Formal properties of eigenfunctions

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SUMMARY

The discussion focuses on the formal properties of energy eigenfunctions in quantum mechanics, specifically addressing the nature of energy eigenstates E(x). It is established that energy eigenstates can be chosen to be purely real functions, even though the physical wavefunction is complex. If an eigenfunction is not real, it can be expressed as a complex linear combination of two real eigenstates with the same energy. The hint provided emphasizes the relevance of the Schrödinger equation in demonstrating the separability of real and imaginary parts of the eigenfunctions.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically energy eigenstates.
  • Familiarity with the Schrödinger equation and its implications.
  • Knowledge of complex numbers and their linear combinations.
  • Basic mathematical proof techniques relevant to physics.
NEXT STEPS
  • Study the implications of the Schrödinger equation on eigenfunctions in quantum mechanics.
  • Explore the concept of complex linear combinations in the context of quantum states.
  • Learn about the physical interpretation of real versus complex wavefunctions.
  • Investigate the mathematical properties of eigenvalues and eigenfunctions in quantum systems.
USEFUL FOR

Students and professionals in physics, particularly those studying quantum mechanics, as well as mathematicians interested in the formal properties of eigenfunctions and their applications in physical theories.

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Homework Statement



Give a physicist's proof of the following statements regarding energy eigenfunctions:
(a) We can always choose the energy eigenstates E(x) we work with to be purely real
functions (unlike the physical wavefunction, which is necessarily complex). Note: This does not mean that every energy eigenfunction is real, rather if you fi nd an eigenfunction that is not real, it can always be written as a complex linear combination
of two real eigenstates with the same energy.

Hint: If E(x) is an energy eigenstate with energy eigenvalue E, what can be said about E(x)
?

Homework Equations





The Attempt at a Solution



I'm having a hard to deciphering here what is warranted I show in this problem. Does anyone know what this is trying to get at. Maybe my mathematical experience with proofs is getting in the way because I'm trying to do it more generally.
 
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black_hole said:

Homework Statement



Give a physicist's proof of the following statements regarding energy eigenfunctions:
(a) We can always choose the energy eigenstates E(x) we work with to be purely real
functions (unlike the physical wavefunction, which is necessarily complex). Note: This does not mean that every energy eigenfunction is real, rather if you find an eigenfunction that is not real, it can always be written as a complex linear combination
of two real eigenstates with the same energy.

Hint: If E(x) is an energy eigenstate with energy eigenvalue E, what can be said about E(x)
?

Homework Equations


The Attempt at a Solution



I'm having a hard to deciphering here what is warranted I show in this problem. Does anyone know what this is trying to get at. Maybe my mathematical experience with proofs is getting in the way because I'm trying to do it more generally.

The hint is probably that it satisfies the Schrödinger equation. Can you show that the real and imaginary parts satisfy the equation separately? Show this wouldn't be true if the eigenvalue were not real.
 
Last edited:

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