Quantum Mechanics hydrogen atom eigenfunction problem

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SUMMARY

The discussion focuses on the orthogonality of eigenfunctions of the hydrogen atom's 3p state, specifically using Hermitian operators. It establishes that for eigenvalues k and l corresponding to eigenstates |k⟩ and |l⟩, where k≠l, the states are orthogonal. The mathematical derivation involves applying the Hermitian operator Lz and utilizing properties of eigenvalues and eigenstates. The conclusion confirms that since k and l are distinct, the inner product ⟨l|k⟩ equals zero, demonstrating the orthogonality of the states.

PREREQUISITES
  • Understanding of Hermitian operators in quantum mechanics
  • Familiarity with eigenvalues and eigenstates
  • Knowledge of ket notation and its application in quantum mechanics
  • Basic principles of angular momentum in quantum systems
NEXT STEPS
  • Study the properties of Hermitian operators in quantum mechanics
  • Learn about the significance of eigenvalues and eigenstates in quantum systems
  • Explore the application of angular momentum operators, specifically Lz, in quantum mechanics
  • Investigate the mathematical framework of ket notation and its advantages in quantum mechanics
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Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators seeking to deepen their understanding of eigenfunction properties in quantum systems.

cemtu
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Homework Statement
How to show that eigenvalues of 3p state of a hydrogen atom are perpendicular to each other?
Relevant Equations
I am not sure if this solution is correct
This is a general property of eigenvectors of Hermitian operators. State functions are a particular class of vector, and it is easiest to work in the general formalism (I am hoping to show how ket notation makes qm easier, not just do standard bookwork at this level). Suppose O is a Hermitian operator with eigenvalues k and l with k≠l corresponding to eigenstates |k⟩ and |l⟩

O|k⟩=k|k⟩(1)

O|l⟩=l|l⟩(2)
For the present case, we are interested in the orthogonality of angular momentum states, so O can be taken to be Lz, but the principle is completely general.

Act on https://physics.stackexchange.com/questions/547478/how-to-show-that-eigenfunctions-of-3p-state-of-a-hydrogen-atom-are-perpendicular#mjx-eqn-eq1 with ⟨k|

⟨k|O|k⟩=k⟨k|k⟩

It follows at once that k is real (as are all eigenvalues of a Hermitian operator). Act on https://physics.stackexchange.com/questions/547478/how-to-show-that-eigenfunctions-of-3p-state-of-a-hydrogen-atom-are-perpendicular#mjx-eqn-eq2 with ⟨k|

⟨k|O|l⟩=l⟨k|l⟩

Take the complex conjugate

⟨l|O|k⟩=l⟨l|k⟩(3)

Act on https://physics.stackexchange.com/questions/547478/how-to-show-that-eigenfunctions-of-3p-state-of-a-hydrogen-atom-are-perpendicular#mjx-eqn-eq1 with ⟨l|⟨l|O|k⟩=k⟨l|k⟩(4)

Subtract https://physics.stackexchange.com/questions/547478/how-to-show-that-eigenfunctions-of-3p-state-of-a-hydrogen-atom-are-perpendicular#mjx-eqn-eq3 from https://physics.stackexchange.com/questions/547478/how-to-show-that-eigenfunctions-of-3p-state-of-a-hydrogen-atom-are-perpendicular#mjx-eqn-eq4

(k−l)⟨l|k⟩=0

Since k≠l, |k⟩ and |l⟩ are orthogonal (not perpendicular, that applies to ordinary 3-vectors).
 
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Looks good to me.
 
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