sinh⁡zπ2⁢∫02⁢πcos⁡t⁢meν′⁡(t,h2)⁢me-ν-2⁢m-1⁡(t,h2)sinh2⁡z+sin2⁡t⁢ⅆ⁡t=(-1)m⁢ⅈ⁢h⁢αν,m(1)⁢D1⁡(ν,ν+2⁢m+1,z),