diff --git a/doc/Eqs/eff_KE.jpg b/doc/Eqs/eff_KE.jpg new file mode 100644 index 0000000000..9fe9c0692e Binary files /dev/null and b/doc/Eqs/eff_KE.jpg differ diff --git a/doc/Eqs/eff_KE.tex b/doc/Eqs/eff_KE.tex new file mode 100644 index 0000000000..9f9af2fa25 --- /dev/null +++ b/doc/Eqs/eff_KE.tex @@ -0,0 +1,9 @@ +\documentclass[12pt]{article} + +\begin{document} + +$$ +E_{KE} = \frac{\hbar^2 }{{m_{e} }}\sum\limits_i {\frac{3}{{2s_i^2 }}} +$$ + +\end{document} diff --git a/doc/Eqs/eff_NN.jpg b/doc/Eqs/eff_NN.jpg new file mode 100644 index 0000000000..f70768bf15 Binary files /dev/null and b/doc/Eqs/eff_NN.jpg differ diff --git a/doc/Eqs/eff_NN.tex b/doc/Eqs/eff_NN.tex new file mode 100644 index 0000000000..4f9bb6d132 --- /dev/null +++ b/doc/Eqs/eff_NN.tex @@ -0,0 +1,9 @@ +\documentclass[12pt]{article} + +\begin{document} + +$$ +E_{NN} = \frac{1}{{4\pi \varepsilon _0 }}\sum\limits_{i < j} {\frac{{Z_i Z_j }}{{R_{ij} }}} +$$ + +\end{document} diff --git a/doc/Eqs/eff_Ne.jpg b/doc/Eqs/eff_Ne.jpg new file mode 100644 index 0000000000..1ce103df6d Binary files /dev/null and b/doc/Eqs/eff_Ne.jpg differ diff --git a/doc/Eqs/eff_Ne.tex b/doc/Eqs/eff_Ne.tex new file mode 100644 index 0000000000..e6813b125c --- /dev/null +++ b/doc/Eqs/eff_Ne.tex @@ -0,0 +1,9 @@ +\documentclass[12pt]{article} + +\begin{document} + +$$ +E_{Ne} = - \frac{1}{{4\pi \varepsilon _0 }}\sum\limits_{i,j} {\frac{{Z_i }}{{R_{ij} }}Erf\left( {\frac{{\sqrt 2 R_{ij} }}{{s_j }}} \right)} +$$ + +\end{document} diff --git a/doc/Eqs/eff_Pauli.jpg b/doc/Eqs/eff_Pauli.jpg new file mode 100644 index 0000000000..82b2c18c23 Binary files /dev/null and b/doc/Eqs/eff_Pauli.jpg differ diff --git a/doc/Eqs/eff_Pauli.tex b/doc/Eqs/eff_Pauli.tex new file mode 100644 index 0000000000..b6b8070cc7 --- /dev/null +++ b/doc/Eqs/eff_Pauli.tex @@ -0,0 +1,9 @@ +\documentclass[12pt]{article} + +\begin{document} + +$$ +E_{Pauli} = \sum\limits_{\sigma _i = \sigma _j } {E\left( { \uparrow \uparrow } \right)_{ij}} + \sum\limits_{\sigma _i \ne \sigma _j } {E\left( { \uparrow \downarrow } \right)_{ij}} +$$ + +\end{document} diff --git a/doc/Eqs/eff_ee.jpg b/doc/Eqs/eff_ee.jpg new file mode 100644 index 0000000000..25871e9b49 Binary files /dev/null and b/doc/Eqs/eff_ee.jpg differ diff --git a/doc/Eqs/eff_ee.tex b/doc/Eqs/eff_ee.tex new file mode 100644 index 0000000000..5d17e5557b --- /dev/null +++ b/doc/Eqs/eff_ee.tex @@ -0,0 +1,9 @@ +\documentclass[12pt]{article} + +\begin{document} + +$$ +E_{ee} = \frac{1}{{4\pi \varepsilon _0 }}\sum\limits_{i < j} {\frac{1}{{r_{ij} }}Erf\left( {\frac{{\sqrt 2 r_{ij} }}{{\sqrt {s_i^2 + s_j^2 } }}} \right)} +$$ + +\end{document} diff --git a/doc/Eqs/eff_energy_expression.jpg b/doc/Eqs/eff_energy_expression.jpg new file mode 100644 index 0000000000..e5ff7a185e Binary files /dev/null and b/doc/Eqs/eff_energy_expression.jpg differ diff --git a/doc/Eqs/eff_energy_expression.tex b/doc/Eqs/eff_energy_expression.tex new file mode 100644 index 0000000000..f56380f646 --- /dev/null +++ b/doc/Eqs/eff_energy_expression.tex @@ -0,0 +1,9 @@ +\documentclass[12pt]{article} + +\begin{document} + +$$ +U\left(R,r,s\right) = E_{NN} \left( R \right) + E_{Ne} \left( {R,r,s} \right) + E_{ee} \left( {r,s} \right) + E_{KE} \left( {r,s} \right) + E_{PR} \left( { \uparrow \downarrow ,S} \right) +$$ + +\end{document}