E m 1 ( z )

= m ! ( i π ) m 2 k = 1 ( 2 k + 1 ) m e i π ( 2 k + 1 ) z

E 2 n 1 ( z )

= ( 1 ) n ( 2 n 1 ) ! π 2 n 4 k = 0 cos ( 2 k + 1 ) π z ( 2 k + 1 ) 2 n

E 2 n 1 ( 0 )

= ( 1 ) n ( 2 n 1 ) ! π 2 n 4 ( 1 1 2 n + 1 3 2 n + + 1 ( 2 k + 1 ) 2 n + )

E 2 n ( z )

= ( 1 ) n ( 2 n ) ! π 2 n + 1 4 k = 0 sin ( 2 k + 1 ) π z ( 2 k + 1 ) 2 n + 1

ζ ( 2 m )

= ( 2 π ) 2 m m 1 2 2 m ( 1 ) m 1 2 ( 2 m ) ! E 2 m 1 ( 0 )

2 B m ( z )

= k = 0 m 1 ( m k ) 1 2 2 m k + 1 E m k 1 ( 0 ) ( E m ( z + 1 ) + E k ( z ) ) + ( E m ( z + 1 ) + E m ( z ) )

2 z m

= E m ( z ) + E m ( z + 1 )

2 z 1 z

= E 1 ( z ) + E 1 ( z + 1 ) + E 2 ( z ) + E 2 ( z + 1 ) +

ln ( 1 z )

= 1 2 ( 1 + e z ) ( E 1 ( z ) + 1 2 E 2 ( z ) + + 1 k E k ( z ) + )