# Solutions of $a^{a^x}=x$ for fixed $a>0$

I am interested in the equation $a^{a^x}=x$ for some fixed $a>0$. Is there some way to rearrange for $x$ or solve otherwise? What about the nature of the solutions? For which fixed $a>0$ are there any real solutions $x>0$, and how many?

I already worked with the equation $a^x=x$ and I can deal with it. I learned from the comments that a real solution exists for $a\le e^{1/e}$ and is given by

$$x=-\frac{W(-\ln(a))}{\ln(a)}$$

with the Lambert W function. But the equation above is out of reach for me.

• I'm curious to see how you solved the first equation.
– user223391
Commented Oct 26, 2017 at 13:02
• Just one short comment, possibly I can do later an answer. If $a^x=x$ then of course $a^{a^x}=x$ so the problem is obviously to find more or the other fixpoints for the latter. Commented Oct 28, 2017 at 6:03
• Also we can write more symmetrical $(a^x)^{(a^x)}=x^x$ where it is also visible, that some fixpoint $x_0=a^{x_0}$ is of course a solution. But it might be also a starting point to find other solutions $x_1$ where $x_1 \ne a^{x_1}$ ... Commented Oct 28, 2017 at 6:49
• By a plot, for $1<a<e^{-e}$ I can't see additional real fixpoints for $\large a^{a ^x}$ besides that of $a ^x$ (The latter are of course given by $x_\text{lo}=\exp(-W_0(-\log(a))$ and $x_\text{hi}=\exp(-W_{-1}(-\log(a))$) Commented Oct 28, 2017 at 7:16
• Plotting shows, that only for $0<a<1/e^e$ there are two more real fixpoints for $a^{a^x}$ besides the real fixpoints of $a^x$. (For $e^{-e} <a$ there are no real fixpoints at all.) Commented Oct 28, 2017 at 8:01

Remark: I have not yet a closed-form formula for the occuring fixpoints, but to put the earlier comments together and to give at least a simple computational procedure to determine the additional fixpoints.

1. ) To "symmetrize" the formula we observe, that we can as well write $$(a^x)^{(a^x)} = x^x \tag 1$$ This makes even more obvious, that $f(x)=a^{a^x}$ has the same fixpoints as $g(x)=a^x$ (We have $f(x)=g(g(x))$ so this is of course basically obvious).
.
Let $t= \exp(-W_0(-\log(a)))$ then $a=t^{1/t}$ and $(t^{1/t})^t=t^1=t$ and $t$ is a fixpoint (may be complex).

2. ) By a plot we find in four ranges for $a$ different behaviour. $$\begin{array} {} (1)& e^{1/e}& <a &<\infty & 0 \text{ real fixpoint for g(x) and f(x) } \\ (2)& e^{1/e} &= a & & 1 \text{ real fixpoint for g(x) and f(x) } \\ (3)& 1 &< a &< e^{1/e} & 2 \text{ real fixpoints for g(x) and f(x) } \\ (4)& e^{-e} &\le a & \le 1 & 1 \text{ real fixpoint for g(x) and f(x) } \\ (5)& 0 &< a & < e^{-e} & 1 \text{ real fixpoint for g(x) and f(x) } \\ & & & & \text {and 2 more real fixpoints for f(x) } \end{array} \tag 2$$

3. ) Where possible, the "standard" real fixpoint $t$ is computed using the LambertW using $W_0(x)$ and in case (3) we find another one using $W_{-1}(x)$. For case 5 we can find the two other fixpoints $u$ (lower),$v$ (upper) by the following routine

Pseudocode:

let a=0.01
let u=0, v=1
for k=1 to 10: u, v = a^v, a^u : end  \\ to approximate initially
\\ use Newton-algorithm to approximate second fixpoint to high precision
err=1
while err>1e-200
err = (a^a^u - u )/(a^a^u * a^u * log(a)^2 - 1)
u = u-err
wend
\\ find the third fixpoint v
v = a^u


Example: For base $a=0.01$ I find the first fixpoint for $f(x)$ and $g(x)$ using the Lambert $W_0()$-function as $t=0.27798742481...$ .
The two additional fixpoints for $f(x)$ are $u=0.013092520508...$ and $v= 0.941488368575...$ .

1. ) We have for bases of the case (5)
$$\large \begin{array} {} a^{a^t}=t & a^{a^u}=u &a^{a^v}=v & \small \text{all are fixpoints of f(x) }\\ a^t = t &a^u = v & a^v = u \\ a=t^{1/t} &a = u^{1/v} & a = v^{1/u} \end{array}$$

Perhaps from the last equalitites one can derive more closed-form expressions using Lambert W...

Picture for the three fixpoints for bases $0<b<1/e^e$ (sorry that I used "b" instead of your "a" for the base, it is my long-trained notation)

• Thank you. You not only answered my question, but also provided me with a new thought toward the “solutions of Lambert W-like functions”. Commented Oct 29, 2017 at 0:45
• You're welcome! You made me myself curious about such a closed-form solution... I'll have my paper&pen at hand later ... Commented Oct 29, 2017 at 0:56
• Of possible historical interest is Jeran-H. Grillet (??-??), Les exponentielles successives d'Euler et les logarithmes des différents ordres des nombres [Successive exponentials of Euler and logarithms of different orders of numbers], Journal de Mathématiques Pures et Appliquées 10 #6 (June 1845), 233-241. The special case $x = b^{b^x}$ is discussed in several places (e.g. pp. 235-237, 240). Commented Oct 29, 2017 at 13:13
• @Dave - thanks for the nice article. I don't understand french besides some "keywords" but with the sequel of formulae I could roughly follow what he was writing. 1845! Clever people use a notation hinting at to what they denote: in particular, they use "b" for the base of exponentiation. And if they have two fixpoints (or periodic points) one low and one high they use the same letter (c) in low and in capital notation so many formulae are better self-explaining than usually. Next: he had no possibility of doing a plot on-the-fly... Commented Oct 29, 2017 at 13:32
• nice work Gottfried! I tried a=0.07, which is a little bit bigger than exp(-e); and I found a complex conjugate fixed point pair; 0.359606324 + 0.135584257*I. So probably there is an analytic function in the square root in the neighborhood of $\sqrt{a-\exp(-e)}$ for the fixed point of $a^{a^z}$.. Commented Oct 30, 2017 at 10:00

I found a way to rearrange for $x$ which works for some $a$ and yields some solution! Some rigorous analysis is necessary to completely understand this procedure and to find similar forms of the other (real) solutions (there are zero to three). I still hope this might help you.

So let's start from $a^{a^x}=x$ for $a,x>0$, and state it like Gottfried did as $(a^x)^{a^x}=x^x$. There is the well known way to parametrize some solutions of $x^x=y^y$, which is

$$x=t^{\frac{1}{1-t}},\qquad y=t^{\frac t{1-t}}$$

for $t>0$. So, to solve the above problem, we are looking for a value $t$ for which we have

$$x=t^{\frac{^1}{1-t}},\qquad a^x=t^{\frac t{1-t}}.$$

The left equation can be rearranged for $t$ and we get $t=\frac{W(x\log x)}{\log x}$. When we plug this into the right side we find

$$a^x = \left(t^{\frac 1{1-t}}\right)^t=x^t=x^{\frac{W(x\log x)}{\log x}}\quad\Rightarrow\quad a=x^{\frac{W(x\log x)}{x\log x}}=x^{\frac{W(u)}u}$$

with $u=x\log x$. This gives $x=u/W(u)$ and

$$a=\left(\frac{W(u)}u\right)^{-\frac{W(u)}u}=z^{-z}$$

with $z=W(u)/u$. We can solve for $z$ and finally find

$$z=-\frac{\log a}{W(-\log a)}.$$

which can be used to find $u$ via $u=-\log (z)/z$. The final solution might look something like this:

Solution. $$x =\frac{u}{W(u)} =\frac{-\frac{\log z}{z}}{W(-\frac{\log z}{z})} =\frac{\frac{\log \left(-\frac{\log a}{W(-\log a)}\right)}{\frac{\log a}{W(-\log a)}}}{W\left(\frac{\log \left(-\frac{\log a}{W(-\log a)}\right)}{\frac{\log a}{W(-\log a)}}\right)}$$

Of course, this monstrous formula should never be used. Instead use the resubstituation like this:

$$z=-\frac{\log a}{W(-\log a)} \quad\to\quad u=-\frac{\log (z)}{z} \quad\to\quad x=\frac{u}{W(u)}.$$

Example. Choosing $a=1/2$ and above formula gave me the solution $x\approx 0.641186$ which indeed solves $a^{a^{x}}=x$.

I also tested it with $a=2$, which yielded a complex solution $x\approx 0.824679 - 1.56743i$ which worked, but shed no light on whether there are any other real ones.

Gottfried mentioned in the comments that it seems not to work for e.g. $a=0.01$. This is why more investigations are necessary.

Gottfried hinted me to the fact that this can be simplified (at least for some $a$) to the function

$$x(a)=\exp(-W(-\log(a))).$$

This seems to work for all $a$ (in contrast to my resubstituation formula above), but still gives only a single solution. Maybe the other branches of $W$ can give other real solutions, but not sure.

• Hmm, that seems to me to contain a needless loop... You get the value $x=0.641186$ simply by $x=\exp(-W(-\log(a)))$ . Simple plots show that for base $a=2$ you won't have any real fixpoint. For the base from the intersting range, where the bases $a$ provide $3$ fixpoints (my example $a=0.01$) your formula gave $0.465786959979$ which I can so far not relate to the three solutions in my answer. (But I'll try to find some ralation) Commented Nov 1, 2017 at 11:36
• @GottfriedHelms That's very interesting! I made no effort to simplify this, because I was satisfied by the fact that I was able to rearrange it! Yes, we probably already know that there is no real solution for $a=2$, but this cannot be seen from my current approach. Commented Nov 1, 2017 at 11:38
• @GottfriedHelms You are right. My approach seems to be restricted so some specific range (which I do not know). Your formula gives $x\approx 0.277987$ which works. Commented Nov 1, 2017 at 11:42
• I just checked a base $1<b< e^{1/e}$ - here your final 3-step formula works. So perhaps this has something to do with range-restrictions in the Lambert W-function. Perhaps try by analysis of different branches? Commented Nov 1, 2017 at 11:47
• For base $a=2$ Wolfram Alpha finds your value too: $x(2) = 0.824678546142 + 1.56743212385*I$ so your method seems to work at least for $1<a$ and not only for the restricted range which I've checked in my previous comment. Commented Nov 1, 2017 at 11:56

In a previous mathstack question I posted a formal series solution for finding the fixed points of $z \mapsto \exp(z)-1+k$. This analytic Taylor series in $\sqrt{-2k}$ can generate both fixed points for bases between $1 < a < \exp(1/e)$ as well as the complex conjugate pair of fixed points for bases $>\exp(1/e)$, and works for complex bases, as well as real bases<1. Since that post, I I have a better way to formally calculate that series.

For the Op's question, it seemed there might be a series that could work in the neighborhood of $\exp(-e)$, to generate the two periodic solutions. I was able to generate just such a series which work wells for $0<a\approx<0.6$. For calculating Gottfried's fixed point pair solution for $a^{a^x}$ for $0<a<e^{-e}$. we need this new Taylor series, which is centered on the parabolic fixed point with multiplier -1. We expect that the solution would be analytic in $\sqrt{x-\exp(-e)}$. But just as with the earlier problem, it is simplest to find such a Taylor series using a mathematically "congruent" problem.

For the Ops problem, $a^{a^x}$, for $0<a<1$ I use this congruence equation, where we want period2 fixed points of $f(y)$ with $$k=\ln(-\ln(a))-1$$ and then we can instead iterate: $$y \mapsto f(y,k);\;\; \text{where} \;\;\;f(y,k)=-\exp(y)+1+k;\;\;\;\;\text{and}\;\;\;\;y=z\ln(a)+\ln(-\ln(a));$$ $$z \mapsto a^z;\;\;\;\text{is congruent to}\;\;\; y \mapsto f(y,k);\;\;\;\; k=\ln(-\ln(a))-1;$$ $$f\big(z\ln(a)+\ln(-\ln(a))\big)=(a^z)\ln(a)+\ln(-\ln(a));\;\;\; f \; \text{is congruent to}\; a^z$$

k=0 corresponds to $a=\exp(-e)$, which has a multiplier of -1. The two periodic fixed points of $f(y,k)$ has a series which I shall call $g$, whose definition is below. We then find a formal series solution for the two periodic fixed point pairs of $f(f(x,k))=x$

$$f(x,k) = -\exp(x)+1+k$$ $$f(g(\sqrt{6k},k) = g(-\sqrt{6k})\;\;\;\;\text{g(-x) is the other fixed point}$$ $$-\exp((g(\sqrt{6k}))+1+k = g(-\sqrt{6k})\;\;\;\;\text{definition of f}$$ $$-\exp(g(x))+1+\frac{x^2}{6}=g(-x)\;\;\;\;\text{by substituting k=x^2/6}$$

That is the formal series definition for g, where the $x^2/6$ term was chosen so that the for the g Taylor series below, the x^1 coefficient=1. In this equation, $g(x)$ corresponds to one fixed point, and $g(-x)$ corresponds to the other fixed point.

And the two cycle fixed point of $y\mapsto -\exp(y)+1+k$ may be found by $y=g(\pm\sqrt{6k})$. And then the fixed point pair of z for $z\mapsto a^{a^z}$ may be found by using this equation:

$$z=\frac{g(\pm\sqrt{6k})-\ln(-\ln(a))}{\ln(a)};\;\;\;\; k=\ln(-\ln(a))+1$$

The first 16 terms of the series for g are as follows. I wrote a pari=gp program to calculate the formal series for g which requires iterating solving 2x2 simultaneous equations for pairs of consecutive terms, but it is not too bad. With enough terms, the series can be used on its own, or the series can be used as an input to Newton's method to get a more accurate answer.

g=
+x^ 1*  1
+x^ 2* -1/6
+x^ 3*  1/20
+x^ 4* -1/90
+x^ 5*  523/151200
+x^ 6* -23/28350
+x^ 7*  239/1008000
+x^ 8* -19/340200
+x^ 9*  1471949/100590336000
+x^10* -6583/1964655000
+x^11*  94891697/130767436800000
+x^12* -49909/328378050000
+x^13*  18670028801/988601822208000000
+x^14* -520019/241357866750000
+x^15* -88448773393/67224923910144000000
+x^16*  254033333/492370048170000000 ....


So lets say we want to two real fixed points for $a^{a^z}$ for a=0.04 Then $k=\ln(-\ln(0.04))-1\approx 0.1690321758870$, and we want $g(\pm\sqrt{6k})$ so we wind up with z=0.0896008408659, 0.749451269718 as the two fixed points. For this case, the 16 term series is accurate to about 10-11 decimal digits, and a 48 term series is accurate to 26 decimal digits. Surprisingly with a 16 term series for a=0.01, we still get ~5 decimal digits of precision.

One can also get the complex conjugate pair of fixed points for $a>-\exp(-e)$, for example for $a=0.1$ we get the following pair of complex conjugate fixed points, also accurate to about 10 decimal digits using the 16 term series above. z=0.294596558514 +/- 0.413195411460*I

Here is a graph of the fixed points from 0.001 to 0.3. You can compare this graph to Gottfried's graph, where I have added the complex conjugate fixed points for x>exp(-e). The fixed points meet at exp(-e). We see the complex conjugate pair of fixed points to the right, and the real pair of fixed points to the left, as well as the primary real fixed point which is calculated by another method.

For the real solutions of equation $$(E): a^{a^x}=x$$. I can provide you with an elementary solution to discuss the number of solutions with respect to the values of $$a$$.

1. First of all, one can easily see that the solutions of $$(E'): {a^x}=x$$ are also solutions of $$(E)$$. So, $$S'\subset S$$.
2. By studying the variations of $$g(x)=a^x-x$$, one finds:

$$\bullet$$ If $$0 or $$a=e^{\frac{1}{e}}$$, then $$\#S'=1$$.

$$\bullet$$ If $$1, then $$\#S'=2$$.

$$\bullet$$ If $$a>e^{\frac{1}{e}}$$, then $$\#S'=0$$.

1. Now, from the variations of $$f(x)=a^x-\dfrac{ln(x)}{ln(a)}$$, where $$a\neq1$$, since $$(E)$$ is equivalent to $$a^x=\dfrac{ln(x)}{ln(a)}$$, one can establish that:

$$\bullet$$ If $$0: Then, $$f$$ has two horizontal tangents at $$\alpha$$ and $$\beta$$ such that $$\alpha<\dfrac{-1}{ln(a)}<\beta$$, with $$\lim_{x\to\pm\infty} f(x)=\pm\infty$$, $$f$$ increasing over $$]0,\alpha[\cup]\beta,+\infty[$$ and decreasing over $$]\alpha,\beta[$$. But since, $$f((\dfrac{-1}{ln(a)})^z)<0,~\forall z\geq1$$. Then, $$f(\alpha)<0$$ and $$f(\beta)<0$$. Hence, $$\#S=1$$.

$$\bullet$$ If $$e^{-e}\leq a<1$$: Then, $$f$$ increasing over $$]0,+\infty[$$, $$f(0)=-1$$ and $$\lim_{x\to+\infty} f(x)=+\infty$$. So, $$\#S=1$$.

$$\bullet$$ If $$1: One has $$S'\subset S$$, $$\#S'=2$$ and $$\#S\leq2$$. So, $$\#S=2$$.

$$\bullet$$ If $$a=e^{\frac{1}{e}}$$: Then, $$f$$ has a horizontal tangent at $$e$$, $$\lim_{x\to\pm\infty} f(x)=+\infty$$ and $$f(e)=0$$. So, $$\#S=1$$.

$$\bullet$$ If $$a>e^{\frac{1}{e}}$$: Then, $$\#S\leq2$$. Let's suppose that $$S=\{x_1,x_2\}$$, with $$x_1. Hence, $$a^{x_1} are also solutions. So, $$a^{x_1}=x_1$$ and $$a^{x_2}=x_2$$. Then, $$S\subset S'=\emptyset$$, a contradiction. Again, by the same argument, we prove that $$\#S=0$$.

To summerize:


$$\#S=0$$ if and only if $$a>e^{\frac{1}{e}}$$.

$$\#S=1$$ if and only if $$0 or $$a=e^{\frac{1}{e}}$$.

$$\#S=2$$ if and only if $$1.

$$a^{a^x}=x$$ $$a^{a^x}-x=0$$

We see, this equation is a polynomial equation of more than one algebraically independent monomials ($$a^{a^x},x$$) and with no univariate factor. We therefore don't know how to rearrange the equation for $$x$$ by applying only finite numbers of elementary functions (elementary operations) we can read from the equation.

a)

As can be seen from the comment of Gottfried Helms, the solution can be guessed with a special trick as the solution of the equation

$$a^x=x$$

as

$$x=-\frac{W_k(-\ln(a))}{\ln(a)}\ \ (\forall k\in\mathbb{Z})$$

in terms of Lambert W.

b)

Without any special trick, we can bring the equation into a form for applying Hyper Lambert W.

$$e^{\ln(a)e^{\ln(a)x}}=x$$ $$1=xe^{-\ln(a)e^{\ln(a)x}}$$ $$xe^{-\ln(a)e^{\ln(a)x}}=1$$

$$G\left(-\ln(a),\ln(a);x\right)=1$$ $$x=HW\left(-\ln(a),\ln(a);1\right)$$

So we have a closed form for $$x$$, and the representations of Hyper Lambert W give some hints for calculating $$x$$.

Galidakis, I. N.: On solving the p-th complex auxiliary equation $$f^{(p)}(z)=z$$. Complex Variables 50 (2005) (13) 977-997

Galidakis, I. N.: On some applications of the generalized hyper-Lambert functions. Complex Variables and Elliptic Equations 52 (2007) (12) 1101-1119