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"http://www.w3.org/TR/xhtml1/DTD/xhtml1-strict.dtd">
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<html xmlns="http://www.w3.org/1999/xhtml" lang="en" xml:lang="en">
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<head>
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<!-- 2021-02-04 Thu 21:33 -->
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<!-- 2021-06-09 Wed 14:50 -->
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<meta http-equiv="Content-Type" content="text/html;charset=utf-8" />
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<meta name="viewport" content="width=device-width, initial-scale=1" />
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<title>Quantum Monte Carlo</title>
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@ -329,152 +329,152 @@ for the JavaScript code in this tag.
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<h2>Table of Contents</h2>
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<div id="text-table-of-contents">
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<ul>
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<li><a href="#org1934ce3">1. Introduction</a>
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<li><a href="#orgaf15119">1. Introduction</a>
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<ul>
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<li><a href="#org0628105">1.1. Energy and local energy</a></li>
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<li><a href="#org2ebf785">1.1. Energy and local energy</a></li>
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</ul>
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</li>
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<li><a href="#org1e16b64">2. Numerical evaluation of the energy of the hydrogen atom</a>
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<li><a href="#org0f69ce9">2. Numerical evaluation of the energy of the hydrogen atom</a>
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<ul>
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<li><a href="#orgb212ef7">2.1. Local energy</a>
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<li><a href="#org6c36cef">2.1. Local energy</a>
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<ul>
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<li><a href="#org12d9267">2.1.1. Exercise 1</a>
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<li><a href="#orge997406">2.1.1. Exercise 1</a>
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||||
<ul>
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||||
<li><a href="#org27d0c0e">2.1.1.1. Solution</a></li>
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||||
<li><a href="#orgb38e582">2.1.1.1. Solution</a></li>
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</ul>
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||||
</li>
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||||
<li><a href="#org692a41b">2.1.2. Exercise 2</a>
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<li><a href="#orge34f95c">2.1.2. Exercise 2</a>
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||||
<ul>
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||||
<li><a href="#orgdba12d5">2.1.2.1. Solution</a></li>
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||||
<li><a href="#orgc1b4d26">2.1.2.1. Solution</a></li>
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</ul>
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</li>
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||||
<li><a href="#org8a0a49f">2.1.3. Exercise 3</a>
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<li><a href="#orgf88e606">2.1.3. Exercise 3</a>
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||||
<ul>
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||||
<li><a href="#orgd1ca369">2.1.3.1. Solution</a></li>
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<li><a href="#org5628b06">2.1.3.1. Solution</a></li>
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</ul>
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</li>
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<li><a href="#org057fb50">2.1.4. Exercise 4</a>
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<li><a href="#org4142f89">2.1.4. Exercise 4</a>
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||||
<ul>
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||||
<li><a href="#org2a52ec1">2.1.4.1. Solution</a></li>
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<li><a href="#orgbde97c7">2.1.4.1. Solution</a></li>
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</ul>
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</li>
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<li><a href="#org969ef99">2.1.5. Exercise 5</a>
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<li><a href="#orgbccab49">2.1.5. Exercise 5</a>
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<ul>
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<li><a href="#org910ee69">2.1.5.1. Solution</a></li>
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<li><a href="#org21ca21b">2.1.5.1. Solution</a></li>
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</ul>
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</li>
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</ul>
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</li>
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<li><a href="#orgcd7ebcc">2.2. Plot of the local energy along the \(x\) axis</a>
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<li><a href="#org8f20008">2.2. Plot of the local energy along the \(x\) axis</a>
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<ul>
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<li><a href="#org5fc436a">2.2.1. Exercise</a>
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<li><a href="#org0831bf2">2.2.1. Exercise</a>
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<ul>
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<li><a href="#orgf0cfffa">2.2.1.1. Solution</a></li>
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<li><a href="#orgd2d3c77">2.2.1.1. Solution</a></li>
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</ul>
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</li>
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</ul>
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</li>
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<li><a href="#org2fdf691">2.3. Numerical estimation of the energy</a>
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<li><a href="#orgfb1720d">2.3. Numerical estimation of the energy</a>
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<ul>
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<li><a href="#orgf7607a5">2.3.1. Exercise</a>
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<li><a href="#orgad64f6c">2.3.1. Exercise</a>
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<ul>
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||||
<li><a href="#org8e7a574">2.3.1.1. Solution</a></li>
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<li><a href="#org935a57d">2.3.1.1. Solution</a></li>
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</ul>
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</li>
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</ul>
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</li>
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<li><a href="#org3eba2de">2.4. Variance of the local energy</a>
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<li><a href="#org7f65d25">2.4. Variance of the local energy</a>
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<ul>
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<li><a href="#org3c4eabf">2.4.1. Exercise (optional)</a>
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<li><a href="#orgde80471">2.4.1. Exercise (optional)</a>
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||||
<ul>
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||||
<li><a href="#org7de5c01">2.4.1.1. Solution</a></li>
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<li><a href="#org4b9d0fe">2.4.1.1. Solution</a></li>
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||||
</ul>
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||||
</li>
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||||
<li><a href="#org7126926">2.4.2. Exercise</a>
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||||
<li><a href="#org36d8871">2.4.2. Exercise</a>
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||||
<ul>
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||||
<li><a href="#org79c36f5">2.4.2.1. Solution</a></li>
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<li><a href="#org1d01a3d">2.4.2.1. Solution</a></li>
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</ul>
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</li>
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</ul>
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</li>
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</ul>
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</li>
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<li><a href="#org4a35629">3. Variational Monte Carlo</a>
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<li><a href="#org2dc2467">3. Variational Monte Carlo</a>
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<ul>
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||||
<li><a href="#orgae557ce">3.1. Computation of the statistical error</a>
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<li><a href="#org0a464ed">3.1. Computation of the statistical error</a>
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<ul>
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||||
<li><a href="#org830fb1c">3.1.1. Exercise</a>
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||||
<li><a href="#orgca74250">3.1.1. Exercise</a>
|
||||
<ul>
|
||||
<li><a href="#orgba28956">3.1.1.1. Solution</a></li>
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||||
<li><a href="#orgb1a5ea0">3.1.1.1. Solution</a></li>
|
||||
</ul>
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||||
</li>
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||||
</ul>
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||||
</li>
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||||
<li><a href="#org3386e65">3.2. Uniform sampling in the box</a>
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||||
<li><a href="#org26a1e8a">3.2. Uniform sampling in the box</a>
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||||
<ul>
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||||
<li><a href="#org7c008e5">3.2.1. Exercise</a>
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||||
<li><a href="#org0b77922">3.2.1. Exercise</a>
|
||||
<ul>
|
||||
<li><a href="#org2bd3d2d">3.2.1.1. Solution</a></li>
|
||||
<li><a href="#org58fa227">3.2.1.1. Solution</a></li>
|
||||
</ul>
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||||
</li>
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||||
</ul>
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||||
</li>
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||||
<li><a href="#orge44c54f">3.3. Metropolis sampling with \(\Psi^2\)</a>
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||||
<li><a href="#org0be623e">3.3. Metropolis sampling with \(\Psi^2\)</a>
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||||
<ul>
|
||||
<li><a href="#orge175862">3.3.1. Optimal step size</a></li>
|
||||
<li><a href="#orgfd02533">3.3.2. Exercise</a>
|
||||
<li><a href="#org5ae0843">3.3.1. Optimal step size</a></li>
|
||||
<li><a href="#orgb39b1a2">3.3.2. Exercise</a>
|
||||
<ul>
|
||||
<li><a href="#orgb2b87cc">3.3.2.1. Solution</a></li>
|
||||
<li><a href="#org702284b">3.3.2.1. Solution</a></li>
|
||||
</ul>
|
||||
</li>
|
||||
</ul>
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||||
</li>
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||||
<li><a href="#org7695cb6">3.4. Generalized Metropolis algorithm</a>
|
||||
<li><a href="#orgc8fd760">3.4. Generalized Metropolis algorithm</a>
|
||||
<ul>
|
||||
<li><a href="#orgb6bf7fa">3.4.1. Gaussian random number generator</a></li>
|
||||
<li><a href="#org0c1e91f">3.4.2. Exercise 1</a>
|
||||
<li><a href="#org23a4975">3.4.1. Gaussian random number generator</a></li>
|
||||
<li><a href="#org4ace332">3.4.2. Exercise 1</a>
|
||||
<ul>
|
||||
<li><a href="#org4cf072a">3.4.2.1. Solution</a></li>
|
||||
<li><a href="#orgc7b1843">3.4.2.1. Solution</a></li>
|
||||
</ul>
|
||||
</li>
|
||||
<li><a href="#org01ca390">3.4.3. Exercise 2</a>
|
||||
<li><a href="#orgb75b96f">3.4.3. Exercise 2</a>
|
||||
<ul>
|
||||
<li><a href="#org792de88">3.4.3.1. Solution</a></li>
|
||||
<li><a href="#org1669705">3.4.3.1. Solution</a></li>
|
||||
</ul>
|
||||
</li>
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||||
</ul>
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||||
</li>
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||||
</ul>
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||||
</li>
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||||
<li><a href="#org69cde24">4. Diffusion Monte Carlo</a>
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||||
<li><a href="#org959001d">4. Diffusion Monte Carlo</a>
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||||
<ul>
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||||
<li><a href="#org5e3aebd">4.1. Schrödinger equation in imaginary time</a></li>
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||||
<li><a href="#orgea867cc">4.2. Relation to diffusion</a></li>
|
||||
<li><a href="#org57d596d">4.3. Importance sampling</a>
|
||||
<li><a href="#org6afa86f">4.1. Schrödinger equation in imaginary time</a></li>
|
||||
<li><a href="#orga80a4f6">4.2. Relation to diffusion</a></li>
|
||||
<li><a href="#orgd352eec">4.3. Importance sampling</a>
|
||||
<ul>
|
||||
<li><a href="#org84cf471">4.3.1. Appendix : Details of the Derivation</a></li>
|
||||
<li><a href="#org9f97703">4.3.1. Appendix : Details of the Derivation</a></li>
|
||||
</ul>
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||||
</li>
|
||||
<li><a href="#orgdaf95c7">4.4. Pure Diffusion Monte Carlo</a></li>
|
||||
<li><a href="#org6535c6a">4.5. Hydrogen atom</a>
|
||||
<li><a href="#orgf705671">4.4. Pure Diffusion Monte Carlo</a></li>
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||||
<li><a href="#orgea32850">4.5. Hydrogen atom</a>
|
||||
<ul>
|
||||
<li><a href="#org3d49d0a">4.5.1. Exercise</a>
|
||||
<li><a href="#orgc0799ee">4.5.1. Exercise</a>
|
||||
<ul>
|
||||
<li><a href="#orgdde440f">4.5.1.1. Solution</a></li>
|
||||
<li><a href="#orge1290ea">4.5.1.1. Solution</a></li>
|
||||
</ul>
|
||||
</li>
|
||||
</ul>
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||||
</li>
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||||
</ul>
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||||
</li>
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||||
<li><a href="#orgc932701">5. Project</a></li>
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||||
<li><a href="#org1d08a7d">6. Acknowledgments</a></li>
|
||||
<li><a href="#org392d105">5. Project</a></li>
|
||||
<li><a href="#orgae7f0d6">6. Acknowledgments</a></li>
|
||||
</ul>
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||||
</div>
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||||
</div>
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||||
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||||
<div id="outline-container-org1934ce3" class="outline-2">
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||||
<h2 id="org1934ce3"><span class="section-number-2">1</span> Introduction</h2>
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||||
<div id="outline-container-orgaf15119" class="outline-2">
|
||||
<h2 id="orgaf15119"><span class="section-number-2">1</span> Introduction</h2>
|
||||
<div class="outline-text-2" id="text-1">
|
||||
<p>
|
||||
This website contains the QMC tutorial of the 2021 LTTC winter school
|
||||
@ -514,8 +514,8 @@ coordinates, etc).
|
||||
</p>
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||||
</div>
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||||
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||||
<div id="outline-container-org0628105" class="outline-3">
|
||||
<h3 id="org0628105"><span class="section-number-3">1.1</span> Energy and local energy</h3>
|
||||
<div id="outline-container-org2ebf785" class="outline-3">
|
||||
<h3 id="org2ebf785"><span class="section-number-3">1.1</span> Energy and local energy</h3>
|
||||
<div class="outline-text-3" id="text-1-1">
|
||||
<p>
|
||||
For a given system with Hamiltonian \(\hat{H}\) and wave function \(\Psi\), we define the local energy as
|
||||
@ -598,8 +598,8 @@ energy computed over these configurations:
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||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org1e16b64" class="outline-2">
|
||||
<h2 id="org1e16b64"><span class="section-number-2">2</span> Numerical evaluation of the energy of the hydrogen atom</h2>
|
||||
<div id="outline-container-org0f69ce9" class="outline-2">
|
||||
<h2 id="org0f69ce9"><span class="section-number-2">2</span> Numerical evaluation of the energy of the hydrogen atom</h2>
|
||||
<div class="outline-text-2" id="text-2">
|
||||
<p>
|
||||
In this section, we consider the hydrogen atom with the following
|
||||
@ -628,8 +628,8 @@ To do that, we will compute the local energy and check whether it is constant.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgb212ef7" class="outline-3">
|
||||
<h3 id="orgb212ef7"><span class="section-number-3">2.1</span> Local energy</h3>
|
||||
<div id="outline-container-org6c36cef" class="outline-3">
|
||||
<h3 id="org6c36cef"><span class="section-number-3">2.1</span> Local energy</h3>
|
||||
<div class="outline-text-3" id="text-2-1">
|
||||
<p>
|
||||
You will now program all quantities needed to compute the local energy of the H atom for the given wave function.
|
||||
@ -656,8 +656,8 @@ to catch the error.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org12d9267" class="outline-4">
|
||||
<h4 id="org12d9267"><span class="section-number-4">2.1.1</span> Exercise 1</h4>
|
||||
<div id="outline-container-orge997406" class="outline-4">
|
||||
<h4 id="orge997406"><span class="section-number-4">2.1.1</span> Exercise 1</h4>
|
||||
<div class="outline-text-4" id="text-2-1-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -702,8 +702,8 @@ and returns the potential.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org27d0c0e" class="outline-5">
|
||||
<h5 id="org27d0c0e"><span class="section-number-5">2.1.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orgb38e582" class="outline-5">
|
||||
<h5 id="orgb38e582"><span class="section-number-5">2.1.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-1-1-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -744,8 +744,8 @@ and returns the potential.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org692a41b" class="outline-4">
|
||||
<h4 id="org692a41b"><span class="section-number-4">2.1.2</span> Exercise 2</h4>
|
||||
<div id="outline-container-orge34f95c" class="outline-4">
|
||||
<h4 id="orge34f95c"><span class="section-number-4">2.1.2</span> Exercise 2</h4>
|
||||
<div class="outline-text-4" id="text-2-1-2">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -780,8 +780,8 @@ input arguments, and returns a scalar.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgdba12d5" class="outline-5">
|
||||
<h5 id="orgdba12d5"><span class="section-number-5">2.1.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orgc1b4d26" class="outline-5">
|
||||
<h5 id="orgc1b4d26"><span class="section-number-5">2.1.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-1-2-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -808,8 +808,8 @@ input arguments, and returns a scalar.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org8a0a49f" class="outline-4">
|
||||
<h4 id="org8a0a49f"><span class="section-number-4">2.1.3</span> Exercise 3</h4>
|
||||
<div id="outline-container-orgf88e606" class="outline-4">
|
||||
<h4 id="orgf88e606"><span class="section-number-4">2.1.3</span> Exercise 3</h4>
|
||||
<div class="outline-text-4" id="text-2-1-3">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -890,8 +890,8 @@ Therefore, the local kinetic energy is
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgd1ca369" class="outline-5">
|
||||
<h5 id="orgd1ca369"><span class="section-number-5">2.1.3.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org5628b06" class="outline-5">
|
||||
<h5 id="org5628b06"><span class="section-number-5">2.1.3.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-1-3-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -932,8 +932,8 @@ Therefore, the local kinetic energy is
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org057fb50" class="outline-4">
|
||||
<h4 id="org057fb50"><span class="section-number-4">2.1.4</span> Exercise 4</h4>
|
||||
<div id="outline-container-org4142f89" class="outline-4">
|
||||
<h4 id="org4142f89"><span class="section-number-4">2.1.4</span> Exercise 4</h4>
|
||||
<div class="outline-text-4" id="text-2-1-4">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -992,8 +992,8 @@ are calling is yours.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org2a52ec1" class="outline-5">
|
||||
<h5 id="org2a52ec1"><span class="section-number-5">2.1.4.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orgbde97c7" class="outline-5">
|
||||
<h5 id="orgbde97c7"><span class="section-number-5">2.1.4.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-1-4-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -1024,8 +1024,8 @@ are calling is yours.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org969ef99" class="outline-4">
|
||||
<h4 id="org969ef99"><span class="section-number-4">2.1.5</span> Exercise 5</h4>
|
||||
<div id="outline-container-orgbccab49" class="outline-4">
|
||||
<h4 id="orgbccab49"><span class="section-number-4">2.1.5</span> Exercise 5</h4>
|
||||
<div class="outline-text-4" id="text-2-1-5">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -1035,8 +1035,8 @@ Find the theoretical value of \(a\) for which \(\Psi\) is an eigenfunction of \(
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org910ee69" class="outline-5">
|
||||
<h5 id="org910ee69"><span class="section-number-5">2.1.5.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org21ca21b" class="outline-5">
|
||||
<h5 id="org21ca21b"><span class="section-number-5">2.1.5.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-1-5-1">
|
||||
\begin{eqnarray*}
|
||||
E &=& \frac{\hat{H} \Psi}{\Psi} = - \frac{1}{2} \frac{\Delta \Psi}{\Psi} -
|
||||
@ -1056,8 +1056,8 @@ equal to -0.5 atomic units.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgcd7ebcc" class="outline-3">
|
||||
<h3 id="orgcd7ebcc"><span class="section-number-3">2.2</span> Plot of the local energy along the \(x\) axis</h3>
|
||||
<div id="outline-container-org8f20008" class="outline-3">
|
||||
<h3 id="org8f20008"><span class="section-number-3">2.2</span> Plot of the local energy along the \(x\) axis</h3>
|
||||
<div class="outline-text-3" id="text-2-2">
|
||||
<p>
|
||||
The program you will write in this section will be written in
|
||||
@ -1088,8 +1088,8 @@ In Fortran, you will need to compile all the source files together:
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org5fc436a" class="outline-4">
|
||||
<h4 id="org5fc436a"><span class="section-number-4">2.2.1</span> Exercise</h4>
|
||||
<div id="outline-container-org0831bf2" class="outline-4">
|
||||
<h4 id="org0831bf2"><span class="section-number-4">2.2.1</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-2-2-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -1183,8 +1183,8 @@ plot './data' index 0 using 1:2 with lines title 'a=0.1', \
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgf0cfffa" class="outline-5">
|
||||
<h5 id="orgf0cfffa"><span class="section-number-5">2.2.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orgd2d3c77" class="outline-5">
|
||||
<h5 id="orgd2d3c77"><span class="section-number-5">2.2.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-2-1-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -1261,8 +1261,8 @@ plt.savefig(<span style="color: #8b2252;">"plot_py.png"</span>)
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org2fdf691" class="outline-3">
|
||||
<h3 id="org2fdf691"><span class="section-number-3">2.3</span> Numerical estimation of the energy</h3>
|
||||
<div id="outline-container-orgfb1720d" class="outline-3">
|
||||
<h3 id="orgfb1720d"><span class="section-number-3">2.3</span> Numerical estimation of the energy</h3>
|
||||
<div class="outline-text-3" id="text-2-3">
|
||||
<p>
|
||||
If the space is discretized in small volume elements \(\mathbf{r}_i\)
|
||||
@ -1292,8 +1292,8 @@ The energy is biased because:
|
||||
</div>
|
||||
|
||||
|
||||
<div id="outline-container-orgf7607a5" class="outline-4">
|
||||
<h4 id="orgf7607a5"><span class="section-number-4">2.3.1</span> Exercise</h4>
|
||||
<div id="outline-container-orgad64f6c" class="outline-4">
|
||||
<h4 id="orgad64f6c"><span class="section-number-4">2.3.1</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-2-3-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -1364,8 +1364,8 @@ To compile the Fortran and run it:
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org8e7a574" class="outline-5">
|
||||
<h5 id="org8e7a574"><span class="section-number-5">2.3.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org935a57d" class="outline-5">
|
||||
<h5 id="org935a57d"><span class="section-number-5">2.3.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-3-1-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -1482,8 +1482,8 @@ a = 2.0000000000000000 E = -8.0869806678448772E-002
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org3eba2de" class="outline-3">
|
||||
<h3 id="org3eba2de"><span class="section-number-3">2.4</span> Variance of the local energy</h3>
|
||||
<div id="outline-container-org7f65d25" class="outline-3">
|
||||
<h3 id="org7f65d25"><span class="section-number-3">2.4</span> Variance of the local energy</h3>
|
||||
<div class="outline-text-3" id="text-2-4">
|
||||
<p>
|
||||
The variance of the local energy is a functional of \(\Psi\)
|
||||
@ -1510,8 +1510,8 @@ energy can be used as a measure of the quality of a wave function.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org3c4eabf" class="outline-4">
|
||||
<h4 id="org3c4eabf"><span class="section-number-4">2.4.1</span> Exercise (optional)</h4>
|
||||
<div id="outline-container-orgde80471" class="outline-4">
|
||||
<h4 id="orgde80471"><span class="section-number-4">2.4.1</span> Exercise (optional)</h4>
|
||||
<div class="outline-text-4" id="text-2-4-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -1522,8 +1522,8 @@ Prove that :
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org7de5c01" class="outline-5">
|
||||
<h5 id="org7de5c01"><span class="section-number-5">2.4.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org4b9d0fe" class="outline-5">
|
||||
<h5 id="org4b9d0fe"><span class="section-number-5">2.4.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-4-1-1">
|
||||
<p>
|
||||
\(\bar{E} = \langle E \rangle\) is a constant, so \(\langle \bar{E}
|
||||
@ -1542,8 +1542,8 @@ Prove that :
|
||||
</div>
|
||||
</div>
|
||||
</div>
|
||||
<div id="outline-container-org7126926" class="outline-4">
|
||||
<h4 id="org7126926"><span class="section-number-4">2.4.2</span> Exercise</h4>
|
||||
<div id="outline-container-org36d8871" class="outline-4">
|
||||
<h4 id="org36d8871"><span class="section-number-4">2.4.2</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-2-4-2">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -1619,8 +1619,8 @@ To compile and run:
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org79c36f5" class="outline-5">
|
||||
<h5 id="org79c36f5"><span class="section-number-5">2.4.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org1d01a3d" class="outline-5">
|
||||
<h5 id="org1d01a3d"><span class="section-number-5">2.4.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-2-4-2-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -1759,8 +1759,8 @@ a = 2.0000000000000000 E = -8.0869806678448772E-002 s2 = 1.8068814
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org4a35629" class="outline-2">
|
||||
<h2 id="org4a35629"><span class="section-number-2">3</span> Variational Monte Carlo</h2>
|
||||
<div id="outline-container-org2dc2467" class="outline-2">
|
||||
<h2 id="org2dc2467"><span class="section-number-2">3</span> Variational Monte Carlo</h2>
|
||||
<div class="outline-text-2" id="text-3">
|
||||
<p>
|
||||
Numerical integration with deterministic methods is very efficient
|
||||
@ -1776,8 +1776,8 @@ interval.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgae557ce" class="outline-3">
|
||||
<h3 id="orgae557ce"><span class="section-number-3">3.1</span> Computation of the statistical error</h3>
|
||||
<div id="outline-container-org0a464ed" class="outline-3">
|
||||
<h3 id="org0a464ed"><span class="section-number-3">3.1</span> Computation of the statistical error</h3>
|
||||
<div class="outline-text-3" id="text-3-1">
|
||||
<p>
|
||||
To compute the statistical error, you need to perform \(M\)
|
||||
@ -1817,8 +1817,8 @@ And the confidence interval is given by
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org830fb1c" class="outline-4">
|
||||
<h4 id="org830fb1c"><span class="section-number-4">3.1.1</span> Exercise</h4>
|
||||
<div id="outline-container-orgca74250" class="outline-4">
|
||||
<h4 id="orgca74250"><span class="section-number-4">3.1.1</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-3-1-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -1858,8 +1858,8 @@ input array.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgba28956" class="outline-5">
|
||||
<h5 id="orgba28956"><span class="section-number-5">3.1.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orgb1a5ea0" class="outline-5">
|
||||
<h5 id="orgb1a5ea0"><span class="section-number-5">3.1.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-3-1-1-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -1920,8 +1920,8 @@ input array.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org3386e65" class="outline-3">
|
||||
<h3 id="org3386e65"><span class="section-number-3">3.2</span> Uniform sampling in the box</h3>
|
||||
<div id="outline-container-org26a1e8a" class="outline-3">
|
||||
<h3 id="org26a1e8a"><span class="section-number-3">3.2</span> Uniform sampling in the box</h3>
|
||||
<div class="outline-text-3" id="text-3-2">
|
||||
<p>
|
||||
We will now perform our first Monte Carlo calculation to compute the
|
||||
@ -1982,8 +1982,8 @@ compute the statistical error.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org7c008e5" class="outline-4">
|
||||
<h4 id="org7c008e5"><span class="section-number-4">3.2.1</span> Exercise</h4>
|
||||
<div id="outline-container-org0b77922" class="outline-4">
|
||||
<h4 id="org0b77922"><span class="section-number-4">3.2.1</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-3-2-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -2085,8 +2085,8 @@ well as the index of the current step.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org2bd3d2d" class="outline-5">
|
||||
<h5 id="org2bd3d2d"><span class="section-number-5">3.2.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org58fa227" class="outline-5">
|
||||
<h5 id="org58fa227"><span class="section-number-5">3.2.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-3-2-1-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -2192,8 +2192,8 @@ E = -0.48084122147238995 +/- 2.4983775878329355E-003
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orge44c54f" class="outline-3">
|
||||
<h3 id="orge44c54f"><span class="section-number-3">3.3</span> Metropolis sampling with \(\Psi^2\)</h3>
|
||||
<div id="outline-container-org0be623e" class="outline-3">
|
||||
<h3 id="org0be623e"><span class="section-number-3">3.3</span> Metropolis sampling with \(\Psi^2\)</h3>
|
||||
<div class="outline-text-3" id="text-3-3">
|
||||
<p>
|
||||
We will now use the square of the wave function to sample random
|
||||
@ -2312,8 +2312,8 @@ All samples should be kept, from both accepted <i>and</i> rejected moves.
|
||||
</div>
|
||||
|
||||
|
||||
<div id="outline-container-orge175862" class="outline-4">
|
||||
<h4 id="orge175862"><span class="section-number-4">3.3.1</span> Optimal step size</h4>
|
||||
<div id="outline-container-org5ae0843" class="outline-4">
|
||||
<h4 id="org5ae0843"><span class="section-number-4">3.3.1</span> Optimal step size</h4>
|
||||
<div class="outline-text-4" id="text-3-3-1">
|
||||
<p>
|
||||
If the box is infinitely small, the ratio will be very close
|
||||
@ -2348,8 +2348,8 @@ the same variable later on to store a time step.
|
||||
</div>
|
||||
|
||||
|
||||
<div id="outline-container-orgfd02533" class="outline-4">
|
||||
<h4 id="orgfd02533"><span class="section-number-4">3.3.2</span> Exercise</h4>
|
||||
<div id="outline-container-orgb39b1a2" class="outline-4">
|
||||
<h4 id="orgb39b1a2"><span class="section-number-4">3.3.2</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-3-3-2">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -2458,8 +2458,8 @@ Can you observe a reduction in the statistical error?
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgb2b87cc" class="outline-5">
|
||||
<h5 id="orgb2b87cc"><span class="section-number-5">3.3.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org702284b" class="outline-5">
|
||||
<h5 id="org702284b"><span class="section-number-5">3.3.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-3-3-2-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -2606,8 +2606,8 @@ A = 0.50762633333333318 +/- 3.4601756760043725E-004
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org7695cb6" class="outline-3">
|
||||
<h3 id="org7695cb6"><span class="section-number-3">3.4</span> Generalized Metropolis algorithm</h3>
|
||||
<div id="outline-container-orgc8fd760" class="outline-3">
|
||||
<h3 id="orgc8fd760"><span class="section-number-3">3.4</span> Generalized Metropolis algorithm</h3>
|
||||
<div class="outline-text-3" id="text-3-4">
|
||||
<p>
|
||||
One can use more efficient numerical schemes to move the electrons by choosing a smarter expression for the transition probability.
|
||||
@ -2728,8 +2728,8 @@ The algorithm of the previous exercise is only slighlty modified as:
|
||||
</ol>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgb6bf7fa" class="outline-4">
|
||||
<h4 id="orgb6bf7fa"><span class="section-number-4">3.4.1</span> Gaussian random number generator</h4>
|
||||
<div id="outline-container-org23a4975" class="outline-4">
|
||||
<h4 id="org23a4975"><span class="section-number-4">3.4.1</span> Gaussian random number generator</h4>
|
||||
<div class="outline-text-4" id="text-3-4-1">
|
||||
<p>
|
||||
To obtain Gaussian-distributed random numbers, you can apply the
|
||||
@ -2793,8 +2793,8 @@ In Python, you can use the <a href="https://numpy.org/doc/stable/reference/rando
|
||||
</div>
|
||||
|
||||
|
||||
<div id="outline-container-org0c1e91f" class="outline-4">
|
||||
<h4 id="org0c1e91f"><span class="section-number-4">3.4.2</span> Exercise 1</h4>
|
||||
<div id="outline-container-org4ace332" class="outline-4">
|
||||
<h4 id="org4ace332"><span class="section-number-4">3.4.2</span> Exercise 1</h4>
|
||||
<div class="outline-text-4" id="text-3-4-2">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -2836,8 +2836,8 @@ Write a function to compute the drift vector \(\frac{\nabla \Psi(\mathbf{r})}{\P
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org4cf072a" class="outline-5">
|
||||
<h5 id="org4cf072a"><span class="section-number-5">3.4.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orgc7b1843" class="outline-5">
|
||||
<h5 id="orgc7b1843"><span class="section-number-5">3.4.2.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-3-4-2-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -2870,8 +2870,8 @@ Write a function to compute the drift vector \(\frac{\nabla \Psi(\mathbf{r})}{\P
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org01ca390" class="outline-4">
|
||||
<h4 id="org01ca390"><span class="section-number-4">3.4.3</span> Exercise 2</h4>
|
||||
<div id="outline-container-orgb75b96f" class="outline-4">
|
||||
<h4 id="orgb75b96f"><span class="section-number-4">3.4.3</span> Exercise 2</h4>
|
||||
<div class="outline-text-4" id="text-3-4-3">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -2967,8 +2967,8 @@ Modify the previous program to introduce the drift-diffusion scheme.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org792de88" class="outline-5">
|
||||
<h5 id="org792de88"><span class="section-number-5">3.4.3.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-org1669705" class="outline-5">
|
||||
<h5 id="org1669705"><span class="section-number-5">3.4.3.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-3-4-3-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -3156,8 +3156,8 @@ A = 0.62037333333333333 +/- 4.8970160591451110E-004
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org69cde24" class="outline-2">
|
||||
<h2 id="org69cde24"><span class="section-number-2">4</span> Diffusion Monte Carlo</h2>
|
||||
<div id="outline-container-org959001d" class="outline-2">
|
||||
<h2 id="org959001d"><span class="section-number-2">4</span> Diffusion Monte Carlo</h2>
|
||||
<div class="outline-text-2" id="text-4">
|
||||
<p>
|
||||
As we have seen, Variational Monte Carlo is a powerful method to
|
||||
@ -3174,8 +3174,8 @@ finding a near-exact numerical solution to the Schrödinger equation.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org5e3aebd" class="outline-3">
|
||||
<h3 id="org5e3aebd"><span class="section-number-3">4.1</span> Schrödinger equation in imaginary time</h3>
|
||||
<div id="outline-container-org6afa86f" class="outline-3">
|
||||
<h3 id="org6afa86f"><span class="section-number-3">4.1</span> Schrödinger equation in imaginary time</h3>
|
||||
<div class="outline-text-3" id="text-4-1">
|
||||
<p>
|
||||
Consider the time-dependent Schrödinger equation:
|
||||
@ -3243,8 +3243,8 @@ system.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgea867cc" class="outline-3">
|
||||
<h3 id="orgea867cc"><span class="section-number-3">4.2</span> Relation to diffusion</h3>
|
||||
<div id="outline-container-orga80a4f6" class="outline-3">
|
||||
<h3 id="orga80a4f6"><span class="section-number-3">4.2</span> Relation to diffusion</h3>
|
||||
<div class="outline-text-3" id="text-4-2">
|
||||
<p>
|
||||
The <a href="https://en.wikipedia.org/wiki/Diffusion_equation">diffusion equation</a> of particles is given by
|
||||
@ -3324,8 +3324,8 @@ Therefore, in both cases, you are dealing with a "Bosonic" ground state.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org57d596d" class="outline-3">
|
||||
<h3 id="org57d596d"><span class="section-number-3">4.3</span> Importance sampling</h3>
|
||||
<div id="outline-container-orgd352eec" class="outline-3">
|
||||
<h3 id="orgd352eec"><span class="section-number-3">4.3</span> Importance sampling</h3>
|
||||
<div class="outline-text-3" id="text-4-3">
|
||||
<p>
|
||||
In a molecular system, the potential is far from being constant
|
||||
@ -3423,8 +3423,8 @@ energies computed with the trial wave function.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org84cf471" class="outline-4">
|
||||
<h4 id="org84cf471"><span class="section-number-4">4.3.1</span> Appendix : Details of the Derivation</h4>
|
||||
<div id="outline-container-org9f97703" class="outline-4">
|
||||
<h4 id="org9f97703"><span class="section-number-4">4.3.1</span> Appendix : Details of the Derivation</h4>
|
||||
<div class="outline-text-4" id="text-4-3-1">
|
||||
<p>
|
||||
\[
|
||||
@ -3485,8 +3485,8 @@ Defining \(\Pi(\mathbf{r},t) = \psi(\mathbf{r},\tau)
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgdaf95c7" class="outline-3">
|
||||
<h3 id="orgdaf95c7"><span class="section-number-3">4.4</span> Pure Diffusion Monte Carlo</h3>
|
||||
<div id="outline-container-orgf705671" class="outline-3">
|
||||
<h3 id="orgf705671"><span class="section-number-3">4.4</span> Pure Diffusion Monte Carlo</h3>
|
||||
<div class="outline-text-3" id="text-4-4">
|
||||
<p>
|
||||
Instead of having a variable number of particles to simulate the
|
||||
@ -3575,13 +3575,13 @@ the DMC algorithm. However, its use reduces significantly the time-step error.</
|
||||
</div>
|
||||
|
||||
|
||||
<div id="outline-container-org6535c6a" class="outline-3">
|
||||
<h3 id="org6535c6a"><span class="section-number-3">4.5</span> Hydrogen atom</h3>
|
||||
<div id="outline-container-orgea32850" class="outline-3">
|
||||
<h3 id="orgea32850"><span class="section-number-3">4.5</span> Hydrogen atom</h3>
|
||||
<div class="outline-text-3" id="text-4-5">
|
||||
</div>
|
||||
|
||||
<div id="outline-container-org3d49d0a" class="outline-4">
|
||||
<h4 id="org3d49d0a"><span class="section-number-4">4.5.1</span> Exercise</h4>
|
||||
<div id="outline-container-orgc0799ee" class="outline-4">
|
||||
<h4 id="orgc0799ee"><span class="section-number-4">4.5.1</span> Exercise</h4>
|
||||
<div class="outline-text-4" id="text-4-5-1">
|
||||
<div class="exercise">
|
||||
<p>
|
||||
@ -3683,8 +3683,8 @@ time \(\tau_{\text{max}}\) =100 a.u.
|
||||
</div>
|
||||
</div>
|
||||
|
||||
<div id="outline-container-orgdde440f" class="outline-5">
|
||||
<h5 id="orgdde440f"><span class="section-number-5">4.5.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div id="outline-container-orge1290ea" class="outline-5">
|
||||
<h5 id="orge1290ea"><span class="section-number-5">4.5.1.1</span> Solution   <span class="tag"><span class="solution">solution</span></span></h5>
|
||||
<div class="outline-text-5" id="text-4-5-1-1">
|
||||
<p>
|
||||
<b>Python</b>
|
||||
@ -3904,8 +3904,8 @@ A = 0.98963533333333342 +/- 6.3052128284666221E-005
|
||||
|
||||
|
||||
|
||||
<div id="outline-container-orgc932701" class="outline-2">
|
||||
<h2 id="orgc932701"><span class="section-number-2">5</span> Project</h2>
|
||||
<div id="outline-container-org392d105" class="outline-2">
|
||||
<h2 id="org392d105"><span class="section-number-2">5</span> Project</h2>
|
||||
<div class="outline-text-2" id="text-5">
|
||||
<p>
|
||||
Change your PDMC code for one of the following:
|
||||
@ -3923,8 +3923,8 @@ And compute the ground state energy.
|
||||
|
||||
|
||||
|
||||
<div id="outline-container-org1d08a7d" class="outline-2">
|
||||
<h2 id="org1d08a7d"><span class="section-number-2">6</span> Acknowledgments</h2>
|
||||
<div id="outline-container-orgae7f0d6" class="outline-2">
|
||||
<h2 id="orgae7f0d6"><span class="section-number-2">6</span> Acknowledgments</h2>
|
||||
<div class="outline-text-2" id="text-6">
|
||||
|
||||
<div class="figure">
|
||||
@ -3944,7 +3944,7 @@ Union is not responsible for any use that might be made of such content.
|
||||
</div>
|
||||
<div id="postamble" class="status">
|
||||
<p class="author">Author: Anthony Scemama, Claudia Filippi</p>
|
||||
<p class="date">Created: 2021-02-04 Thu 21:33</p>
|
||||
<p class="date">Created: 2021-06-09 Wed 14:50</p>
|
||||
<p class="validation"><a href="http://validator.w3.org/check?uri=referer">Validate</a></p>
|
||||
</div>
|
||||
</body>
|
||||
|
||||
Loading…
Reference in New Issue
Block a user