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Integral representations and integral transforms of some families of ...

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8 N. Elezović et al.<br />

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For the Fourier cosine transform, we similarly find that<br />

F c (S(r))(x) =<br />

=<br />

=<br />

∫ ∞<br />

0<br />

∫ ∞<br />

0<br />

∫ ∞<br />

= π 4<br />

= π 2<br />

0<br />

∫ ∞<br />

cos(xr)S(r)dr<br />

( ∫ 1 ∞<br />

cos(xr)<br />

r 0<br />

(∫ ∞<br />

t<br />

e t − 1<br />

0<br />

∫ ∞<br />

x<br />

0<br />

)<br />

t sin(rt)<br />

e t − 1 dt dr<br />

sin(rt) cos(xr)<br />

dr<br />

r<br />

t<br />

[1 + sgn(t − x)]dt<br />

e t − 1<br />

)<br />

dt<br />

t<br />

dt<br />

e t − 1<br />

(x > 0). (35)<br />

II. In order to obtain the Fourier sine <strong>and</strong> the Fourier cosine <strong>transforms</strong> <strong>of</strong> S μ+1 (r), we first<br />

set ν = 1/2 <strong>and</strong> ν =−1/2 in the Sonine–Schafheitlin formula (see, for example, [18, p. 401,<br />

Equation 13.4 (2)]):<br />

∫ ∞<br />

0<br />

t −λ a μ Ɣ (μ + ν − λ + 1/2)<br />

J μ (at)J ν (bt)dt =<br />

2 λ b μ−λ+1 Ɣ(μ + 1)Ɣ (λ − μ + ν + 1/2)<br />

( μ + ν − λ + 1<br />

· 2F 1 , μ − ν − λ + 1 )<br />

; μ + 1; a2<br />

2<br />

2<br />

b 2<br />

( )<br />

R(μ + ν + 1) >R(λ) > −1; 0

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