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88 ON q-LAPLACE TRANSFORMS OF A GENERAL CLASS OF q ...

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82 R. K. YADAV, S. D. PUROHIT AND P. NIRWAN<br />

And<br />

E q (x) =<br />

∞∑ (−1) n q n(n−1)/2 x n<br />

, (1.5)<br />

(q ; q) n<br />

n=0<br />

The basic integrals cf. Gasper and Rahman [7], are defined as:<br />

∫ x<br />

0<br />

∫ ∞<br />

x<br />

∫ ∞<br />

0<br />

f(t) d(t ; q) = x(1 − q)<br />

f(t) d(t ; q) = x(1 − q)<br />

f(t) d(t ; q) = (1 − q)<br />

∞∑<br />

q k f(xq k ), (1.6)<br />

k=0<br />

∞∑<br />

q −k f(xq −k ), (1.7)<br />

k=1<br />

∞∑<br />

k=−∞<br />

q k f(q k ). (1.8)<br />

By virtue of the results (1.6), the integral equation (1.2) can be expressed as:<br />

ϕ(s) ≡ q L s {f(t)} = (q; q) ∞<br />

s<br />

∞∑<br />

j=0<br />

q j f(s −1 q j )<br />

(q; q) j<br />

. (1.9)<br />

Where the function ϕ(s) is called as q-Laplace transform or q-image of the original<br />

functions f(t).<br />

For real, or complex α and 0 < |q| < 1 , the q-shifted factorial is defined by:<br />

(α ; q) n<br />

=<br />

{<br />

1, if n = 0<br />

(1 − α)(1 − αq) · · · (1 − αq n−1 ) , if n ∈ N.<br />

(1.10)<br />

Also, for x ≠ 0, we have<br />

and<br />

[x − y] ν<br />

= x ν ∞ ∏<br />

n=o<br />

where α ≠ 0, −1, −2, · · · .<br />

The q-binomial series is given by<br />

{ (1 −<br />

y }<br />

x qn )<br />

(1 − y = x ν ( y<br />

x qν+n )<br />

x ; q) ν, (1.11)<br />

Γ q (α) = (q; q) ∞(1 − q) 1−α<br />

(q α ; q) ∞<br />

, (1.12)<br />

1Φ 0 (α; − ; q, x) = (αx; q) ∞<br />

(x; q) ∞<br />

. (1.13)<br />

The q-binomial coefficients are given by<br />

[ ]<br />

n (q; q) n<br />

=<br />

. (1.14)<br />

k (q; q) n−k (q; q) k<br />

q

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