10 Bessel FunctionsBessel and Hankel Functions

§10.11 Analytic Continuation

When m∈ℤ,

10.11.1 Jν⁡(z⁢em⁢π⁢i)=em⁢ν⁢π⁢i⁢Jν⁡(z),
10.11.2 Yν⁡(z⁢em⁢π⁢i)=e−m⁢ν⁢π⁢i⁢Yν⁡(z)+2⁢i⁢sin⁡(m⁢ν⁢π)⁢cot⁡(ν⁢π)⁢Jν⁡(z).
10.11.3 sin⁡(ν⁢π)⁢Hν(1)⁡(z⁢em⁢π⁢i)=−sin⁡((m−1)⁢ν⁢π)⁢Hν(1)⁡(z)−e−ν⁢π⁢i⁢sin⁡(m⁢ν⁢π)⁢Hν(2)⁡(z),
10.11.4 sin⁡(ν⁢π)⁢Hν(2)⁡(z⁢em⁢π⁢i)=eν⁢π⁢i⁢sin⁡(m⁢ν⁢π)⁢Hν(1)⁡(z)+sin⁡((m+1)⁢ν⁢π)⁢Hν(2)⁡(z).
10.11.5 Hν(1)⁡(z⁢eπ⁢i) =−e−ν⁢π⁢i⁢Hν(2)⁡(z),
Hν(2)⁡(z⁢e−π⁢i) =−eν⁢π⁢i⁢Hν(1)⁡(z).

If ν=n (∈ℤ), then limiting values are taken in (10.11.2)–(10.11.4):

For real ν,

10.11.9 Jν⁡(z¯) =Jν⁡(z)¯, Yν⁡(z¯) =Yν⁡(z)¯,
Hν(1)⁡(z¯) =Hν(2)⁡(z)¯, Hν(2)⁡(z¯) =Hν(1)⁡(z)¯.

For complex ν replace ν by ν¯ on the right-hand sides.