Frobenius method for Hermite Equation

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SUMMARY

The discussion focuses on solving the Hermite Differential Equation using the Frobenius method. The participant identifies the indicial equation as r(r-1)=0, yielding roots r=0 and r=1. They derive two series solutions, one for each root, but express confusion regarding the nature of the solutions and the applicability of the Frobenius method at ordinary points. The participant also references Arfken & Weber's guidance on the expected even and odd solutions corresponding to the roots.

PREREQUISITES
  • Understanding of differential equations, specifically the Hermite Differential Equation.
  • Familiarity with the Frobenius method for solving differential equations.
  • Knowledge of power series expansions and their convergence.
  • Ability to solve indicial equations and interpret their roots.
NEXT STEPS
  • Study the Frobenius method in detail, focusing on its application to both ordinary and singular points.
  • Explore the properties of Hermite polynomials and their relationship to the Hermite Differential Equation.
  • Learn about the classification of singular points in differential equations.
  • Investigate the implications of the indicial equation and its roots on the nature of solutions.
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Students and researchers in mathematics, particularly those studying differential equations and series solutions, as well as educators seeking to clarify the Frobenius method's application.

sunquick
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Homework Statement


I'm asked to solve the Hermite Differential Equation
y''(x) - 2 x y'(x) + \lambda y(x) = 0

using the Frobenius method

2. Homework Equations

I am to assume the solution is in the form
y(x) = \sum a_n x^{n+r}
where r are the roots of the indicial equation that in this case reads
r(r-1)=0

The Attempt at a Solution


Solving the indicial equation, I get r=0 and r=1. If r=0, then the Frobenius method is just the ordinary power series method (expanding around an ordinary point) and I every worked example of the same problem I'm attempting to solve do use the ordinary power series method without mentioning the indicial equation or the name of Frobenius.

Indeed going with r = 0 I get
y(x) = a_0 \left( 1 - \frac{\lambda}{2!} x^2 - \frac{(4-\lambda) \lambda}{4!} x^4 - \frac{(8-\lambda)(4- \lambda)\lambda}{6!} x^6 - ...\right) + a_1 \left( x + \frac{2-\lambda}{3!} x^3 + \frac{(6-\lambda)(2-\lambda)}{5!} x^5 + ...\right)

but going with r =1 I get
<br /> \sum (n+1) n a_n x^{n-1} - 2 \sum (n+1) a_n x^{n+1} + \sum \lambda x^{n+1} = 0<br />
<br /> a_{n+2} = \frac{2(n+1)- \lambda}{(n+2)(n+1)}<br />
<br /> y(x) = a_0 \left(x + \frac{2 - \lambda}{2!} x^3 + \frac{(6-\lambda)(2-\lambda)}{4!} x^5 + ...\right) + a_1 \left( x^2 + \frac{4-\lambda}{3!} x^4 + \frac{(6-\lambda)(4-\lambda)}{5!} x^6 + ... \right)<br />

Sou now I'm confused
1. Because I get four different linearly independent solutions to a second order equation, even though they're very similar which makes me think they might be related
2. I'm not sure how the method of Frobenius is supposed to work around ordinary points. I thought it was a more general power series method good for both ordinary and regular singular points, but now I'm not so sure if it's supposed to be used around ordinary points.
3. Arfken&Weber says I should have an even solution for r=0, with all powers of x even in the power expansion, and for r=1 I should take only odd powers of x for the power series expansion. That might make sense, but I can't understand where that comes from, it seems just pulled out of hat.Why can't we have both even and odd powers for r=0 and r=1?
 
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sunquick said:
the indicial equation that in this case reads
r(r-1)=0
Are you sure?
 
Well now I'm not ..
 

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