Monday, 25 June 2012

ho.history overview - Historical question in analytic number theory

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)n1ns=1frac12s+frac13sfrac14s+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)=(121s)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)n1nm=12m+3m4m+dots,


which he proceeded to evaluate as follows. Differentiate
the equation
sumngeq0Xn=frac11X

to get
sumngeq1nXn1=frac1(1X)2.

Setting X=1,
zeta2(1)=frac14.

Since zeta2(1)=(122)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
sumngeq1n2Xn1=frac1+X(1X)3.


Setting X=1,
zeta2(2)=0.

By more successive multiplications by X and differentiations, we get
sumngeq1n3Xn1=fracX2+4X+1(1X)4,

and
sumngeq1n4Xn1=frac(X+1)(X2+10X+1)(1X)5.

Setting X=1, we find zeta2(3)=1/8 and
zeta2(4)=0. Continuing further, with the recursion
fracddxfracP(x)(1x)n=frac(1x)P(x)+nP(x)(1x)n+1,

we get
sumngeq1n5Xn1=fracX4+26X3+66X2+26X+1(1X)6,

sumngeq1n6Xn1=frac(X+1)(X4+56X3+246X2+56X+1)(1X)7,

sumngeq1n7Xn1=fracX6+120X5+1191X4+2416X3+1191X2+120X+1(1X)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(1n)zeta2(n)=frac(1)n/2+1(2n1)(n1)!(2n11)pin


if n is even and
fraczeta2(1n)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
(n1)! written as Gamma(n) we get
fraczeta2(1n)zeta2(n)=Gamma(n)frac2n1(2n11)pincosleft(fracpin2right).


Writing zeta2(n) as (121n)zeta(n) gives the
asymmetric functional
equation
fraczeta(1n)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



  1. Show that Euler's computation of zeta values at negative
    integers can be put in the form
    (12n+1)zeta(n)=left.left(ufracdduright)nrightvertu=1left(fracu1+uright)=left.left(fracddxright)nrightvertx=0left(fracex1+exright).


  2. To compute the divergent series
    L(n,chi4)=sumjgeq0(1)j(2j+1)n=13n+5n7n9n+11ndots


    for nonnegative integers n, begin with the formal identity
    sumjgeq0X2j=frac11X2.

    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(1n,chi4)/L(n,chi4). Treat alternating signs like special values of a suitable trigonometric function.


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