In q-analog theory, the Jackson integral series in the theory of special functions that expresses the operation inverse to q-differentiation.
The Jackson integral was introduced by Frank Hilton Jackson. For methods of numerical evaluation, see [1] and .
Let f(x) be a function of a real variable x. For a a real variable, the Jackson integral of f is defined by the following series expansion:
a | |
\int | |
0 |
f(x){\rmd}qx=
infty | |
(1-q)a\sum | |
k=0 |
qkf(qka).
Consistent with this is the definition for
a\toinfty
infty | |
\int | |
0 |
f(x){\rmd}qx=
infty | |
(1-q)\sum | |
k=-infty |
qkf(qk).
More generally, if g(x) is another function and Dqg denotes its q-derivative, we can formally write
\intf(x)Dqg{\rmd}qx=
infty | |
(1-q)x\sum | |
k=0 |
qkf(qkx)Dqg(qkx)=
infty | |
(1-q)x\sum | |
k=0 |
qkf(qkx)\tfrac{g(qkx)-g(qk+1x)}{(1-q)qkx},
\intf(x){\rmd}qg(x)=
infty | |
\sum | |
k=0 |
f(qkx) ⋅ (g(qkx)-g(qk+1x)),
giving a q-analogue of the Riemann–Stieltjes integral.
Just as the ordinary antiderivative of a continuous function can be represented by its Riemann integral, it is possible to show that the Jackson integral gives a unique q-antiderivative within a certain class of functions (see [2]).
Suppose that
0<q<1.
|f(x)x\alpha|
[0,A)
0\leq\alpha<1,
F(x)
[0,A)
f(x).
F(x)
x=0
F(0)=0
f(x)