The Dirac Delta Function: A Comprehensive Guide with Examples, Study Guides, Projects, Research of Mathematical Physics

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106
THE
DIRAC
&FUNCTION
L..
t
nln
Figure
5.9
The Sinc
Squared
Sequence Function
5.2.2
Defining
S(t)
by
Integral
Operations
In mathematics, the 6-function is defined by how it behaves inside an integral. Any
function which behaves
as
6(t)
in the following equation is
by
dejnition
a 6-function,
t-
<
to
<
t+
otherwise
L-“
dt
6(t
-
to)f(t)
=
(5.14)
where
t-
<
t+
and
f
(t)
is
any continuous, well-behaved function. This operation
is sometimes called a
sifiing integral
because it selects the single value
f(to)
out of
Because
this
is a definition, it need not be proven, but its consistency with
our
previous definition and applications
of
the
6-function must be shown.
If
t-
<
to
<
t+
,
the range of the integral can be changed
to
be an infinitesimal region of size
2~
centered
around
to,
without changing the value
of
the integral.
This
is true because
6(t
-
to)
vanishes everywhere except at
t
=
to.
This
means
L-‘+
dt
6(t
-
to)f(t)
=
s,-,
dt
60
-
to)f(t>-
(5.15)
Because
f(t)
is a continuous function, over the infinitesimal region it is effectively a
constant, with the value
f(to).
Therefore,
f
(0.
f0+E
to+€
dt
S(t
-
to)
=
f(to).
(5.16)
This “proves” the first part
of
Equation 5.14. The second part, when
to
is not inside
the range
t-
<
t
<
t+,
easily follows because, in
this
case,
6(t
-
to)
is zero for the
entire range
of
the integrand.
Figure
5.10
shows a representation of the integration in Equation 5.14. The inte-
grand is a product of a shifted 6-function and the continuous function
f(t).
Because
the &function is zero everywhere except at
t
=
to,
the integrand goes to a &function
located at
t
=
to,
with an area scaled by
the
value of
f(to).
s,.
[
dt
60
-
t0)f
(t)
=
f(t0)
pf3

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106 THE DIRAC &FUNCTION

L..t

nln Figure 5.9 The Sinc Squared Sequence Function

5. 2. 2 Defining S(t) by Integral Operations

In mathematics, the 6-function is defined by how it behaves inside an integral. Any

function which behaves as 6(t)in the following equation is by dejnition a 6-function,

t- < to < t+ otherwise ’ L-“ dt 6(t - t o ) f ( t ) = (5.14)

where t- < t+ and f (t) is any continuous, well-behaved function. This operation is sometimes called a sifiing integral because it selects the single value f ( t o ) out of

Because this is a definition, it need not be proven, but its consistency with our previous definitionand applications of the 6-function must be shown. If t - < to < t+ , the range of the integral can be changed to be an infinitesimal region of size 2~ centered around to, without changing the value of the integral. This is true because 6(t - to) vanishes everywhere except at t = to. This means

L-‘+ dt 6(t - t o ) f ( t ) = s,-, dt 60 - t o ) f ( t > - (5.15)

Because f ( t ) is a continuous function, over the infinitesimal region it is effectively a constant, with the value f ( t o ). Therefore,

f (0.

f 0 + E

to+€ dt S ( t - t o ) = f ( t o ). (5.16)

This “proves” the first part of Equation 5.14. The second part, when to is not inside the range t - < t < t + , easily follows because, in this case, 6(t - to) is zero for the entire range of the integrand. Figure 5.10 shows a representation of the integration in Equation 5.14. The inte- grand is a product of a shifted 6-function and the continuous function f ( t ). Because the &function is zero everywhere except at t = to, the integrand goes to a &function located at t = to, with an area scaled by the value of f ( t o ).

s,.

[ dt 6 0 - t0)f ( t ) = f(t0)

TWO DEFINITIONS OF S(f) (^107)

f(t>

6 ( t- t o) with unit area

t Figure 5.10 (^) A Graphical Intcrprctation of the Sifting Integral

5.2.3 The Sinc Sequence Function The sinc function can be used to form another set of sequence functions which, in the limit as n -+ m, approach the behavior of a 6-function. The sinc function sequence is shown in Figure 5.1 1 and is defined by

sin nt Sinc: 6,(t) = -. 9l-t (5.17)

Notice, however, that as n ---f m this & ( t ) does not approach zero for all t # 0, so the sinc sequence does not have the characteristic infinitely narrow, infinitely tall peak

that we have come to expect. How, then, can we claim this sequence approaches a

&function? The answer is that the sinc function approaches the &function behavior from a completely different route, which can only be understood in the context of the integral definition of the &function. In the limit as n + w, the sinc function oscillatesinfinitely

fast except at t = 0. Thus, when the sequence is applied to a continuous function

f ( t ) in a sifting integral, the only contribution which is not canceled out by rapid oscillations comes from the point t = 0. The result is, as you will prove in one of the

7cin Figure 5.11 The Sinc Sequence Function