logo

Hankel Functions, Bessel Functions of the Third Kind 📂Functions

Hankel Functions, Bessel Functions of the Third Kind

Definition

A Hankel function, also known as a Bessel function of the third kind, is defined as the following two linear combinations of the Bessel function of the first kind JνJ_{\nu} and the Bessel function of the second kind NνN_{\nu}.

Hν(1)(x)=Jν(x)+iNν(x) H_{\nu}^{(1)}(x) = J_{\nu}(x)+iN_{\nu}(x) Hν(2)(x)=Jν(x)iNν(x) H_{\nu}^{(2)}(x) = J_{\nu}(x)-iN_{\nu}(x)

Explanation

It was introduced by the German mathematician Hermann Hankel in 1869. Specifically, Hν(1)H_{\nu}^{(1)} is called the Hankel function of the first kind, and Hν(2)H_{\nu}^{(2)} is called the Hankel function of the second kind.

To understand the definition, consider the differential equation y+y=0y^{\prime \prime}+y=0. The solutions to this differential equation are cosx\cos x and sinx\sin x. The general solution is represented as a linear combination of these, with the most commonly used form being cosx+±isinx=e±ix\cos x + \pm i \sin x=e^{\pm ix}. Similarly, the general solution of the Bessel equation represented as a linear combination of two solutions, Jν(x)J_{\nu}(x) and Nν(x)N_{\nu}(x), is the Hankel function.