{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "# Chapter8 - Optoelectronic detectors" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.1 : Page 204" ] }, { "cell_type": "code", "execution_count": 1, "metadata": { "collapsed": false, "scrolled": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "The photon energy = 1.31 micro-m \n", "part (b)\n", "The optical power = 4.07 micro W \n" ] } ], "source": [ "from __future__ import division\n", "#The photon energy and optical power\n", "#given data :\n", "print \"part (a)\"\n", "h=6.626*10**-34## in Js\n", "c=3*10**8## in ms**-1\n", "E=1.52*10**-19## in J\n", "lamda=((h*c)/E)*10**6#\n", "print \"The photon energy = %0.2f micro-m \"%lamda\n", "print \"part (b)\"\n", "e=1.6*10**-19## in J\n", "Ip=3*10**6## in A\n", "E=1.52*10**-19## in J\n", "eta=70/100#\n", "R=(eta*e)/E#\n", "P_in=(Ip/R)*10**-6#\n", "print \"The optical power = %0.2f micro W \"%P_in" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.2 : Page 205" ] }, { "cell_type": "code", "execution_count": 2, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "The quantum efficiency, eta = 50.00 %\n", "part (b)\n", "Maximum possible band gap energy,Eg = 1.46 eV \n", "part (c)\n", "The mean output, Ip = 3.42 micro A\n" ] } ], "source": [ "#The quantum efficiency,Maximum possible band gap energy and mean output\n", "#given data :\n", "print \"part (a)\"\n", "e=1## electron\n", "p=2## photon\n", "eta=(e/p)*100#\n", "print \"The quantum efficiency, eta = %0.2f %%\"%eta\n", "print \"part (b)\"\n", "h=6.626*10**-34##in Js\n", "c=3*10**8## in m s**-1\n", "lamda_c=0.85*10**-6## in m\n", "Eg=((h*c)/lamda_c)/1.6*10**19#\n", "print \"Maximum possible band gap energy,Eg = %0.2f eV \"%Eg\n", "print \"part (c)\"\n", "e=1## electron\n", "p=2## photon\n", "eta=(e/p)#\n", "e=1.6*10**-19## in J\n", "h=6.626*10**-34##in Js\n", "c=3*10**8## in m s**-1\n", "lamda_c=0.85*10**-6## in m\n", "Eg=((h*c)/lamda_c)#\n", "P_in=10*10**-6## in W\n", "Ip=((eta*e*P_in)/Eg)*10**6#\n", "print \"The mean output, Ip = %0.2f micro A\"%Ip" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.3 : Page 205" ] }, { "cell_type": "code", "execution_count": 3, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "The quantum efficiency = 0.4\n", "part (b)\n", "The responsivity of the diode,R = 0.29 AW**-1\n" ] } ], "source": [ "#The quantum efficiency and The responsivity of the diode\n", "#given data :\n", "print \"part (a)\"\n", "e=2*10**10## in s**-1\n", "p=5*10**10## in s**-1\n", "eta=e/p#\n", "print \"The quantum efficiency = \",eta\n", "print \"part (b)\"\n", "e=2*10**10## in s**-1\n", "p=5*10**10## in s**-1\n", "eta=e/p#\n", "e=1.6*10**-19## in J\n", "h=6.626*10**-34##in Js\n", "c=3*10**8## in m s**-1\n", "lamda=0.90*10**-6## in m\n", "R=(eta*e*lamda)/(h*c)#\n", "print \"The responsivity of the diode,R = %0.2f AW**-1\"%R" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.4 : Page 210" ] }, { "cell_type": "code", "execution_count": 4, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "The multiplication factor,M = 47.8\n" ] } ], "source": [ "#The multiplication\n", "#given data :\n", "eta=40/100##\n", "e=1.6*10**-19## in J\n", "h=6.626*10**-34##in Js\n", "c=3*10**8## in m s**-1\n", "lamda=1.3*10**-6## in m\n", "P_in=0.3*10**-6## in W\n", "I=6*10**-6## in A\n", "M=(I*h*c)/(P_in*eta*e*lamda)#\n", "print \"The multiplication factor,M = %0.1f\"%M" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.5 : Page 210" ] }, { "cell_type": "code", "execution_count": 5, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Photon incident rate = 1.74e+07 s**-1\n" ] } ], "source": [ "#Photon rate\n", "#given data :\n", "e=1.6*10**-19## in J\n", "M=800#\n", "eta=90/100## quantum efficiency\n", "I=2*10**-9## in A\n", "P_rate=I/(e*eta*M)#\n", "print \"Photon incident rate = %0.2e s**-1\"%P_rate" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.6 : Page 212" ] }, { "cell_type": "code", "execution_count": 6, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "the gain = 58.95\n", "part (b)\n", "The output photo-current, I = 2.313e-04 A\n" ] } ], "source": [ "from math import pi\n", "#Gain and The output photocurrent\n", "#given data :\n", "print \"part (a)\"\n", "tf=6*10**-12## in s\n", "del_f=450*10**6## in Hz\n", "G=1/(2*pi*tf*del_f)#\n", "print \"the gain = %0.2f\"%G\n", "print \"part (b)\"\n", "tf=6*10**-12## in s\n", "del_f=450*10**6## in Hz\n", "G=1/(2*pi*tf*del_f)#\n", "eta=75/100#\n", "P_in=5*10**-6## in W\n", "e=1.6*10**-19## in J\n", "lamda=1.3*10**-6#\n", "h=6.626*10**-34##in Js\n", "c=3*10**8## in m s**-1\n", "I=(G*eta*P_in*e*lamda)/(h*c)#\n", "print \"The output photo-current, I = %0.3e A\"%I" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 8.7 : Page 215" ] }, { "cell_type": "code", "execution_count": 7, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "rms value of shot noise current is = 1.712 nA\n", "rms value of dark current is = 0.20 nA\n", "rms value of thermal noise current is = 20.35 nA \n", "part (b)\n", "S/N ratio = 321\n" ] } ], "source": [ "from math import sqrt\n", "#rms value of shot noise ,dark noise and thermal noise current and S/N ratio\n", "print \"part (a)\"\n", "n=0.7##efficiency\n", "e=1.6*10**-19##charge\n", "h=1.3##in micro meter\n", "hc=6.626*10**-34##plack constant\n", "c=3*10**8##m/s\n", "pin=500##nW\n", "Ip=((n*e*h*10**-6*pin*10**-9)/(hc*c))##in amperes\n", "df=25##Mhz\n", "f1=1##\n", "is2=(2*e*Ip*df*10**6*f1)##\n", "Is=sqrt(is2)##in amperes\n", "Id=5*10**-9##amperes\n", "id2=(2*e*Id*df*10**6)##\n", "Id=sqrt(id2)##in amperes\n", "k=1.38*10**-23##\n", "t=300##in kelvin\n", "rl=1000##ohms\n", "it2=((4*k*t*df*10**6)/rl)##\n", "it=sqrt(it2)##in amperes\n", "print \"rms value of shot noise current is = %0.3f nA\"%(Is*10**9)\n", "print \"rms value of dark current is = %0.2f nA\"%(Id*10**9)\n", "print \"rms value of thermal noise current is = %0.2f nA \"%(it*10**9)\n", "print \"part (b)\"\n", "n=0.7##efficiency\n", "e=1.6*10**-19##charge\n", "h=1.3##in micro meter\n", "hc=6.626*10**-34##plack constant\n", "c=3*10**8##m/s\n", "pin=500##nW\n", "Ip=((n*e*h*10**-6*pin*10**-9)/(hc*c))##in amperes\n", "df=25##Mhz\n", "f1=1##\n", "is2=(2*e*Ip*df*10**6*f1)##\n", "Is=sqrt(is2)##in amperes\n", "Id=5*10**-9##amperes\n", "id2=(2*e*Id*df*10**6)##\n", "Id=sqrt(id2)##in amperes\n", "k=1.38*10**-23##\n", "t=300##in kelvin\n", "rl=1000##ohms\n", "it2=((4*k*t*df*10**6)/rl)##\n", "it=sqrt(it2)##in amperes\n", "itt2=is2+id2+it2##in A**2\n", "ip2=Ip**2##\n", "sn=ip2/itt2##\n", "print \"S/N ratio = %d\"%sn\n", "#S/N ratio is calculated wrong in the textbook" ] } ], "metadata": { "kernelspec": { "display_name": "Python 2", "language": "python", "name": "python2" }, "language_info": { "codemirror_mode": { "name": "ipython", "version": 2 }, "file_extension": ".py", "mimetype": "text/x-python", "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython2", "version": "2.7.9" } }, "nbformat": 4, "nbformat_minor": 0 }