q-exponential
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The term q-exponential occurs in two contexts. The q-exponential distribution, based on the Tsallis q-exponential is discussed in elsewhere.
In combinatorial mathematics, a q-exponential is a q-analog of the exponential function, namely the eigenfunction of a q-derivative. There are many q-derivatives, for example, the classical q-derivative, the Askey–Wilson operator, etc. Therefore, unlike the classical exponentials, q-exponentials are not unique. For example, e q ( z ) {\displaystyle e_{q}(z)} is the q-exponential corresponding to the classical q-derivative while E q ( z ) {\displaystyle {\mathcal {E}}_{q}(z)} are eigenfunctions of the Askey–Wilson operators.
The q-exponential is also known as the quantum dilogarithm.
Definition
The q-exponential e q ( z ) {\displaystyle e_{q}(z)} is defined as
e q ( z ) = ∑ n = 0 ∞ z n [ n ] ! q = ∑ n = 0 ∞ z n ( 1 − q ) n ( q ; q ) n = ∑ n = 0 ∞ z n ( 1 − q ) n ( 1 − q n ) ( 1 − q n − 1 ) ⋯ ( 1 − q ) {\displaystyle e_{q}(z)=\sum _{n=0}^{\infty }{\frac {z^{n}}{[n]!_{q}}}=\sum _{n=0}^{\infty }{\frac {z^{n}(1-q)^{n}}{(q;q)_{n}}}=\sum _{n=0}^{\infty }z^{n}{\frac {(1-q)^{n}}{(1-q^{n})(1-q^{n-1})\cdots (1-q)}}}
where [ n ] ! q {\displaystyle [n]!_{q}} is the q-factorial and
( q ; q ) n = ( 1 − q n ) ( 1 − q n − 1 ) ⋯ ( 1 − q ) {\displaystyle (q;q)_{n}=(1-q^{n})(1-q^{n-1})\cdots (1-q)}
is the q-Pochhammer symbol. That this is the q-analog of the exponential follows from the property
( d d z ) q e q ( z ) = e q ( z ) {\displaystyle \left({\frac {d}{dz}}\right)_{q}e_{q}(z)=e_{q}(z)}
where the derivative on the left is the q-derivative. The above is easily verified by considering the q-derivative of the monomial
( d d z ) q z n = z n − 1 1 − q n 1 − q = [ n ] q z n − 1 . {\displaystyle \left({\frac {d}{dz}}\right)_{q}z^{n}=z^{n-1}{\frac {1-q^{n}}{1-q}}=[n]_{q}z^{n-1}.}
Here, [ n ] q {\displaystyle [n]_{q}} is the q-bracket. For other definitions of the q-exponential function, see Exton (1983), Ismail & Zhang (1994), and Cieśliński (2011).
Properties
For real q > 1 {\displaystyle q>1}, the function e q ( z ) {\displaystyle e_{q}(z)} is an entire function of z {\displaystyle z}. For q < 1 {\displaystyle q<1}, e q ( z ) {\displaystyle e_{q}(z)} is regular in the disk | z | < 1 / ( 1 − q ) {\displaystyle |z|<1/(1-q)}.
Note the inverse, e q ( z ) e 1 / q ( − z ) = 1 {\displaystyle ~e_{q}(z)~e_{1/q}(-z)=1}.
Addition Formula
The analogue of exp ( x ) exp ( y ) = exp ( x + y ) {\displaystyle \exp(x)\exp(y)=\exp(x+y)} does not hold for real numbers x {\displaystyle x} and y {\displaystyle y}. However, if these are operators satisfying the commutation relation x y = q y x {\displaystyle xy=qyx}, then e q ( x ) e q ( y ) = e q ( x + y ) {\displaystyle e_{q}(x)e_{q}(y)=e_{q}(x+y)} holds true.
Relations
For − 1 < q < 1 {\displaystyle -1<q<1}, a function that is closely related is E q ( z ) . {\displaystyle E_{q}(z).} It is a special case of the basic hypergeometric series,
E q ( z ) = 1 ϕ 1 ( 0 0 ; z ) = ∑ n = 0 ∞ q ( n 2 ) ( − z ) n ( q ; q ) n = ∏ n = 0 ∞ ( 1 − q n z ) = ( z ; q ) ∞ . {\displaystyle E_{q}(z)=\;_{1}\phi _{1}\left({\scriptstyle {0 \atop 0}}\,;\,z\right)=\sum _{n=0}^{\infty }{\frac {q^{\binom {n}{2}}(-z)^{n}}{(q;q)_{n}}}=\prod _{n=0}^{\infty }(1-q^{n}z)=(z;q)_{\infty }.}
Clearly,
lim q → 1 E q ( z ( 1 − q ) ) = lim q → 1 ∑ n = 0 ∞ q ( n 2 ) ( 1 − q ) n ( q ; q ) n ( − z ) n = e − z . {\displaystyle \lim _{q\to 1}E_{q}\left(z(1-q)\right)=\lim _{q\to 1}\sum _{n=0}^{\infty }{\frac {q^{\binom {n}{2}}(1-q)^{n}}{(q;q)_{n}}}(-z)^{n}=e^{-z}.~}
Relation with Dilogarithm
e q ( x ) {\displaystyle e_{q}(x)} has the following infinite product representation:
e q ( x ) = ( ∏ k = 0 ∞ ( 1 − q k ( 1 − q ) x ) ) − 1 . {\displaystyle e_{q}(x)=\left(\prod _{k=0}^{\infty }(1-q^{k}(1-q)x)\right)^{-1}.}
On the other hand, log ( 1 − x ) = − ∑ n = 1 ∞ x n n {\displaystyle \log(1-x)=-\sum _{n=1}^{\infty }{\frac {x^{n}}{n}}} holds. When | q | < 1 {\displaystyle |q|<1},
log e q ( x ) = − ∑ k = 0 ∞ log ( 1 − q k ( 1 − q ) x ) = ∑ k = 0 ∞ ∑ n = 1 ∞ ( q k ( 1 − q ) x ) n n = ∑ n = 1 ∞ ( ( 1 − q ) x ) n ( 1 − q n ) n = 1 1 − q ∑ n = 1 ∞ ( ( 1 − q ) x ) n [ n ] q n . {\displaystyle {\begin{aligned}\log e_{q}(x)&=-\sum _{k=0}^{\infty }\log(1-q^{k}(1-q)x)\\&=\sum _{k=0}^{\infty }\sum _{n=1}^{\infty }{\frac {(q^{k}(1-q)x)^{n}}{n}}\\&=\sum _{n=1}^{\infty }{\frac {((1-q)x)^{n}}{(1-q^{n})n}}\\&={\frac {1}{1-q}}\sum _{n=1}^{\infty }{\frac {((1-q)x)^{n}}{[n]_{q}n}}\end{aligned}}.}
By taking the limit q → 1 {\displaystyle q\to 1},
lim q → 1 ( 1 − q ) log e q ( x / ( 1 − q ) ) = L i 2 ( x ) , {\displaystyle \lim _{q\to 1}(1-q)\log e_{q}(x/(1-q))=\mathrm {Li} _{2}(x),}
where L i 2 ( x ) {\displaystyle \mathrm {Li} _{2}(x)} is the dilogarithm.
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- Gasper, George; Rahman, Mizan Rahman (2004). Basic Hypergeometric Series. Cambridge University Press. ISBN0521833574.
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