08/29/2022, 07:51 AM
Thank you Gottfried, for giving me some introduction to divergent summation!
But with this approach we might not need Borel summation at all, we can just take a truncation of the divergent series - say \(h_N(x)\) - and set
\begin{align}
h_{\leftarrow}(x) &= \lim_{n\to\infty} (f^{\circ -n}(h_N(f^{\circ n}(x))))\\
h_{\rightarrow}(x) &= \lim_{n\to\infty} (f^{\circ n}(h_N(f^{\circ -n}(x))))
\end{align}
where \(f(x)=e^x-1\).
I am not completely sure how big N needs to be, but practically you get high precision with N=20 (I guess N=2 would be the minimum).
It is very similar to the hyperbolic half iterate where you have the formula
\[ \lim_{n\to\infty} (f^{\circ -n}(f'(0)^{\frac{1}{2}}(f^{\circ n}(x)))) \]
where so to say only the first coefficient of the formal powerseries of the half-iterate is taken, but which you could improve by taking more coefficients.
(08/28/2022, 09:26 PM)Gottfried Wrote: Practically using software we deal with truncated series; but the Borel-sum requires that in the terms of the series as well as the coefficient \( x^k \) or \( x^{rk} \) is present, and we know, that for large \( x \) the exponential series increases to huge values before the influence of the denominator begins to diminuish and suppress that \(x^k\) term. So we cannot really compute with arbitrary large \( x \) (which would be required) but only such large values, that our finitely long exponentialseries has dominated that \(x^k \) or \( x^{rk}\) values. So the implementation of this version of the Borel sum is never really perfectI think what you describe they call "weak Borel summation" and it seems it has the same issue as the "strong" integral version, that you need to check how big your x or t should grow.
For instance, to sum the halfiterate of the \( \exp(z)-1 \) I needed order \( r=2 \) but could not use \( x \gt 70 \) say, because of having only 256 or 512 transformed terms. Having 1024 terms, one could insert \( x \) with value of around 80 or 100 and can thus achieve more digits precision.
(08/28/2022, 09:26 PM)Gottfried Wrote: P.s.: Practically we need only the proof on concept. After we know that Borel-summation can manage the current growthrate of the \( a_k \) or more precisely that of the \( s_k \) we had of course the possibility not to use \( z=1 \) but the -say- 40th iteration towards 0 by negative height getting \( z_{-40} \lt 1e-10 \), use then for the partial sums \( s_k = \sum_{j=0}^k z_{-40}^k \cdot a_k \) and get nearly exact values for the Borel-sum because \( x \) can now go much farther to \( \infty \) .
But with this approach we might not need Borel summation at all, we can just take a truncation of the divergent series - say \(h_N(x)\) - and set
\begin{align}
h_{\leftarrow}(x) &= \lim_{n\to\infty} (f^{\circ -n}(h_N(f^{\circ n}(x))))\\
h_{\rightarrow}(x) &= \lim_{n\to\infty} (f^{\circ n}(h_N(f^{\circ -n}(x))))
\end{align}
where \(f(x)=e^x-1\).
I am not completely sure how big N needs to be, but practically you get high precision with N=20 (I guess N=2 would be the minimum).
It is very similar to the hyperbolic half iterate where you have the formula
\[ \lim_{n\to\infty} (f^{\circ -n}(f'(0)^{\frac{1}{2}}(f^{\circ n}(x)))) \]
where so to say only the first coefficient of the formal powerseries of the half-iterate is taken, but which you could improve by taking more coefficients.
