Sec III
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@ -312,7 +312,8 @@ which satisfied the following condition \cite{Kehrein_2006}
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This implies that the matrix elements of the off-diagonal part decrease in a monotonic way throughout the transformation.
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Moreover, the coupling coefficients associated with the highest-energy determinants are removed first as we shall evidence in the perturbative analysis below.
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The main drawback of this generator is that it generates a stiff set of ODE which is therefore difficult to solve numerically. \cite{Hergert_2016a}
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However, here we will not tackle the full SRG problem but only consider analytical low-order perturbative expressions so we will not be affected by this problem. \cite{Evangelista_2014,Hergert_2016}
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However, here we will not tackle the full SRG problem but only consider analytical low-order perturbative expressions.
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Hence, we will not be affected by this problem. \cite{Evangelista_2014,Hergert_2016}
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Let us now perform the perturbative analysis of the SRG equations.
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For $s=0$, the initial problem is
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