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Marius Hope
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Typos week 2
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doc/pub/week2/ipynb/week2.ipynb

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"source": [
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"$$\n",
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"\\boldsymbol{P}_a=\\vert \\psi_a\\rangle \\langle \\psi_a\\vert = \\begin{bmatrix} \\vert \\alpha_0\\vert^2 &\\alpha_0\\alpha_1^* \\\\\n",
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" \\alpha_1\\alpha_0^* & \\vert \\alpha_1\\vert^* \\end{bmatrix},\n",
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" \\alpha_1\\alpha_0^* & \\vert \\alpha_1\\vert^2 \\end{bmatrix},\n",
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"$$"
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]
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},
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"source": [
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"$$\n",
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"\\boldsymbol{P}_b=\\vert \\psi_b\\rangle \\langle \\psi_b\\vert = \\begin{bmatrix} \\vert \\beta_0\\vert^2 &\\beta_0\\beta_1^* \\\\\n",
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" \\beta_1\\beta_0^* & \\vert \\beta_1\\vert^* \\end{bmatrix}.\n",
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" \\beta_1\\beta_0^* & \\vert \\beta_1\\vert^2 \\end{bmatrix}.\n",
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"$$"
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]
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},
@@ -558,8 +558,8 @@
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"source": [
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"$$\n",
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"\\boldsymbol{A}=\\lambda_a\\begin{bmatrix} \\vert \\alpha_0\\vert^2 &\\alpha_0\\alpha_1^* \\\\\n",
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" \\alpha_1\\alpha_0^* & \\vert \\alpha_1\\vert^* \\end{bmatrix} +\\lambda_b\\begin{bmatrix} \\vert \\beta_0\\vert^2 &\\beta_0\\beta_1^* \\\\\n",
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" \\beta_1\\beta_0^* & \\vert \\beta_1\\vert^* \\end{bmatrix}.\n",
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" \\alpha_1\\alpha_0^* & \\vert \\alpha_1\\vert^2 \\end{bmatrix} +\\lambda_b\\begin{bmatrix} \\vert \\beta_0\\vert^2 &\\beta_0\\beta_1^* \\\\\n",
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" \\beta_1\\beta_0^* & \\vert \\beta_1\\vert^2 \\end{bmatrix}.\n",
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"$$"
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]
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},
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"metadata": {},
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"source": [
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"$$\n",
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"\\sum_{i=0}^1\\boldsymbol{P}_i^{\\dagger}\\boldsymbol{P}_1=\\boldsymbol{I},\n",
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"\\sum_{i=0}^1\\boldsymbol{P}_i^{\\dagger}\\boldsymbol{P}_i=\\boldsymbol{I},\n",
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"$$"
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]
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},
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"source": [
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"## Simple Hamiltonian models\n",
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"\n",
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"In order to study get started with coding, we will study two simple Hamiltonian systems, one which we can use for a single qubit systems and one which has as basis functions a two-qubit system. These two simple Hamiltonians exhibit also something which is called level crossing, a feature which we will use in later studies of entanglement.\n",
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"In order to get started with coding, we will study two simple Hamiltonian systems, one which we can use for a single qubit systems and one which has as basis functions a two-qubit system. These two simple Hamiltonians exhibit also something which is called level crossing, a feature which we will use in later studies of entanglement.\n",
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"\n",
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"We study first a simple two-level system. Thereafter we\n",
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"extend our model to a four-level system which can be\n",
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"interpreted as composed of two separate (not necesseraly identical)\n",
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"subsystems.\n",
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"\n",
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"We let our hamiltonian depend linearly on a strength parameter $z$"
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"We let our hamiltonian depend linearly on a strength parameter $\\lambda$"
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]
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},
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{
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"is $\\vert 0 \\rangle$. At $\\lambda=1$ the $\\vert 0 \\rangle$ mixing of\n",
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"the lowest eigenvalue is $1\\%$ while for $\\lambda\\leq 2/3$ we have a\n",
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"$\\vert 0 \\rangle$ component of more than $90\\%$. The character of the\n",
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"eigenvectors has therefore been interchanged when passing $z=2/3$. The\n",
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"eigenvectors has therefore been interchanged when passing $\\lambda=2/3$. The\n",
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"value of the parameter $X$ represents the strength of the coupling\n",
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"between the model space and the excluded space. The following code\n",
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"computes and plots the eigenvalues."
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"metadata": {},
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"source": [
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"$$\n",
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"\\vert 10\\rangle = \\vert 1\\rangle_{\\mathrm{A}}\\otimes \\vert 0\\rangle_{\\mathrm{B}}=\\begin{bmatrix} 0 & 1 & 0 &0\\end{bmatrix}^T,\n",
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"\\vert 01\\rangle = \\vert 0\\rangle_{\\mathrm{A}}\\otimes \\vert 1\\rangle_{\\mathrm{B}}=\\begin{bmatrix} 0 & 1 & 0 &0\\end{bmatrix}^T,\n",
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"$$"
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]
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},
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"metadata": {},
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"source": [
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"$$\n",
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"\\vert 01\\rangle = \\vert 0\\rangle_{\\mathrm{A}}\\otimes \\vert 1\\rangle_{\\mathrm{B}}=\\begin{bmatrix} 0 & 0 & 1 &0\\end{bmatrix}^T,\n",
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"\\vert 10\\rangle = \\vert 1\\rangle_{\\mathrm{A}}\\otimes \\vert 0\\rangle_{\\mathrm{B}}=\\begin{bmatrix} 0 & 0 & 1 &0\\end{bmatrix}^T,\n",
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"$$"
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]
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},
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"metadata": {},
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"source": [
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"$$\n",
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"H_0\\vert 10 \\rangle = \\epsilon_{10}\\vert 10 \\rangle,\n",
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"H_0\\vert 01 \\rangle = \\epsilon_{01}\\vert 01 \\rangle,\n",
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"$$"
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]
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},
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"metadata": {},
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"source": [
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"$$\n",
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"H_0\\vert 01 \\rangle = \\epsilon_{01}\\vert 01 \\rangle,\n",
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"H_0\\vert 10 \\rangle = \\epsilon_{10}\\vert 10 \\rangle,\n",
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"$$"
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]
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},
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"source": [
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"$$\n",
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"\\boldsymbol{H}=\\begin{bmatrix} \\epsilon_{00}+H_z & 0 & 0 & H_x \\\\\n",
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" 0 & \\epsilon_{10}-H_z & H_x & 0 \\\\\n",
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"\t\t 0 & H_x & \\epsilon_{01}-H_z & 0 \\\\\n",
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" 0 & \\epsilon_{01}-H_z & H_x & 0 \\\\\n",
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"\t\t 0 & H_x & \\epsilon_{10}-H_z & 0 \\\\\n",
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"\t\t H_x & 0 & 0 & \\epsilon_{11} +H_z \\end{bmatrix}.\n",
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"$$"
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]
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"metadata": {},
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"source": [
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"$$\n",
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"\\rho_0=\\left(\\alpha_{00}\\vert 00 \\rangle\\langle 00\\vert+\\alpha_{10}\\vert 10 \\rangle\\langle 10\\vert+\\alpha_{01}\\vert 01 \\rangle\\langle 01\\vert+\\alpha_{11}\\vert 11 \\rangle\\langle 11\\vert\\right),\n",
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"\\rho_0=\\left(\\alpha_{00}\\vert 00 \\rangle\\langle 00\\vert+\\alpha_{01}\\vert 01 \\rangle\\langle 01\\vert+\\alpha_{10}\\vert 10 \\rangle\\langle 10\\vert+\\alpha_{11}\\vert 11 \\rangle\\langle 11\\vert\\right),\n",
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"$$"
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]
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},

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