Math 2.0

Special functions Object

Hermite polynomials

Description

The (physicists') Hermite polynomials are the polynomials Hn∈ℤ[x]H_n \in \Z[x], n≥0n \ge 0, given by Hn(x)=(−1)nex2dndxne−x2.H_n(x) = (-1)^n e^{x^2} \frac{d^n}{dx^n} e^{-x^2}. Equivalently, H0=1H_0 = 1, H1=2xH_1 = 2x and Hn+1=2x Hn−2n Hn−1H_{n+1} = 2x \, H_n - 2n \, H_{n-1} for n≥1n \ge 1. The probabilists' Hermite polynomials He⁡n\operatorname{He}_n use the weight e−x2/2e^{-x^2/2} instead: He⁡n(x)=(−1)nex2/2dndxne−x2/2\operatorname{He}_n(x) = (-1)^n e^{x^2/2} \frac{d^n}{dx^n} e^{-x^2/2}.

Remarks

The first values are H2=4x2−2H_2 = 4x^2 - 2, H3=8x3−12xH_3 = 8x^3 - 12x, and He⁡2=x2−1\operatorname{He}_2 = x^2 - 1, He⁡3=x3−3x\operatorname{He}_3 = x^3 - 3x. Check for H2H_2 with the recursion: 2x⋅2x−2⋅1⋅1=4x2−22x \cdot 2x - 2 \cdot 1 \cdot 1 = 4x^2 - 2. The polynomial HnH_n has degree nn and leading coefficient 2n2^n, while He⁡n\operatorname{He}_n is monic. The two families are related by Hn(x)=2n/2He⁡n(2 x)H_n(x) = 2^{n/2} \operatorname{He}_n(\sqrt{2} \, x). They are orthogonal on ℝ\R: ∫−∞∞Hm(x)Hn(x)e−x2 dx=π 2nn! δmn\int_{-\infty}^{\infty} H_m(x) H_n(x) e^{-x^2} \, dx = \sqrt{\pi} \, 2^n n! \, \delta_{mn}. They satisfy Hn′=2n Hn−1H_n' = 2n \, H_{n-1} and He⁡n′=nHe⁡n−1\operatorname{He}_n' = n \operatorname{He}_{n-1}. In quantum mechanics, the eigenfunctions of the harmonic oscillator are Hn(x)e−x2/2H_n(x) e^{-x^2/2} up to scaling.

Further reading

  1. Web https://en.wikipedia.org/wiki/Hermite_polynomials
About this page
TagMGACY98E9H
URIm2://MGACY98E9H
Kindobject
WritingW0 stub
MSC33C45, 12E10
Same as
Changed2 November 2026

Markdown · JSON · Edit on GitHub

What this page needs for W1

  • a source with a locator (0 of 1)

The writing levels say how complete the text of a page is. They do not measure its truth.

What links here

No page links to this page yet.