saving work in Shanks
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@ -1581,7 +1581,7 @@ While the diagonal quadratic approximants provide significanty improved estimate
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ground-state energy, we can use our knowledge of the UMP singularity structure to develop
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even more accurate results.
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We have seen in previous sections that the UMP energy surface
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contains only \titou{square-root branch cuts} that approach the real axis in the limit $U/t \to \infty$.
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contains only square-root branch cuts that approach the real axis in the limit $U/t \to \infty$.
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Since there are no true poles on this surface, we can obtain more accurate quadratic approximants by
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taking $d_q = 0$ and increasing $d_r$ to retain equivalent accuracy in the square-root term [see Eq.\eqref{eq:QuadApp}].
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Figure~\ref{fig:nopole_quad} illustrates this improvement for the pole-free [3/0,4] quadratic
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@ -1633,7 +1633,8 @@ that can be used to extract further information about the exact result.
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The Shanks transformation presents one approach for extracting this information
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and accelerating the rate of convergence of a sequence.\cite{Shanks_1955,BenderBook}
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\hugh{Consider the partial sums
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\titou{T2: $N$ is defined as the number of electrons. Maybe we should use $n$ instead?}
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Consider the partial sums
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$S_N = \sum_{k=0}^{N} a_k$
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defined from the truncated summation of an infinite series
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$ S = \sum_{k=0}^{\infty} a_k$.
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@ -1642,7 +1643,7 @@ If the series converges, then the partial sums will tend to the exact result
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\lim_{N\rightarrow \infty} S_N = S.
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\end{equation}
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The Shanks transformation attempts to generate increasingly accurate estimates of this
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limt by defining a new series as
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limit by defining a new series as
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\begin{equation}
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T(S_N) = \frac{S_{N+1} S_{N-1} - S_{N}^2}{S_{N+1} + S_{N-1} - 2 S_{N}}.
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\end{equation}
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@ -1655,7 +1656,7 @@ the approximate form
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\end{equation}
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Furthermore, while this transformation can accelerate the convergence of a series,
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there is no guarantee that this acceleration will be fast enough to significantly
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improve the accuracy of low-order approximations.}
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improve the accuracy of low-order approximations.
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\hugh{To the best of our knowledge, the Shanks transformation has never previously been applied
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to the acceleration of the MP series.
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