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, ${\displaystyle e_{q}(z)}$ is the q-exponential corresponding to the classical q-derivative while ${\displaystyle {\mathcal {E}}_{q}(z)}$ are eigenfunctions of the Askey–Wilson operators.

The q-exponential is also known as the quantum dilogarithm.^[1][2]

Definition

The q-exponential ${\displaystyle e_{q}(z)}$ is defined as

${\displaystyle e_{q}(z)=\sum _{n=0}^{\infty }{\frac {z^{n}}{[n]_{q}!}}=\sum _{n=0}^{\infty }{\frac {z^{n}(1-q)^{n}}{(q;q)_{n}}}=\sum _{n=0}^{\infty }z^{n}{\frac {(1-q)^{n}}{(1-q^{n})(1-q^{n-1})\cdots (1-q)}}}$

where ${\displaystyle [n]!_{q}}$ is the q-factorial and

${\displaystyle (q;q)_{n}=(1-q^{n})(1-q^{n-1})\cdots (1-q)}$

is the q-Pochhammer symbol. That this is the q-analog of the exponential follows from the property

${\displaystyle \left({\frac {d}{dz}}\right)_{q}e_{q}(z)=e_{q}(z)}$

where the derivative on the left is the q-derivative. The above is easily verified by considering the q-derivative of the monomial

${\displaystyle \left({\frac {d}{dz}}\right)_{q}z^{n}=z^{n-1}{\frac {1-q^{n}}{1-q}}=[n]_{q}z^{n-1}.}$

Here, ${\displaystyle [n]_{q}}$ is the q-bracket. For other definitions of the q-exponential function, see Exton (1983), Ismail & Zhang (1994), Suslov (2003) harvtxt error: no target: CITEREFSuslov2003 (help) and Cieśliński (2011).

Properties

For real ${\displaystyle q>1}$, the function ${\displaystyle e_{q}(z)}$ is an entire function of ${\displaystyle z}$. For ${\displaystyle q<1}$, ${\displaystyle e_{q}(z)}$ is regular in the disk ${\displaystyle |z|<1/(1-q)}$.

Note the inverse, ${\displaystyle ~e_{q}(z)~e_{1/q}(-z)=1}$.

Relations

For ${\displaystyle -1<q<1}$, a function that is closely related is ${\displaystyle E_{q}(z).}$ It is a special case of the basic hypergeometric series,

${\displaystyle E_{q}(z)=\;_{1}\phi _{1}\left({\scriptstyle {0 \atop 0}}\,;\,z\right)=\sum _{n=0}^{\infty }{\frac {q^{\binom {n}{2}}(-z)^{n}}{(q;q)_{n}}}=\prod _{n=0}^{\infty }(1-q^{n}z)=(z;q)_{\infty }.}$

Clearly,

${\displaystyle \lim _{q\to 1}E_{q}\left(z(1-q)\right)=\lim _{q\to 1}\sum _{n=0}^{\infty }{\frac {q^{\binom {n}{2}}(1-q)^{n}}{(q;q)_{n}}}(-z)^{n}=e^{-z}.~}$

References

• Cieśliński, Jan L. (2011). "Improved q-exponential and q-trigonometric functions". Applied Mathematics Letters. 24 (12): 2110–2114. arXiv:1006.5652. doi:10.1016/j.aml.2011.06.009. S2CID 205496812.
• Exton, Harold (1983). q-Hypergeometric Functions and Applications. New York: Halstead Press, Chichester: Ellis Horwood. ISBN 0853124914.
• Gasper, George; Rahman, Mizan Rahman (2004). Basic Hypergeometric Series. Cambridge University Press. ISBN 0521833574.
• Ismail, Mourad E. H. (2005). Classical and Quantum Orthogonal Polynomials in One Variable. Cambridge University Press. doi:10.1017/CBO9781107325982. ISBN 9780521782012.
• Ismail, Mourad E. H.; Zhang, Ruiming (1994). "Diagonalization of certain integral operators". Advances in Mathematics. 108 (1): 1–33. doi:10.1006/aima.1994.1077.
• Ismail, Mourad E. H.; Rahman, Mizan; Zhang, Ruiming (1996). "Diagonalization of certain integral operators II". Journal of Computational and Applied Mathematics. 68 (1–2): 163–196. CiteSeerX 10.1.1.234.4251. doi:10.1016/0377-0427(95)00263-4.
• Jackson, F. H. (1909). "On q-functions and a certain difference operator". Transactions of the Royal Society of Edinburgh. 46 (2): 253–281. doi:10.1017/S0080456800002751. S2CID 123927312.