Manu: added some notes to explain the final energy expressions
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@ -426,7 +426,45 @@ Hxc}\left[n\right]}{\partial w_K}\right|_{n=n^{{\bw}}}.
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\eeq
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%+\Tr(\bmg^{(I)} \, \bG \, \bmg^{\bw})
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%-\dfrac{1}{2}\Tr(\bmg^{\bw} \, \bG \, \bmg^{\bw})+...
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\alert{
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Note that
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\beq
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\overline{E}^{{\bw}}_{\rm
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Hx}\left[n^{{\bw}}\right]=
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\frac{1}{2} \sum_{L\geq0}w_L \Tr(\bmg^{(L)} \, \bG \, \bmg^{(L)})
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-\frac{1}{2}\Tr(\bmg^{\bw} \, \bG \, \bmg^{\bw})
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\nonumber\\
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\eeq
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and
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\beq
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\left.\dfrac{\partial \overline{E}^{{\bw}}_{\rm
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Hx}[n]}{\partial w_K}\right|_{n=n^{\bw}}&=&
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\frac{1}{2} \Tr(\bmg^{(K)} \, \bG \, \bmg^{(K)})-\frac{1}{2}
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\Tr(\bmg^{(0)} \, \bG \, \bmg^{(0)})
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\nonumber\\
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&&-\Tr\left[\left({\bmg}^{(K)}-{\bmg}^{(0)}\right) \, \bG \, \bmg^{\bw}\right]
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+\ldots
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\eeq
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thus leading to
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\beq
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&&\overline{E}^{{\bw}}_{\rm
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Hx}\left[n^{{\bw}}\right]+\sum_{K>0}\left(\delta_{IK}-w_K\right)\left. \dfrac{\partial \overline{E}^{{\bw}}_{\rm
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Hx}\left[n\right]}{\partial w_K}\right|_{n=n^{{\bw}}}
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\nonumber\\
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&&=
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\overline{E}^{{\bw}}_{\rm
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Hx}\left[n^{{\bw}}\right]+\frac{1}{2} \Tr(\bmg^{(I)} \, \bG \, \bmg^{(I)})
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-\frac{1}{2} \sum_{L\geq0}w_L \Tr(\bmg^{(L)} \, \bG \, \bmg^{(L)})
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\nonumber\\
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&&-\Tr\left[\left({\bmg}^{(I)}-{\bmg}^{\bw}\right) \, \bG \, \bmg^{\bw}\right]
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+\ldots
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\nonumber\\
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&&=\frac{1}{2} \Tr(\bmg^{(I)} \, \bG \,
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\bmg^{(I)})-\Tr\left[\left({\bmg}^{(I)}-\dfrac{1}{2}\bmg^{\bw}\right)
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\, \bG \, \bmg^{\bw}\right]
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+\ldots
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\eeq
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}
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At the eLDA level:
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\beq
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