the latest developments and innovations in the field. These resources collectively offer a comprehensive overview of the current state and future directions of optical engineering, catering to both beginners and seasoned professionals.中文翻译:对于光学工程的英文文献,人们可以深入研究该领域的各个方面,从基本原理到先进应用。
Photoelectric sensorKey word: photoelectric effect photoelectric element photoelectric sensor classification sensor application characteristics .Abstract: in the rapid development of science and technology in the modern society, mankind has into the rapidly changing information era, people in daily life, the production process, rely mainly on the detection of information technology by acquiring, screening and transmission, to achieve the brake control, automatic adjustment, at present our country has put detection techniques listed in one of the priority to the development of science and technology. Because of microelectronics technology, photoelectric semiconductor technology, optical fiber technology and grating technical development makes the application of the photoelectric sensor is growing. The sensor has simple structure, non-contact, high reliability, high precision, measurable parameters and quick response and more simple structure, form etc, and flexible in automatic detection technology, it has been widely applied in photoelectric effect as the theoretical basis, the device by photoelectric material composition. Text:First, theoretical foundation - photoelectric effectPhotoelectric effect generally have the photoelectric effect, optical effect, light born volts effect.The light shines in photoelectric material, according to the electronic absorption material surface energy, if absorbed energy large enough electronic electronic will overcome bound from material surface and enter the outside space, which changes photoelectron materials, this kind of phenomenon become the conductivity of the photoelectric effectAccording to Einstein's photoelectron effect, photon is moving particles, each photon energy for hv (v for light frequency, h for Planck's constant, h = 6.63 * 10-34 J/HZ), thus different frequency of photons have different energy, light, the higher the frequency, the photon energy is bigger. Assuming all the energy photons to photons, electronic energy will increase, increased energy part of the fetter, positive ions used to overcome another part of converted into electronic energy. According to the law of conservation of energy:Type, m for electronic quality, v for electronic escaping the velocity, A microelectronics the work done.From the type that will make the optoelectronic cathode surface escape the necessary conditions are h > A. Due to the different materials have different escaping, so reactive to each kind of cathode materials, incident light has a certain frequency is restricted, when the frequency of incident light under this frequency limit, no matter how the light intensity, won't produce photoelectron launch, this frequency limitA -h m 212νν=called "red limit". The corresponding wavelength for type, c for the speed of light, A reactive for escaping.When is the sun, its electronic energy, absorb the resistivity reduce conductive phenomenon called optical effects. It belongs to the photoelectric effect within. When light is, if in semiconductor electronic energy big with semiconductor of forbidden band width, the electronic energy from the valence band jump into the conduction band, form, and at the same time, the valence band electronic left the corresponding cavities. Electronics, cavitation remained in semiconductor, and participate in electric conductive outside formed under the current role.In addition to metal outer, most insulators and semiconductor have photoelectric effect, particularly remarkable, semiconductor optical effect according to the optoelectronics manufacturing incident light inherent frequency, when light resistance in light, its conductivity increases, resistance drops. The light intensity is strong, its value, if the smaller, its resistance to stop light back to the original value. Semiconductor produced by light illuminate the phenomenon is called light emf, born volts effect on the effect of photoelectric devices have made si-based ones, photoelectric diode, control thyristor and optical couplers, etc.Second, optoelectronic components and characteristicsAccording to the outside optoelectronics manufacturing optoelectronic devices have photoelectron, inflatable phototubes and photoelectric times once tube.1. Phototubes phototubes are various and typical products are vacuum phototubes and inflatable phototubes, light its appearance and structure as shown in figure 1 shows, made of cylindrical metal half cathodic K and is located in the wires cathodic axis of anode in A package of smoke into the vacuum, when incident light within glass shell in the cathode, illuminate A single photon took all of its energy transfer to the cathode materials A free electrons, so as to make the freedom electronic energy increase h. When electrons gain energy more than escape of cathode materials, it reactive A metal surface constraints can overcome escape, form electron emission. This kind of electronic called optoelectronics, optoelectronic escaping the metal surface for after initial kinetic energyPhototubes normal work, anode potential than the cathode, shown in figure 2. In one shot more than "red light frequency is premise, escape from the optoelectronic cathode surface by positive potential attracted the anode in photoelectric tube forming space, called the current stream. Then if light intensity increases, the number of photons bombarded the cathode multiplied, unit of time to launch photoelectron number are also increasing, photo-current greatens. In figure 2 shows circuit, current and resistance is the voltage drop across the only a function of light intensity relations, so as to achieve a photoelectric conversion. When the LTT optoelectronic cathode K, electronic escape from the cathode surface, and was the photoelectric anode is an electric current, power plants absorb deoxidization device in the load resistance - I, the voltagePhototubes photoelectric characteristics fig.03 shows, from the graph in flux knowable, not too big, photoelectric basic characteristics is a straight line.2. Photoelectric times had the sensitivity of vacuum tube due to low, so with people developed has magnified the photomultiplier tubes photo-current ability. Figure 4 is photomultiplier tube structure schematic drawing.图4光电倍增结构示意图From the graph can see photomultiplier tubes also have A cathode K and an anode A, and phototubes different is in its between anode and cathode set up several secondary emission electrodes, D1, D2 and D3... They called the first multiply electrode, the second multiply electrode,... Usually, double electrode for 10 ~ 15 levels. Photomultiplier tubes work between adjacent electrode, keeping a certain minimum, including the cathode potential potentials, each multiply electrode potential filtering increases, the anode potential supreme. When the incident light irradiation, cathodic K escape from the optoelectronic cathode multiplied by first accelerated, by high speed electrode D1 bombarded caused secondary electron emission, D1, an incident can generate multiple secondary electron photonics, D1 emit of secondary electron wasD1, D2 asked electric field acceleration, converged on D2 and again produce secondary electron emission... So gradually produce secondary electron emission, make electronic increased rapidly, these electronic finally arrived at the anode, form a larger anode current. If a n level, multiply electrodes at all levels for sigma, the multiplication of rate is the multiplication of photomultiplier tubes can be considered sigma n rate, therefore, photomultiplier tube has high sensitivity. In the output current is less than 1mA circumstances, it in a very wide photoelectric properties within the scope of the linear relationship with good. Photomultiplier tubes this characteristic, make it more for light measurement.3 and photoconductive resistance photoconductive resistance within the working principle is based on the photoelectric effect. In semiconductor photosensitive material ends of mount electrode lead, it contains transparent window sealed in the tube and shell element photoconductive resistance. Photoconductive resistance properties and parameters are:1) dark resistance photoconductive resistance at room temperature, total dark conditions stable resistance called dark resistance, at the current flow resistance is called dark current.2) light resistance photoconductive resistance at room temperature and certain lighting conditions stable resistance measured, right now is called light resistance of current flow resistance is called light current.4, volt-ampere characteristics of both ends photoconductive resistance added voltage and current flows through photoconductive resistance of the relationship between called volt-ampere characteristics shown, as shown in figure 5. From the graph, the approximate linear volt-ampere characteristics that use should be limited, but when the voltage ends photoconductive resistance, lest than shown dotted lines of power consumption area5, photoelectric characteristics photoconductive resistance between the poles, light when voltage fixed the relationship between with bright current photoelectric characteristics. Called Photoconductive resistance photoelectric characteristics is nonlinear, this is one of the major drawback of photoconductive resistance.6, spectral characteristics is not the same incident wavelength, the sensitivity of photoconductive resistance is different also. Incidence wavelength and photodetector the relationship between relative sensitivity called spectral characteristics. When used according to the wavelength range by metering, choose different material photoconductive resistance.7, response time by photoconductive resistance after photo-current need light, over a period of time (time) rise to reach its steady value. Similarly, in stop lightphoto-current also need, over a period of time (down time) to restore the its dark current, this is photoconductive resistance delay characteristics. Photoconductive resistance rise response time and falling response time about 10-1 ~ 10-3s, namely the frequency response is 10Hz ~ 1000Hz, visible photoconductive resistance cannot be used in demand quick response occasion, this is one of the main photoconductive resistance shortcomings.8 and temperature characteristic photoconductive resistance by temperature affects greatly, temperature rise, dark current increase, reduced sensitivity, which is another photoconductive resistance shortcomings.9, frequency characteristic frequency characteristics refers to an external voltage and incident light, strong must be photo-current I and incident light modulation frequency, the relationship between the f, photoelectric diode is the frequency characteristic of the photoelectric triode frequency characteristics, this is because of the photoelectrictriode shot "yankees there capacitance and carrier base-combed need time's sake. By using the principle of the photoelectric efficiency of optoelectronics manufacturing frequency characteristics of the worst, this is due to capture charge carriers and release charge need a certain time's sake.Three, photoelectric sensorsPhotoelectric sensor is through the light intensity changes into electrical signal changes to achieve control, its basic structure, it first figure 6 by measuring the change of change of converting the light signal, and then using photoelectric element further will light signals into electrical signal by photoelectric sensor general. Illuminant, optical path and optoelectronics. Three components of photoelectric detection method has high precision, fast response, non-contact wait for an advantage, but measurable parameters of simple structure, sensors, form flexible, therefore, photoelectric sensor in the test and control is widely used.By photoelectric sensor generally is composed of three parts, they are divided into: transmitter and receiver and detection circuit shown, as shown in figure 7, transmitter aimed at the target launch beam, the launch of the beam from semiconductor illuminant, general light emitting diode (LED), laser diode and infrared emission diode. Beam uninterrupted launch, or change the pulse width. Receivers have photoelectric diode, photoelectric triode, composed si-based ones. In front of the receiver, equipped with optical components such as lens and aperture, etc. In its back is detection circuit, it can filter out effective signal and the application of the signal. In addition, the structural components in photoelectric switch and launch plate and optical fiber, triangle reflex plate is solid structure launch device. It consists of small triangle cone of reflective materials, can make a beam accurately reflected back from plate, with practical significance. It can be in with the scope of optical axis 0 to 25, make beams change launch Angle from a root almost after launch line, passes reflection or from the rotating polygon.some basic returns.图7Photoelectric sensor is a kind of depend on is analyte and optoelectronics and light source, to achieve the relationship between the measured purpose, so the light source photoelectric sensor plays a very important role, photoelectric sensor power if a constant source, power is very important for design, the stability of the stability of power directly affect the accuracy of measurement, commonly used illuminant have the following kinds:1, leds is a change electric energy into light energy semiconductor devices. It has small volume, low power consumption, long life, fast response, the advantages of high mechanical strength, and can match and integrated circuits. Therefore, widely used in computer, instruments and automatic control equipment.2, silk light bulb that is one of the most commonly used illuminant, it has rich infrared light. If chosen optoelectronics, constitutes of infrared sensor sensitive colour filter can be added to the visible tungsten lamps, but only filter with its infrared does illuminant, such, which can effectively prevent other light interference.3, compared with ordinary light laser laser with energy concentration, directional good, frequency pure, coherence as well as good, is very ideal light sources.The light source, optical path and photoelectric device composition photoelectric sensor used in photoelectric detection, still must be equipped with appropriate measurement circuit. The photoelectric effect to the measurement circuit of photoelectric element of widerange caused changes needed to convert the voltage or current. Different photoelectric element, the measurement circuit required is not identical also. Several semiconductor introduces below optoelectronic devices commonly used measurement circuit.Semiconductor photoconductive resistance can through large current, be in so usually, need not equipped with amplifier. In the output power of demand is bigger, can use figure 8 shows circuit.Figure 9 (a) with temperature compensation given the photosensitive diode bridge type measuring circuit. When the incident light intensity slow change, the reverse resistance photosensitive diode is the slow change, the change of the temperature will cause the bridge output voltage, must compensate. Drift Picture a photosensitive diode as the test components, another into Windows, in neighboring bridge, the change of the temperature in the arms of the influence of two photosensitive diode, therefore, can eliminate the same output with temperature bridge road drift.Light activated triode incident light in work under low illumination, or hope to getbigger output power, also can match with amplifying circuit, as shown in figure 9 shows.Because even in the glare photosensitive batteries, maximum output voltage also only 0.6 V, still cannot make the next level 1 transistor have larger current output, so must add positive bias, as shown in figure 9 (a) below. In order to reduce the transistor circuit impedance variations, base si-based ones to reduce as much as possible without light, when the reverse bias inherit in parallel a resistor si-based ones at both ends. Or like figure 9 (b) as shown by the positive ge diode produces pressure drop and test the voltage produced when exposed to light, make silicon tube e stack, b the voltage between actuators than 0.7 V, and conduction work. This kind of circumstance also can use silicon light batteries, as shown in figure 10 (c) below. Semiconductor photoelectric element of photoelectric circuit can also use integrated operational amplifier. Silicon photosensitive diode can be obtained by integratingop-amp larger output amplitude, as shown in figure 11 (a) below. When light is produced, the optical output voltage in order to guarantee photosensitive diode isreverse biased, in its positive to add a load voltage. Figure 11. (b) give the photocell transform circuit, because the photoelectric si-based ones short-circuit current and illumination of a linear relationship between, so will it up in the op-amp is,inverse-phase input, using these two potential difference between the characteristicsof close to zero, can get better effect. In the picture shows conditions, the output voltageThe photoelectric element by flux the role of different made from the principle of optical measurement and control system is varied, press the photoelectric element (optical measurement and control system) output nature, namely, can be divided into second analog photoelectric sensor and pulse (switch) photoelectric sensor. Analog photoelectric sensors will be converted into continuous variation of the measure, it is measured optical with a single value relations between analog photoelectric sensor. According to be measured (objects) method detection of target can be divided into transmission (absorption) type, diffuse type, shading type (beam resistance gears) three categories. So-called transmission style means the object to be tested in optical path in constant light source, the light energy through things, part of being measured by absorption, transmitted light onto photoelectric element, such as measured liquid, gas transparency and photoelectric BiSeJi etc; speed.gratifying The so-called diffuse style means the constant light by the light onto the analyte from the object to be tested, and projected onto surfaces reflect on after optoelectronic devices, such as photoelectric colorimetric thermometer and light gauge etc; The so-called shading style means the when illuminant issued by the flux of light analyte covered by a part Jing optoelectronics, make projection on the flux change, change the object to be tested and extent of the position with the light path, such as vibration measurement, the size measurement; And in pulse photoelectric sensor in the sensors, photoelectric element acceptable optical signal is intermittent change, therefore photoelectric element in switch work of the state, the current output it is usually only two steady state of the signal, the pulse form used for photoelectric counting and photoelectric speed measurement and so on.And infrared photoelectric sensor classification and working way generally have thefollowing kinds:1, groove photoelectric sensor put a light emitter and a receiver in a slot face-to-face outfit are on opposite sides of the photoelectric groove. Lighter emits infrared light or visible light, and in unimpeded cases light receptors can receive light. But when tested objects from slot zhongtong obsolete, light occluded, photoelectric switches and action. Output a switch control signal, cut off or connect load current, thus completing a control movement. Groove switch is the overall of detection distance because general structure limits only a few centimeters.2, DuiShe type optoelectronic sensor if you put lighter and receive light is separated, can make the detection distance increase. By a lighter and an inbox light sensor into a photoelectric switch is called DuiShe separate photoelectric switches, referred to DuiShe photoelectric switch. Its detection distance can reach a few meters and even a dozen meters. When using light-emitting device and receive light device are installed in test object through the path of the sides, test object by blocking light path, accept light implement action output a switch control signals.3, reflex plate.it photoelectric switch light-emitting device type and receive light device into the same device inside, in its front pack a reflex plate.the using the reflection principle of complete photoelectric control function is called reflex plate.it reflex (or reflector reflex) photoelectric switch. Under normal circumstances, lighter the light reflected by reflex plate.it is received by accept light; Once the light path be test object to block, accept light, the light is not receive photoelectric switch is action, output a switch control signals.4, diffusion reflective photoelectric switches its detection head with a lighter and also an inbox light ware, but no reflex plate.it ahead. Normally lighter for the light collect light is not found. When test object by blocking the light, and the light reflected light, receive part implement received light signals, output a switch signals.Four, I'm the idea of photoelectric sensorWith the development of science and technology people on measuring accuracy had the higher request, this has prompted the pace with The Times photoelectric sensor have updated, improve the main means photoelectric sensor performance is the application of new materials, new technology manufacturing performance is more superior photoelectric element. For example, today the prototype of the photoelectric sensor is a small metal cylindrical equipment, with a calibration lens, transmitter into receiver focused light, the receiver out of cable to the device got a vacuum tube amplifiers in metal cylinder on the incandescent light bulb inside a small as the light source a strong incandescent lamp sensor. Due to the sensor various defects existing in the fields, gradually faded. To appear, because of it of fiber of excellent performance, then appeared with sensors supporting the use of optical passive components, another fiber without any interference of electromagnetic signal, and can make the sensor of the electronic components and other electrical disturbance in isolation. Have a piece of plastic optical fiber core or glass light core, light outside a metallic core skins and bread this layer metal cortical density lower than light core, so low, the beam refraction in the two materials according to the border (incident Anglewithin a certain range, reflected), is all. Based on optical principle, all beams can be made by optical fiber to transmission. Two incident beam Angle in an Angle (along the fiber length direction within) by multiple reflections from the other end after injection, another incident angles than accept the incident light in metal skin, loss. This accept Angle within the biggest incident Angle than two times, this is because fiber slightly larger from air into density larger fiber materials hitting may have a slight refraction. In light of the optical fiber transmission from inside the influence of fiber bending (whether more than bending radius minimal bending radius). Most optical fiber is flexible, easy to install in the narrow space. Photoelectric sensor is a kind of non-contact measurement small electronic measurement equipment, rely on detect its receives the light intensity change, to achieve measurement purposes, andit's also a vulnerable to external disturbance and lose the measurement accuracy of the device. When be being designed so besides the choice optoelectronic components, still must set GSCC signal and temperature compensating measures used to weaken or eliminate the impact of these factors.Photoelectric sensor must pass a light modulation, like radio waves of light modulation of sends and receives, the radio to a station, can ignore other radio signal sensors without modulation long-focal-length only through the use of mechanical shielded, scenes that receiver transmitter only can receive the emission of light, can make its energy becomes very high. In contrast, through modulation transceivers can ignore ambient light, only to own light or with the same modulation frequencies of light without modulation response. The sensor used to test the infrared rays or around the radiation, if just baked red bottle, in this application situation if use other sensor, may be incorrect actions.Photoelectric sensor due to non-contact, high reliability, etc, and to change in measurement, damage the object to be testedSo since its invention in fields since play a significant role, at present it has been widely used in measuring mechanical quantity, thermal quantity, weight, intelligent vehicle system into etc. Now it in power system automatically grid device plays a very important role, because generator input power grid operation often USES accurate with law, must meet: three-phase line sequence is consistent, frequency, phase agree unanimously, voltage amplitude equal, one of the conditions in system design has been satisfied, after three conditions must also meet to grid, of course, artificially grid is more difficult, photoelectric grid is easier.The development of times, science and technology in the update, photoelectric sensor types are increasing and application domain more and more widely, such as a recent kind of infrared already in intelligent vehicle electrical sensors in to the application, one of which had based on infrared sensor is the core of intelligent vehicle, reflective type infrared sensor using reflex infrared sensor design path detection module and speed monitoring module; Another method based on infrared sensor using the car tracing is to collect infrared sensor data.Photoelectric sensor has cannot be replaced by other sensors superiority, so it development foreground is very good, the application will also become more widespread.光电传感器关键字:光电效应 光电元件 光电特性 传感器分类 传感器应用 摘要:在科学技术高速发展的现代社会中,人类已经入瞬息万变的信息时代,人们在日常生活,生产过程中,主要依靠检测技术对信息经获取、筛选和传输,来实现制动控制,自动调节,目前我国已将检测技术列入优先发展的科学技术之一。
Definition of optical constantsCASTEP can calculate the optical properties of solids that are due to electronic transitions.In general, the difference in the propagation of an electromagnetic wave through vacuum and some other material can be described by a complex refractive index, N:Eq. CASTEP 48In vacuum N is real, and equal to unity. For transparent materials it is purely real, the imaginary part being related to the absorption coefficient by:Eq. CASTEP 49The absorption coefficient indicates the fraction of energy lost by the wave when it passes through the material, so that the intensity at the distance x from the surface is I(x)=I(0)exp(-2πηx), where I(0) is the intensity of the incident light.The reflection coefficient can be obtained for the simple case of normal incidence onto a plane surface by matching both the electric and magnetic fields at the surface:Eq. CASTEP 50However, when performing calculations of optical properties it is common to evaluate the complex dielectric constant and then express other properties in terms of it. The complex dielectric constant, ε(ω), is given by:Eq. CASTEP 51and hence the relation between the real and imaginary parts of the refractive index and dielectric constant is:Eq. CASTEP 52Another frequently used quantity for expressing optical properties is the optical conductivity, σ(ω):Eq. CASTEP 53Optical conductivity is usually used to characterize metals, however CASTEP is aimed more toward the optical properties of insulators and semiconductors. The main difference between the two is that intraband transitions play important role in the IR part of the optical spectra of metals and these transitions are not considered at all in CASTEP.A further property that can be calculated from the complex dielectric constant is the energy loss function. It describes the energy lost by an electron passing through a homogeneous dielectric material and is given by:Eq. CASTEP 54Connection to experimental observablesExperimentally, the most accessible optical parameters are the absorption, η(ω), and the reflection, R(ω), coefficients. In principle, given the knowledge of both of these, the real and imaginary parts of N can be determined, through Eq. CASTEP 49and Eq. CASTEP 50. Eq. CASTEP 51 allows expression in terms of thecomplex dielectric constant. However, in practice, the experiments are more complicated than the case of normal incidence considered above. Polarization effects must be accounted for and the geometry can become quite complex (for example, transmission through multilayered films or incidence at a general angle). CASTEP supports spin-polarized calculations of optical properties for magnetic systems. Only transitions between the states with the same spin are allowed. For a more general discussion of the analysis of optical data see Palik (1985). Connection to electronic structureThe interaction of a photon with the electrons in the system is described in terms of time dependent perturbations of the ground state electronic states. Transitions between occupied and unoccupied states are caused by the electric field of the photon (the magnetic field effect is weaker by a factor of v/c). When these excitations are collective they are known as plasmons (which are most easily observed by the passing of a fast electron through the system rather than a photon, in a technique known as Electron Energy Loss Spectroscopy, described by Eq. CASTEP 54 , since transverse photons do not excite longitudinal plasmons). When the transitions are independent they are known as single particleexcitations. The spectra resulting from these excitations can be thought of as a joint density of states between the valence and conduction bands, weighted by appropriate matrix elements (introducing selection rules).Evaluation of the dielectric constantCASTEP calculates the imaginary part of the dielectric constant, which is given by:Eq. CASTEP 55where u is the vector defining the polarization of the incident electric field.This expression is similar to Fermi's Golden rule for time dependent perturbations, and ε2(ω) can be thought of as detailing the real transitions between occupied and unoccupied electronic states. Since the dielectric constant describes a causal response, the real and imaginary parts are linked by a Kramers-Kronig transform. This transform is used to obtain the real part of the dielectric function, ε1(ω).Details of the calculationEvaluation of matrix elementsThe matrix elements of the position operator that are required to describe the electronic transitions in Eq. CASTEP 55may normally be written as matrix elements of the momentum operator allowing straightforward calculation in reciprocal space. However, this depends on the use of local potentials (Read and Needs, 1991), while in CASTEP nonlocal potentials are more often used. The corrected form of the matrix elements is:Eq. CASTEP 56Ultrasoft pseudopotentials produce an additional contribution to optical matrix elements that is also included in CASTEP results. Drude correctionThe intraband contribution to the optical properties affects mainly the low energy infrared part of the spectra. It can be described sufficiently accurately via an semiempirical Drude term in the optical conductivity:Eq. CASTEP 57in terms of the plasma frequency ωP and damping parameter γD which depends on many details of the material and is usually obtained from experiment. The Drude damping parameter describes the broadening of the spectra due to effects not included in the calculation. Examples of processes that contribute to this broadening are electron-electron scattering (including Auger processes), electron-phonon scattering, and electron-defect scattering. This last contribution is usually the most important. As a result an a priori determination of the broadening would require knowledge as to the concentrations and kinds of defects present in the sample under study.PolarizationFor materials that do not display full cubic symmetry, the optical properties will display some anisotropy. This can be included in the calculations by taking the polarization of the electromagnetic field into account. As mentioned above, the unit vector u defines the polarization direction of the electric field. When evaluating the dielectric constant there are three options: polarized: requires a vector to define the direction of the electric field vector for the light at normal incidence to the crystal.∙unpolarized: requires a vector to define the direction of propagation of incident light at normal incidence to the crystal. The electric field vector is taken as an average over the plane perpendicular to this direction.∙polycrystal: no direction need be specified, the electric field vectors are taken as a fully isotropic average. Scissors operatorAs discussed below, the relative position of the conduction to valence bands is erroneous when the Kohn-Sham eigenvalues are used. In an attempt to fix this problem, inherent in DFT, we allow a rigid shift of the conduction band with respect to the valence band. This procedure of artificially increasing the band gap is know as a scissor operator.Limitations of the methodLocal field effectsThe level of approximation used here does not take any local field effects into account. These arise from the fact that the electric field experienced at a particular site in the system is screened by the polarizability of the system itself. So, the local field is different from the applied external field (that is, the photon electric field). This can have a significant effect on the spectracalculated (see the example of bulk silicon calculation below) but it is prohibitively expensive to calculate for general systems at present.Quasiparticles and the DFT bandgapIn order to calculate any spectral properties it is necessary to identify the Kohn-Sham eigenvalues with quasiparticle energies. Although there is no formal connection between the two, the similarities between the Schrödinger-like equation for the quasiparticles and the Kohn-Sham equations allow the two to be identified. For semiconductors, it has been shown computationally (by comparing GW and DFT band structures) that most of the difference between Kohn-Sham eigenvalues and the true excitation energies can be accounted for by a rigid shift of the conduction band upward with respect to the valence band (Godby et al., 1992). This is attributed to a discontinuity in the exchange-correlation potential as the system goes from (N)-electrons to (N+1)-electrons during the excitation process. There can, in some systems, be considerable dispersion of this shift across the Brillouin zone, and the scissor operator used here will be insufficient.Excitonic effectsIn connection with the absence of local field effects, excitonic effects are not treated in the present formalism. This will be of particular importance for ionic crystals (for example NaCl) where such effects are well known.Other limitations∙The nonlocal nature of the GGA exchange-correlation functionals is not taken into account when evaluating the matrix elements but it is expected that this will have a small effect on the calculated spectra.∙Phonons and their optical effects have been neglected.∙Finally, there is an intrinsic error in the matrix elements for optical transition due to the fact that pseudowavefunctions have been used (that is they deviate from the true wavefunctions in the core region). However, the selection rules will not be changed when going from pseudo- to all-electron wavefunctions.Sensitivity of optical properties to calculation parametersNumber of conduction bandsThis parameter defines the energy range covered in the calculation, and it also determines the accuracy of the Kramers-Kronigtransform. It is clear from Figure 1that ε2(ω) converges rapidly with the number of conduction bands included.Figure 1. Convergence of the dielectric function with the number of conduction bandsEnergy cutoffThe value of the energy cutoff that was used in the original SCF calculation of the ground state electron density is an important factor that determines the accuracy of the calculated optical properties. A bigger basis set provides more accurate self-consistent charge density and more variational freedom when searching for wavefunctions of unoccupied states. Figure 2showsthat while it is important to converge the calculation with respect to the planewave cutoff to obtain the correct energies for the spectral features, the shape of those features is reached rapidly.Figure 2. Convergence of the dielectric function with the cutoff energyNumber of k-points in the SCF calculationThe accuracy of the ground state electron density depends on the number of k-points used in the SCF run as well as on the basis set quality. Figure 3reveals that the optical properties converge rapidly with the number of k-points used in the SCF run, whichimplies low sensitivity to the details of the charge density. Figure 3. Convergence of the dielectric function with the number of k-points in the SCF calculationNumber of k-points for Brillouin zone integrationIt is important to use a sufficient number of k-points in the Brillouin zone when running optical matrix element calculations. The matrix element changes more rapidly within the Brillouin zone than electronic energies themselves. Therefore, one requires more k-points to integrate this property accurately than are needed for an ordinary SCF calculation. Figure 4 clearly demonstrates the importance of converging the Brillouin zone integration forthe optical properties with respect to the k-point density. Both energies and spectral features are strongly affected by the accuracy of this integration.Figure 4. Convergence of the dielectric function with the number of k-points in the optical matrix elements calculationSee Also:Theory in CASTEP。
一首先是关于LDA+U的认知。
二用LDA+U计算ZnO的energy gap 以及所遇到的问题一首先是关于LDA+U的认知1.对于强关联体系,往往需要在密度泛函理论中加入一个HUBBARD模型中的院子占据位(on site)库伦排斥项,这就是我们所说的DFT+U(或者说LDA+U)方法。
DFT+U提出的背景是传统的密度泛函理论计算不能成功的应用到Mott绝缘体体系。
我们知道电子从一个原子位跳到另一个原子位时,如果那个原子位已经有一个电子,那么这种跳跃需要克服一个库伦相互作用。
如果这个能量比能带宽度大的话,尽管能带没有全满,电子也不能自由运输,系统表现绝缘性质。
我们称这种绝缘体为Mott绝缘体。
强关联Mott绝缘体体系可以由Hubbard紧束缚模型很好的描述,在Hubbard模型中通过一个Hubbard参数U 来描述这种库伦排斥。
下面是英文解释(摘自另一PDF)Two quantities are to be considered:U “on site” electron-electron repulsionW bandwidth (hopping amplitude, related to kinetic energy)Two different regimes:W/U>>1: the energy is minimized making the kinetic term as small as possible through delocalization (little price is paid on the occupied atomic sites to overcome repulsion U)W/U<<1: the kinetic energy of electrons is not large enough to overcome the on-site repulsion. Electrons undergo a Mott localizationLDA/GGA approximations to DFT always tend to over-delocalize electrons:U is not well accounted forElectronic energy functionals are affected by selt-interaction二用LDA+U计算ZnO的energy gap 以及所遇到的问题R. Michael Sheetz[1]等人使用CASTEP计算了bulk ZnO的energy gap(3.4ev) 参数如下cutoff 600ev Pseudopotentials Norm-conserving convergence criterion 10-6 ev Functional: GGA PBE U Zn d =10.5ev U Zn s =0 ev U O p =7.0ev1 import ZnO2 对bulk ZnO 结构优化(还没有选LDA+U,为了下面比较)结果分析我们可以看到band gap is 0.269ev 与3.4ev 相差很大3. 选上LDA+U 看看结果如何。
视镜法兰英文表示方法In the realm of optical engineering, the spectacle flange represents a critical interface component that connects various parts of an optical system, such as lenses, mirrors, or other optical devices, to a frame or mount. The design and specification of spectacle flanges are paramount for ensuring the precise alignment and secure attachment of optical elements, which, in turn, affects the overall performance and functionality of the optical system.The term "spectacle flange" is derived from its resemblance to a pair of glasses, or "spectacles," due to the dual openings or "eyes" that are typically present in the flange design. These openings allow for the passage of light and the mounting of optical components. The flange itself is usually a flat, circular disk with a specified thickness, made from materials that offer stability and minimal thermal expansion, such as aluminum or stainless steel.The central role of a spectacle flange is to provide a stable and reliable method for mounting optical components within a system. This is achieved through precision-engineered holes and slots on the flange surface, which align with corresponding features on the optical components or the mount. The use of screws, bolts, or clamps through these holes ensures that the components are held firmly in place, preventing any movement that could disrupt the optical path or alignment.When designing a spectacle flange, several factors must be considered to ensure optimal performance. The material selection is crucial, as it must not only provide structural integrity but also minimize any adverse effects on the optical properties of the system, such as unwanted reflections or absorption of light. The surface finish of the flange is another important aspect, as a smooth, polished surface can reduce scattering of light and improve the efficiency of the optical system.The dimensional tolerances of the spectacle flange are also of utmost importance. Precise measurements are required to ensure that the flange fits perfectly with the optical components and the mount. This includes the diameter of the flange, the size and positionof the holes, and the thickness of the material. Any deviation from the specified tolerances can lead to misalignment, which can significantly degrade the performance of the optical system.In addition to the physical design, the method of attachment is a key consideration. The choice between permanent and removable connections depends on the application and the need for maintenance or upgrades. For systems that require frequent adjustments or component replacements, a removable connection using screws or quick-release mechanisms may be preferred. For more permanent installations, welding or adhesive bonding might be employed to ensure a secure and long-lasting mount.The application of spectacle flanges extends across various fields, from simple magnifying glasses to complex astronomical telescopes. In each case, the flange serves as the foundational element that maintains the integrity and accuracy of the optical system. Whether in research laboratories, industrial settings, or consumer products, the spectacle flange plays an indispensable role in the functionality and success of optical devices.In conclusion, the spectacle flange is a vital component in optical engineering, serving as the connecting point between optical elements and their mounts. Its design and implementation require careful consideration of materials, dimensions, surface finish, and attachment methods to achieve the desired optical performance. Through meticulous engineering and attention to detail, spectacle flanges contribute significantly to the advancement of optical technologies and their applications in various sectors. 。
Optical CommunicationsOptical communications have become an essential part of our daily lives, playing a crucial role in enabling high-speed data transmission over long distances. However, like any technology, optical communications also come with their own set of challenges and problems. One of the primary issues faced in optical communications is signal loss, which occurs due to various factors such as attenuation, scattering, and dispersion. This can significantly impact the quality and reliability of the transmitted data, leading to the need for effective solutions to mitigate signal loss in optical communications. Attenuation, or the reduction in signal strength as it travels through the optical fiber, is a major cause of signal loss in optical communications. This can be attributed to factors such as absorption of light by the fiber material, scattering of light due to impurities or imperfections in the fiber, and bending losses. As a result, the transmitted signal may weaken as it travels through the fiber, ultimately leading to a decrease in the signal-to-noise ratio and affecting the overall performance of the communication system. In addition to attenuation, scattering and dispersion also contribute to signal loss in optical communications. Scattering occurs when light is redirected in different directions as it interacts with particles or irregularities in the fiber, leading to a loss of signal intensity. On the other hand, dispersion refers to the spreading of the optical signal as it travels through the fiber, causing different components of the signal to arrive at the receiver at different times. This can result in signal distortion and ultimately impact the accuracy of the transmitted data. To address the issue of signal loss in optical communications, various strategies and technologies have been developed to improve the efficiency and reliability of data transmission. One approach is the use of optical amplifiers, such as erbium-doped fiber amplifiers (EDFAs), to boost the signal strength as it travels through the fiber. By incorporating these amplifiers at regular intervals along the transmission path, the signal loss can be effectively compensated, ensuring that the transmitted data maintains its integrity and quality. Furthermore, advancements in fiber optic technology have led to the development of low-loss fibers that minimize the impact of attenuation and scattering on the transmitted signal. These fibers are designedto have reduced levels of impurities and imperfections, allowing the light to propagate with minimal loss and distortion. Additionally, the use of dispersion-compensating fibers and techniques such as dispersion compensation can help mitigate the effects of dispersion, ensuring that the different components of the signal arrive at the receiver simultaneously. Another key aspect in addressing signal loss in optical communications is the advancement of signal processing and modulation techniques. By implementing advanced modulation formats and signal processing algorithms, it is possible to enhance the spectral efficiency and tolerance to signal impairments, thereby improving the overall performance of optical communication systems. This can include the use of coherent detection, digital signal processing, and advanced error correction coding schemes to effectively mitigate the impact of signal loss and distortion. In conclusion, while signal loss remains a significant challenge in optical communications, ongoing research and technological advancements continue to drive the development of innovative solutions to address this issue. By leveraging optical amplifiers, low-loss fibers, dispersion compensation, and advanced signal processing techniques, it is possible to minimize the impact of attenuation, scattering, and dispersion on the transmitted signal, ultimately ensuring high-quality and reliable data transmission over optical communication networks. As the demand for high-speed and high-capacity communication systems continues to grow, the ongoing efforts to mitigate signal loss in optical communications will play a critical role in shaping the future of data transmission technologies.。
光学吸收系数一、直接带隙与间接带隙1. 直接带隙直接带隙是指在晶体能带结构中,价带最高点(即导带最低点)与导带最低点(即价带最高点)之间能量差的最小值。
在直接带隙材料中,光子被吸收后会直接激发价带中的电子跃迁到导带中。
2. 间接带隙间接带隙是指在晶体能带结构中,价带最高点(即导带最低点)与导带最低点(即价带最高点)之间能量差的最小值不在晶格动量为零的点上。
在间接带隙材料中,光子被吸收后需要通过晶格振动来实现电子从价带到导带的跃迁。
二、光学吸收系数的定义与性质光学吸收系数是描述光在物质中被吸收程度的物理量,用符号α表示。
它与物质的光学性质密切相关,可以反映出物质的透明度和光学吸收强度。
光学吸收系数的定义如下:其中,I0表示入射光强度,I表示透射光强度,d表示物质的厚度。
光学吸收系数的主要性质如下:1.光学吸收系数与光的频率有关。
在材料中,物质对光的吸收程度与光的频率密切相关。
当光的频率与物质的能带结构中电子的跃迁能量匹配时,吸收强度最大。
2.光学吸收系数随波长的变化而变化。
根据光的频率与波长的关系,光学吸收系数与波长存在反比关系。
即光波长越短,吸收强度越大。
三、光学吸收系数的计算方法光学吸收系数的计算方法可以基于多种理论模型,常用的有色散理论、固体受限模型和光子能带理论等。
1. 色散理论色散理论是一种假设材料对光的吸收行为受其电子能级的色散关系控制的模型。
它基于电子在材料中的运动和跃迁理论,通过讨论材料中的电子束缚态和连续态,推导出了光学吸收系数与频率的关系。
2. 固体受限模型固体受限模型假设光在材料中的传播受到其表面的影响。
通过考虑材料表面的散射和反射等现象,推导出了光在材料中的传播公式,从而计算光学吸收系数。
3. 光子能带理论光子能带理论是一种基于能带结构的理论模型。
通过分析材料中电子的能带结构和跃迁行为,可以计算出光学吸收系数与能带宽度、态密度等参数之间的关系。
四、应用领域与研究进展光学吸收系数在材料科学和光电子学等领域具有重要的应用价值。
折射率复数英语Refraction Index Complex EnglishThe concept of refraction index is a fundamental principle in the field of optics, which describes the way light behaves when it travels from one medium to another. The refraction index, also known as the index of refraction, is a dimensionless number that quantifies the degree to which the speed of light is reduced as it passes through a particular material. This phenomenon is crucial in understanding the behavior of light in various applications, such as in the design of optical devices, the analysis of light-based phenomena, and the study of the properties of materials.The refraction index is typically denoted by the symbol "n" and is defined as the ratio of the speed of light in a vacuum (c) to the speed of light in the medium (v). Mathematically, this can be expressed as n = c/v. The value of the refraction index is always greater than or equal to 1, with a value of 1 corresponding to the speed of light in a vacuum.When light travels from one medium to another, such as from air to water or from glass to air, the change in the speed of light results ina change in the direction of the light beam. This phenomenon is known as refraction, and it is governed by Snell's law, which states that the ratio of the sin e of the angle of incidence (θ1) to the sine of the angle of refraction (θ2) is equal to the ratio of the refraction indices of the two media (n1/n2).The refraction index can be a complex number, which means that it has both a real and an imaginary component. The real part of the refraction index, denoted as n, represents the degree to which the speed of light is reduced in the medium, while the imaginary part, denoted as k, represents the degree to which the light is absorbed or attenuated as it travels through the medium.The complex refraction index can be written as n + ik, where i is the imaginary unit (i^2 = -1). The real part, n, is often referred to as the refractive index, while the imaginary part, k, is known as the extinction coefficient.The complex refraction index is particularly important in the study of the optical properties of materials, as it can provide information about the absorption and dispersion of light within the material. This information is crucial in the design of various optical devices, such as lasers, optical fibers, and thin-film coatings.One of the key applications of the complex refraction index is in thestudy of the optical properties of materials in the field of photonics. Photonics is the study of the generation, manipulation, and detection of light, and it has a wide range of applications in fields such as telecommunications, imaging, and sensing.In the context of photonics, the complex refraction index is used to describe the propagation of light through various materials, such as semiconductors, dielectrics, and metals. The real part of the refraction index determines the phase velocity of the light, while the imaginary part determines the attenuation of the light as it travels through the material.The complex refraction index can also be used to analyze the reflectivity and transmissivity of light at the interface between two materials. This information is crucial in the design of optical devices, such as mirrors, lenses, and thin-film coatings, where the control of light propagation is essential.In addition to its applications in photonics, the complex refraction index is also important in the field of materials science. The complex refraction index can provide information about the electronic and atomic structure of materials, as well as their optical properties. This information can be used to study the fundamental properties of materials and to design new materials with desired optical characteristics.Overall, the concept of the complex refraction index is a crucial tool in the study of light and its interactions with matter. It has a wide range of applications in fields such as photonics, materials science, and optics, and continues to be an active area of research and development.。
光学透明度的英文Optical TransparencyOptical transparency is a fundamental property of materials that describes their ability to transmit light without significant attenuation or distortion. This property is of paramount importance in a wide range of applications, from optical communication and display technologies to medical imaging and scientific instrumentation. In this essay, we will explore the concept of optical transparency, its underlying principles, and its practical implications.At its core, optical transparency is determined by the interaction between light and the material's molecular structure. When light encounters a transparent material, such as glass or water, it is able to pass through with minimal scattering or absorption. This is because the material's atoms or molecules are arranged in a way that allows the light to propagate unimpeded, without significant interference.The degree of optical transparency is typically measured by the material's transmittance, which is the ratio of the intensity of light that emerges from the material to the intensity of the light that enters it. A perfectly transparent material would have a transmittanceof 100%, meaning that all the light that enters it is transmitted without any loss. In contrast, a completely opaque material would have a transmittance of 0%, as no light would be able to pass through it.The optical transparency of a material is influenced by several factors, including its chemical composition, molecular structure, and physical properties. For example, the presence of impurities or defects in the material can scatter or absorb light, reducing its transparency. Similarly, the material's thickness and surface roughness can also affect its optical properties.One of the most well-known examples of a highly transparent material is glass. Glass is a non-crystalline solid material composed primarily of silicon dioxide (SiO2) and other oxides. The molecular structure of glass allows light to pass through it with minimal scattering or absorption, making it an ideal material for a wide range of applications, from windows and lenses to fiber optic cables and display screens.Another example of a highly transparent material is water. Water is a clear, colorless liquid that is essential for life on Earth. Its optical transparency is a result of the specific arrangement of its hydrogen and oxygen atoms, which allows light to pass through it with little interference. This property of water is crucial for underwaterphotography, marine biology, and other applications that rely on the transmission of light through aqueous environments.In addition to these natural materials, researchers and engineers have developed a wide range of synthetic materials with exceptional optical transparency. These include materials such as transparent ceramics, polymers, and even engineered nanostructures. These advanced materials have enabled the development of cutting-edge technologies, such as high-efficiency solar cells, advanced display technologies, and specialized optical components for scientific and medical applications.The applications of optical transparency are vast and diverse. In the field of communications, optical transparency is the foundation of fiber optic technology, which has revolutionized the way we transmit data over long distances. Optical fibers, which are made of highly transparent glass or plastic, can carry vast amounts of information in the form of light signals, enabling high-speed internet, telephone, and television services.In the field of optics and photonics, optical transparency is essential for the development of advanced imaging and sensing technologies. Transparent materials are used to create lenses, mirrors, and other optical components that are crucial for applications such as telescopes, microscopes, and medical imaging devices. The ability totransmit light with minimal distortion is also essential for the development of high-performance display technologies, such as LED and OLED displays.In the field of energy, optical transparency plays a crucial role in the development of solar energy technologies. Transparent materials, such as glass and transparent polymers, are used to create the protective covers and enclosures for solar cells, allowing sunlight to reach the photovoltaic materials and generate electricity.Beyond these technological applications, optical transparency also has important implications for our understanding of the natural world. The ability of light to pass through transparent materials has enabled scientists to study the structure and composition of materials at the atomic and molecular scale, using techniques such as X-ray crystallography and spectroscopy.In conclusion, optical transparency is a fundamental property of materials that has far-reaching implications for a wide range of scientific and technological applications. From communication and imaging to energy and materials science, the ability of light to pass through transparent materials has been a driving force behind many of the most important advancements in modern society. As our understanding of the principles of optical transparency continues todeepen, we can expect to see even more remarkable innovations and breakthroughs in the years to come.。
光密度法测定微藻生物量沈萍萍,王朝晖,齐雨藻,谢隆处,王艳(暨南大学水生生物研究所,广东广州510632)[摘要]目的:为准确而又快速的测量微藻生物量.方法:选用15种不同微藻,在实验室中分别测定其细胞密度及光密度并进行直线回归分析,同时采用吸光系数来估算浮游植物生物量.结果:得出了浮游植物吸光系数与细胞碳含量(即生物量)的回归方程:Ig (!)=-1.0465In (")+4.2551.结论:这是一种利用光密度法来测量微藻生物量的简单有效的方法.[关键词]微藻;吸光系数;生物量;碳含量;光密度法[中图分类号]@949[文献标识码]A[文章编号]1000-9965(2001)03-0115-05藻类的生物量测定是藻类生长、生理生化、生态等方面研究的必要手段,藻类生物量测定方法很多,常使用的有:计数细胞个体数,测干重,叶绿素法,浊度法,最大比生长速率法等[1].通常的显微直接计数法,光密度(OD )测量法,叶绿素测量法,COunter 电子显微计数法等各有优缺点.最后一种方法由于大多数微藻形状不规则,加之仪器本身昂贵,因此在一般实验室中应用并不普遍.而叶绿素法操作复杂且所需样品量较大,相比而言直接计数法和光密度法适用的范围就广泛的多.到目前为止,计数细胞个体数仍然是最准确,最令人满意的方法之一,可以获得最基本的种群信息[2].但对于微藻来说,大小相差很大,小的只有几个微米,大的可达几百微米,而且形态各异,有的是单细胞(运动或不运动),有的是群体,其体型也多种多样,有球形、椭圆形、锥形、链状、丝状等.因此微藻的直接计数法不但工作量大,不同种类间由此估算的生物量差异也较大.光密度法操作简单,需要样品量少,能够实现快速测定.因此我们在实验室培养中期望能找到一条简便有效的途径,准确而又快速的测量出微藻的生物量.!材料与方法!.!藻种实验选用了5种绿藻,4种甲藻,1种金藻,1种针胞藻,1种棕囊藻作为实验材料.均由暨南大学水生生物研究所藻种室提供.其形态特征[3]及大小见表1.!."方法藻种培养于20C ,光照度4000Ix ,光暗比为1211121.待培养4~5c ,用754-UV 分光光度计在600~750nm 之间每隔10nm 进行波长扫描,绘制吸收曲线,确定最大吸收峰波长.然后将藻液稀释成浓度梯度,在最大吸收峰处测其OD 值,同时显微计数.小于10!m 的藻,用血球计数板计数,大于10!m 的藻用0.1mL 浮游植物计数框计数细胞密度(至少计数3次).以OD 值对细胞密度作图,求其吸光系数.[收稿日期]2000-11-15[作者简介]沈萍萍(1975~),女,山东青岛,98级硕士研究生.第22卷第3期2001年6月暨南大学学报(自然科学版)JOurnaI Of Jinan University (NaturaI Science )VOI.22NO.3Jun.2001表!微藻形态特征微藻名称(学名)形状特征大小是否群体扁藻(Platymonas elliptica)细胞卵圆型.具有两条鞭毛,20~24(11~16)!m X12~否游动活泼.15(11~14)!m X7~10!m绿微小小球藻和蛋白核小球藻单细胞,球形.否(Chlorella minutissima直径3~5!m和C.pyrenoidosa)直径3~10!m盐藻(两株)(Dunaliella salina Strain1)(Dunaliella salina Strain2)单细胞,梨形.无细胞壁,有两条鞭毛,游动活泼.Strain122!m X14!mStrain29!m X3!m否藻羊角月牙藻单细胞,呈镰刀形弓状,无8~12!m X5~6!m否(Selenastrum copricornutum)鞭毛,不能运动.异鞭藻微球藻(Nanochlorpsis Sp.)单细胞,圆形,无鞭毛.直径2~4!m否海洋原甲藻(Prorocentrum micans)单细胞,一侧较扁,另一侧圆弧形.具鞭毛,运动.30!m X20!m否甲锥状施氏藻(Scrippsiella trochoidea)单细胞,细胞前端锥形,底端钝圆.有时聚集在一起.20!m X15!m否具有鞭毛,能够运动.塔玛亚历山大藻单细胞或少数几个细胞连接40!m X45!m否/是(Alexandrum tamarense)成链状.具鞭毛,能运动.藻红色裸甲藻单细胞,无细胞壁,具有30!m X20!m否(Gymnodinium sanguineum)鞭毛,游动.金藻球等鞭金藻(Isochrysis galbana)裸露的运动细胞,椭圆形.具有两条等长的鞭毛,运动缓慢.5~6!m X2~4!m X2.5~3!m否针胞藻赤潮异湾藻(Heterosigma akashiwo)单细胞,呈长椭圆形,具鞭毛,能游动.15!m X10!m否定鞭藻球形棕囊藻(两株)(Phaeocystis globosa)HK株ST株圆形或卵圆形单细胞及球形群体两种形态,群体有胶质囊.单细胞具有两条等长鞭毛,运动活跃.直径3~8!m是"结果与讨论".!吸收曲线与标准曲线由各种微藻的吸收曲线可以看出:藻类的吸收光谱曲线具有明显的相似性,最大吸收峰即光密度值位于670~680nm处.吸收峰与微藻色素种类组成及含量有关,从不同藻类吸收峰值来看,具有一致性,670~680nm之间的吸收峰,一般是细胞内色素的吸收峰.因为藻类都含有叶绿素a[3],差别只在于含量的多少,例如绿藻含有叶绿素a、D的含量高于其它藻类,金藻中胡萝卜素占细胞内色素总量的75%[4].所以选择合适的波长有利于藻类比色测定的准确度,结果具有可比性,便于种类间比较研究.出于实验目的,我们选择680nm作为测量波长[5].611暨南大学学报(自然科学版)2001年由标准曲线可以看出:不同生长期,尤其是对数期的微藻个体数与光密度值基本成正比.不同浓度的藻液与细胞密度之间的相关系数均较好.但较特殊的是细胞较小的藻种,如小球藻、微球藻等,可能因为藻细胞过小,密度过大,在显微镜下计数时容易出现较大的人为误差,同时当微藻的光密度测量值过高超过0.8(例如微球藻)或者过小低于0.05时(例如几种甲藻),对于微藻数量的测定也有很大的影响,将大大降低其准确度,相关性不显著.所以制作一条精确的标准曲线,必须同时考虑到细胞的密度与细胞本身的大小以及形态,对于提高微藻的计数准确度具有关键的作用.经回归分析,微藻的细胞密度与光密度之间呈直线关系,其吸光系数(即斜率K )各不相同,这与微藻本身的特性有关,例如:藻体体积大小、内容物的含量、颜色及分布或运动情况等.斜率K 与细胞大小(体积)有关,不同种微藻(例如微小小球藻、蛋白核小球藻、微球藻、棕囊藻等),细胞大小(体积)相近,其相关的吸光系数也比较接近.而细胞大小(体积)相差较大的同种微藻(盐藻)或不同种微藻,其吸光系数相差较大.可以看出,细胞体积越大,吸光系数越小;相反,细胞体积越小,其吸光系数越大.而且,形状越规则的细胞,光密度与细胞密度之间的相关性愈好.例如小球藻、微球藻、棕囊藻、球形等鞭金藻等,而如甲藻类细胞形状多样,且细胞体积较大,其相关性明显较差.!.!生物量与吸光系数的关系另外按照文献[6]中方法计算出微藻的体积,然后利用公式(lg (m )=0.94lg (V )-0.6其中m 为碳含量,V 为细胞体积)将体积转化为生物量[7],得出结果如表2所示.将生物量与吸光系数进行回归,发现两者之间存在关系如下.回归方程:y =-l.0465ln (x )+4.255l 即:lg (m )=-l.0465ln (x )+4.255l 相关系数;R 2=0.77l 4(>0.388=R 20.0l ,I =l5),极显著.其中m 为生物量,x 为吸光系数.所以只要测得单种微藻或者混合藻类的吸光系数,就可以直接求得它们的生物量,从而大大简化浮游植物生物量的测定方法.微藻的形状多样,如球形,椭圆形及锥形、镰刀形等,又有单细胞、群体之分,其中有的具有鞭毛,能够游动,而有些不具备运动能力,因此使得显微计数方法相对复杂且结果不十分准确.同时细胞大小差别较大,因此用细胞个体数量来表达生物量很难取得一致,结果不够精确,没有可比性.相反,光密度法能够较好的处理以上缺点,并且操作简便,结果相对准确."结论这种光密度法在实际中具有应用价值,除了能够简化测定纯种培养中微藻生物量的方法外,在野外调查中,例如微型浮游植物大小一般小于20!m 大于2!m ,在通常生态研究中往往忽略,现在随着检测技术和方法的进步,实际上已经证明微型浮游植物在水域生态系统的生物地球化学循环和能量流动种占有重要地位[8~l0].但是由于它们体积微小,在普通的观测方法中往往观察不到,利用光密度法测定它们的生物量,不仅可以使生态研究更精确,同时又简化测定程序.7l l 第3期沈萍萍等:光密度法测定微藻生物量表!各种微藻的细胞密度与光密度回归直线,相关系数!!及体积、生物量等比较微藻种名(学名)直线回归方程(R2)P值V/!m3生物量(lg m)吸光系数(斜率K)扁藻Y=406.24X<0.0l709.4l2.08406.240(Platymonas elliptica.)(0.9987)微小小球藻Y=3375.7X<0.0522.830.683375.700(Chlorella minutissima)(0.9622)蛋白核小球藻Y=3682.4X<0.05l9.860.623682.400(C.pyrenoidosa)(0.975l)盐藻l Y=l2l.2l X<0.05l537.942.40l2l.2l0(Dunaliella salina Strainl)(0.9328)盐藻2Y=l73.67X>0.0528.890.77l73.670(D.salin Strain2)(0.89l2)羊角月牙藻Y=994.45X<0.0l l78.30l.52994.450(Selenastrum copricornutum)(0.9877)微球藻Y=3266.6X<0.05l5.290.5l3266.600(Nanochlorpsis Sp)(0.9488)海洋原甲藻Y=28.92l X0.052996.002.6728.92l (Prorocentrum micans)(0.8357)锥状施氏藻Y=ll3.24X>0.05l270.602.32ll3.240(Scrippsiella trochoidea)(0.8764)塔玛亚历山大藻Y=25.243X>0.05l9702.273.4425.243(Alexandrum tamarense)(0.8903)红色裸甲藻Y=l5.242X>0.0532l0.002.70l5.242(Gymnodinium sanguineum)(0.8987)球形等鞭金藻Y=95l.59X<0.0l l6.480.5495l.590(Isochrysis galbana)(0.9897)赤潮异湾藻Y=l33.8l X<0.05428.00l.87l33.8l0(Heterosigmaakashiwo)(0.9779)球形棕囊藻HK Y=l l28X<0.0544.580.95l l28.00(Phaeocystis globosa HK)(0.9722)球形棕囊藻ST Y=l348.7X<0.0577.04l.l7l348.70(Phaeocystis globosa ST)(0.9787)当然,这种方法选择叶绿素活体吸收常数亦有限制因素,因为叶绿素含量与藻类的生长条件,尤其是光照强度及其它因子有很大的关系,因此不同地域生态研究中这一相关性具有不同的特点.野外条件下生长的微藻与实验室培养的藻细胞生长周期可能不同,大多数藻达不到同步生长,体内叶绿素含量有差别,因此应该在实验室中继续进行模拟野外条件下混合微藻的OD值与生物量之间的关系的研究.8l l暨南大学学报(自然科学版)200l年[参考文献][1]周永欣,章宗涉.水生生物毒理试验方法[M ].北京:农业出版社,1989.179.[2]STEIN J R.Dry weight ,volume and optical density.In :Stein J R.Handbook of Phycological Methods :CultureMethods and Growth Measurements [M ].New York :1973.21.[3]HAROLD C B ,MICHEAL J W.Introduction to the Algae ,Structure and Reproduction [M ].2nd ed.New Jersey :Prentice -Hall ,Inc ,Englewood Cliffs ,1985.17~20.[4]郑重.海洋浮游生物学[M ].北京:海洋出版社,1984.17,120.[5]张志良.植物生理学实验指导[M ].北京:高等教育出版社,1990.78~88.[6]孙军,刘东艳,钱树本.浮游植物生物量研究I.浮游植物生物量细胞体积转化法[J ].海洋学报,1999,21(2):75~85.[7]EPPLY R W ,REID F M H ,STRICKLAND J D H.The ecology of the plankton off La Jolla ,California ,in the periodApril through September 1967Part !.Estimates of phytoplankton crop size ,growth rate and primary production [J ].Bull Scripps Inst Oceanogr ,1970,17:33~42.[8]孙书存,陆健健,张利华.流式细胞仪在微型浮游植物生态学中的应用[J ].生态学杂志,2000,19(1):72~78.[9]BURKILL P H.Biogeochemical cycling in the northwestern Indian Ocean :a brief overview [J ].Deep Sea ResearchII ,1993,40(3):59~62.[10]LE BOUTEILLER.Size distribution pattern of phytoplankton in the western Pacific :towards a generation for tropicalopen ocean [J ].Deep Sea Research ,1992,39:501~509.An optical density method for determination of microalgal biomassSHEN Ping -ping ,WANG Zhao -hui ,OI Yu -zao ,XIE Long -chu ,WANG Yan(Institute of Hydrobiology ,Jinan University ,Guangzhou 510632,China )[Abstract ]Aim :To investigate the relationship between optical density (OD )and the biomass of microalgae.Methods :15microalgal species were used under laboratory conditions to study the relation-ship between the cell density and its related OD.Meanwhile ,the optical absorption coefficient ,namely the slope of the linear graph which showed the relationship between cell density and OD ,was utilized to estimate the phytoplankton biomass.Results :Regression analysis results showed the linear function :lg (!)=-0.4511ln (")+4.2422,in which #is the carbon content and "is the optical absorption co-efficient of microalgae.Conclusion :This is a useful and rapid OD method to measure the biomass of microalgae.[Key words ]microalgae ;optical absorption coefficient ;biomass ;carbon content ;OD911第3期沈萍萍等:光密度法测定微藻生物量光密度法测定微藻生物量作者:沈萍萍, 王朝晖, 齐雨藻, 谢隆处, 王艳作者单位:暨南大学水生生物研究所,刊名:暨南大学学报(自然科学与医学版)英文刊名:JOURNAL OF JINAN UNIVERSITY年,卷(期):2001,22(3)被引用次数:49次1.周永欣;章宗涉水生生物毒性试验方法 19892.Stein J R Dry weight,volume and optical density 19733.HAROLD C B;MICHEAL J W Introduction to the Algae,Structure and Reproduction .2nd ed 19854.郑重海洋浮游生物学 19845.张志良植物生理学实验指导 19906.孙军;刘东艳;钱树本浮游植物生物量研究I.浮游植物生物量细胞体积转化法 1999(02)7.EPPLY R W;REID F M H;STRICKLAND J D H The ecology of the plankton off LaJolla,California,in the period April through September 1967 Part Ⅲ.Estimates of 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半导体ndc薄膜成分Semiconductor NdC (neodymium-doped cerium oxide) thin films have gained significant attention in recent years due to their unique properties and potential applications in various fields. NdC thin films are composed of a combination of neodymium (Nd) and cerium oxide (CeO2), which offers distinct advantages in terms of optical, electrical, and magnetic properties.From an optical perspective, NdC thin films exhibit excellent transparency in the visible range, making them suitable for applications in optoelectronic devices such as transparent conductive electrodes, touchscreens, and solar cells. The addition of neodymium ions enhances the optical absorption and emission properties of the thin films, enabling the development of efficient light-emitting devices and lasers. These optical characteristics make NdC thin films highly desirable for next-generation display technologies and solid-state lighting.In terms of electrical properties, NdC thin films possess high electrical conductivity due to the presence of neodymium ions, which act as charge carriers. This property makes them suitable for applications in electronic devices, such as transistors and integrated circuits. The conductivity of NdC thin films can be further enhanced by optimizing the doping concentration of neodymium ions, leading to improved device performance and reduced power consumption.Furthermore, NdC thin films exhibit interesting magnetic properties, making them attractive forapplications in spintronics and magnetic storage devices. The neodymium ions introduce magnetic moments into the cerium oxide lattice, resulting in enhanced magnetic behavior. This opens up possibilities for the development of novel magnetic sensors, magnetic random access memories (MRAMs), and other spintronic devices.In addition to their unique optical, electrical, and magnetic properties, NdC thin films also offer exceptional chemical stability and corrosion resistance. The ceriumoxide matrix acts as a protective layer, preventing the degradation of the thin films in harsh environments. This makes NdC thin films suitable for applications in corrosive atmospheres, such as high-temperature and high-pressure environments.To summarize, semiconductor NdC thin films composed of neodymium-doped cerium oxide offer a wide range ofpotential applications due to their excellent optical transparency, electrical conductivity, magnetic properties, and chemical stability. These thin films have the potential to revolutionize various fields, including optoelectronics, electronics, spintronics, and magnetic storage. Continued research and development in this area will undoubtedly lead to further advancements and the realization of innovative devices and technologies.。
英文回答:Left— and right—turn—sided oscillations are two special oscillations in optical science and are uniquely transmitted in plasma。
The left and right vortex vibrates in different directions。
The electron vector of the left oscillation is rotated in the direction of light in reverse—clockwise, while the right oscillation is rotated in the light。
In plasma, the transmission of the dioxidation is influenced by the plasma, or some interesting phenomena。
Plasma is a substance consisting of a positive ion and a free electron, which has a non—linear response to electromagnetic waves, resulting in a left oscillation and a right oscillation in the plasma, or in the creation of new phenomena。
左旋偏振光和右旋偏振光乃光学中两种特殊偏振状态,于等离子体中之传播具有独特特性。
左旋偏振光与右旋偏振光异者,在于其振动方向有所不同。
左旋偏振光之电矢沿光传播方向逆时针旋转,而右旋偏振光则为顺时针旋转。
于等离子体中,此两偏振光之传播受等离子体之影响,或发生一些有趣现象。
Research Highlights► A multi-section circuit model for QD-SOA is presented with convergency improved. ► PSPICE simulator guarantees an efficient simulation for the circuit model. ► Pattern effect reduction isinvestigated by this circuit subsystem in detail. 190 Organizational routines, innovation, and flexibility: The application of narrative networks to dynamicworkflow Original Research ArticleInternational Journal of Medical Informatics , In Press,Corrected Proof , Available online 17 February 2011Gillian R. Hayes, Charlotte P. Lee, Paul Dourish Close preview | Related articles |Related reference w ork articles Abstract | Figures/Tables | ReferencesAbstractObjectiveThe purpose of this paper is to demonstrate how current visual representationsof organizational and technological processes do not fully account for thevariability present in everyday practices. We further demonstrate how narrativenetworks can augment these representations to indicate potential areas forsuccessful or problematic adoption of new technologies and potential needsfor additional training.MethodsWe conducted a qualitative study of the processes and routines at a majoracademic medical center slated to be supported by the development andinstallation of a new comprehensive HIT system. We used qualitative dataPurchasecollection techniques including observations of the activities to be supported by the new system and interviews with department heads, researchers, and both clinical and non-clinical staff. We conducted a narrative network analysis of these data by choosing exemplar processes to be modeled, selecting and analyzing narrative fragments, and developing visual representations of the interconnection of these narratives.ResultsNarrative networks enable us to view the variety of ways work has been and can be performed in practice, influencing our ability to design for innovation in use.DiscussionNarrative networks are a means for analyzing and visualizing organizational routines in concert with more traditional requirements engineering, workflow modeling, and quality improvement outcome measurement. This type of analysis can support a deeper and more nuanced understanding of how and why certain routines continue to exist, change, or stop entirely. At the same time, it can illuminate areas in which adoption may be slow, more training or communication may be needed, and routines preferred by the leadership are subverted by routines preferred by the staff.A rticle Outline1. Introduction2. Approaches to representing organizational processes3. Research site and methods: a narrative network analysis of organizational routines at UniHospital3.1. Development of narrative networks3.1.1. Choose a focal phenomenon and define its boundary3.1.2. Choose a point of view3.1.3. Collect narratives and code fragments3.1.4. Relate nodes by sequence4. Introducing two case studies: patient scheduling and chart delivery 4.1. Patient scheduling 4.2. Records management and chart delivery5. Narrative networks in Health IT5.1. “A Broader Range of Possibilities”5.2. Generative routines5.3. Considering multiple viewpoints6. Implications for Health IT6.1. Using narrative networks in practice7. ConclusionAuthors’ contributionsConflict of interest statementAcknowledgementsReferencesResearch highlights► We analyze empirical data from a major medical center using narrative networks . ► Designing for Health IT should include processes that focus on live routines and multiple viewpoints. ► Narrativenetworks provide insight into what can and does happen in organizational routines. ► Narrative networks enable designing for innovation in use.191 Water network design with stochastic optimization approach Original Research ArticleChemical Engineering Research and Design , In Press,Corrected Proof , Available online 15 January 2011Grzegorz Poplewski, Jacek M. Jeżowski, Alina Jeżowska Close preview | Related articles | Related reference w ork articlesPurchaseAbstract | Figures/Tables | ReferencesAbstractWater network (called also water allocation) problem has been addressed in more than 200 papers to date –see recent reviews by Jeżowski (2010) and Foo (2009). Though various solution methods have been developed they all have some limitations. This paper addresses water usage network with regeneration processes. Multiple contaminants and two types of water using processes are taken into regard. Simultaneous one stage optimization method was developed to synthesize the network. In order to solve complex MINLP formulation we propose to apply meta-heuristic optimization – adaptive random search method.The paper contains detailed solution algorithm. Several examples with specific features are solved to show efficiency and flexibility of the approach.A rticle Outline1. Introduction2. WUN superstructure and its optimization model3. Solution algorithm3.1. Mechanism for binary variables3.2. Solution of constraints3.3. Generation of initial point4. Examples of method application4.1. Example 14.2. Example 24.3. Examples 3a and 3b4.4. Example 44.5. Example 55. Performance analysis6. SummaryAcknowledgementsAppendix A. AppendixReferences Research highlights► This paper addresses water usage network with regeneration processes. Multiple contaminants and two types of water using processes are taken into regard. Simultaneous one stage optimization method was developed to synthesize the network . ► Merits of the approach are illustrated by examples that contain design problem with: structural issues, cost function and regeneration processes, fixed load and fixed flow rate water using processes, regeneration recycles elimination, over-constrained feasible region. ► The proposed approach generates solutions that are optimal or a set of near optimal networks. 192 Cost-effective heuristics for planning GMPLS-basedtransport networks Original Research ArticleOptical Sw itching and Networking , Volume 7, Issue 1,January 2010, Pages 12-27Nabil Naas, H.T. Mouftah Close preview | Related articles | Related reference work articlesAbstract | Figures/Tables | ReferencesAbstractWith the ever-increasing traffic in WDM transport networks, the developmentof GMPLS (or multi-granular) transport networks becomes essential to avoidthe cost explosion of OXCs. Much work has been devoted to the developmentof Multi-Granular Optical Crossconnect (MG-OXC) architectures and networkdesign and planning methods. Extending these efforts here, we address a newproblem of planning the GMPLS-based transport network by (1) consideringthe whole traffic hierarchy defined in GMPLS; and (2) allowing the bifurcationof multi-granularity traffic demands among different physical routes. We callPurchasesuch a problem the Routing and Multi-Granular Paths Assignment (RMGPA). The objective of the problem is to minimize the total weighted port count in the transport network. Due to the computational complexity of the problem, only very small-sized planning problems can be solved exactly through Mixed Integer Linear Programming (MILP) optimization. In this paper, we proposeefficient heuristics that are capable of solving large-sized planning problems ina reasonable amount of time.A rticle Outline1. Introduction2. Network architecture2.1. Node architecture2.2. Path types3. Solution of the planning problem3.1. Adjusting traffic demands3.2. Multi-granular virtual topology design3.3. Increasing pass-through segments4. Numerical results4.1. Verification of the heuristic approach4.2. Impact of increasing fiber resources4.3. Why bifurcating all demands is an expensive choice4.4. Heuristics evaluation5. ConclusionsReferences193Forcing technological change: A case of automobileemissions control technology development in theUS Original Research ArticleTechnovation, Volume 30, Issue 4, April 2010, Pages249-264Jaegul Lee, Francisco M. Veloso, David A. Hounshell,PurchaseEdward S. RubinClose preview | Related articles | Related reference w ork articlesAbstract | Figures/Tables | ReferencesAbstractThis article investigates how regulated automakers and upstream component suppliers comply with “technology-forcing” regulations, or laws that set performance standards beyond their usual technological capabilities. In particular, this article examines how firms manage and organize their research and development (R&D) processes concerning automobile emissions control technologies amid the uncertainties resulting from the issuance of new regulations. This study involves the analyses of patents, interviews with experts, references to technical papers published for conferences of the Society of Automotive Engineers (SAE), and use of learning curves. The results of this study show that the high regulatory standards under the technology-forcing regulation played an important role in forcing technological innovations and determining subsequent direction of technological change. Component suppliers were important sources of innovation in the 1970s, but over the course of technological evolution, automakers gradually emerged as the locus of innovation. This study also shows that firms strategically manage architectural and component knowledge in the presence of uncertainties about their technological capacity to meet new auto emissions control standards.A rticle Outline1. Introduction2. Overview of technology-forcing regulations and innovation in auto emissions control2.1. Government regulations2.2. Innovation in automobile emissions control technologies3. Methods 3.1. Data 3.1.1. Patent database3.1.2. Technical publications database3.1.3. Cost database3.2. Expert interviews4.Results4.1. Inventive activities: timing of technology introductions and patenting trend4.2. Sources and the locus of innovation4.2.1. Sources of innovation: the overall picture4.2.2. Locus of innovation and technology evolution4.3. Knowledge management and task uncertainty4.4. Learning by doing4.4.1. Learning in the 1980s5. Discussion and conclusions5.1. Policy and managerial implications5.1.1. Command-and-control type regulation5.1.2. Internal structures of regulations and technological change5.1.3. Technological advances and the sources of innovation5.1.3.1. Science, University, and Technological Change5.1.3.2. Incumbent as the locus of innovation6. Conclusion and future researchAcknowledgementsReferencesVitae194 A multi-objective optimization for green supply chain network design Original Research ArticleDecision Support Systems , In Press, Corrected Proof ,Available online 26 November 2010Fan Wang, Xiaofan Lai, Ning Shi PurchaseClose preview | Related articles | Related reference w ork articlesAbstract | Figures/Tables | ReferencesAbstractIn this paper, we study a supply chain network design problem withenvironmental concerns. We are interested in the environmental investmentsdecisions in the design phase and propose a multi-objective optimizationmodel that captures the trade-off between the total cost and the environmentinfluence. We conduct a comprehensive set of numerical experiments. Theresults show that our model can be applied as an effective tool in the strategicplanning for green supply chain. Meanwhile, the sensitivity analysis providessome interesting managerial insights for firms.A rticle Outline1. Introduction2. Problem definition and modeling3. Solving approach4. Computational experiments4.1. A six-node example4.2. Case study5. ConclusionsAcknowledgementsReferencesVitaeResearch Highlights► We study a supply chain network design problem with environmental considerations. ► We find that supply chain networks with larger capacities exhibits lower total cost and lower CO2emission. ►Consideration of environmental emissions of supply chain network is more effective and necessary at a higher demand level.195 Design of the optical Raman amplifier for the shorestation of NEMO phase 2Original Research ArticleNuclear Instruments and Methods in Physics ResearchSection A: Accelerators, Spectrometers, Detectors and Associated Equipment, Volumes 626-627, Supplement 1,11 January 2011-21 January 2011, Pages S173-S175A. D’Amico and for the NEMO collaborationShow preview | Related articles | Related reference w ork articlesPurchase196 Optically injected logic circuits for remote-poweredsystems on a chip Original Research ArticleComputers & Electrical Engineering, Volume 36, Issue 6, November 2010, Pages 1075-1092Dorin Patru, R. Scott HudsonShow preview | Related articles | Related reference w ork articlesPurchase197 Knowledge absorption of optical technologycompanies in Shanghai, Pudong: Successes, barriersand structural impediments Original Research ArticleApplied Geography, In Press, Corrected Proof,Availableonline 25 February 2011Ingo Liefner, Christian Brömer, Gang ZengShow preview | Related articles | Related reference w ork articlesPurchaseResearch highlights► We examine knowledge absorption in the Optical Technology (OT) industry in Shanghai. ► We pay particular attention to linkage, leverage and learning. ► Shanghai's OT companies aim at establishing linkages with foreign companies. ► The privately owned OT companies lack key resources for leverage and learning. ► Foreign-invested OT companies' learning activities depend on their parent firms.198 Design and development of a data acquisition systemfor photovoltaic modules characterization OriginalResearch ArticleRenew able Energy, Volume 35, Issue 7, July 2010, Pages1484-1492Hocine Belmili, Salah Med Ait Cheikh, Mourad Haddadi,Cherif LarbesPurchaseShow preview | Related articles | Related reference w ork articles199 Personnel selection using analytic network processand fuzzy data envelopment analysisapproaches Original Research ArticleComputers & Industrial Engineering, Volume 59, Issue 4, November 2010, Pages 937-944Hung-Tso LinShow preview | Related articles | Related reference w ork articlesPurchaseResearch highlights►TFN scheme catches the subjectiveness and vagueness of assessments. ► ANP incorporates the evaluation criteria with the staffing philosophy. ► Precision a nd confidence of assessment are considered by using different α values.200 A slender string design for deep-sea neutrinotelescopes Original Research ArticleNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Volumes 626-627, Supplement 1, 11 January 2011-21 January2011, Pages S136-S138E. Heine, E. Berbee, R. de Boer, H. Boer Rookhuizen, J. Hogenbirk, H. Kok, P. Kooijman, A. Korporaal, S. Mos, G. Mul, H. Peek, P. Timmer, E. de Wolf and On behalf of the KM3NeT consortium Show preview | Related articles | Related reference w ork articles。