mhill
- 180
- 1
it is true in general that the sum (density of states for a physicst)
[tex]\sum_{n=0}^{\infty} \delta (x- \gamma _{n})[/tex]
is related to the value [tex]\frac{ \zeta '(1/2+is)}{\zeta (1/2+is)}+\frac{ \zeta '(1/2-is)}{\zeta (1/2-is)}[/tex]
here the 'gamma' are the imaginary parts of the non-trivial zeros of Riemann zeta function
[tex]\sum_{n=0}^{\infty} \delta (x- \gamma _{n})[/tex]
is related to the value [tex]\frac{ \zeta '(1/2+is)}{\zeta (1/2+is)}+\frac{ \zeta '(1/2-is)}{\zeta (1/2-is)}[/tex]
here the 'gamma' are the imaginary parts of the non-trivial zeros of Riemann zeta function