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@ -482,7 +482,7 @@ and ensuring that $\w{}{\lr,\rsmu{}{}}(\br{1},\br{2})$ and $\W{\wf{}{\Bas}}{}(\b
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\label{eq:mu_of_r}
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\label{eq:mu_of_r}
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\rsmu{\wf{}{\Bas}}{}(\br{}) = \frac{\sqrt{\pi}}{2} \W{\wf{}{\Bas}}{}(\bx{},\Bar{\bx{}}),
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\rsmu{\wf{}{\Bas}}{}(\br{}) = \frac{\sqrt{\pi}}{2} \W{\wf{}{\Bas}}{}(\bx{},\Bar{\bx{}}),
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\end{equation}
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\end{equation}
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where $(\bx{},\Bar{\bx{}})$ represents a couple of same-spin electrons at the same position $\br{}$.
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where $(\bx{},\Bar{\bx{}})$ represents a couple of opposite-spin electrons at the same position $\br{}$.
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%More precisely, if we define the value of the interaction at coalescence as
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%More precisely, if we define the value of the interaction at coalescence as
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%\begin{equation}
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%\begin{equation}
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% \label{eq:def_wcoal}
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% \label{eq:def_wcoal}
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References/ Gruneis_2017.pdf
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References/Gruneis_2013.pdf
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References/Gruneis_2013.pdf
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References/Haunschild_2009(SI).pdf
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References/Haunschild_2009(SI).pdf
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References/Haunschild_2009.pdf
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References/Haunschild_2009.pdf
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References/Irmler_2019a.pdf
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References/Irmler_2019a.pdf
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References/Irmler_2019b.pdf
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References/Irmler_2019b.pdf
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