Dirac Delta Function: Properties, Integrals, and Derivatives, Study Guides, Projects, Research of Mathematical Physics

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109
S-FUNCTIONS
WITH
COMPLICATED ARGUMENTS
t-
<
0
<
t+
otherwise
.
lt
dt
s(t)f(t)
=
{
i")
(5.23)
Remember, by definition, anything that behaves like a 6-function inside an integral
is a &function,
so
S(-t)
=
i3(t).
This implies the &function is an even function.
5.3.2
S(at)
Now consider another simple variation
6(at),
where
a
is any positive constant. Again,
start with a sifting integral in the form
(5.24)
With a variable change
oft'
=
at,
this
becomes
so
that
t-
<
0
<
t+
otherwise
l-'+
dt
f(t>&(at)
=
{
L(0)"
(5.26)
Notice again, this is just the definition of the function
6(t)
multiplied by the constant
l/a,
so
Wx)
=
S(x)/a
a
>
0.
(5.27)
This derivation was made assuming a positive
a.
The same manipulations can be
performed with a negative
a,
and combined with the previous result, to obtain the
more general expression
6(ax)
=
6(n)/lal.
(5.28)
Notice that
our
first example,
6(t)
=
8(-t),
can
be derived from Equation
5.28
by
setting
a
=
-
1.
5.3.3
S(tZ
-
2)
As
a bit more complicated argument for the Dirac &function, consider
6(t2
-
aL).
The argument
of
this function goes to zero when
t
=
fa
and
t
=
-a,
which seems
to imply two &functions.
To
test this theory, place the function in the sifting integral
lr+
dt
f(t)6(t2
-
a2).
(5.29)
pf3

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S-FUNCTIONS WITH COMPLICATED ARGUMENTS 109

t- < 0 < t+

otherwise. lt dt s ( t ) f ( t )= { i") (5.23)

Remember, by definition, anything that behaves like a 6-function inside an integral is a &function, so S ( - t ) = i3(t). This implies the &function is an even function.

5.3.2 S(at)

Now consider another simple variation 6(at), where a is any positive constant. Again, start with a sifting integral in the form

With a variable change oft' = at, this becomes

so that

t- < 0 < t+

otherwise l-'+ dt f(t>&(at)= { L(0)" (5.26)

Notice again, this is just the definition of the function 6 ( t )multiplied by the constant l/a, so

W x ) = S ( x ) / a a > 0. (5.27)

This derivation was made assuming a positive a. The same manipulations can be performed with a negative a, and combined with the previous result, to obtain the more general expression

6(ax) = 6(n)/lal. (5.28)

Notice that our first example, 6 ( t ) = 8 ( - t ) , can be derived from Equation 5.28 by setting a = - 1.

5. 3. 3 S(tZ - 2)

As a bit more complicated argument for the Dirac &function, consider 6(t2 - a L ).

The argument of this function goes to zero when t = f a and t = -a, which seems

to imply two &functions. To test this theory, place the function in the sifting integral

lr+dt f ( t ) 6 ( t 2- a2). (5.29)

110 THE DIRAC 6-FUNCTION

There can be contributions to this integral only at the zeros of the argument of the 6-function. Assuming that the integral range includes both these zeros, i.e.,

t- < --a and t+ > +a, this integral becomes

dt f ( t ) 6 ( t 2- a2) + 1

+a+€ dt f ( t ) 6 ( t 2- a2), (5.30) fa-€

which is valid for any value of 0 < E < a.

NOWt2 - a2 = (t - a)(t + a), which near the two zeros can be approximated by

(t + a)(-2a) (5.31) ( t - a ) ( + k )

t --t -a t2 - a2 = (t - a)(t + a ) = t ---f +a.

Formally, these results are obtained by performing a Taylor series expansion of t2 - a

about both t = -a and t = +a and keeping terms up to the first order. The Taylor series expansion of t2 - a2 around an arbitrary point to is, to first order, given by

to). (5.32) It=t', In the limit as E -+ 0, Integral 5.30 then becomes -a+€ +a+€

la-c d t f W ( - W + 4)+ la-, dt f ( t P ( k ( t - a ) ). (5.33)

Using the result from the previous section, 6(at) = 6(t)/lal, gives

2a

1' dt f ( t ) 6 ( t 2 - a2) = --(-a) + -f(+a).2a

Therefore, S ( t 2 - a2) is equivalent to the sum of two 6-functions:

2a 2a 6(t2 - a2) = - S ( t - a) + -6(t + a),

as shown in Figure 5.12.

6(x2 - a2) 03 00

area = 1/2a

i -' X

area - = 1/2a

-a^ 1,-^ a

The Plot of S(x2 - a 2 )

 **Figure 5. 12**