Difference between revisions of "Shell-Thron region"
(Adding Tetrationforum reference) |
m (explicating) |
||
| Line 15: | Line 15: | ||
These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch. | These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch. | ||
| − | The following picture was made by [[User:Andydude|Andrew]]. | + | The following picture of the upper part of the Shell-Thron region was made by [[User:Andydude|Andrew]]. |
[[File:Shell-region.png]] | [[File:Shell-region.png]] | ||
Revision as of 17:54, 4 June 2011
The Shell-Thron region is the region of complex numbers $b$ where the limit of the infinite exponential tower $$\lambda=\lim_{n\to\infty} \exp_b^{\circ n}(1)$$ exists; to be explicit we mean the main branch of the power: $\exp_b(z):=b^z:=\exp(\log(b)z)$.
If this limit $\lambda$ exists then must $b^\lambda=\lambda$, i.e. $\lambda$ must be a fixpoint of $f(z)=b^z$ and $b=\lambda^{1/\lambda}$, or $$\lambda=\frac{W(-\log(b))}{-\log(b)}$$
By a result of Barrow the limit $\lambda$ exists exactly for all $b$ where $|\log(\lambda)|\le 1$.
The boundary of the Thron-Shell region, i.e. all bases $b$ where $|\log(\lambda)|=1$, is given by all $b$ where $|\exp_b'(\lambda)|=1$ due to the following rearrangements: $$\begin{align*} 1=|\exp_b'(\lambda)|=|\log(b)\exp_b(\lambda)|=|\log(b)\lambda|=|\log(\lambda^{1/\lambda})\lambda|=|\log(\lambda)| \end{align*}$$
These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch.
The following picture of the upper part of the Shell-Thron region was made by Andrew.