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A–8 The Dirac Delta Function 675<br />

A–7 HILBERT TRANSFORM PAIRS †<br />

Definition of Hilbert Transform: xN(t) ! x(t) * 1 pt<br />

= 1 p L<br />

q<br />

-q<br />

x(l)<br />

t - l dl<br />

Function<br />

Hilbert Transform<br />

1. x(at b) xN (at + b)<br />

2. x(t) y(t) xN (t) + yN (t)<br />

3.<br />

d n x(t)<br />

dt n<br />

d n<br />

dt n xN(t)<br />

4. A constant 0<br />

5.<br />

1<br />

-pd(t)<br />

t<br />

6. sin (v 0 t + u) -cos (v 0 t + u)<br />

7.<br />

sin at<br />

= Sa(at)<br />

at<br />

- 1<br />

2p at Sa2 (at)<br />

8. e ;jv 0t<br />

< je ;jv 0t<br />

9. d (t) 1<br />

10.<br />

pt<br />

a<br />

t<br />

p(t 2 + a 2 )<br />

pAt 2 + a 2 B<br />

11. a t 1, ƒ t ƒ … T>2<br />

b ! e<br />

T 0, t elsewhere<br />

1<br />

p ln 2t + T<br />

2t - T <br />

A–8 THE DIRAC DELTA FUNCTION<br />

DEFINITION. The Dirac delta function δ(x), also called the unit impulse function,<br />

satisfies both of the following conditions:<br />

L<br />

q<br />

-q<br />

d(x) dx = 1 and d(x) = e q, x = 0<br />

0, x = 0 f<br />

Consequently, δ (x) is a “singular” function. ‡<br />

† Fourier transform theorems are given in Table 2–1, and Fourier transform pairs are given in Table 2–2.<br />

‡ The Dirac delta function is not an ordinary function since it is really undefined at x = 0. However, it is<br />

described by the mathematical theory of distributions [Bremermann, 1965].

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