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riemann_zeta_function [2016/05/31 20:20]
nikolaj
riemann_zeta_function [2016/06/02 10:58]
nikolaj
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 == Functional equation ==  == Functional equation == 
 Tells you most values: Tells you most values:
-^ $ \zeta(s) = 2(2\pi)^{s-1}\sin{\left(\pi\,​s/​2\right)}\,​\Gamma(1-s)\,​\zeta(1-s)$ ^+^ $ \zeta(s) = 2\,(2\pi)^{s-1}\sin{\left(\pi\,​s/​2\right)}\,​\Gamma(1-s)\,​\zeta(1-s)$ ^
  
 == Specific values == == Specific values ==
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 so that so that
 +
 +$\zeta(1-2m) = \dfrac{2(2m-1)!}{(4\pi^2)^m}\cos(m\pi)\zeta(2m)$
  
 $\zeta(1-2m)=(-1)^{m+1}\frac{1}{2m}B_{2m}$ $\zeta(1-2m)=(-1)^{m+1}\frac{1}{2m}B_{2m}$
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 $\sum_{n=1}^\infty \frac{1}{n^s} = \frac{1} { \Gamma(s) } \int_0^\infty \frac{x^{s-1}} { {\mathrm e}^x-1} \, {\mathrm d}x $ $\sum_{n=1}^\infty \frac{1}{n^s} = \frac{1} { \Gamma(s) } \int_0^\infty \frac{x^{s-1}} { {\mathrm e}^x-1} \, {\mathrm d}x $
  
-He takes the integral into the complex plane, where he $ \frac{1} { {\mathrm e}^x-1}$ diverges periodically in steps of $2\pi\,​i$. ​+He takes the integral into the complex plane, where the $ \frac{1} { {\mathrm e}^x-1}$ diverges periodically in steps of $2\pi\,​i$. ​
 He discovers that the function obeys a reflection formula He discovers that the function obeys a reflection formula
  
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