Chapter 3: Problem 5
The Hermite polynomials \(H_{n}(x)\) are defined by $$ H_{n}(x)=(-1)^{n} e^{x^{2} / 2} \frac{d^{n}}{d x^{n}} e^{-x^{2} / 2}, \quad(n=0,1,2, \ldots) $$ Show that $$ H_{0}(x)=1, \quad H_{1}(x)=x, \quad H_{2}(x)=x^{2}-1, \quad H_{3}(x)=x^{3}-3 x $$ and verify by direct integration that these four functions are orthogonal on the interval \((-\infty, \infty)\) with respect to the weight function \(\omega(x)=\mathrm{e}^{-x^{2} / 2}\)
Short Answer
Step by step solution
Calculate $H_0(x)$
Calculate $H_1(x)$
Calculate $H_2(x)$
Calculate $H_3(x)$
Verify Orthogonality
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Orthogonality
Weight Function
- The weight function normalizes the polynomials; without it, the aspect of orthogonality might fail.
- The Gaussian form of the weight function is inherent to many physical and probabilistic applications, making Hermite polynomials particularly useful in areas like quantum mechanics.
- It allows for the evaluation and computation of polynomial integrals that might otherwise be divergent over \((-\infty, \infty)\).
Differential Equations
- They arise naturally in systems with Gaussian potentials, such as in the quantum harmonic oscillator.
- The solutions (Hermite polynomials) provide the wave functions for particles in a potential field.
- They possess useful properties such as recurrence relations, which simplify the computation of higher-degree polynomials.