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DUAL INTEGRAL EQUATIONS INVOLVING LEGENDRE ...

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58 P. K. BANERJI, DESHNA LOONKER<br />

∫ ∞<br />

h(α) = τ tanh(π τ)f(τ)P 1 (cosh α)dτ = h −<br />

2(α); α > α 1 . (2.2)<br />

0<br />

2 +iτ<br />

where α 1 is an arbitrary positive number. By virtue of the validity of embedding<br />

from the linear spaces into their duals [2, pp. 121-23], for the distribution spaces,<br />

considered in this paper, the imbeddings are D → M α β<br />

(I) → S → E and their duals<br />

E ′ → S ′ → M ′ β α → D ′ for the generalized Mehler-Fock transform of order zero.<br />

The equation (1.31) is obtained due to the property<br />

∫ b<br />

∫ d<br />

f(h(t))ϕ(t)dt = f(x) ϕ(h−1 (x))<br />

a<br />

c h ′ (h −1 dx, (2.3)<br />

(x))<br />

where f is locally integrable on [a, b). If x 0 ∈ [c, d), then<br />

T h {δ(x − x 0 ); t} = δ(h(t) − x 0 ) = δ(t − h−1 (x 0 ))<br />

h ′ (h −1 (x 0 )) . (2.4)<br />

The operator T h −1 : D 41[a, ′ b) → D 41[c, ′ d)is defined by<br />

(T h ) −1 = T h −1. (2.5)<br />

The distributional interpretation of (1.28), in terms of T h and T h −1, is, see [3, p.<br />

188],<br />

[ ( g<br />

)]<br />

f = T h x −α<br />

+ ∗ T h −1<br />

h ′ , (2.6)<br />

and the solution for (1.28) is<br />

sin απ d<br />

g(t) =<br />

π dt T (<br />

h x<br />

−α<br />

+ ∗ T h −1(f); t ) , (2.7)<br />

where f is the usual locally integrable function.<br />

We notice [7, pp. 407-408] that the involvement of functions F 1 (x) and F 2 (x)in<br />

terms of the prescribed functions g 1 (α) and h 2 (α) are given by<br />

and<br />

F 1 (x) = √ 1 ∫<br />

d x<br />

g 1 (α) sinh α dα<br />

√ (2.8)<br />

π dx 0 (cosh x − cosh α)<br />

F 2 (x) = √ 1 ∫ ∞<br />

h 2 (α) sinh α dα<br />

√ , x ≥ α 1 (2.9)<br />

π (cosh α − cosh x)<br />

x<br />

The function F 1 (x), that is given by (2.8), is similar to the distributional solution<br />

obtained in (1.30). Further, by considering cosh α as a strictly increasing function,<br />

the function F 1 (x) in (2.8) is similar to the distributional solution given by (2.7).<br />

By virtue of relations (1.28) – (1.31) and (2.3) – (2.7), we justify to state that g 1 (α)<br />

is a locally integrable function and since the properties of the operators cosh α and<br />

cosh x has the correspondence D ′ 41[0, ∞)→ D ′ 41(x, ∞], the function F 1 (x)turns out<br />

to be locally integrable and hence it is, indeed, true that (2.8) is the required distributional<br />

solution. This allow us, simultaneously, to confirm that F 1 (x)is defined<br />

on spaces D ′ , M ′ β α ,E ′ , S ′ , respectively, by considering distributional generalized<br />

Mehler-Fock transform of order zero, i.e. ,

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