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doc/Projects/2020/Project1/html/Project1-bs.html

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<center><b>Department of Physics, University of Oslo, Norway</b></center>
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<br>
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<p>
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<center><h4>Jan 14, 2020</h4></center> <!-- date -->
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<center><h4>Jan 21, 2020</h4></center> <!-- date -->
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<br>
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<p>
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</div> <!-- end jumbotron -->
@@ -160,7 +160,7 @@ <h2 id="___sec0" class="anchor">Introduction </h2>
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\( a_{h0}=\left( {\hbar}/{m\omega_\perp}\right)^\frac{1}{2}=1-2 \times 10^4 \)
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\AA\ . The interaction between $^{87}$Rb atoms can be well represented
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by its s-wave scattering length, \( a_{Rb} \). This scattering length lies in the
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range \( 85 < a_{Rb} < 140 a_0 \) where \( a_0 = 0.5292 \) \AA\ is the Bohr radius.
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range \( 85 a_0 < a_{Rb} < 140 a_0 \) where \( a_0 = 0.5292 \) \AA\ is the Bohr radius.
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The definite value \( a_{Rb} = 100 a_0 \) is usually selected and
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for calculations the definite ratio of atom size to trap size
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\( a_{Rb}/a_{h0} = 4.33 \times 10^{-3} \)
@@ -215,7 +215,7 @@ <h2 id="___sec0" class="anchor">Introduction </h2>
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\end{equation}
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$$
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where (S) stands for symmetric and
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where (S) stands for spherical and
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$$
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\begin{equation}

doc/Projects/2020/Project1/html/Project1.html

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<center><b>Department of Physics, University of Oslo, Norway</b></center>
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<br>
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<p>
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<center><h4>Jan 14, 2020</h4></center> <!-- date -->
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<center><h4>Jan 21, 2020</h4></center> <!-- date -->
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<br>
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<h2 id="___sec0">Introduction </h2>
@@ -117,7 +117,7 @@ <h2 id="___sec0">Introduction </h2>
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\( a_{h0}=\left( {\hbar}/{m\omega_\perp}\right)^\frac{1}{2}=1-2 \times 10^4 \)
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\AA\ . The interaction between $^{87}$Rb atoms can be well represented
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by its s-wave scattering length, \( a_{Rb} \). This scattering length lies in the
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range \( 85 < a_{Rb} < 140 a_0 \) where \( a_0 = 0.5292 \) \AA\ is the Bohr radius.
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range \( 85 a_0 < a_{Rb} < 140 a_0 \) where \( a_0 = 0.5292 \) \AA\ is the Bohr radius.
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The definite value \( a_{Rb} = 100 a_0 \) is usually selected and
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for calculations the definite ratio of atom size to trap size
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\( a_{Rb}/a_{h0} = 4.33 \times 10^{-3} \)
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\end{equation}
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$$
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where (S) stands for symmetric and
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where (S) stands for spherical and
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$$
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\begin{equation}

doc/Projects/2020/Project1/ipynb/Project1.ipynb

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"<!-- Author: --> \n",
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"**[Computational Physics I FYS4411/FYS9411](http://www.uio.no/studier/emner/matnat/fys/FYS4411/index-eng.html)**, Department of Physics, University of Oslo, Norway\n",
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"\n",
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"Date: **Jan 14, 2020**\n",
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"Date: **Jan 21, 2020**\n",
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"\n",
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"Copyright 1999-2020, [Computational Physics I FYS4411/FYS9411](http://www.uio.no/studier/emner/matnat/fys/FYS4411/index-eng.html). Released under CC Attribution-NonCommercial 4.0 license\n",
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"\n",
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" $a_{h0}=\\left( {\\hbar}/{m\\omega_\\perp}\\right)^\\frac{1}{2}=1-2 \\times 10^4$\n",
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" \\AA\\ . The interaction between $^{87}$Rb atoms can be well represented\n",
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" by its s-wave scattering length, $a_{Rb}$. This scattering length lies in the\n",
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" range $85 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \\AA\\ is the Bohr radius.\n",
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" range $85 a_0 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \\AA\\ is the Bohr radius.\n",
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" The definite value $a_{Rb} = 100 a_0$ is usually selected and\n",
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" for calculations the definite ratio of atom size to trap size \n",
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" $a_{Rb}/a_{h0} = 4.33 \\times 10^{-3}$ \n",
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"cell_type": "markdown",
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"metadata": {},
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"source": [
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"where (S) stands for symmetric and"
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"where (S) stands for spherical and"
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]
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},
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{
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doc/Projects/2020/Project1/pdf/Project1.p.tex

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% --- begin date ---
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\begin{center}
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Jan 14, 2020
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Jan 21, 2020
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\end{center}
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% --- end date ---
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@@ -174,7 +174,7 @@ \subsection{Introduction}
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$a_{h0}=\left( {\hbar}/{m\omega_\perp}\right)^\frac{1}{2}=1-2 \times 10^4$
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\AA\ . The interaction between $^{87}$Rb atoms can be well represented
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by its s-wave scattering length, $a_{Rb}$. This scattering length lies in the
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range $85 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \AA\ is the Bohr radius.
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range $85 a_0 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \AA\ is the Bohr radius.
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The definite value $a_{Rb} = 100 a_0$ is usually selected and
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for calculations the definite ratio of atom size to trap size
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$a_{Rb}/a_{h0} = 4.33 \times 10^{-3}$
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\label{trap_eqn}
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\end{array}
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\end{equation}
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where (S) stands for symmetric and
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where (S) stands for spherical and
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\begin{equation}
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H = \sum_i^N \left(\frac{-\hbar^2}{2m}{\bigtriangledown }_{i}^2 +V_{ext}({\mathbf{r}}_i)\right) +
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doc/Projects/2020/Project1/pdf/Project1.tex

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% --- begin date ---
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\begin{center}
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Jan 14, 2020
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Jan 21, 2020
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\end{center}
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% --- end date ---
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$a_{h0}=\left( {\hbar}/{m\omega_\perp}\right)^\frac{1}{2}=1-2 \times 10^4$
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\AA\ . The interaction between $^{87}$Rb atoms can be well represented
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by its s-wave scattering length, $a_{Rb}$. This scattering length lies in the
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range $85 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \AA\ is the Bohr radius.
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range $85 a_0 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \AA\ is the Bohr radius.
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The definite value $a_{Rb} = 100 a_0$ is usually selected and
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for calculations the definite ratio of atom size to trap size
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$a_{Rb}/a_{h0} = 4.33 \times 10^{-3}$
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\label{trap_eqn}
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\end{array}
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\end{equation}
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where (S) stands for symmetric and
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where (S) stands for spherical and
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\begin{equation}
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H = \sum_i^N \left(\frac{-\hbar^2}{2m}{\bigtriangledown }_{i}^2 +V_{ext}({\mathbf{r}}_i)\right) +

doc/src/Projects/2020/Project1/Project1.do.txt

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$a_{h0}=\left( {\hbar}/{m\omega_\perp}\right)^\frac{1}{2}=1-2 \times 10^4$
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\AA\ . The interaction between $^{87}$Rb atoms can be well represented
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by its s-wave scattering length, $a_{Rb}$. This scattering length lies in the
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range $85 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \AA\ is the Bohr radius.
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range $85 a_0 < a_{Rb} < 140 a_0$ where $a_0 = 0.5292$ \AA\ is the Bohr radius.
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The definite value $a_{Rb} = 100 a_0$ is usually selected and
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for calculations the definite ratio of atom size to trap size
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$a_{Rb}/a_{h0} = 4.33 \times 10^{-3}$
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\end{array}
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\end{equation}
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!et
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where (S) stands for symmetric and
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where (S) stands for spherical and
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!bt
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\begin{equation}

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