Linear equations and superposition of wavefunctions

Click For Summary

Discussion Overview

The discussion revolves around the linearity of the Schrödinger equation and the conditions under which superpositions of wavefunctions are solutions to eigenvalue equations, particularly in the context of quantum mechanics. Participants explore the implications of linearity in differential equations and eigenvalue problems.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the term "linear" in the context of the Schrödinger equation aligns with its general use in differential equations.
  • Another participant confirms that the term is indeed used in the same way and explains that the superposition of wavefunctions corresponds to different eigenvalues, which affects their status as solutions to the momentum eigenvalue equation.
  • A participant seeks clarification on the condition that superpositions of wavefunctions must satisfy to solve the eigenvalue equation, specifically that they must be linear and share the same eigenvalues.
  • Further clarification is provided that while eigenvalue equations are typically linear, distinct eigenvalues lead to sums that do not satisfy the eigenvalue equation, contrasting with cases where eigenvalues are the same.
  • Participants discuss the nature of the Schrödinger equation as a partial differential equation and draw parallels with linear ordinary differential equations, emphasizing the importance of eigenvalues in determining the validity of superpositions as solutions.

Areas of Agreement / Disagreement

Participants generally agree on the linearity of the Schrödinger equation and the conditions for superpositions to be solutions, but there is an ongoing exploration of the implications of eigenvalues, suggesting some unresolved nuances in understanding.

Contextual Notes

The discussion touches on the distinction between linear and nonlinear eigenvalue problems, but does not delve into the specifics of nonlinear cases, which remain outside the primary focus.

dyn
Messages
774
Reaction score
63
Hi. I have read many times that the Schrödinger equation is a linear equation and so if Ψ1 and Ψ2 are both solutions to the equation then so is Ψ1 + Ψ2. Is this use of the word linear the same as generally used for differential equations ? As the Schrödinger equation is also an eigenvalue equation for the Hamiltonian.

My main confusion is why a superposition of wavefunctions such as eikx + e-ikx is not a solution to the momentum eigenvalue equation as this also looks like a linear equation ?
Thanks
 
Physics news on Phys.org
dyn said:
Is this use of the word linear the same as generally used for differential equations ?
Yes.
dyn said:
My main confusion is why a superposition of wavefunctions such as eikx + e-ikx is not a solution to the momentum eigenvalue equation as this also looks like a linear equation ?
Because the summands correspond to different eigenvalues.
 
Thanks. So the condition that the superposition of wavefunctions also solves the eigenvalue equation is that it is both linear and the wavefunctions also have the same eigenvalues ?
 
dyn said:
Thanks. So the condition that the superposition of wavefunctions also solves the eigenvalue equation is that it is both linear and the wavefunctions also have the same eigenvalues ?
Yes. (Eigenvalue equations are usually linear, by the way. There does exist something called a "nonlinear eigenvalue problem", but that is not relevant here.)

The SE is a partial differential equation, but for your understanding perhaps consider the setting of a linear ordinary differential equation. In the simplest case (constant coefficients, homogeneous) a linear ODE can be written as
$$
\frac{dx}{dt}(t) = Ax(t) \qquad (\ast)
$$
(Think, for example, about the simple harmonic oscillator.) If ##x_1## and ##x_2## are both solutions, then their sum is also a solution and hence satisfies ##(\ast)##. This is superposition.

Regarding the corresponding eigenvalue problem, if ##\lambda## and ##\mu## are distinct eigenvalues of ##A## with eigenvectors ##u## and ##v##, then ##u + v## is not an eigenvector of ##A##. (Try it out.) In contrast, if ##\lambda = \mu## then it is true that
$$
A(u + v) = \lambda(u + v)
$$
In case of the SE similar remarks hold, but the matrices are replaced by (unbounded) operators that act on function spaces instead of ##\mathbb{R}^n## or ##\mathbb{C}^n##. Does this clarify matters a bit?
 
  • Like
Likes   Reactions: dyn and Nugatory
Yes. Thanks for your help.
 

Similar threads

  • · Replies 24 ·
Replies
24
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 19 ·
Replies
19
Views
2K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 31 ·
2
Replies
31
Views
4K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 8 ·
Replies
8
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 26 ·
Replies
26
Views
4K