{ "metadata": { "name": "", "signature": "sha256:a64f8a075a2d5dd425c32cb6c1ff132f9bd11e79217b7f0abfb1af46a904ad28" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Reproduce: Gr\u00f6blacher et. al., Nature 460, 724 (2009)." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Reproduced by: Eunjong Kim (ekim7206@gmail.com)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "In this notebook, I find the expression for the normal mode splitting of optomechanical system, following the supplementary information of [Gr\u00f6blacher et. al., Nature 460, 724 (2009).]" ] }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Setup Modules" ] }, { "cell_type": "code", "collapsed": false, "input": [ "from sympy import *\n", "init_printing(use_latex='png')" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 1 }, { "cell_type": "code", "collapsed": false, "input": [ "from sympsi.operator import Operator\n", "from sympsi.boson import BosonOp\n", "from sympsi.dagger import Dagger" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 2 }, { "cell_type": "code", "collapsed": false, "input": [ "# Constants\n", "d = symbols(\"Delta\", real=True) # detuning\n", "hbar, g, O, wp, wm = symbols(\"hbar, g, Omega, omega_+, omega_-\", positive=True)" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 3 }, { "cell_type": "markdown", "metadata": {}, "source": [ "The linearized Hamiltonian for a driven cavity mode coupled via radiation pressure to a harmonically bound mirror is\n", "\n", "$$\n", "H = -\\frac{\\hbar\\Delta}{2} (X_c^2 + P_c^2 ) + \\frac{\\hbar\\Omega}{2} (X_m^2 + P_m^2 ) - \\hbar g X_c X_m\n", "$$\n", "\n", "where $\\Omega$ is the frequency of the mechanical resonator, $\\Delta\\equiv \\omega_L - (\\omega_c-\\delta_{rp})$ is the effective detuning between the driving field and the cavity frequency$.($\\delta_{rp}$ is the mean shift of the cavity frequency arising from radiation frequency.)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "This can either be expressed in terms of the matrix equation with vector $\\vec{R}\\equiv [X_c,\\ P_c,\\ X_m,\\ P_m]^T$:\n", "\n", "$$\n", "H =\\frac{\\hbar}{2} \\vec{R}^T M \\vec{R}\n", "$$\n", "where $M$ is the matrix defined as" ] }, { "cell_type": "code", "collapsed": false, "input": [ "M = Matrix([[-d, 0, -g, 0],\n", " [0, -d, 0, 0],\n", " [-g, 0, O, 0],\n", " [0, 0, 0, O]])\n", "M" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAAALsAAABkCAMAAADpJrGiAAAAP1BMVEX///8AAAAAAAAAAAAAAAAA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\n", "prompt_number": 4, "text": [ "\u23a1-\u0394 0 -g 0\u23a4\n", "\u23a2 \u23a5\n", "\u23a20 -\u0394 0 0\u23a5\n", "\u23a2 \u23a5\n", "\u23a2-g 0 \u03a9 0\u23a5\n", "\u23a2 \u23a5\n", "\u23a30 0 0 \u03a9\u23a6" ] } ], "prompt_number": 4 }, { "cell_type": "code", "collapsed": false, "input": [ "# Operators\n", "Xc, Xm = Operator('X_c'), Operator('X_m') # Position Quadratures\n", "Pc, Pm = Operator('P_c'), Operator('P_m') # Momentum Quadratures\n", "ac, am = BosonOp('a_c'), BosonOp('a_m') # Boson Operators" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 5 }, { "cell_type": "markdown", "metadata": {}, "source": [ "The quadrature operators are related to the annihilation and creation operators by the following linear equation:\n", "$$ \\vec{R} = Q \\vec{a}$$\n", "where $\\vec{a} \\equiv [a_c,\\ a^\\dagger_c,\\ a_m,\\ a^\\dagger_m]^T$, and $Q$ is the coefficient matrix" ] }, { "cell_type": "code", "collapsed": false, "input": [ "R = Matrix([Xc, Pc, Xm, Pm])\n", "a = Matrix([ac, Dagger(ac), am, Dagger(am)])\n", "Q = Matrix([[1, 1, 0, 0],\n", " [-I, I, 0, 0],\n", " [0, 0, 1, 1],\n", " [0, 0, -I, I]])/sqrt(2)\n", "Eq(R, MatMul(Q, a))" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 6, "text": [ " \u23a1 ___ ___ \u23a4 \n", " \u23a2 \u2572\u2571 2 \u2572\u2571 2 \u23a5 \n", "\u23a1X_c\u23a4 = \u23a2 \u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500 0 0 \u23a5\u22c5\u23a1a_c \u23a4\n", "\u23a2 \u23a5 \u23a2 2 2 \u23a5 \u23a2 \u23a5\n", "\u23a2P_c\u23a5 \u23a2 \u23a5 \u23a2 \u2020\u23a5\n", "\u23a2 \u23a5 \u23a2 ___ ___ \u23a5 \u23a2a_c \u23a5\n", "\u23a2X_m\u23a5 \u23a2-\u2572\u2571 2 \u22c5\u2148 \u2572\u2571 2 \u22c5\u2148 \u23a5 \u23a2 \u23a5\n", "\u23a2 \u23a5 \u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 0 \u23a5 \u23a2a_m \u23a5\n", "\u23a3P_m\u23a6 \u23a2 2 2 \u23a5 \u23a2 \u23a5\n", " \u23a2 \u23a5 \u23a2 \u2020\u23a5\n", " \u23a2 ___ ___ \u23a5 \u23a3a_m \u23a6\n", " \u23a2 \u2572\u2571 2 \u2572\u2571 2 \u23a5 \n", " \u23a2 0 0 \u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500 \u23a5 \n", " \u23a2 2 2 \u23a5 \n", " \u23a2 \u23a5 \n", " \u23a2 ___ ___ \u23a5 \n", " \u23a2 -\u2572\u2571 2 \u22c5\u2148 \u2572\u2571 2 \u22c5\u2148\u23a5 \n", " \u23a2 0 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5 \n", " \u23a3 2 2 \u23a6 " ] } ], "prompt_number": 6 }, { "cell_type": "markdown", "metadata": {}, "source": [ "i.e., $$X_{\\alpha} = \\frac{a_{\\alpha}+a^\\dagger_{\\alpha}}{\\sqrt{2}},\\quad P_{\\alpha} = -i\\frac{a_{\\alpha}-a^\\dagger_{\\alpha}}{\\sqrt{2}}\\quad (\\alpha = c, m)$$" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The quadratures satisfy the canonical commutation relations $$[X_\\alpha, P_\\beta] = i \\delta_{\\alpha, \\beta},\\quad [X_\\alpha, X_\\beta] = [P_\\alpha, P_\\beta] = 0.$$\n", "which are condensed into one simple equation\n", "$$\n", "[\\vec{R}_{i}, \\vec{R}_{j}] = i J_{ij}\n", "$$\n", "where $J$ is the matrix defined as" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# Constraint representative of the canonical commutation relation\n", "J = Matrix([[0, 1, 0, 0],\n", " [-1, 0, 0, 0],\n", " [0, 0, 0, 1],\n", " [0, 0, -1, 0]])\n", "J" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAAAJgAAABkCAMAAABNTAlxAAAAP1BMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAADFBd4eAAAAFHRS\nTlMAMquZdlQQQO0wRInN3SJm77t8bMVussMAAAAJcEhZcwAADsQAAA7EAZUrDhsAAAN1SURBVGgF\n7ZvrlqIwEISjIM6oeNnN+z/rcjmBdNNJKg0zyp74h5hTVL4tIlrraA52eBzNhzzakceYg63q7nH6\nEC7z6GmOtgc7fArTzPEQwZrqWlcQ7a2ZvUIj0I3KZLBbd1mb9h5aaZq/vywABrpRmQj2ePZLX28T\ngDxoXtURAAPdmEwEew0v0BOwaA1oQDcmE8HsAHax6dcpAga6MZkE1tiqv3YXW8uX0JsFwEA3LpPA\n7vbar30YDx7GcgiAgW5ctiuwZoxqs0s55J9y44tKiZlxj5222vzDjk26sUVFsPbV76YHcCsA9pgB\n3ZhMBKuHG2yVusF28AgY6MZkIphp+7ekJ/BmiYChbnRRGay5dp870lzV8Wnb42N5F6EzoBuVyWDU\n+C3PClhu7CWxklhuArn6ssdKYrkJ5OqTeyzWaGlFDS6tkiXA4o2WVtQgmEoWBUs0WlZRQ2A6WRSs\nWyr2gYtV1BCYTrYGjFXUEJhOtgKMV9QAmFK2AoxX1ACYUrYPsObWTo/b+JE/svl5RQ0kppT1iZ3t\nOWAaf1Wyihry0Mn+iP/VOa8RSUzZZGdvOkIKr3dGDIxVVO8sMtTJVmx+o2uyBNp/ghRep080WlpR\n3UmLo0qWSmyxym9NFLDcpEtiJbHcBHL1/R5rauCbqlzjtfp79+3Hjr6vXPvP3eD8nd0uVBU1GBPo\n1p3vtWs5MVVFDYKBboa0axFMV1FDYKAba9cimK6ihsBAt+50/1OpCKarqCEw0A0AU1bUABjo1p+d\nSkxZUQNgoNuuwZQVNZAY6CYldv76pqa6iko95megW3eCv8f+fglv4qx7zmvQ0bYyBibeLnQVlVLP\nz0A3BOxHm+xMvBj5l1JMzKgq6mIdNwG60XYtgznLNx4LWG74JbGSWG4Cufqyx0piuQnk6uU9BlZU\nUOYxeY3Wmx2H1E0GAysqKJsQSKOdZt2AuolgYEUFZW5h1mjdtDsyNxEMrKigzK3cHf0PXN70MGRu\nIhhYUUGZRxADY24SGFhRQZnHFUuMu0lgYEUFZSAYd9sVGFhRU7J13xdLiaF/0ow3WXc5o5uf/uWz\nCLZ5k0XA2KIiGFhRQZmj6o6xxJibCLZx4Z3JYmBsURkMrKigzIHRRutmpyN1k8Em8fsGBSw3+5LY\nf5bYh/4itel/AVrXl9y0f0o//CK1rs0/v51EehgG0m0AAAAASUVORK5CYII=\n", "prompt_number": 7, "text": [ "\u23a10 1 0 0\u23a4\n", "\u23a2 \u23a5\n", "\u23a2-1 0 0 0\u23a5\n", "\u23a2 \u23a5\n", "\u23a20 0 0 1\u23a5\n", "\u23a2 \u23a5\n", "\u23a30 0 -1 0\u23a6" ] } ], "prompt_number": 7 }, { "cell_type": "markdown", "metadata": {}, "source": [ "Note that the matrix $J$ has simple properties: $\\quad J^T = J^{-1} = -J, \\quad J^2=-I$." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Our goal is to find a linear transformation $S$ that converts the original coordinates $\\vec{R}$ into the normal mode coordinates $\\vec{R}^{NM} = [X_+, P_+, X_-, P_-]^T = S\\vec{R}$, whose Hamiltonian representation is\n", "$$ H = \\frac{\\hbar\\omega_+}{2} \\left( X_+^2 + P_+^2 \\right) + \\frac{\\hbar \\omega_-}{2} \\left( X_-^2 + P_-^2\\right) $$" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# Operators in the normal mode coordinates\n", "X_p, X_m = Operator('X_+'), Operator('X_-') # Position Quadratures\n", "P_p, P_m = Operator('P_+'), Operator('P_-') # Momentum Quadratures\n", "a_p, a_m = BosonOp('a_+'), BosonOp('a_-') # Boson Operators" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 8 }, { "cell_type": "code", "collapsed": false, "input": [ "Rnm = Matrix([X_p, P_p, X_m, P_m])\n", "anm = Matrix([a_p, Dagger(a_p), a_m, Dagger(a_m)])\n", "Eq(Rnm, MatMul(Q, anm))" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 9, "text": [ " \u23a1 ___ ___ \u23a4 \n", " \u23a2 \u2572\u2571 2 \u2572\u2571 2 \u23a5 \n", "\u23a1X\u208a\u23a4 = \u23a2 \u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500 0 0 \u23a5\u22c5\u23a1a\u208a \u23a4\n", "\u23a2 \u23a5 \u23a2 2 2 \u23a5 \u23a2 \u23a5\n", "\u23a2P\u208a\u23a5 \u23a2 \u23a5 \u23a2 \u2020\u23a5\n", "\u23a2 \u23a5 \u23a2 ___ ___ \u23a5 \u23a2a\u208a \u23a5\n", "\u23a2X\u208b\u23a5 \u23a2-\u2572\u2571 2 \u22c5\u2148 \u2572\u2571 2 \u22c5\u2148 \u23a5 \u23a2 \u23a5\n", "\u23a2 \u23a5 \u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 0 \u23a5 \u23a2a\u208b \u23a5\n", "\u23a3P\u208b\u23a6 \u23a2 2 2 \u23a5 \u23a2 \u23a5\n", " \u23a2 \u23a5 \u23a2 \u2020\u23a5\n", " \u23a2 ___ ___ \u23a5 \u23a3a\u208b \u23a6\n", " \u23a2 \u2572\u2571 2 \u2572\u2571 2 \u23a5 \n", " \u23a2 0 0 \u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500 \u23a5 \n", " \u23a2 2 2 \u23a5 \n", " \u23a2 \u23a5 \n", " \u23a2 ___ ___ \u23a5 \n", " \u23a2 -\u2572\u2571 2 \u22c5\u2148 \u2572\u2571 2 \u22c5\u2148\u23a5 \n", " \u23a2 0 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5 \n", " \u23a3 2 2 \u23a6 " ] } ], "prompt_number": 9 }, { "cell_type": "markdown", "metadata": {}, "source": [ "This can either be expressed in terms of the matrix equation with vector $\\vec{R}^{NM}$:\n", "\n", "$$\n", "H = \\frac{\\hbar}{2} \\left(\\vec{R}^{NM}\\right)^T D \\vec{R}^{NM}\n", "= \\frac{\\hbar}{2} \\left(S\\vec{R}\\right)^T D \\left(S\\vec{R}\\right)\n", "= \\frac{\\hbar}{2} \\vec{R}^T \\left(S^T D S\\right)\\vec{R}\n", "$$\n", "where $D$ is the diagonal matrix defined as" ] }, { "cell_type": "code", "collapsed": false, "input": [ "D = diag(wp, wp, wm, wm)\n", "D" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 10, "text": [ "\u23a1\u03c9\u208a 0 0 0 \u23a4\n", "\u23a2 \u23a5\n", "\u23a20 \u03c9\u208a 0 0 \u23a5\n", "\u23a2 \u23a5\n", "\u23a20 0 \u03c9\u208b 0 \u23a5\n", "\u23a2 \u23a5\n", "\u23a30 0 0 \u03c9\u208b\u23a6" ] } ], "prompt_number": 10 }, { "cell_type": "markdown", "metadata": {}, "source": [ "1) Comparing with the matrix representation of Hamiltonian in the original coordinates, it follows that $M = S^T D S$.\n", "\n", "(NOTE: This transformation betweeen $M$ and $D$ is not in general a similarity transformation, so that $M$ and $D$ doesn't need not share a same set of eigenvalues.)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "2) In addition to this condition, the transformation matrix $S$ is subject to the cannonical commutation relations between quadratures of the normal mode coordinates, which gives another constraint on $S$ :\n", "\n", "\\begin{align}\n", "iJ_{ij} = \\left[\\vec{R}^{NM}_{i}, \\vec{R}^{NM}_{j}\\right] = \\left[\\sum_{k} S_{ik} \\vec{R}_{k}, \\sum_{l} S_{jl} \\vec{R}_{l}\\right] = \\sum_{k, l} S_{ik} \\left[ \\vec{R}_{k}, \\vec{R}_{l}\\right] (S^T)_{lj} = i \\sum_{k, l} S_{ik} J_{kl} (S^T)_{lj} = i(SJS^T)_{ij} \\quad\\Rightarrow\\quad J=SJS^T\n", "\\end{align}" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The latter property, which guarantees that the canonical commutation relations are conserved under the transformation, are often termed as a symplectic transformation." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The conditions 1) and 2) described above themselves doesn't say anything about the normal mode frequencies $\\omega_+,\\ \\omega_-$ or the transformation matrix $S$. But, combining two matrix equations, we can get a meaningful relation useful in getting normal mode frequencies." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "First, we can readily notice that the matrix $S$ should be invertible. This is due to the fact that $\\det{J} = 1$, so the determinant of the rhs of condition 2),\n", "\n", "$$\\det{(SJS^T)} = \\det{S} \\cdot\\det{J}\\cdot \\det{S^T} = \\det{J} (\\det{S})^2$$\n", "\n", "should also be 1. If $\\det{S} = 0$, this cannot be the case. It naturally follows that $|\\det{S}|=1$." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Second, multiplying $J^{-1} S^{-1}$ on the left of the both sides of 2), we get\n", "\n", "$$\n", "J^{-1} S ^{-1}J = -J S ^{-1} J = (-J S^{-1}) SJS^T = -J^2 S^T = S^T.\n", "$$" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Finally, substituting into 1),\n", "\n", "$$\n", "M = S^T D S = (J^{-1} S^{-1} J)DS = J^{-1} S^{-1}(JD) S \\quad \\Rightarrow \\quad JM = S^{-1}(JD) S.\n", "$$\n", "\n", "we find that $JM$ and $JD$ are related by the similarity transformation. As a consequence, the matrices $JD$ and $JM$ share the same set of eigenvalues." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Now, let \n", "$$\n", "A^{-1} (JM) A = B^{-1} (JD) B = \\mathrm{diag}{(\\lambda_1, \\lambda_2, \\lambda_3, \\lambda_4)}.\n", "$$\n", "\n", "(with this definition, $S = BA^{-1}$)." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Extracting the eigenvectors and eigenvalues for two matrices $JM$ and $JD$," ] }, { "cell_type": "code", "collapsed": false, "input": [ "# extracting eigenvectors and eigenvalues for J*M\n", "[(e1,_,[v1]), (e2,_,[v2]), (e3,_,[v3]), (e4,_,[v4])] = (J * M).eigenvects()" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 11 }, { "cell_type": "code", "collapsed": false, "input": [ "e1, e2, e3, e4" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 12, "text": [ "\u239b _______________________________________________ _______________\n", "\u239c \u2571 ______________________________ \u2571 \n", "\u239c \u2571 2 2 \u2571 4 2 2 2 4 \u2571 2 2 \n", "\u239c \u2571 \u0394 \u03a9 \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u2571 \u0394 \u03a9 \u2572\u2571\n", "\u239c- \u2571 - \u2500\u2500 - \u2500\u2500 - \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 , \u2571 - \u2500\u2500 - \u2500\u2500 - \u2500\u2500\n", "\u239d \u2572\u2571 2 2 2 \u2572\u2571 2 2 \n", "\n", "________________________________ _____________________________________\n", " ______________________________ \u2571 _____________________\n", "\u2571 4 2 2 2 4 \u2571 2 2 \u2571 4 2 2 \n", " \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u2571 \u0394 \u03a9 \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 , - \u2571 - \u2500\u2500 - \u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " 2 \u2572\u2571 2 2 2 \n", "\n", "__________ _______________________________________________\u239e\n", "_________ \u2571 ______________________________ \u239f\n", " 2 4 \u2571 2 2 \u2571 4 2 2 2 4 \u239f\n", "\u22c5g + \u03a9 \u2571 \u0394 \u03a9 \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u239f\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 , \u2571 - \u2500\u2500 - \u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u239f\n", " \u2572\u2571 2 2 2 \u23a0" ] } ], "prompt_number": 12 }, { "cell_type": "code", "collapsed": false, "input": [ "# extracting eigenvectors and eigenvalues for J*D\n", "[(f1,_,[w1]), (f2,_,[w2]), (f3,_,[w3]), (f4,_,[w4])] = (J * D).eigenvects()" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 13 }, { "cell_type": "code", "collapsed": false, "input": [ "f1, f2, f3, f4" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAAAQ4AAAAVBAMAAABF+R16AAAAMFBMVEX///8AAAAAAAAAAAAAAAAA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\nAAAAAElFTkSuQmCC\n", "prompt_number": 14, "text": [ "(-\u2148\u22c5\u03c9\u208a, \u2148\u22c5\u03c9\u208a, -\u2148\u22c5\u03c9\u208b, \u2148\u22c5\u03c9\u208b)" ] } ], "prompt_number": 14 }, { "cell_type": "markdown", "metadata": {}, "source": [ "there is a one-to-one correspondence between eigenvalues, which gives us the normal mode frequencies $\\omega_{\\pm}$:" ] }, { "cell_type": "code", "collapsed": false, "input": [ "wpsol = solve(e2-f2, wp)[0]\n", "Eq(wp, wpsol)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 15, "text": [ " _______________________________________________ \n", " \u2571 ______________________________ \n", " ___ \u2571 2 2 \u2571 4 2 2 2 4 \n", " -\u2572\u2571 2 \u22c5\u2148\u22c5\u2572\u2571 - \u0394 - \u03a9 - \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \n", "\u03c9\u208a = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " 2 " ] } ], "prompt_number": 15 }, { "cell_type": "code", "collapsed": false, "input": [ "wmsol = solve(e4-f4, wm)[0]\n", "Eq(wm, wmsol)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAAAgoAAAAvBAMAAABwEf/KAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA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\nOgvsdtfpJAC73S1IFv4G1juMuTc3SfQAAAAASUVORK5CYII=\n", "prompt_number": 16, "text": [ " _______________________________________________ \n", " \u2571 ______________________________ \n", " ___ \u2571 2 2 \u2571 4 2 2 2 4 \n", " -\u2572\u2571 2 \u22c5\u2148\u22c5\u2572\u2571 - \u0394 - \u03a9 + \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \n", "\u03c9\u208b = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " 2 " ] } ], "prompt_number": 16 }, { "cell_type": "code", "collapsed": false, "input": [ "# simpler expression without an imaginary number\n", "wpsol = sqrt((d**2 + O**2 + sqrt((d**2 -O**2)**2 -4*d*O*g**2))/2)\n", "wmsol = sqrt((d**2 + O**2 - sqrt((d**2 -O**2)**2 -4*d*O*g**2))/2)" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 17 }, { "cell_type": "code", "collapsed": false, "input": [ "Eq(wp, wpsol), Eq(wm, wmsol)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 18, "text": [ "\u239b _________________________________________ __________\n", "\u239c \u2571 _________________________ \u2571 \n", "\u239c \u2571 \u2571 2 \u2571 \n", "\u239c \u2571 2 2 \u2571 2 \u239b 2 2\u239e \u2571 2 2 \n", "\u239c \u2571 \u0394 \u03a9 \u2572\u2571 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u239d\u0394 - \u03a9 \u23a0 \u2571 \u0394 \u03a9 \n", "\u239c\u03c9\u208a = \u2571 \u2500\u2500 + \u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 , \u03c9\u208b = \u2571 \u2500\u2500 + \u2500\u2500 -\n", "\u239d \u2572\u2571 2 2 2 \u2572\u2571 2 2 \n", "\n", "_______________________________\u239e\n", " _________________________ \u239f\n", " \u2571 2 \u239f\n", " \u2571 2 \u239b 2 2\u239e \u239f\n", " \u2572\u2571 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u239d\u0394 - \u03a9 \u23a0 \u239f\n", " \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u239f\n", " 2 \u23a0" ] } ], "prompt_number": 18 }, { "cell_type": "markdown", "metadata": {}, "source": [ "Now, try to find the transformation matrix $S$. First construct matrices $A$ and $B$ from the eigenvectors multiplied by arbitrary constants (which will be determined later)" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# arbitrary constants\n", "aa, bb, cc, dd = symbols(\"alpha, beta, gamma, delta\")\n", "x, y, z, w = symbols(\"x, y, z, w\")" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 19 }, { "cell_type": "code", "collapsed": false, "input": [ "ee2, ff2 = simplify(sqrt(2)*e2), sqrt(2)*f2\n", "ee4, ff4 = simplify(sqrt(2)*e4), sqrt(2)*f4\n", "subs_dic = {ee2:ff2, ee2**2+2*d**2:ff2**2+2*d**2, ee4:ff4, ee4**2+2*d**2: ff4**2+2*d**2}\n", "u1, u2, u3, u4 = (v1.subs(subs_dic), v2.subs(subs_dic),\n", " v3.subs(subs_dic), v4.subs(subs_dic))" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 20 }, { "cell_type": "code", "collapsed": false, "input": [ "A = (x*u1).row_join(y*u2).row_join(z*u3).row_join(w*u4)\n", "A = simplify(A)\n", "A" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 21, "text": [ "\u23a1 -\u2148\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5x \u2148\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5y -\u2148\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5z \u2148\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5w \u23a4\n", "\u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5\n", "\u23a2 \u239b 2 2\u239e \u239b 2 2\u239e \u239b 2 2\u239e \u239b 2 2\u239e\u23a5\n", "\u23a2\u03c9\u208a\u22c5\u239d\u0394 - \u03c9\u208a \u23a0 \u03c9\u208a\u22c5\u239d\u0394 - \u03c9\u208a \u23a0 \u03c9\u208b\u22c5\u239d\u0394 - \u03c9\u208b \u23a0 \u03c9\u208b\u22c5\u239d\u0394 - \u03c9\u208b \u23a0\u23a5\n", "\u23a2 \u23a5\n", "\u23a2 \u03a9\u22c5g\u22c5x \u03a9\u22c5g\u22c5y \u03a9\u22c5g\u22c5z \u03a9\u22c5g\u22c5w \u23a5\n", "\u23a2 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u23a5\n", "\u23a2 2 2 2 2 2 2 2 2 \u23a5\n", "\u23a2 \u0394 - \u03c9\u208a \u0394 - \u03c9\u208a \u0394 - \u03c9\u208b \u0394 - \u03c9\u208b \u23a5\n", "\u23a2 \u23a5\n", "\u23a2 \u2148\u22c5\u03a9\u22c5x -\u2148\u22c5\u03a9\u22c5y \u2148\u22c5\u03a9\u22c5z -\u2148\u22c5\u03a9\u22c5w \u23a5\n", "\u23a2 \u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u23a5\n", "\u23a2 \u03c9\u208a \u03c9\u208a \u03c9\u208b \u03c9\u208b \u23a5\n", "\u23a2 \u23a5\n", "\u23a3 x y z w \u23a6" ] } ], "prompt_number": 21 }, { "cell_type": "code", "collapsed": false, "input": [ "B = (aa*w1).row_join(bb*w2).row_join(cc*w3).row_join(dd*w4)\n", "B" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 22, "text": [ "\u23a1\u2148\u22c5\u03b1 -\u2148\u22c5\u03b2 0 0 \u23a4\n", "\u23a2 \u23a5\n", "\u23a2 \u03b1 \u03b2 0 0 \u23a5\n", "\u23a2 \u23a5\n", "\u23a2 0 0 \u2148\u22c5\u03b3 -\u2148\u22c5\u03b4\u23a5\n", "\u23a2 \u23a5\n", "\u23a3 0 0 \u03b3 \u03b4 \u23a6" ] } ], "prompt_number": 22 }, { "cell_type": "markdown", "metadata": {}, "source": [ "and use the relation $S = B A^{-1}$." ] }, { "cell_type": "code", "collapsed": false, "input": [ "Ainv = A.inv()\n", "Ainv = simplify(Ainv)\n", "S = simplify(B * Ainv)\n", "\n", "S = Matrix([[simplify(S[i, j].factor()) for j in range(4)] for i in range(4)])\n", "S" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 23, "text": [ "\u23a1-\u03c9\u208a\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b1\u22c5y + \u03b2\u22c5x) \u2148\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 \n", "\u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", "\u23a2 2\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5x\u22c5y\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5g\u22c5x\u22c5y\u22c5(\u03c9\u208a\n", "\u23a2 \n", "\u23a2\u2148\u22c5\u03c9\u208a\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b1\u22c5y - \u03b2\u22c5x) (\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 -\n", "\u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", "\u23a2 2\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5x\u22c5y\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5g\u22c5x\u22c5y\u22c5(\u03c9\u208a\n", "\u23a2 \n", "\u23a2 \u03c9\u208b\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b4\u22c5z + \u03b3\u22c5w) \u2148\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 \n", "\u23a2 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", "\u23a2 2\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5w\u22c5z\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5g\u22c5w\u22c5z\u22c5(\u03c9\u208a\n", "\u23a2 \n", "\u23a2\u2148\u22c5\u03c9\u208b\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b4\u22c5z - \u03b3\u22c5w) -(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 -\n", "\u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", "\u23a3 2\u22c5\u0394\u22c5\u03a9\u22c5g\u22c5w\u22c5z\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5g\u22c5w\u22c5z\u22c5(\u03c9\u208a\n", "\n", "- \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b1\u22c5y - \u03b2\u22c5x) -\u03c9\u208a\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u03b1\u22c5y + \u03b2\u22c5x) -\u2148\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5x\u22c5y\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5x\u22c5y\u22c5(\u03c9\u208a \n", " \n", " \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b1\u22c5y + \u03b2\u22c5x) \u2148\u22c5\u03c9\u208a\u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u03b1\u22c5y - \u03b2\u22c5x) -(\u0394 - \u03c9\u208a)\u22c5(\u0394 \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5x\u22c5y\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5x\u22c5y\u22c5(\u03c9\u208a \n", " \n", "- \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b4\u22c5z - \u03b3\u22c5w) \u03c9\u208b\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b4\u22c5z + \u03b3\u22c5w) -\u2148\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5w\u22c5z\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5w\u22c5z\u22c5(\u03c9\u208a \n", " \n", " \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b4\u22c5z + \u03b3\u22c5w) \u2148\u22c5\u03c9\u208b\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b)\u22c5(\u03b4\u22c5z - \u03b3\u22c5w) (\u0394 - \u03c9\u208b)\u22c5(\u0394 \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5\u03a9\u22c5w\u22c5z\u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) 2\u22c5w\u22c5z\u22c5(\u03c9\u208a \n", "\n", " + \u03c9\u208a)\u22c5(\u03b1\u22c5y - \u03b2\u22c5x) \u23a4\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5\n", "- \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a5\n", " \u23a5\n", "+ \u03c9\u208a)\u22c5(\u03b1\u22c5y + \u03b2\u22c5x) \u23a5\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u23a5\n", "- \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a5\n", " \u23a5\n", " + \u03c9\u208b)\u22c5(\u03b4\u22c5z - \u03b3\u22c5w) \u23a5\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5\n", "- \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a5\n", " \u23a5\n", "+ \u03c9\u208b)\u22c5(\u03b4\u22c5z + \u03b3\u22c5w) \u23a5\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u23a5\n", "- \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a6" ] } ], "prompt_number": 23 }, { "cell_type": "markdown", "metadata": {}, "source": [ "The aritrary constants can be determined by the condition 2), $J = SJS^T$. Calculating $SJS^T$, we get " ] }, { "cell_type": "code", "collapsed": false, "input": [ "SJST = simplify(S * J * S.T)\n", "SJST = Matrix([[simplify(SJST[i,j].subs({wp:wpsol, wm:wmsol}).factor()) for j in range(4)] for i in range(4)])" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 24 }, { "cell_type": "markdown", "metadata": {}, "source": [ "The non-vanishing terms are (0, 1), (1, 0), (2, 3), (3, 2)-th elements and should be set to be equal to" ] }, { "cell_type": "code", "collapsed": false, "input": [ "Eq(1, simplify(SJST[0, 1].subs(subs_dic).factor()))" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAABYIAAABBBAMAAACeBs2WAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA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\nBJUAAAAASUVORK5CYII=\n", "prompt_number": 25, "text": [ " _____________________________________________ \n", " \u2571 ______________________________ \u239b \n", " ___ \u2571 2 2 \u2571 4 2 2 2 4 \u239c 4 2 2 \n", " \u2572\u2571 2 \u22c5\u03b1\u22c5\u03b2\u22c5\u2572\u2571 \u0394 + \u03a9 + \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u22c5\u239d\u0394 - 2\u22c5\u0394 \u22c5\u03a9 \n", "1 = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \u239b\n", " 4\u22c5\u03a9\u22c5x\u22c5y\u22c5\u239d\n", "\n", " \n", " ______________________________ _______________\n", " 2 \u2571 4 2 2 2 4 2 4 2 \u2571 4 2 2 \n", "- \u0394 \u22c5\u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 + \u03a9 \u22c5\u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 -\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " 4 2 2 2 4\u239e \n", "\u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u23a0 \n", "\n", " \n", "_______________\u239e\n", " 2 4 \u239f\n", " 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u23a0\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \n", " " ] } ], "prompt_number": 25 }, { "cell_type": "code", "collapsed": false, "input": [ "Eq(1, simplify(SJST[2, 3].subs(subs_dic).factor()))" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAABX4AAABBBAMAAACUdqGBAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA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\nksqXZyW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"prompt_number": 26, "text": [ " _____________________________________________ \n", " \u2571 ______________________________ \u239b \n", " ___ \u2571 2 2 \u2571 4 2 2 2 4 \u239c 4 2 2 \n", " \u2572\u2571 2 \u22c5\u03b4\u22c5\u03b3\u22c5\u2572\u2571 \u0394 + \u03a9 - \u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u22c5\u239d\u0394 - 2\u22c5\u0394 \u22c5\u03a9 \n", "1 = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \u239b\n", " 4\u22c5\u03a9\u22c5w\u22c5z\u22c5\u239d\n", "\n", " \n", " ______________________________ _______________\n", " 2 \u2571 4 2 2 2 4 2 4 2 \u2571 4 2 2 \n", "+ \u0394 \u22c5\u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 - \u03a9 \u22c5\u2572\u2571 \u0394 - 2\u22c5\u0394 \u22c5\u03a9 -\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " 4 2 2 2 4\u239e \n", "\u0394 - 2\u22c5\u0394 \u22c5\u03a9 - 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u23a0 \n", "\n", " \n", "_______________\u239e\n", " 2 4 \u239f\n", " 4\u22c5\u0394\u22c5\u03a9\u22c5g + \u03a9 \u23a0\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \n", " " ] } ], "prompt_number": 26 }, { "cell_type": "markdown", "metadata": {}, "source": [ "I will choose the arbitrary constants to be\n", "\n", "\\begin{align}\n", "x &= y = \\sqrt{\\frac{\\omega_+ (\\omega_+^2 - \\Delta^2)}{\\Omega (\\omega_+^2 - \\omega_-^2)}},\\\\\n", "z &= w = \\sqrt{\\frac{\\omega_- (\\Delta^2 - \\omega_-^2)}{\\Omega (\\omega_+^2 - \\omega_-^2)}},\\\\\n", "\\alpha&=\\beta=\\gamma=\\delta = 1\n", "\\end{align}" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "then, the transformation matrix $S$ becomes" ] }, { "cell_type": "code", "collapsed": false, "input": [ "S_ = S.subs({x: sqrt(wp * (wp**2 - d**2)/(O*(wp**2-wm**2))),\n", " y: sqrt(wp * (wp**2 - d**2)/(O*(wp**2-wm**2))),\n", " z: sqrt(wm * (d**2 - wm**2)/(O*(wp**2-wm**2))),\n", " w: sqrt(wm * (d**2 - wm**2)/(O*(wp**2-wm**2))),\n", " aa:1, bb:1, cc:1, dd:1})\n", "S_ = Matrix([[simplify(S_[i,j].factor()).factor() for j in range(4)] for i in range(4)])\n", "S_" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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MMbAxA6TpNKH/wX1P79ZK81RTip6/K61kuBymq4c3FsLaO/EYSJ/EwO4MkKbT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\nmnGN8yvy5VNODh3SDG17xZVq1oh6rNA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"prompt_number": 27, "text": [ "\u23a1 ____ \n", "\u23a2 -\u2572\u2571 \u03c9\u208a \u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", "\u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \n", "\u23a2 _____________________ \n", "\u23a2 ___ \u2571 -(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a) \n", "\u23a2\u0394\u22c5\u2572\u2571 \u03a9 \u22c5g\u22c5 \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \n", "\u23a2 \u2571 2 2 \n", "\u23a2 \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", "\u23a2 \n", "\u23a2 \n", "\u23a2 (\u0394 - \u03c9\n", "\u23a2 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", "\u23a2 \n", "\u23a2 ___ ____ \n", "\u23a2 \u2572\u2571 \u03a9 \u22c5g\u22c5\u2572\u2571 \u03c9\u208a \u22c5 \u2571\n", "\u23a2 \u2571 \n", "\u23a2 \u2572\u2571 \n", "\u23a2 \n", "\u23a2 ____ \n", "\u23a2 \u2572\u2571 \u03c9\u208b \u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", "\u23a2 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \n", "\u23a2 ___________________ \n", "\u23a2 ___ \u2571 (\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", "\u23a2 \u0394\u22c5\u2572\u2571 \u03a9 \u22c5g\u22c5 \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \n", "\u23a2 \u2571 2 2 \n", "\u23a2 \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", "\u23a2 \n", "\u23a2 \n", "\u23a2 -(\u0394 - \u03c9\n", "\u23a2 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", "\u23a2 \n", "\u23a2 ___ ____ \n", "\u23a2 \u2572\u2571 \u03a9 \u22c5g\u22c5\u2572\u2571 \u03c9\u208b \u22c5 \n", "\u23a2 \u2571\n", "\u23a3 \u2572\u2571 \n", "\n", " ____ \n", " -\u2572\u2571 \u03c9\u208a \u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 +\n", " 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " _____________________ \n", " ___ \u2571 -(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a) \n", " \u2572\u2571 \u03a9 \u22c5 \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\n", " \u2571 2 2 \n", " \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", " \n", " \n", "\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \n", " _____________________ \n", "\u2571 -(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a) \n", " \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \n", " 2 2 \n", " \u03c9\u208a - \u03c9\u208b \n", " \n", " ____ \n", " \u2572\u2571 \u03c9\u208b \u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 +\n", " 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " ___________________ \n", " ___ \u2571 (\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", " \u2572\u2571 \u03a9 \u22c5 \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\n", " \u2571 2 2 \n", " \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", " \n", " \n", "\u208a)\u22c5(\u0394 + \u03c9\u208a)\u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \n", " ___________________ \n", " \u2571 (\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \n", "\u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \n", " 2 2 \n", " \u03c9\u208a - \u03c9\u208b \n", "\n", " \u23a4\n", " \u03c9\u208a) \u23a5\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u23a5\n", " \u23a5\n", " \u23a5\n", "\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a5\n", " \u23a5\n", " \u23a5\n", " \u23a5\n", " ___ \u23a5\n", " -\u2572\u2571 \u03a9 \u22c5(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a) \u23a5\n", " \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5\n", " _____________________ \u23a5\n", " ____ \u2571 -(\u0394 - \u03c9\u208a)\u22c5(\u0394 + \u03c9\u208a) \u23a5\n", " \u2572\u2571 \u03c9\u208a \u22c5 \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b)\u23a5\n", " \u2571 2 2 \u23a5\n", " \u2572\u2571 \u03c9\u208a - \u03c9\u208b \u23a5\n", " \u23a5\n", " \u23a5\n", " \u03c9\u208b) \u23a5\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u23a5\n", " \u23a5\n", " \u23a5\n", "\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a5\n", " \u23a5\n", " \u23a5\n", " \u23a5\n", " ___ \u23a5\n", " \u2572\u2571 \u03a9 \u22c5(\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \u23a5\n", " \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u23a5\n", " ___________________ \u23a5\n", " ____ \u2571 (\u0394 - \u03c9\u208b)\u22c5(\u0394 + \u03c9\u208b) \u23a5\n", " \u2572\u2571 \u03c9\u208b \u22c5 \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5(\u03c9\u208a - \u03c9\u208b)\u22c5(\u03c9\u208a + \u03c9\u208b) \u23a5\n", " \u2571 2 2 \u23a5\n", " \u2572\u2571 \u03c9\u208a - \u03c9\u208b \u23a6" ] } ], "prompt_number": 27 }, { "cell_type": "markdown", "metadata": {}, "source": [ "Let's check if this matrix satisfies the two conditions we discussed above:" ] }, { "cell_type": "heading", "level": 5, "metadata": {}, "source": [ "Check 1 : $M = S^T D S$" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#check1\n", "STDS_ = simplify(S_.T * D * S_)\n", "STDS_ = Matrix([[simplify(STDS_[i,j].subs({wp:wpsol, wm:wmsol}).factor()) for j in range(4)] for i in range(4)])\n", "STDS_" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAAALsAAABkCAMAAADpJrGiAAAAP1BMVEX///8AAAAAAAAAAAAAAAAA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\n", "prompt_number": 28, "text": [ "\u23a1-\u0394 0 -g 0\u23a4\n", "\u23a2 \u23a5\n", "\u23a20 -\u0394 0 0\u23a5\n", "\u23a2 \u23a5\n", "\u23a2-g 0 \u03a9 0\u23a5\n", "\u23a2 \u23a5\n", "\u23a30 0 0 \u03a9\u23a6" ] } ], "prompt_number": 28 }, { "cell_type": "heading", "level": 5, "metadata": {}, "source": [ "Check 2 : $J = S J S^T$" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#check2\n", "SJST_ = simplify(S_ * J * S_.T)\n", "SJST_ = Matrix([[simplify(SJST_[i,j].subs({wp:wpsol, wm:wmsol}).factor()) for j in range(4)] for i in range(4)])\n", "SJST_" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": "iVBORw0KGgoAAAANSUhEUgAAAJgAAABkCAMAAABNTAlxAAAAP1BMVEX///8AAAAAAAAAAAAAAAAA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\nf5bYh/4itel/AVrXl9y0f0o//CK1rs0/v51EehgG0m0AAAAASUVORK5CYII=\n", "prompt_number": 29, "text": [ "\u23a10 1 0 0\u23a4\n", "\u23a2 \u23a5\n", "\u23a2-1 0 0 0\u23a5\n", "\u23a2 \u23a5\n", "\u23a20 0 0 1\u23a5\n", "\u23a2 \u23a5\n", "\u23a30 0 -1 0\u23a6" ] } ], "prompt_number": 29 }, { "cell_type": "markdown", "metadata": {}, "source": [ "Both conditions are fully satisfied with this transformation $S$." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The transformation between bosonic operators in different frames is readily obtained:\n", "$$\n", "Q\\vec{a}^{NM} = S \\left(Q\\vec{a}\\right) \\quad \\Rightarrow \\quad \\vec{a}^{NM} = (Q^{-1} S Q) \\vec{a} = T\\vec{a}\n", "$$" ] }, { "cell_type": "code", "collapsed": false, "input": [ "T = simplify((Q.inv() * S_ * Q))" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 30 }, { "cell_type": "code", "collapsed": false, "input": [ "lhs = anm[0]\n", "rhs = simplify((T * a)[0])\n", "Eq(lhs, rhs)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 31, "text": [ " ____________ \n", " \u2571 2 2 \n", " \u2571 - \u0394 + \u03c9\u208a \u239b \u239b \u2020 \u239e \u239b 2 2\u239e \u239b \n", " \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5\u239d\u0394\u22c5g\u22c5\u239d(-\u03a9 + \u03c9\u208a)\u22c5a_m + (\u03a9 + \u03c9\u208a)\u22c5a_m\u23a0 + \u239d\u0394 - \u03c9\u208b \u23a0\u22c5\u239d(-\u0394\n", " \u2571 2 2 \n", " \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", "a\u208a = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " ___ ____ \n", " 2\u22c5\u0394\u22c5\u2572\u2571 \u03a9 \u22c5g\u22c5\u2572\u2571 \u03c9\u208a \n", "\n", " \n", " \n", " \u2020\u239e\u239e\n", " + \u03c9\u208a)\u22c5a_c + (\u0394 + \u03c9\u208a)\u22c5a_c \u23a0\u23a0\n", " \n", " \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \n", " " ] } ], "prompt_number": 31 }, { "cell_type": "code", "collapsed": false, "input": [ "lhs = anm[1]\n", "rhs = simplify((T * a)[1])\n", "Eq(lhs, rhs)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 32, "text": [ " ____________ \n", " \u2571 2 2 \n", " \u2571 - \u0394 + \u03c9\u208a \u239b \u239b \u2020\u239e \u239b 2 2\u239e \u239b \n", " \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5\u239d\u0394\u22c5g\u22c5\u239d(-\u03a9 + \u03c9\u208a)\u22c5a_m + (\u03a9 + \u03c9\u208a)\u22c5a_m \u23a0 + \u239d\u0394 - \u03c9\u208b \u23a0\u22c5\u239d(-\n", " \u2571 2 2 \n", " \u2020 \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", "a\u208a = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " ___ ____ \n", " 2\u22c5\u0394\u22c5\u2572\u2571 \u03a9 \u22c5g\u22c5\u2572\u2571 \u03c9\u208a \n", "\n", " \n", " \n", " \u2020 \u239e\u239e\n", "\u0394 + \u03c9\u208a)\u22c5a_c + (\u0394 + \u03c9\u208a)\u22c5a_c\u23a0\u23a0\n", " \n", " \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \n", " " ] } ], "prompt_number": 32 }, { "cell_type": "code", "collapsed": false, "input": [ "lhs = anm[2]\n", "rhs = simplify((T * a)[2])\n", "Eq(lhs, rhs)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 33, "text": [ " ___________ \n", " \u2571 2 2 \n", " \u2571 \u0394 - \u03c9\u208b \u239b \u239b \u2020 \u239e \u239b 2 2\u239e \u239b \n", " \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5\u239d\u0394\u22c5g\u22c5\u239d(-\u03a9 + \u03c9\u208b)\u22c5a_m + (\u03a9 + \u03c9\u208b)\u22c5a_m\u23a0 + \u239d\u0394 - \u03c9\u208a \u23a0\u22c5\u239d(-\u0394 \n", " \u2571 2 2 \n", " \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", "a\u208b = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " ___ ____ \n", " 2\u22c5\u0394\u22c5\u2572\u2571 \u03a9 \u22c5g\u22c5\u2572\u2571 \u03c9\u208b \n", "\n", " \n", " \n", " \u2020\u239e\u239e\n", "+ \u03c9\u208b)\u22c5a_c + (\u0394 + \u03c9\u208b)\u22c5a_c \u23a0\u23a0\n", " \n", " \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \n", " " ] } ], "prompt_number": 33 }, { "cell_type": "code", "collapsed": false, "input": [ "lhs = anm[3]\n", "rhs = simplify((T * a)[3])\n", "Eq(lhs, rhs)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 34, "text": [ " ___________ \n", " \u2571 2 2 \n", " \u2571 \u0394 - \u03c9\u208b \u239b \u239b \u2020\u239e \u239b 2 2\u239e \u239b \n", " \u2571 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 \u22c5\u239d\u0394\u22c5g\u22c5\u239d(-\u03a9 + \u03c9\u208b)\u22c5a_m + (\u03a9 + \u03c9\u208b)\u22c5a_m \u23a0 + \u239d\u0394 - \u03c9\u208a \u23a0\u22c5\u239d(-\u0394\n", " \u2571 2 2 \n", " \u2020 \u2572\u2571 \u03c9\u208a - \u03c9\u208b \n", "a\u208b = \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " ___ ____ \n", " 2\u22c5\u0394\u22c5\u2572\u2571 \u03a9 \u22c5g\u22c5\u2572\u2571 \u03c9\u208b \n", "\n", " \n", " \n", " \u2020 \u239e\u239e\n", " + \u03c9\u208b)\u22c5a_c + (\u0394 + \u03c9\u208b)\u22c5a_c\u23a0\u23a0\n", " \n", " \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " \n", " " ] } ], "prompt_number": 34 }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Special Case: Red-detuned side ($\\Delta = -\\Omega$)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Here, I will consider the special case of the optomechanical system, where the driving field is tuned to the upper sideband ($\\Delta = -\\Omega$). The transformation matrix $S$ becomes" ] }, { "cell_type": "code", "collapsed": false, "input": [ "S__ = simplify(S_.subs({d: -O, wp: wpsol.subs(d, -O), wm: wmsol.subs(d, -O)}))\n", "lhs = Rnm\n", "rhs = MatMul(S__, R)\n", "Eq(lhs, rhs)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 35, "text": [ " \u23a1 ___ 4 _______ ___ 4 _______ \u23a4 \n", " \u23a2-\u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 + g \u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 + g \u23a5 \n", "\u23a1X\u208a\u23a4 = \u23a2\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u23a5\u22c5\u23a1X_c\u23a4\n", "\u23a2 \u23a5 \u23a2 4 ___ 4 ___ \u23a5 \u23a2 \u23a5\n", "\u23a2P\u208a\u23a5 \u23a2 2\u22c5\u2572\u2571 \u03a9 2\u22c5\u2572\u2571 \u03a9 \u23a5 \u23a2P_c\u23a5\n", "\u23a2 \u23a5 \u23a2 \u23a5 \u23a2 \u23a5\n", "\u23a2X\u208b\u23a5 \u23a2 ___ 4 ___ ___ 4 ___\u23a5 \u23a2X_m\u23a5\n", "\u23a2 \u23a5 \u23a2 -\u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 \u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 \u23a5 \u23a2 \u23a5\n", "\u23a3P\u208b\u23a6 \u23a2 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5 \u23a3P_m\u23a6\n", " \u23a2 4 _______ 4 _______\u23a5 \n", " \u23a2 2\u22c5\u2572\u2571 \u03a9 + g 2\u22c5\u2572\u2571 \u03a9 + g \u23a5 \n", " \u23a2 \u23a5 \n", " \u23a2 ___ 4 _______ ___ 4 _______ \u23a5 \n", " \u23a2 \u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 - g \u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 - g \u23a5 \n", " \u23a2 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u23a5 \n", " \u23a2 4 ___ 4 ___ \u23a5 \n", " \u23a2 2\u22c5\u2572\u2571 \u03a9 2\u22c5\u2572\u2571 \u03a9 \u23a5 \n", " \u23a2 \u23a5 \n", " \u23a2 ___ 4 ___ ___ 4 ___\u23a5 \n", " \u23a2 \u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 \u2572\u2571 2 \u22c5\u2572\u2571 \u03a9 \u23a5 \n", " \u23a2 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 0 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u23a5 \n", " \u23a2 4 _______ 4 _______\u23a5 \n", " \u23a3 2\u22c5\u2572\u2571 \u03a9 - g 2\u22c5\u2572\u2571 \u03a9 - g \u23a6 " ] } ], "prompt_number": 35 }, { "cell_type": "markdown", "metadata": {}, "source": [ "so that\n", "\n", "\n", "\\begin{align}\n", "X_{\\pm} &= \\sqrt[4]{\\frac{\\Omega\\pm g}{\\Omega}} \\frac{\\mp X_c + X_p}{\\sqrt{2}},\\\\\n", "P_{\\pm} &= \\sqrt[4]{\\frac{\\Omega}{(\\Omega\\pm g)}} \\frac{\\mp P_c + P_p}{\\sqrt{2}}.\n", "\\end{align}" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "It can be easily shown that this transformation is in consistent with the original Hamiltonian." ] }, { "cell_type": "code", "collapsed": false, "input": [ "H = hbar * wp/2 *(X_p**2 + P_p**2) + hbar * wm/2 * (X_m**2 + P_m**2)\n", "H" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 36, "text": [ " \u239b 2 2\u239e \u239b 2 2\u239e\n", "h\u0305\u22c5\u03c9\u208a\u22c5\u239dP\u208a + X\u208a \u23a0 h\u0305\u22c5\u03c9\u208b\u22c5\u239dP\u208b + X\u208b \u23a0\n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\n", " 2 2 " ] } ], "prompt_number": 36 }, { "cell_type": "markdown", "metadata": {}, "source": [ "By substituting into the normal mode Hamiltonian," ] }, { "cell_type": "code", "collapsed": false, "input": [ "H_ = H.subs({wp: wpsol.subs(d, -O), wm: wmsol.subs(d, -O),\n", " X_p: (rhs.doit())[0],\n", " P_p: (rhs.doit())[1],\n", " X_m: (rhs.doit())[2],\n", " P_m: (rhs.doit())[3],\n", " })\n", "simplify(H_.expand().factor()).subs({sqrt(((O+g)**2).expand()): O+g,\n", " Xm * Xc: Xc * Xm,\n", " Pm * Pc: Pc * Pm}).expand()" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "pyout", "png": 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"prompt_number": 37, "text": [ " 2 2 2 2 \n", "\u03a9\u22c5h\u0305\u22c5P_c \u03a9\u22c5h\u0305\u22c5P_m \u03a9\u22c5h\u0305\u22c5X_c \u03a9\u22c5h\u0305\u22c5X_m \n", "\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 + \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500 - g\u22c5h\u0305\u22c5X_c\u22c5X_m\n", " 2 2 2 2 " ] } ], "prompt_number": 37 }, { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Version Information" ] }, { "cell_type": "code", "collapsed": false, "input": [ "%reload_ext version_information\n", "\n", "%version_information sympy, sympsi" ], "language": "python", "metadata": {}, "outputs": [ { "html": [ "
SoftwareVersion
Python3.4.1 (default, Sep 20 2014, 19:44:17) [GCC 4.2.1 Compatible Apple LLVM 5.1 (clang-503.0.40)]
IPython2.3.0
OSposix [darwin]
sympy0.7.5-git
sympsi0.1.0.dev-11eaf6c
Fri Oct 24 15:05:38 2014 JST
" ], "json": [ "{\"Software versions\": [{\"version\": \"3.4.1 (default, Sep 20 2014, 19:44:17) [GCC 4.2.1 Compatible Apple LLVM 5.1 (clang-503.0.40)]\", \"module\": \"Python\"}, {\"version\": \"2.3.0\", \"module\": \"IPython\"}, {\"version\": \"posix [darwin]\", \"module\": \"OS\"}, {\"version\": \"0.7.5-git\", \"module\": \"sympy\"}, {\"version\": \"0.1.0.dev-11eaf6c\", \"module\": \"sympsi\"}]}" ], "latex": [ "\\begin{tabular}{|l|l|}\\hline\n", "{\\bf Software} & {\\bf Version} \\\\ \\hline\\hline\n", "Python & 3.4.1 (default, Sep 20 2014, 19:44:17) [GCC 4.2.1 Compatible Apple LLVM 5.1 (clang-503.0.40)] \\\\ \\hline\n", "IPython & 2.3.0 \\\\ \\hline\n", "OS & posix [darwin] \\\\ \\hline\n", "sympy & 0.7.5-git \\\\ \\hline\n", "sympsi & 0.1.0.dev-11eaf6c \\\\ \\hline\n", "\\hline \\multicolumn{2}{|l|}{Fri Oct 24 15:05:38 2014 JST} \\\\ \\hline\n", "\\end{tabular}\n" ], "metadata": {}, "output_type": "pyout", "prompt_number": 1, "text": [ "Software versions\n", "Python 3.4.1 (default, Sep 20 2014, 19:44:17) [GCC 4.2.1 Compatible Apple LLVM 5.1 (clang-503.0.40)]\n", "IPython 2.3.0\n", "OS posix [darwin]\n", "sympy 0.7.5-git\n", "sympsi 0.1.0.dev-11eaf6c\n", "Fri Oct 24 15:05:38 2014 JST" ] } ], "prompt_number": 1 } ], "metadata": {} } ] }