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nonpositive integers. It also yields the relation Γ( n )=( n
1)! for positive
integers n .
COROLLARY 14.5
Let E and N be as in T heorem 14.4. T hen
( N/ 2 π ) s Γ( s ) L E ( s )= ( N/ 2 π ) 2 −s Γ(2 − s ) L E (2 − s )
for all s ∈ C (an d bothsides continue analyticallytoallof C ). T he sign here
isthe oppositeofthe sign in (2) of T heorem 14.4.
PROOF
Using the definition of the gamma function, we have
a n ( N/ 2 πn ) s
0
( N/ 2 π ) s Γ( s ) L E ( s )=
t s− 1 e −t dt
n =1
a n
0
=
( u N ) s e 2 πnu du
u
(let t =2 πnu )
n =1
=
0
( u N ) s f E ( iu ) du
u
= 1 / N
0
+
1 / N
( u N ) s f E ( iu ) du
u
( u N ) s f E ( iu ) du
u .
(The interchange of summation and integration to obtain the third equality
is justified since the sum for f ( iu ) converges very quickly near
.) Let be
the sign in part (2) of Theorem 14.4. Then
f E ( i/ ( Nu )) = ( iu ) 2 f E ( iu )= −u 2 f E ( iu ) .
Therefore, let u =1 /N v to obtain
1 / N
=
( u N ) s f E ( iu ) du
( v N ) 2 −s f E ( iv ) dv
.
1 / N
u
v
0
This implies that
( N/ 2 π ) s Γ( s ) L E ( s )=
1 / N
( u N ) s f E ( iu ) du
( v N ) 2 −s f E ( iv ) dv
.
1 / N
u
v
Since f ( iu ) 0 exponentially as u →∞ , it follows easily that both integrals
converge and define analytic functions of s . Under s → 2 − s ,therightside,
hence the left side, is multiplied by . This is precisely what the functional
equation claims.
 
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