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paper/basic_training.bib

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@@ -985,6 +985,18 @@ @article{Isele-Holder:2012:JChemPhys
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pages = {174107},
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}
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@article{Ewald_1921,
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author = {Ewald, P. P.},
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title = {Die Berechnung optischer und elektrostatischer Gitterpotentiale},
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journal = {Annalen der Physik},
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volume = {369},
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number = {3},
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pages = {253-287},
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doi = {10.1002/andp.19213690304},
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url = {https://onlinelibrary.wiley.com/doi/abs/10.1002/andp.19213690304},
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eprint = {https://onlinelibrary.wiley.com/doi/pdf/10.1002/andp.19213690304}
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}
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@article{Paliwal:2013:J.Chem.TheoryComput.,
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title = {Using {{Multistate Reweighting}} to {{Rapidly}} and {{Efficiently Explore Molecular Simulation Parameters Space}} for {{Nonbonded Interactions}}},
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volume = {9},

paper/basic_training.pdf

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paper/basic_training.tex

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\subsubsection{ Ewald Summation}
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The Ewald summation technique [ref Ewald, 1921] provides one way to efficiently handle long-range electrostatics in periodic systems.
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The Ewald summation technique~\cite{Ewald_1921} provides one way to efficiently handle long-range electrostatics in periodic systems.
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To understand this technique, consider the relationship between the charge distribution and the Coulombic potential written in the differential form (the Poisson equation):
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\todo[inline, color={yellow!20}]{DLM: Fill in Ewald reference}
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\[
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\Delta \phi(\boldsymbol{x}) = - \frac{1}{\epsilon} \rho(\boldsymbol{x})

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