Cutoff_energy.ipynb
17.6 KB
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{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Beware this code take time to run!"
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {
"collapsed": false,
"scrolled": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"[ 0.01 0.01217357 0.01481958 0.01804072 0.021962 0.0267356\n",
" 0.03254677 0.03962104 0.04823295 0.05871672 0.07147921 0.08701572\n",
" 0.1059292 0.12895366 0.15698264 0.19110393 0.23264171 0.28320803\n",
" 0.34476529 0.41970246 0.51092774 0.62198149 0.75717355 0.92175056\n",
" 1.12209954 1.36599578 1.66290459 2.02434862 2.46435506 3. ] [ 19199.20665593 17508.27031736 15966.26022101 14426.43951218\n",
" 12796.96868216 10940.54707206 8932.04599858 6836.51600451\n",
" 4771.76094894 2954.40799888 1607.70442167 1091.53593533\n",
" 835.45280584 675.81811682 562.01738481 471.70846909\n",
" 399.57803019 338.47728559 284.08836902 234.08272762\n",
" 182.49932448 161.88596902 139.6835118 117.23818033\n",
" 102.09606623 94.83681866 87.28526624 82.58799388\n",
" 92.24970053 102.09606623]\n"
]
}
],
"source": [
"from modules.analytic import distance, lambda_gg\n",
"from numpy import logspace, log10, shape, zeros, nditer\n",
"\n",
"z_tab=logspace(-2,log10(3),num=30)\n",
"E_save=zeros(shape(z_tab)[0])\n",
"it=nditer(E_save, op_flags=['writeonly'])\n",
"\n",
"for z in z_tab:\n",
" diff_save=1e5\n",
" for E in logspace(1,5,num=1000):\n",
" diff = abs(lambda_gg(E,z)[0]-distance(z)[1]) \n",
" if diff < diff_save:\n",
" it[0] = E\n",
" diff_save = diff\n",
" it.iternext()\n",
" \n",
"print z_tab, E_save "
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"[ 1.91992047e+04 -1.00002070e+00]\n"
]
}
],
"source": [
"from numpy.random import normal\n",
"from scipy.optimize import curve_fit\n",
"\n",
"def Ecut(z,E0,alpha):\n",
" return E0*(z/1e-2)**alpha\n",
"\n",
"E_approx=Ecut(z_tab,E_save[0],-1) + 0.2 * normal(size=len(z_tab))\n",
"\n",
"param, pcov = curve_fit(Ecut, z_tab, E_approx)\n",
"\n",
"print param"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {
"collapsed": false,
"scrolled": false
},
"outputs": [
{
"data": {
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bvNHB5kDb+IokIuXWtSuceSa88AI8+2yYQtGvH5xwQmiBxNbD26nTl5PjffqE\nIV8KHJkUZeLeKcClwP2E5UEGAle5+73xF6/JMimHIVKiJUtCruOmm8L+HOefHwJIuzi3R6uvD1sQ\n/uu/wjAtep20RCbumdmuQH/AgSnuPrPYB5aDAoZI+axeDZMnw403hq6r884L6w5utlnaJZNyS2Ti\nnru/6e63uvvouIOFmR1rZmPMbKKZHRbnsyQdymFUlrZtw/pVzz0X5nhMmwY9esDw4fD221++Nta6\nW7VKXVUVrqCZ3klw94fd/UzCJk3fS7s8ItVk773ht78NKYcOHWC//WD//WH0aPjgg5gfPm2a9uOo\ncIkEDDMba2YLzeyN9c4PMLPZZjbXzC5e72M/A0YnUT5JlhYerHw1NXDttfDee2FTp7/8BXr1gmuu\nqeXee+Gzz2J4aL9+MH16SK4ocFSkRCbumdmBwBLgXnffPX+uLTAH+HfgPeBlYBAwm7AHx5Pu/kwT\n91MOQyRhy5bBI4+EYbq5XNivY/DgMOO8Y8cyP6zxRk5TpsAee5T5AdUp0dVqS2Fm3YFHGgWM/YCR\n7j4gf9yw+u1S4FRCAJnu7r/awL0UMDJMy5tnV0PdffxxyHeMHx+6r/bZJ6wM0vDq2TPkRkq2YEGY\nrl6Wm60zf36IQ1OmhD8//3xZb1+xSg0YcQ6ga8l2QH2j4wXAPu5+LnBrSx8eMmQI3fObA3Tt2pW+\nffuu/RJqSMzpuDKPp0+fXlHl0XFxx0OH1jJ0KDz0UI7Zs2H16lruvx+GD8/xySfQt28tffvCRhvl\n6NkThgyppXPnAp/XrVtZyvvRR7BiRS1TpsCjj+b44gsYMKCW/v1D+XK59P894zjO5XKMGzcOYO33\nZSnSbGGcAAxw96H545NZFzBaupdaGCIV7NNP4fXXQ0qi4TVrFuy0U0hVNLx23bXIeR+33x6aBk3s\nx/Hpp6H18PTT4b8LF4Y90vv3D6+dd67O/Z+y3MJ4D6hpdFxDaGWISMZttlnYr+PAA9edW7EiBJGX\nXgpdQDfeGFIVe+755SDSvXuEL/Ojjgo5jt69YehQ1px/ITPe34rHH4fHHw8DrvbfPyyNcvrpIQVS\n5l6tqpRmC6MdIel9KPA+8BIwyN1nRbiXjxw5ktra2rXNMMmOnHIYmVXuuvv0U3jllRBEGl6LFoUN\nonr2/OqrWzdokx/b+dFH8KeJ9Ww8+hr2emsCD35tKLMGX8nh327PQQdB585lK2bm5XI5crkco0aN\nqvykt5lBPVGXAAAHOUlEQVRNAA4GtgA+AC5397vN7D+AmwlrU/2vu18d8X7qksowBYzsSqLuFi8O\nEwbnzfvq65//DJMKO3UK1xxyCAwYAEfuXs/2f74PLrigOvuaIsrMKKlyUsAQqU7LloVVdj/7LEwy\n7NAh7RJlS5ZzGCWpq6tTl5RIlencGXbbrcAPPfZYiC4bSI5Xi4YuqVKphSGJU5dUdmWy7i66CO66\nC4YObXJUVbVIZPFBEZHMuu66MLtwyRJt5FSizLYwNEpKRArWsORIw2YgVSJTo6TKTV1SIlIS96oc\nTaUuKcmcciTfJB2tpu6qMFiUgwKGiIhEktmAUVdX13p+26kyyjtll+oum3K5HHV1dSXfRzkMEZEq\noRyGZI5ahtmluqtuChgiIhJJZgOGchjZpX7w7FLdZZNyGBkst4hImpTDkMxRyzC7VHfVTQFDREQi\nUZeUiEiVqNouKSW9RUSiUdI7g+WWIJN7Kgigusu6qm1hiIhIstTCEBGpEmphiIhIIhQwJHEarJBd\nqrvqpoAhIiKRZDZgaFhtdmmUTXap7rJJw2ozWG4RkTQp6S2Zo5ZhdqnuqpsChoiIRKIuKRGRKqEu\nKRERSYQChiRO/eDZpbqrbgoYIiISiXIYIiJVQjkMERFJRGYDhmZ6Z5fqLbtUd9mkmd4ZLLcE2oQn\nu1R32VZql5QChohIlVAOQ0REEqGAIYlTP3h2qe6qmwKGiIhEohyGiEiVUA5DREQSoYAhiVM/eHap\n7qqbAoaIiESiHIaISJVQDkNERBJRUQHDzHqY2V1m9kDaZZH4qB88u1R31a2iAoa7v+vuZ6RdDonX\n9OnT0y6CFEl1V91iDxhmNtbMFprZG+udH2Bms81srpldHHc5pHIsWrQo7SJIkVR31S2JFsbdwIDG\nJ8ysLTA6f34XYJCZ7ZxAWcqqnM3zYu9VyOeiXNvcNYW+V8ndF+UuWyXUX7HvF3q+Euhnr+X34qi/\n2AOGu08FPlnvdD9gnrvPd/eVwETgWDPb3MzuAPpmodWh/2mbf6+p6+fPn99iOeKmgFHc+UqoO9DP\nXpT34ggYiQyrNbPuwCPuvnv++LvAEe4+NH98MrCPu58b8X4aUysiUoRShtW2K2dBClDSF34pf2ER\nESlOWqOk3gNqGh3XAAtSKouIiESQVsB4BdjJzLqbWQfge8CklMoiIiIRJDGsdgLwAtDLzOrN7DR3\nXwWcAzwBzATuc/dZcZdFRESKl8m1pEREJHkVNdNbREQqV6sJGGZ2rJmNMbOJZnZY2uWRwmgdsWwy\ns43N7J78z97gtMsj0RXzM9fquqTMrCtwvdakyiYze8DdB6ZdDonGzH4AfOzuj5rZRHc/Ke0ySWEK\n+ZmruBZGGdae+hlh2RFJgdYOy74C63A7oD7/59WJFlS+Iu6fv4oLGBSw9pSZ/cDMbjKzb1hwLfCY\nu2tJzfQUVX8plFOaVsj6bwtYN6eqEr9Pqk2sa/dVXAUXsvaUu//a3Ye7+/vAucChwHfN7KxkSy0N\niq2/rK0j1poVUofAQ8AJZnYbmkuVurjX7ktraZBCNW72QvitZp/GF7j7LcAtSRZKIotSfx8Dw5Is\nlBRkg3Xo7suAH6ZTJImoqbor+Geu4loYTWhdmfnqo/rLPtVhdpWt7rISMLT2VLap/rJPdZhdZau7\nrAQMrT2Vbaq/7FMdZlfZ6q7iAobWnso21V/2qQ6zK+66a3UT90REJB4V18IQEZHKpIAhIiKRKGCI\niEgkChgiIhKJAoaIiESigCEiIpEoYIiISCQKGCJFMrM6M7ugmPfN7E+N/vwLM/urmV1nZqea2dfj\nKK9IqbKyWq1IYszMALzlWa1Fv+/u32p0OBT4mru7mT0L/BX4e5SyiiRJLQwRIL/Ozhwzuwd4A7jM\nzF4ysxlmVtfoukvz100Fejc6f56ZvZm/fnyjW+9iZs+a2dtmdm6j65fk/zsJ6AJMM7MTgb2B35rZ\nNDPrFOtfWqRAamGIrNMT+AGwGfBdd+9nZm2Ah83sQGAZYeG2PYD2wDTCwm4AFwPd3X2lmW2aP2dA\nH6AW2BSYY2a3uftq8q0Pdz/GzBa7+54AZnY2cIG7T4v/rytSGLUwRNb5m7u/BBwBHG5mrwGvEloS\nOwEHAA+5+3J3X8yXV/x8HRhvZt9n3d7WDkx295Xu/k/gA2CbCOWw8vx1RMpLAUNknaWN/ny1u++Z\nf/Vy97H5842/zK3R8beB/wG+Cbyc30cZ4ItG168mWqteK4JKRVLAEPmqJ4AfmtnGAGa2nZltBfwf\ncJyZdTKzTYCjAM8nybd39xxwCaFLqwvFtRQWE7qvRCqOchgi6zTkFZ4ys52BP+cHTC0GTnb318zs\nPmAGoXvppfzn2gK/NrPNCEHil+7+qZk5TbcWvIk/jwPuMLNlwP7uvrw8fzWR0mk/DBERiURdUiIi\nEokChoiIRKKAISIikShgiIhIJAoYIiISiQKGiIhEooAhIiKR/H8KlBdMSMD06wAAAABJRU5ErkJg\ngg==\n",
"text/plain": [
"<matplotlib.figure.Figure at 0x7f6ae6708150>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"from matplotlib.pyplot import figure, show\n",
"%matplotlib inline\n",
"fig = figure() \n",
"ax1 = fig.add_subplot(111)\n",
"ax1.plot(z_tab,E_save,drawstyle='-')\n",
"ax1.plot(z_tab,Ecut(z_tab,param[0],param[1]),\"r--\")\n",
"ax1.set_xscale('log') \n",
"ax1.set_yscale('log')\n",
"ax1.grid(b=True,which='major')\n",
"ax1.set_xlabel(\"redshift\")\n",
"ax1.set_ylabel(\"cutoff energy [GeV]\")\n",
"show()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"$$E_{cut}(z) \\simeq 2.10^4 \\left(\\frac{z}{10^{-2}}\\right)^{-1} \\textrm{ GeV}$$ \n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": []
}
],
"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": "2.7.10"
}
},
"nbformat": 4,
"nbformat_minor": 0
}