To extend on Matt's comment about Euler, here is something I wrote up some years ago about Euler's discovery of the functional equation only at integral points. I hope there are no typos.
Although Euler never found a convergent analytic expression for
zeta(s) at negative numbers, in 1749 he published a method of
computing
values of the zeta function at negative integers by a precursor of
Abel's Theorem applied to a divergent series. The
computation led him to the asymmetric functional equation of
zeta(s).
The technique uses the function
zeta2(s)=sumngeq1frac(−1)n−1ns=1−frac12s+frac13s−frac14s+dots.
This looks not too different from zeta(s), but has the advantage
as an alternating series of
converging for all positive s. For s>1,
zeta2(s)=(1−21−s)zeta(s).
Of course this is true for complex s, but
Euler only worked with real s, so we shall as well.
Disregarding convergence issues, Euler wrote
zeta2(−m)=sumngeq1(−1)n−1nm=1−2m+3m−4m+dots,
which he proceeded to evaluate as follows. Differentiate
the equation
sumngeq0Xn=frac11−X
to get
sumngeq1nXn−1=frac1(1−X)2.
Setting X=−1,
zeta2(−1)=frac14.
Since zeta2(−1)=(1−22)zeta(−1), zeta(−1)=−1/12. Notice we can't set X=1 in the second power series and compute sumn=zeta(−1) directly. So zeta2(s) is nicer than zeta(s) in this Eulerian way.
Multiplying the second power series by X and then differentiating, we get
sumngeq1n2Xn−1=frac1+X(1−X)3.
Setting X=−1,
zeta2(−2)=0.
By more successive multiplications by X and differentiations, we get
sumngeq1n3Xn−1=fracX2+4X+1(1−X)4,
and
sumngeq1n4Xn−1=frac(X+1)(X2+10X+1)(1−X)5.
Setting X=−1, we find zeta2(−3)=−1/8 and
zeta2(−4)=0. Continuing further, with the recursion
fracddxfracP(x)(1−x)n=frac(1−x)P′(x)+nP(x)(1−x)n+1,
we get
sumngeq1n5Xn−1=fracX4+26X3+66X2+26X+1(1−X)6,
sumngeq1n6Xn−1=frac(X+1)(X4+56X3+246X2+56X+1)(1−X)7,
sumngeq1n7Xn−1=fracX6+120X5+1191X4+2416X3+1191X2+120X+1(1−X)8.
Setting X=−1, we get zeta2(−5)=1/4,zeta2(−6)=0,zeta2(−7)=−17/16.
Apparently zeta2 vanishes at the negative even integers, while
fraczeta2(−1)zeta2(2)=frac14cdotfrac6cdot2pi2=frac3cdot1!1cdotpi2,fraczeta2(−3)zeta2(4)=−frac18cdotfrac30cdot247pi4=−frac15cdot3!7cdotpi4,
fraczeta2(−5)zeta2(6)=frac14cdotfrac42cdot6!31pi6=frac63cdot5!31cdotpi6,fraczeta2(−7)zeta2(8)=−frac1716cdotfrac30cdot8!127cdotpi8=−frac255cdot7!127pi8.
The numbers 1,3,7,15,31,63,127,255 are all one less than a power of 2,
so Euler was led to the observation that for ngeq2,
fraczeta2(1−n)zeta2(n)=frac(−1)n/2+1(2n−1)(n−1)!(2n−1−1)pin
if n is even and
fraczeta2(1−n)zeta2(n)=0
if n is odd. Notice how
the vanishing of zeta2(s)
at negative even integers nicely compensates for
the lack of knowledge of zeta2(s) at positive odd integers >1 (which
is the same as not knowing zeta(s) at positive odd integers >1).
Euler interpreted the pm sign at even n and the vanishing
at odd n as the single factor −cos(pin/2), and with
(n−1)! written as Gamma(n) we get
fraczeta2(1−n)zeta2(n)=−Gamma(n)frac2n−1(2n−1−1)pincosleft(fracpin2right).
Writing zeta2(n) as (1−21−n)zeta(n) gives the
asymmetric functional
equation
fraczeta(1−n)zeta(n)=frac2(2pi)nGamma(n)cosleft(fracpin2right).
Euler applied similar ideas to L(s,chi4) and found its
functional equation. You can work this out yourself in
Exercise 2 below.
Exercises
Show that Euler's computation of zeta values at negative
integers can be put in the form
(1−2n+1)zeta(−n)=left.left(ufracdduright)nrightvertu=1left(fracu1+uright)=left.left(fracddxright)nrightvertx=0left(fracex1+exright).To compute the divergent series
L(−n,chi4)=sumjgeq0(−1)j(2j+1)n=1−3n+5n−7n−9n+11n−dots
for nonnegative integers n, begin with the formal identity
sumjgeq0X2j=frac11−X2.
Differentiate and set X=i to show L(0,chi4)=1/2.
Repeatedly multiply by X, differentiate, and set
X=i in order to compute L(−n,chi4) for 0leqnleq10. This computational technique is not rigorous, but the answers are correct. Compare with the values of L(n,chi4) for positive n, if you know those, to get a formula for L(1−n,chi4)/L(n,chi4). Treat alternating signs like special values of a suitable trigonometric function.
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