FDTD_solutions操作案例1
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知识库安装和设置入门教程参考指南用户指南应用实例天线艺术ASAPBSDF谐振腔CMOS增益材料缺陷检测光栅OLEDs材料科学超材料显微镜多层堆叠結構非线性光学镊子光子晶体太阳能电池表面等离子波导A cavity is called a low Q cavity when the electromagnetic fields decay completely from the simulation in a timeFDTD Solutions 在线帮助Quality factor calculations FDTD Solutions product page Training workshop schedule Webinar schedule Download page)SearchResonance 2:frequency = 205.814THz, or 1456.62 nmQ = 77.498 +/- 0.226738The analysis script also creates two plots. The plot shown below to the left contains one of the field components (Hz). You can see that the fields have decayed by the end of the simulation time. The second plot shows the location and relative amplitude of the resonance peaks.Note that the initial transients of the source are neglected by setting the "start time" for the time monitors to 200fs. The "start time" for the time monitors is the time at which the monitors begin recording data. This setting can be changed in the user properties for the analysis group. Also, note that in the analysis group, it is possible to use one time monitor or an array of time monitors for the Q factor calculation. The problem with using one time monitor is that if the one monitor is placed at or near a null of the cavity mode, then due to the fact that the field intensity is very low, the Q factor can have a large uncertainty (if it is even possible to obtain a meaningful result).The low_quality_factor_3D.fsp simulation file contains a 3D version of the low Q analysis object.High Q cavitiesA cavity is considered to be a high Q cavity when the electromagnetic fields cannot completely decay from the simulation in a time that can be simulated reasonably by FDTD. In this case, we cannot determine Q from the frequency spectrum because the FWHM of each resonance in the spectrum is limited by the time of simulation,Tsim , by FWHM ~ 1/Tsim. Instead, the quality factor should be determined by the slope of the envelope of thedecaying signal using the formulawhere fRis the resonant frequency of the mode, and m is the slope of the decay in SI units.Derivation of Q factor formula:The quality factor (Q) is defined aswhere wris the resonant frequency and FWHM is the full width half max of the resonance intensity spectrum. The time domain signal of the resonance is described bywhere α is the decay constant. The fourier transform of E(t) is easy to calculate.The maximum value of |E(w)|^2 is clearly 1/α^2, at w=wr. With a little more work, we can determine that thehalf max frequencies occurs at w=wr + α and w=wr- α. Therefore, FWHM = 2α. Substituting this value intothe original Q formula and solving for α givesNow that we know how to relate α to Q, we must determine how the slope of the time signal decay is related to Q. We must take the log of the time signal to make the envelope a linear function.where m is the slope of the log of the time signal envelope. Solving for Q, we get.Example:Calculation of the Q factor for high Q cavities is complicated because•separating the decay of the envelope from the underlying sinusoidal signal is difficult since the fields are typically real-valued•if there are multiple resonant modes, they will interfere with each other in the time domain, making it hard to estimate the decay rate.By opening the edit dialog box for the Q factor analysis object located in quality_factor_3D.fsp, you can see that the analysis object solves these problems by•accurately calculating the envelope of the time-domain field signal•isolating each resonance peak in the frequency domain using a Gaussian filter, and then taking the inverse Fourier transform to calculate the time decay separately for each peak. The slope of the time decay is then used to calculate the Q factor and obtain an error estimate.In addition, note that:•the Q analysis object has setup variables that allow you to choose how many time monitors to use to calculate the Q factor. It is often a good idea to add a few point monitors at different locations to reduce the chances that a monitor is placed at a node in the mode profile of a cavity mode yielding a weak signal.•in the analysis tab, there is a parameter that can be set to choose how many resonant peaks to look for •all the field components that are available are used to calculate the Q factor•it is possible to change other parameters, such as the Gaussian filter width and resolution in the frequency domain. These parameters are set in the analysis script.•in the script, only the part of the time signal lying in 40-60% of the time signal collected is used for the slope calculation. These percentages can easily be changed. However, setting the upper limit to anything greater than 90% can lead to errors due to the fact that Fourier transforms, and inverse transforms were used when the Gaussian filter was used to isolate the peak. The Fourier transforms introduce errors to the end of the time signal due to the fact that discrete Fourier transforms assume periodicity of the signal.Next, run the simulation. When the simulation is complete, choose to edit the analysis object and press RUN ANALYSIS button. The analysis script output will contain the location of the resonance frequencies and their corresponding Q factors.Resonance 1:frequency = 178.786THz, or 1676.82 nmQ = 306.279 +/- 1.41318Resonance 2:frequency = 227.307THz, or 1318.89 nmQ = 274.874 +/- 4.50921The analysis object also produces the following plots.The time decay of the field components and their envelopes. Note The spectrum and the Gaussian filtersThe spectrum of resonances. Each resonant peak appears in a The time decay of the sum of squared Other versions of this page:Events。
一基于A u薄膜正三角形孔阵列提取光场强度分布图本例子中取Au薄膜厚度30nm,三角形孔阵周期800nm,小孔直径600nm。
Au的材料模型选取“Au (Gold)–CRC”,或者自建材料模型。
参见hole arrays_E fied 文件。
1.添加金薄膜,打开FDTD Solution 软件后点击“structure”,添加长方体模块。
如下图所示。
点击,对几何参数和材料类型等进行编辑。
参照下图。
先将“name”改为“Au 30nm”,在“Geometry”下设置金薄膜的几何尺寸,我们只需要对下图红框所示的左边一栏进行编辑,其中“x span、y span、z span”分别对应金薄膜的长、宽和厚度,而“x、y、z”表示其几何中心的坐标值,均设置为0。
在“x span”中输入“*2+”,“y span”中输入“*sqrt(3)+”,“z span”中输入“”,对应金薄膜厚度为30nm,便可得到如下图所示的结果。
点击“material”,选择所使用的材料类型,如下图所示,选中“Au (Gold) - CRC”,点“OK”保存即可。
现在对金膜的几何尺寸和材料类型设置完成。
2.在金薄膜中添加小孔阵列。
点击中的三角形,在下拉菜单中选择“Photonic crystals”。
然后在屏幕右侧的“Object”一栏中选中“Hexagonal lattice PC array”,点击“Insert”进行添加。
在左侧的结构树“object tree”中选中“hex_pc”,即我们刚才添加进去的六边形阵列,点击对它进行编辑。
各参数设置如下图所示,其中“a”表示小孔之间的间距,即三角形孔阵的周期,“radius”表示小孔半径。
设置完成后,点“ok”保存。
经过上面的步骤,我们搭建的模型的如下图所示。
我们发现经过上面的设置所得到的三角形孔阵列其中两个小孔超出了金膜,为了好看起见,希望将多余的这两个小孔删掉,首先,如下图所示,在结构树下选中“hex_pc”,单击鼠标右键在菜单中选择“break groups”,不进行这项操作无法删掉多余的小孔。
一基于AU 薄膜正三角形孔阵列提取光场强度分布图本例子中取AU薄膜厚度30nm ,三角形孔阵周期800nm,小孔直径600nm。
AU的材料模型选取"AU (Gold) - CRC ”,或者自建材料模型。
参见hole arrays_E fied Profile.fsp文件。
1.添加金薄膜,打开FDTD Solution软件后点击“StrUCtUre”,添加长方体模块。
如下图所示。
IVn Ala e⅛ιl 先将“ name'改为“ AU 30nm”,在“ Geometry”下设置金薄膜的几何尺寸, IiJul ÷lF-I♦ < * ∙T wWModel• ITrtBPgle⅛C⅛∏fl⅛■1III__________ _ ”对几何参数和材料类型等进行编辑。
参照下图。
⅜•*4 ,□ T/** 迦^⅞4 ・⅝ ▼B ∙βilcrτ 门零S⅞j⅛c⅞urts ftttribnUi CwfOMntE ⅛f OTflIS ArllIyEi ιI*P4iFt Scnurcis两In £灯E BtE4TKf<!⅛G ct⅞⅛HLame⅛* m□t⅛lιA<lpr⅛∣lririlMame-DimefISECIm∕⅛akIB.■Iy XJ-Iripa-ClLm Ti.I oll I JllrStE Tr-Iril;2寻XFnD LTKau⅛Dlm» & o M点击T J-∣4XT TIrR 5⅛-jp∣KS 址Farl l H⅞UVl VL*τRιτul LTIrH我们只需要对下图红框所示的左边一栏进行编辑,其中“X SPan、y SPan、z SPan” 分别对应金薄膜的长、宽和厚度,而“ x、y、z”表示其几何中心的坐标值,均设置为0。
在“X span” 中输入“0.8*2+0.6 ”,“y SPan” 中输入"0.8*sqrt(3)+0.6 ”“Z SPan ”中输入“ 0.03 ”,对应金薄膜厚度为30nm便可得到如下图所示的结果。
以上面图像为例子,设置时只需要设置一个周期,然后将边界设为周期结构即可。
1.打开fdtd软件
2.单击structures设置结构。
3.选中物体单击右键设置参数。
给结构命名,x,y,z确定结构在各个方向上的范围。
5设置选中结构的材料,如果material里有想要的材料直接选中即可,没有的可以通过查询,将其折射率直接输入到index中。
6.当结构重叠时,可勾选下面按钮,设置重叠部分的优先性,数字越小优先性越高。
7.设置基底上的光栅结构,先设置下层Al。
8.设置中间层PMMA
9.设置上层Al
10.单击Simulation选中region设置模拟区域。
Geometry设置单元结构参数,一般选取一个周期即可,所以X span和Y span就是周期,然后在boundary conditions中将x,y都选为periodic。
点击OK.
11.在Source中选取plane wave,genaral中入射方向改为向下入射,geometry中X span和Y span选取的要比周期大,Frequency/wavelength中改变入射波长范围。
12.在Monitor中选取frequency domain field and power探测器。
勾选第一项,将frequency points变为200,将探测器放于光源上方探测反射率。
还可以在选取一个探测器放于下方探测投射,一次模拟可以放入多个探测器。
13.结构设置完成之后,点击RUN,运行,待运行完毕后,选择对应的探测器,可以看出探测到的结果。
欢迎进入FDTD Solutions 的入门教程!入门教程由四章内容组成。
第一章介绍FDTD Solutions 的基本功能,以及器件建构,程序运行和结果分析。
后面三章则针对v个实际问题,提供详细指导,帮助用户一步步地了解每一模块的功能及其使用。
文中涉及的所有模拟设计文件都可以从LUMERICAL 的相应网页上免费下载。
第一章简介第二章银质纳米线谐振腔散射教程第三章环形谐振腔教程第四章光子晶体微腔教程简介The goal of the Getting Started Guide is to introduce the Finite Difference Time Domain (FDTD) technique and explain how modeling is done with the software.The FDTD algorithm is useful for design and investigation in a wide variety of applications involving the propagation of electromagnetic radiation through complicated media. It is especially useful for describing radiation incident upon or propagating through structures with strong scattering or diffractive properties. The available alternative computational methods - often relying on approximate models - frequently provide inaccurate results. FDTD Solutions is useful for numerous engineering problems of commercial interest including:• display technologies• optical storage devices• LED design• biophotonic sensors• plasmon polariton resonance devices• optical waveguide devices• photonic crystal devices• integrated optical filters• optical micro cavity designFDTD Solutions is an accurate and easy to use, versatile design tool capable of treating this wide variety of applications. This introductory chapter of the Getting Started Guide introduces the general FDTD method and provides a basic overview of the product usage. The final sections contain examples that are accompanied by step-by-step instructions so that you can set up and run the simulations yourself.什么是时域有限差分?The Finite Difference Time Domain (FDTD) method has become the state-of-the-art method for solving Maxwell’s equations in complex geometries. It is a fully vectorialmethod that naturally gives both time domain , and frequency domain information to the user, offering unique insight into all types of problems and applications inelectromagnetics and photonics .The technique is discrete in both space and time . The electromagnetic fields and structural materials of interest are described on a discrete mesh made up of so-called Yee cells . Maxwell’s equations are solved discretely in time, where the time step used is related to the mesh size through the speed of light. This technique is an exactrepresentation of Maxwell’s equations in the limit that the mesh cell size goes to zero. Structures to be simulated can have a wide variety of electromagnetic material properties. Light sources may be added to the simulation. The FDTD method is used to calculate how the EM fields propagate from the source through the structure . Subsequent iteration results in the electromagnetic field propagation in time. Typically, the simulation is run until there are essentially no electromagnetic fields left in the simulation region.Time domain information can be recorded at any spatial point (or group of points). This data can be recorded for the duration of the simulation, or it can be recorded as a series of "snapshots" at times specified by the user.Frequency domain information at any spatial point (or group of points) may be obtained through the Fourier transform of the time domain information at that point. Thus, the frequency dependence of power flow and modal profiles may be obtained over a wide range of frequencies from a single simulation.In addition, results obtained in the near field using the FDTD technique may be transformed to the far field, in applications where scattering patterns are important.More information about the FDTD method, including references, can be found in the Physics of the FDTD Algorithm section of the reference guide.FDTD的用户界面This section discusses useful features of the FDTD Solutions Graphical User Interface (GUI).In this topicGraphical User Interface: Windows andToolbarsAdd Objects to the simulationEdit ObjectsStart a new 2D/3D simulationGraphical User Interface: Windows and ToolbarsThe graphical user interface contains useful tools for editing simulations, including• a toolbar for adding objects to the simulation• a toolbar to edit objects• a toolbar to run simulations•an objects tree to show the objects which are currently included in the simulation• a script file editor window•an object library• a window to set up parameter sweeps and optimizationsIn the default configuration some of the Windows are hidden. To open hidden windows, click the right mouse button anywhere on the main title bar or the toolbar to get the pop up window shown in the screen shot below. The visible windows/toolbars have a check mark next to their name; the hidden ones do not have check marks. A second way to obtain the pop up window is to go to the main title toolbar and select VIEW->WINDOWS.For more information about the toolbars and windows see the Layout editor section of the reference guide.Add Objects to the simulationThe Graphical User interface contains buttons to add objects to the simulation. Click on the arrow next to the image to get a pull down menu which shows all the available options in a group. The screenshot below shows what happens when we click on the arrow next to the COMPONENTS button. Note that the picture on the button is the same as the MORE CHOICES option in the list. If we click on the button itself (instead of the arrow) we will go directly to the MORE CHOICES section of the object library.Also notice that the picture for the COMPONENTS button will change depending on what the last component that was added to the simulation was. Finally, the ZOOM EXTENTbutton in the toolbar will resize the viewports to fit all the objects currently included in the simulation.Edit objectsTo edit an object, select the object and press E on the keyboard or press the EDIT buttonon the toolbar. The easiest way to select an object is to click on the name of the object in the objects tree. However, objects can also be selected by clicking on the graphical depiction of them when the SELECT button is pressed. For more information see the Layout editor section of the reference guide.When we edit objects in FDTD, we get an edit window. The edit windows have units for the settings; in the GEOMETRY tab, the x, y and z location will be in μm by default. The units can be changed to nm if we choose SETTINGS->LENGTH units in the main menu. Fields in the edit windows act like calculators, so that equations can be entered in the fields. See the y span field below for an example.Start a new 2D/3D simulationBy default FDTD Solutions opens with a blank 3D simulation. In the following Getting Started Examples, we often begin with a 2D simulation, which can be obtained as shown in the screenshot below.模拟运行与优化This section discusses important checks which should be made before running a simulation (memory requirements, material fits) and gives links to more information about running simulations and parameter sweeps or optimizations.In this topicCheck memory requirementsCheck material fitsSetup parallel optionsRun simulationRun parameter sweeps and optimizationsCheck memory requirementsTo check the memory requirements, press the CHECK button If this is not the current icon, you can find it by pressing the arrow. Note that the memory report indicates the amount of memory used by each object in the simulation project as well as the total memory requirements. This allows for judicious choice of monitor properties in large and extensive simulations.Check material fitsThe CHECK button also contains a material explorer option . Many of the materials used in FDTD Simulations come from experimental data (see the materials section of the Reference Guide for references for the material data and descriptions of the FDTD material models). Before running a simulation, FDTD Solutions automatically generates a multi-coefficient model fit to the material data in the wavelength range for the source. It is a good idea to check and optimize the material fit before running a simulation. Setup the resource configurationBefore running any simulations, the resource options must be set up. These options canbe accessed by pressing the Resources button . In most cases, the default settings should be fine. The 'number of processes' is typically set to the number of cores in your computer.Run simulationYou can run simulations by pressing the RUN button on the mail toolbar. For more details, such as how to run multiple simulations in distributed mode, please see the RunSimulations section in the online User Guide, or the Running simulations and analysis section of the Reference Guide.Run parameter sweeps and OptimizationsFDTD Solutions also has a built in parameter sweep and optimization window. This window can be seen at the top of the page, and can be opened using the instructions in the Graphical User Interface discussion just prior to this topic.Optimization Window includes buttons to add a parameter sweep and add an optimization. Parameter sweeps and optimizations can include multiple parameters, or be nested. Each optimization or sweep can be run by pressing the right-most button.仿真数据分析This section discusses the tools used to analyze simulation data: the Analysis Window, the script environment and data export to third party software such as MATLAB. For more details please see the Analysis tools and the Scripting language chapters in the Reference Guide.In this topicAnalysis windowScriptingData exportAnalysis windowThe screen shot below shows the open analysis window. The analysis window can be used to plot monitor data.A variety of monitor data can be plotted via the Analysis window, depending on the monitor type. Spatial refractive index data, field vs time, field vs frequency, fields vs spatial dimensions, and power transmission vs frequency are a few examples. The terminology 'Intensity' indicates a squared quantity. For example, 'E intensity' means |E|^2. 'Ex intensity' means |Ex|^2. Field data from frequency monitors is always plotted as an Intensity. If you want to see the real or imaginary parts of the field, or if you want to obtain phase information, the scripting language will be required.ScriptingFDTD Solutions contains a built in scripting language which can be used to obtain simulation data, and do plotting or post-processing of data. The script prompt can be used to execute a few commands, or the built in script file editor can be used to create more complex scripts.A thorough introduction to the Lumerical scripting language can be found in the Scripting section of the FDTD Solutions online user guide. Definitions for all of the script commands are given in the Scripting language chapter in the Reference Guide.Data ExportFDTD simulation data can be exported into text file format using the analysis window, into a Lumerical data file format (*.ldf) which can be loaded into another simulation, or into a Matlab data (*.mat) file. Instructions for exporting to these file formats can be found in the links under the Scripting section.银质纳米线谐振腔散射教程问题综述当光波入射到金属纳米粒子上时,光与金属表面附近的电荷密度相互作用产生的表面等离子体极化surface plasmon polaritons 扮演着重要角色。
Lumerical2013Suite光学设计软件的安装、破解和后续安装FDTD Solutions的方法1软件的来源来自于网页/06/15036.html网页面的:Download城通网盘X32:/file/23031069X64:/file/23031070此处可以下载到这个软件的32位和64位版本。
另外再给出360网盘的下载地址:32位版本:/cwU9xDN27Bvke访问密码894a64位版本:/cwU9SBWj9nNx2访问密码adca2安装方法Lumerical2013Suite光学设计软件(以x64版本为例)1下载好文件第一个是32位系统版,第二个是64位系统版。
根据自己电脑的系统,下载好安装包,这里以64位版本为例。
2解压解压后,得到这样几个文件夹。
3开始安装Lumerical_FlexLM-1.0.0打开文件夹Lumerical_FlexLM-1.0.0,看到双击LFLM,开始安装。
一般,x64默认安装在C:\Program Files(x86)\Lumerical可以修改为自己希望的位置,但是要求路径为全英文和数字。
4身份证问题安装开始后,出现对话框第一行就是你的安装路径,不用修改;第二行,写入身份证文件,位置如下:第一个文件就是身份证文件,把它的路径填入对话框第二行。
安装身份证后,出现5关闭身份认证服务Win7系统是安装window键和R打开,xp是点击启动菜单中的运行,输入下图所示命令,回车。
这个时候,出现下图:选中这一项,点击左侧的停止。
6替换打开前面身份证所在的path文件夹,复制第三项文件到安装文件夹C:\Program Files(x86)\Lumerical\Lumerical-FlexLM7重新开启服务方法类似第5步选中Lumerical项,点击左侧启动。
8验证是否破解成功http://localhost:8095/dashboard?vendor=&licenseTab=&selected=点击进入这个网页,出现下图点击右侧图标若出现下图(每项都是permenent):说明破解成功。
以下是关于FDTD(Finite Difference Time Domain)方法的Matlab代码。
1. FDTD方法简介FDTD方法是一种数值分析电磁场问题的方法,最早应用于求解Maxwell方程组。
该方法的基本思想是将时间和空间分割为离散网格,并利用差分法求解Maxwell方程组。
FDTD方法广泛应用于天线设计、电磁兼容性分析、光学器件仿真等领域。
2. FDTD方法的Matlab代码以下是一个简单的一维FDTD方法的Matlab代码示例:```matlab定义常数c = 3e8; 光速dx = 0.01; 空间步长dt = dx/(2*c); 时间步长初始化场量Ez = zeros(1,1000); 电场Hy = zeros(1,1000); 磁场模拟时间步进for n = 1:1000更新磁场for i = 1:999Hy(i) = Hy(i) + (Ez(i+1) - Ez(i))/(c*dx);end更新电场for i = 2:1000Ez(i) = Ez(i) + (Hy(i) - Hy(i-1))*(c*dt/dx);endend绘制结果figure;plot(Ez);xlabel('空间步长');ylabel('电场强度');title('FDTD方法仿真结果');```3. 代码解释- 代码首先定义了常数c(光速)、空间步长dx和时间步长dt。
- 然后初始化了电场Ez和磁场Hy的空间网格。
- 在时间步进的循环中,首先更新磁场Hy,然后更新电场Ez。
- 最后绘制了Ez随空间步长的变化图。
这是一个非常简单的一维FDTD方法的Matlab代码示例,实际应用中可能会有更复杂的三维情况,需要考虑更多的边界条件和介质性质。
4. FDTD方法的应用FDTD方法在天线设计、电磁兼容性分析、光学器件仿真等领域有着广泛的应用。
通过编写相应的Matlab代码,可以对复杂的电磁场问题进行数值分析,得到定量的仿真结果,为工程设计和科学研究提供重要的参考。
第一章FDTD Sol u tions 简介使用FDTD Solutions来进行仿真设计计算简单易懂。
首先要在FDTD Solutions的CAD 编辑状态建立一个要运算的文件(文件扩展名是.fsp),它必须包含有关物理结构、光源、监视器、以及仿真运算所需要的参数。
将此文件SAVE后就可以运行。
运行结束后,计算所得数据添加在原文件之内,然后就可以进行分析。
进行仿真设计计算这一简单过程一般需要如下图所示的步骤。
在随后的章节中将会详细讲解这些步骤。
1.1什么是FDTD?FDTD是F inite -D ifference T ime-D omain 的简写。
现在该方法已经成为求解复杂结构中麦克斯韦方程的最常用方法。
它是一种全矢量法,因此很自然地就会给出用户所需要的时域和频域信息。
这是该方法在电磁学和光子学所有应用中所拥有的独特优点。
FDTD技术在时间和空间都是离散的。
因此电磁场和所感兴趣结构材料必须在由所谓的YEE元胞构成的网格上予以描述。
麦克斯韦方程的求解在时间上是离散的,所用的时间步长通过光速与网格尺寸紧密相关。
在网格尺寸趋于零的极限情况下,这项技术准确无误地描述麦克斯韦方程。
所要仿真计算的结构可以具有各种各样的多种电磁材料特性。
根据需要,可以同时使用多个光源。
典型情况下,程序一直运行,直到电磁场能量几乎全部离开整个仿真计算区为止。
时域信息可以在任何一个或多个空间点上予以记录。
这些数据的纪录可以贯穿整个计算过程,也可以仅在用户设立的时间点上进行。
频域信息也可以在任何一个或多个空间点或面上予以记录,它们是通过对时域信息进行傅立叶变换获得的。
正因为如此,一次运行就可以获得能流和模式结构的频率依赖关系。
此外,应用FDTD技术获得的近场结果也可以变换到远场。
这种近场-远场变换在诸如散射研究等应用方面是非常重要的。
1.2 第一步:创建器件的物理结构打开FDTD Solutions 后,一个有三维视窗的外形编辑器(Layout Editor,简称编辑状态)就呈现在眼前。
第一部分简介本入门指南对FDTD Solutions进行初步介绍,并演示如何模拟一些简单的体系。
在涉及电磁辐射在复杂媒介中转播方面的许多应用过程的设计和分析方面,FDTD算法非常有用。
特别适用于描述光线在具有较强散射和衍射特性的物体的入射以及传播。
而其它一些可选择的采用近似模型的计算方法,通常给出的结果不太精确。
FDTD Solutions可用来解决工程方面的许多实际问题,包括:●集成光学器件●显示技术●光学存储设备●OLED 设计●生物光子传感器●等离子体极化声子共振设备●光波导器件●光子晶体的设备●LCD设备FDTD Solutions是一种可处理这方面许多实际问题的可靠、易用、通用的开发工具。
简介部分对FDTD方法进行大概说明,并初步介绍使用方法。
随后是一些范例,并给出建模的每个步骤,这样你就可以建模并进行模拟计算。
1.1 什么是FDTD?时域有限差分(Finite Difference Time Domain:FDTD)法已经成为求解复杂几何体麦克斯韦方程的比较先进的方法。
并且完全以矢量法给出时域和频域方面的信息,有助于对电磁学以及光子学的各种类型的问题以及FDTD的应用有更深入的了解。
该技术在空间和时间上采用离散方式。
电磁场以及结构材料独立的的Yee元胞网格所描述,在时间上采用离散方式解麦克斯韦方程,所选用的时间步长在整个光速范围同元胞大小相关,当元胞大小趋于零时,可得到麦克斯韦方程的严格解。
模拟结构单元材料的电磁特性可以在很大范围变化。
可以将光源加入到模拟中,采用FDTD方法可以计算电磁场是如何从光源通过结构单元的。
在电磁波传播期间采用连续迭代方法进行计算。
通常情况下直到模拟区间没有电磁场存在时,模拟计算过程才停止。
在任何空间点(或点群)均可以记录时域信息。
这类数据既可以在模拟过程记录下来,也可以在用户规定的时间以一系列“快照”的方式记录下来。
同样也可能得到任何空间点(或点群)的频域信息,即通过对该点的时域信息进行傅里叶变换而得到。
以上面图像为例子,设置时只需要设置一个周期,然后将边界设为周期结构即可。
1.打开fdtd软件
2.单击structures设置结构。
3.选中物体单击右键设置参数。
给结构命名,x,y,z确定结构在各个方向上的范围。
5设置选中结构的材料,如果material里有想要的材料直接选中即可,没有的可以通过查询,将其折射率直接输入到index中。
6.当结构重叠时,可勾选下面按钮,设置重叠部分的优先性,数字越小优先性越高。
7.设置基底上的光栅结构,先设置下层Al。
8.设置中间层PMMA
9.设置上层Al
10.单击Simulation选中region设置模拟区域。
Geometry设置单元结构参数,一般选取一个周期即可,所以X span和Y span就是周期,然后在boundary conditions中将x,y都选为periodic。
点击OK.
11.在Source中选取plane wave,genaral中入射方向改为向下入射,geometry中X span和Y span选取的要比周期大,Frequency/wavelength中改变入射波长范围。
12.在Monitor中选取frequency domain field and power探测器。
勾选第一项,将frequency points变为200,将探测器放于光源上方探测反射率。
还可以在选取一个探测器放于下方探测投射,一次模拟可以放入多个探测器。
13.结构设置完成之后,点击RUN,运行,待运行完毕后,选择对应的探测器,可以看出探测到的结果。
以上面图像为例子,设置时只需要设置一个周期,然后将边界设为周期结构即可。
1.打开fdtd软件
2.单击structures设置结构。
3.选中物体单击右键设置参数。
给结构命名,x,y,z确定结构在各个方向上的范围。
5设置选中结构的材料,如果material里有想要的材料直接选中即可,没有的可以通过查询,将其折射率直接输入到index中。
6.当结构重叠时,可勾选下面按钮,设置重叠部分的优先性,数字越小优先性越高。
7.设置基底上的光栅结构,先设置下层Al。
8.设置中间层PMMA
9.设置上层Al
10.单击Simulation选中region设置模拟区域。
Geometry设置单元结构参数,一般选取一个周期即可,所以X span和Y span就是周期,然后在boundary conditions中将x,y都选为periodic。
点击OK.
11.在Source中选取plane wave,genaral中入射方向改为向下入射,geometry中X span和Y span选取的要比周期大,Frequency/wavelength中改变入射波长范围。
12.在Monitor中选取frequency domain field and power探测器。
勾选第一项,将frequency points变为200,将探测器放于光源上方探测反射率。
还可以在选取一个探测器放于下方探测投射,一次模拟可以放入多个探测器。
13.结构设置完成之后,点击RUN,运行,待运行完毕后,选择对应的探测器,可以看出探测到的结果。