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diff --git a/Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter7.ipynb b/Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter7.ipynb deleted file mode 100755 index a97cee35..00000000 --- a/Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter7.ipynb +++ /dev/null @@ -1,334 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "# Chapter7 - Optoelectronic sources" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.1: Page 153" - ] - }, - { - "cell_type": "code", - "execution_count": 1, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Intrinsic carrier concentration ,ni = 2.2e+12 m**-3\n" - ] - } - ], - "source": [ - "from __future__ import division\n", - "from math import sqrt, pi, exp\n", - "#Intrinsic carrier\n", - "#given data :\n", - "m=9.11*10**-31## in kg\n", - "k=1.38*10**-23## in JK**-1\n", - "h=6.626*10**-34## in Js\n", - "ev=1.6*10**-19## in J\n", - "T=300## in K\n", - "me=0.07*m## in kg\n", - "mh=0.56*m## in kg\n", - "Eg=1.43*ev## in J\n", - "ni=2*((2*pi*k*T)/h**2)**(3/2)*(me*mh)**(3/4)*exp(-Eg/(2*k*T))#\n", - "print \"Intrinsic carrier concentration ,ni = %0.1e m**-3\"%ni" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.2: Page 155" - ] - }, - { - "cell_type": "code", - "execution_count": 2, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Diffusion potential, Vd = 1.234 V\n" - ] - } - ], - "source": [ - "#Diffusion potential\n", - "from math import log\n", - "#given data :\n", - "Na=5*10**23## in m**-3\n", - "Nd=5*10**21## in m**-3\n", - "T=300## in K\n", - "e=1.6*10**-19## in J\n", - "k=1.38*10**-23## in JK**-1\n", - "V=(k*T)/e#\n", - "ni=2.2*10**12## in m**-3\n", - "Vd=V*log((Na*Nd)/ni**2)#\n", - "print \"Diffusion potential, Vd = %0.3f V\"%Vd" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.3: Page 161" - ] - }, - { - "cell_type": "code", - "execution_count": 3, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Injection efficiency, eta_inj = 0.8247\n" - ] - } - ], - "source": [ - "#Injection efficiency\n", - "#given data :\n", - "Na=10**23## in m**-3\n", - "Nd=10**21## in m**-3\n", - "T=300## in K\n", - "e=1.6*10**-19## in J\n", - "k=1.38*10**-23## in JK**-1\n", - "mue=0.85## in m**2V**-1s**-1\n", - "muh=0.04## in m**2V**-1s**-1\n", - "De=(mue*k*T)/e## in m**2s**-1\n", - "Dh=(muh*k*T)/e## in m**2s**-1\n", - "Le=1#\n", - "Lh=Le#\n", - "eta_inj=1/(1+((De/Dh)*(Lh/Le)*(Nd/Na)))#\n", - "print \"Injection efficiency, eta_inj = %0.4f\"%eta_inj" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.4: Page 171" - ] - }, - { - "cell_type": "code", - "execution_count": 4, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "part (a)\n", - "Internal quantum efficiency = 0.50\n", - "part (b)\n", - "External quantum efficiency = 0.0337\n" - ] - } - ], - "source": [ - "#Internal and quantum efficiency\n", - "#given data :\n", - "print \"part (a)\"\n", - "tau_rr=1#\n", - "tau_nr=tau_rr#\n", - "eta_int=1/(1+(tau_rr/tau_nr))#\n", - "print \"Internal quantum efficiency = %0.2f\"%eta_int\n", - "print \"part (b)\"\n", - "ns=3.7#\n", - "na=1.5#\n", - "As=0#\n", - "eta_ext=eta_int*(1-As)*((2*na**3)/(ns*(ns+na)**2))#\n", - "print \"External quantum efficiency = %0.4f\"%eta_ext" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.5: Page 180" - ] - }, - { - "cell_type": "code", - "execution_count": 5, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "The number of longitudinal modes excited = 1.001e-03 nm\n" - ] - } - ], - "source": [ - "#The number of longitudinal modes excited\n", - "#given data :\n", - "lamda=632.8*10**-9## in m\n", - "n=1#\n", - "L=20*10**-2## in m\n", - "del_lamda=((lamda)**2/(2*n*L))*10**9#\n", - "print \"The number of longitudinal modes excited = %0.3e nm\"%del_lamda" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.6: Page 183" - ] - }, - { - "cell_type": "code", - "execution_count": 6, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "part (a)\n", - "The reduction in threshold gain = 1.31 mm**-1\n", - "part (b)\n", - "Differential quantum efficiency = 0.42\n" - ] - } - ], - "source": [ - "#The reduction and Differential quantum efficiency\n", - "#given data :\n", - "print \"part (a)\"\n", - "alfa_eff=1.5## in mm**-1\n", - "gama=0.8#\n", - "L=0.5## in mm\n", - "R1=0.35#\n", - "R2=R1#\n", - "R2a=1.0#\n", - "g_th1=(1/gama)*(alfa_eff+(1/(2*L))*log(1/(R1*R2)))#\n", - "g_th2=(1/gama)*(alfa_eff+(1/(2*L))*log(1/(R1*R2a)))#\n", - "del_gth=g_th1-g_th2#\n", - "print \"The reduction in threshold gain = %0.2f mm**-1\"%del_gth\n", - "print \"part (b)\"\n", - "eta_D=(gama*(g_th2-alfa_eff))/(g_th2)#\n", - "print \"Differential quantum efficiency = %0.2f\"%eta_D" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 7.7: Page 192" - ] - }, - { - "cell_type": "code", - "execution_count": 7, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "part (a)\n", - "The internal power efficiency = 0.48\n", - "part (b)\n", - "The external power efficiency = 0.012\n", - "part (c)\n", - "The overall source fiber power coupling efficiency = 8.51e-04\n", - "The optical loss = 30.70 dB\n" - ] - } - ], - "source": [ - "from math import log10\n", - "#Internal and external power efficiency\n", - "#given data :\n", - "print \"part (a)\"\n", - "As=0##\n", - "ns=3.7## assuming that the example 7.4\n", - "eta_int=0.50## internal efficiency\n", - "V=1.5## in V\n", - "I=120*10**-3## in A\n", - "IBYe=120*10**-3## \n", - "Eph=1.43## in eV\n", - "eta_int=0.50## internal efficiency\n", - "fi_int=eta_int*IBYe*Eph#\n", - "t_power=I*V#\n", - "P_int=fi_int/t_power#\n", - "print \"The internal power efficiency = %0.2f\"%P_int\n", - "print \"part (b)\"\n", - "eta_ext=eta_int*(1-As)*2/(ns*(ns+1)**2)#\n", - "fi_ext=eta_ext*IBYe*Eph#\n", - "t_power=I*V#\n", - "P_ext=fi_ext/t_power#\n", - "print \"The external power efficiency = %0.3f\"%P_ext\n", - "print \"part (c)\"\n", - "V=1.5## in V\n", - "I=120*10**-3## in A\n", - "IBYe=120*10**-3## \n", - "Eph=1.43## in eV\n", - "n1=1.5#\n", - "n2=1.48#\n", - "na=n1#\n", - "eta_ext=0.0337#\n", - "eta_T=eta_ext*((n1**2-n2**2)/na**2)#\n", - "fi_T=eta_T*IBYe*Eph#\n", - "t_power=I*V#\n", - "sfpc=fi_T/t_power#\n", - "O_loss=-10*log10(sfpc)#\n", - "print \"The overall source fiber power coupling efficiency = %0.2e\"%sfpc\n", - "print \"The optical loss = %0.2f dB\"%O_loss" - ] - } - ], - "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 -} |