Checking if Momentum Operator is Hermitian - Integration

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SUMMARY

The discussion focuses on verifying the Hermitian nature of the momentum operator in quantum mechanics, specifically through integration by parts. The user references Griffiths' solution but struggles with the application of the integration by parts formula, int(u dv) = uv - int(v du). They express confusion regarding the presence of 'dx' in the terms and how it affects the integration process. The user identifies u = f^* and derives du = (df^*/dx) dx as part of their attempt to clarify the integration steps.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically operators
  • Familiarity with integration techniques, particularly integration by parts
  • Knowledge of complex functions and their derivatives
  • Basic grasp of Griffiths' "Introduction to Quantum Mechanics" concepts
NEXT STEPS
  • Review the integration by parts method in the context of quantum mechanics
  • Study the properties of Hermitian operators in quantum mechanics
  • Explore examples of momentum operator applications in quantum systems
  • Examine Griffiths' "Introduction to Quantum Mechanics" for detailed explanations
USEFUL FOR

Students of quantum mechanics, particularly those studying operator theory and integration techniques, as well as educators seeking to clarify the Hermitian properties of operators.

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Homework Statement



I'm checking to see if the momentum operator is Hermitian. Griffiths has the solution worked out, I'm just not following the integration by parts.

Homework Equations



int(u dv) = uv - int(v du)

The Attempt at a Solution



I've attached an image of my work.

It seems there should be an additional 'dx' with my 'v' term, but then the 'uv' portion would have a 'dx', which wouldn't make much sense to me.

Thanks for your time.
 

Attachments

  • integral.jpg
    integral.jpg
    21.7 KB · Views: 524
Physics news on Phys.org
If you set ##u = f^*##, then
$$
\frac{du}{dx} = \frac{df^*}{dx}
$$
hence
$$
du = \frac{df^*}{dx} dx
$$
 

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