2π2⁢∫02⁢πcos⁡t⁢sin⁡t⁢meν⁡(t,h2)⁢me-ν-2⁢m⁡(t,h2)sinh2⁡z+sin2⁡t⁢ⅆ⁡t=(-1)m⁢ⅈ⁢γν,m⁢D0⁡(ν,ν+2⁢m,z),