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	<title>Double exponential function - Revision history</title>
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		<title>imported&gt;Grafen: /* top */ clean up, replaced: due to the fact that → because</title>
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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;top: &lt;/span&gt; clean up, replaced: due to the fact that → because&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{short description|Exponential function of an exponential function}}&lt;br /&gt;
[[Image:Double Exponential Function.svg|right|thumb|320px|A double exponential function (red curve) compared to a single exponential function (blue curve).]]&lt;br /&gt;
&lt;br /&gt;
A &amp;#039;&amp;#039;&amp;#039;double exponential&amp;#039;&amp;#039;&amp;#039; function is a [[Constant (mathematics)|constant]] raised to the power of an [[Exponentiation|exponential function]].  The general formula is &amp;lt;math&amp;gt;f(x) = a^{b^x}=a^{(b^x)}&amp;lt;/math&amp;gt; (where &amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;gt;1 and &amp;#039;&amp;#039;b&amp;#039;&amp;#039;&amp;gt;1), which grows much more quickly than an exponential function. For example, if &amp;#039;&amp;#039;a&amp;#039;&amp;#039; = &amp;#039;&amp;#039;b&amp;#039;&amp;#039; = 10:&lt;br /&gt;
*&amp;#039;&amp;#039;f&amp;#039;&amp;#039;(x) = 10&amp;lt;sup&amp;gt;10&amp;lt;sup&amp;gt;x&amp;lt;/sup&amp;gt;&amp;lt;/sup&amp;gt;&lt;br /&gt;
*&amp;#039;&amp;#039;f&amp;#039;&amp;#039;(0) = 10&lt;br /&gt;
*&amp;#039;&amp;#039;f&amp;#039;&amp;#039;(1) = 10&amp;lt;sup&amp;gt;10&amp;lt;/sup&amp;gt;&lt;br /&gt;
*&amp;#039;&amp;#039;f&amp;#039;&amp;#039;(2) = 10&amp;lt;sup&amp;gt;100&amp;lt;/sup&amp;gt; = [[googol]]&lt;br /&gt;
*&amp;#039;&amp;#039;f&amp;#039;&amp;#039;(3) = 10&amp;lt;sup&amp;gt;1000&amp;lt;/sup&amp;gt;&lt;br /&gt;
*&amp;#039;&amp;#039;f&amp;#039;&amp;#039;(100) = 10&amp;lt;sup&amp;gt;10&amp;lt;sup&amp;gt;100&amp;lt;/sup&amp;gt;&amp;lt;/sup&amp;gt; = [[googolplex]].&lt;br /&gt;
&lt;br /&gt;
[[Factorial]]s grow faster than exponential functions, but much more slowly than double exponential functions. However, [[tetration]] and the [[Ackermann function]] grow faster. See [[Big O notation]] for a comparison of the rate of growth of various functions.&lt;br /&gt;
&lt;br /&gt;
The inverse of the double exponential function is the [[Logarithm#double logarithm|double logarithm]] log(log(&amp;#039;&amp;#039;x&amp;#039;&amp;#039;)). The complex double exponential function is [[Entire function|entire]], because it is the composition of two entire functions &amp;lt;math&amp;gt;f(x)=a^x=e^{x\ln a}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;g(x)=b^x=e^{x\ln b}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Double exponential sequences==&lt;br /&gt;
&lt;br /&gt;
A sequence of positive integers (or real numbers) is said to have &amp;#039;&amp;#039;double exponential rate of growth&amp;#039;&amp;#039; if the function giving the {{mvar|n}}th term of the sequence is bounded above and below by double exponential functions of {{mvar|n}}.&lt;br /&gt;
Examples include&lt;br /&gt;
* The [[Fermat number]]s &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;F(m) = 2^{2^m}+1&amp;lt;/math&amp;gt;&lt;br /&gt;
* The harmonic primes: The primes &amp;#039;&amp;#039;p&amp;#039;&amp;#039;, in which the sequence {{nowrap|1/2 + 1/3 + 1/5 + 1/7 + ⋯ + 1/&amp;#039;&amp;#039;p&amp;#039;&amp;#039;}} exceeds 0, 1, 2, 3, …{{pb}}The first few numbers, starting with 0, are 2, 5, 277, 5195977, ... {{OEIS|A016088}}&lt;br /&gt;
* The [[Double Mersenne number]]s &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;MM(p) = 2^{2^p-1}-1&amp;lt;/math&amp;gt;&lt;br /&gt;
* The elements of [[Sylvester&amp;#039;s sequence]] {{OEIS|A000058}} &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;s_n = \left\lfloor E^{2^{n+1}}+\frac12 \right\rfloor&amp;lt;/math&amp;gt; where &amp;#039;&amp;#039;E&amp;#039;&amp;#039; ≈ 1.264084735305302 is [[Vardi&amp;#039;s constant]] {{OEIS|A076393}}.&lt;br /&gt;
* The number of [[Arity|&amp;#039;&amp;#039;k&amp;#039;&amp;#039;-ary]] [[Boolean function]]s: &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;2^{2^k}&amp;lt;/math&amp;gt;&lt;br /&gt;
* The prime numbers 2, 11, 1361, ... {{OEIS|A051254}} &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;a(n) = \left\lfloor A^{3^n}\right\rfloor&amp;lt;/math&amp;gt; where &amp;#039;&amp;#039;A&amp;#039;&amp;#039; ≈ 1.306377883863 is [[Mills&amp;#039; constant]].&lt;br /&gt;
&lt;br /&gt;
[[Alfred Aho|Aho]] and [[Neil Sloane|Sloane]] observed that in several important [[integer sequence]]s, each term is a constant plus the square of the previous term. They show that such sequences can be formed by rounding to the nearest integer the values of a double exponential function with middle exponent 2.&amp;lt;ref&amp;gt;{{citation|first1=A. V.|last1=Aho|author-link1=Alfred Aho|first2=N. J. A.|last2=Sloane|author-link2=N. J. A. Sloane|url=http://neilsloane.com/doc/doubly.html|title=Some doubly exponential sequences|journal=[[Fibonacci Quarterly]]|volume=11|year=1973|pages=429–437}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
Ionaşcu and Stănică describe some more general sufficient conditions for a sequence to be the floor of a double exponential sequence plus a constant.&amp;lt;ref&amp;gt;{{citation&lt;br /&gt;
 | last1 = Ionaşcu | first1 = Eugen-Julien&lt;br /&gt;
 | last2 = Stănică | first2 = Pantelimon&lt;br /&gt;
 | issue = 1&lt;br /&gt;
 | journal = Acta Mathematica Universitatis Comenianae&lt;br /&gt;
 | pages = 75–87&lt;br /&gt;
 | title = Effective asymptotics for some nonlinear recurrences and almost doubly-exponential sequences&lt;br /&gt;
 | volume = LXXIII&lt;br /&gt;
 | url = http://faculty.nps.edu/pstanica/research/AMUC04.pdf&lt;br /&gt;
 | year = 2004}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Applications==&lt;br /&gt;
===Algorithmic complexity===&lt;br /&gt;
In [[computational complexity theory]], [[2-EXPTIME]] is the class of decision problems solvable in double exponential time. It is equivalent to AEXPSPACE, the set of decision problems solvable by an [[alternating Turing machine]] in exponential space, and is a superset of [[EXPSPACE]].&amp;lt;ref&amp;gt;[[Christos Papadimitriou]], Computational Complexity (1994), {{isbn|978-0-201-53082-7}}. Section 20.1, corollary 3, page 495.&amp;lt;/ref&amp;gt; An example of a problem in 2-EXPTIME that is not in EXPTIME is the problem of proving or disproving statements in [[Presburger arithmetic]].&amp;lt;ref&amp;gt;[[Michael J. Fischer|Fischer, M. J.]], and [[Michael O. Rabin]], 1974, &amp;quot;[http://www.lcs.mit.edu/publications/pubs/ps/MIT-LCS-TM-043.ps &amp;quot;Super-Exponential Complexity of Presburger Arithmetic.] {{Webarchive|url=https://web.archive.org/web/20060915010325/http://www.lcs.mit.edu/publications/pubs/ps/MIT-LCS-TM-043.ps |date=2006-09-15 }}&amp;quot; &amp;#039;&amp;#039;Proceedings of the SIAM-AMS Symposium in Applied Mathematics Vol. 7&amp;#039;&amp;#039;: 27–41&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In some other problems in the design and analysis of algorithms, double exponential sequences are used within the design of an algorithm rather than in its analysis. An example is [[Chan&amp;#039;s algorithm]] for computing [[convex hull]]s, which performs a sequence of computations using test values &amp;#039;&amp;#039;h&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;amp;nbsp;=&amp;amp;nbsp;2&amp;lt;sup&amp;gt;2&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;&amp;lt;/sup&amp;gt; (estimates for the eventual output size), taking time O(&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&amp;amp;nbsp;log&amp;amp;nbsp;&amp;#039;&amp;#039;h&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;) for each test value in the sequence. Because of the double exponential growth of these test values, the time for each computation in the sequence grows singly exponentially as a function of &amp;#039;&amp;#039;i&amp;#039;&amp;#039;, and the total time is dominated by the time for the final step of the sequence. Thus, the overall time for the algorithm is O(&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&amp;amp;nbsp;log&amp;amp;nbsp;&amp;#039;&amp;#039;h&amp;#039;&amp;#039;) where &amp;#039;&amp;#039;h&amp;#039;&amp;#039; is the actual output size.&amp;lt;ref&amp;gt;{{citation&lt;br /&gt;
 | last = Chan | first = T. M. | author-link = Timothy M. Chan&lt;br /&gt;
 | doi = 10.1007/BF02712873&lt;br /&gt;
 | issue = 4&lt;br /&gt;
 | journal = [[Discrete and Computational Geometry]]&lt;br /&gt;
 | mr = 1414961&lt;br /&gt;
 | pages = 361–368&lt;br /&gt;
 | title = Optimal output-sensitive convex hull algorithms in two and three dimensions&lt;br /&gt;
 | volume = 16&lt;br /&gt;
 | year = 1996| doi-access = free&lt;br /&gt;
 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Number theory===&lt;br /&gt;
Some [[number theory|number theoretical]] bounds are double exponential. [[Odd perfect number]]s with &amp;#039;&amp;#039;n&amp;#039;&amp;#039; distinct prime factors are known to be at most &amp;lt;math&amp;gt;2^{4^n}&amp;lt;/math&amp;gt;, a result of Nielsen (2003).&amp;lt;ref&amp;gt;{{citation&lt;br /&gt;
 | last = Nielsen | first = Pace P.&lt;br /&gt;
 | journal = INTEGERS: The Electronic Journal of Combinatorial Number Theory&lt;br /&gt;
 | pages = A14&lt;br /&gt;
 | title = An upper bound for odd perfect numbers&lt;br /&gt;
 | url = http://www.integers-ejcnt.org/vol3.html&lt;br /&gt;
 | volume = 3&lt;br /&gt;
 | year = 2003}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The maximal volume of a [[polytope]] in a &amp;#039;&amp;#039;d&amp;#039;&amp;#039;-dimensional [[integer lattice]] with &amp;#039;&amp;#039;k&amp;#039;&amp;#039; ≥ 1 [[Integer points in convex polyhedra|interior lattice points]] is at most&lt;br /&gt;
:&amp;lt;math&amp;gt;k\cdot(8d)^d\cdot15^{d\cdot2^{2d+1}},&amp;lt;/math&amp;gt;&lt;br /&gt;
a result of Pikhurko (2001).&amp;lt;ref&amp;gt;{{citation|last=Pikhurko&lt;br /&gt;
 | first=Oleg&lt;br /&gt;
 | title=Lattice points in lattice polytopes&lt;br /&gt;
 | journal=[[Mathematika]]&lt;br /&gt;
 | volume=48&lt;br /&gt;
 | year=2001&lt;br /&gt;
 | issue=1–2&lt;br /&gt;
 | pages=15–24&lt;br /&gt;
 | arxiv=math/0008028&lt;br /&gt;
|bibcode = 2000math......8028P&lt;br /&gt;
 | doi=10.1112/s0025579300014339}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The [[largest known prime number]] in the electronic era has grown roughly as a double exponential function of the year since [[J. C. P. Miller|Miller]] and [[David Wheeler (computer scientist)|Wheeler]] found a 79-digit prime on [[EDSAC]]1 in 1951.&amp;lt;ref&amp;gt;{{citation&lt;br /&gt;
 | last1 = Miller | first1 = J. C. P.&lt;br /&gt;
 | last2 = Wheeler | first2 = D. J.&lt;br /&gt;
 | doi = 10.1038/168838b0&lt;br /&gt;
 | journal = [[Nature (journal)|Nature]]&lt;br /&gt;
 |page=838&lt;br /&gt;
 | title = Large prime numbers&lt;br /&gt;
 | volume = 168&lt;br /&gt;
 | year = 1951&lt;br /&gt;
 | issue=4280|bibcode = 1951Natur.168..838M | doi-access = free&lt;br /&gt;
 }}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Theoretical biology===&lt;br /&gt;
&lt;br /&gt;
In [[population dynamics]] the growth of human population is sometimes supposed to be double exponential. Varfolomeyev and Gurevich&amp;lt;ref&amp;gt;{{citation&lt;br /&gt;
 | last1 = Varfolomeyev | first1 = S. D.&lt;br /&gt;
 | last2 = Gurevich | first2 = K. G.&lt;br /&gt;
 | doi = 10.1006/jtbi.2001.2384&lt;br /&gt;
 | issue = 3&lt;br /&gt;
 | journal = Journal of Theoretical Biology&lt;br /&gt;
 | pages = 367–372&lt;br /&gt;
 | title = The hyperexponential growth of the human population on a macrohistorical scale&lt;br /&gt;
 | volume = 212&lt;br /&gt;
 | year = 2001&lt;br /&gt;
 | pmid = 11829357| bibcode = 2001JThBi.212..367V&lt;br /&gt;
 }}.&amp;lt;/ref&amp;gt; experimentally fit&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; N(y)=375.6\cdot 1.00185^{1.00737^{y-1000}} \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;#039;&amp;#039;N&amp;#039;&amp;#039;(&amp;#039;&amp;#039;y&amp;#039;&amp;#039;) is the population in millions in year &amp;#039;&amp;#039;y&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
===Physics===&lt;br /&gt;
In the [[Toda oscillator]] model of [[self-pulsation]], the logarithm of amplitude varies exponentially with time (for large amplitudes), thus the amplitude varies as double exponential function of time.&amp;lt;ref name=&amp;quot;kouz&amp;quot;&amp;gt;{{citation&lt;br /&gt;
 | last1 = Kouznetsov | first1 = D.&lt;br /&gt;
 | last2 = Bisson | first2 = J.-F.&lt;br /&gt;
 | last3 = Li | first3 = J.&lt;br /&gt;
 | last4 = Ueda | first4 = K.&lt;br /&gt;
 | doi = 10.1088/1751-8113/40/9/016&lt;br /&gt;
 | journal = [[Journal of Physics A]]&lt;br /&gt;
 | pages = 1–18&lt;br /&gt;
 | title = Self-pulsing laser as oscillator Toda: Approximation through elementary functions&lt;br /&gt;
 | url = http://www.iop.org/EJ/abstract/-search=15823442.1/1751-8121/40/9/016&lt;br /&gt;
 | volume = 40&lt;br /&gt;
 | year = 2007&lt;br /&gt;
 | issue = 9 | bibcode=2007JPhA...40.2107K| s2cid = 53330023&lt;br /&gt;
 | citeseerx = 10.1.1.535.5379&lt;br /&gt;
 }}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Dendritic [[macromolecule]]s have been observed to grow in a doubly-exponential fashion.&amp;lt;ref&amp;gt;{{cite journal|title=Double Exponential Dendrimer Growth |first1=Tohru |last1=Kawaguchi |first2=Kathleen L. |last2=Walker |first3=Charles L. |last3=Wilkins |first4=Jeffrey S. |last4=Moore |journal=[[Journal of the American Chemical Society]] |year=1995 |volume=117 |number=8 |pages=2159–2165 |doi=10.1021/ja00113a005}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist|2}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Elementary special functions]]&lt;br /&gt;
[[Category:Exponentials]]&lt;/div&gt;</summary>
		<author><name>imported&gt;Grafen</name></author>
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