Self-adjoint extensions of operators and the teaching of quantum mechanics (original) (raw)

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Abstract

For the example of the infinite well potential, we point out some paradoxes which are solved by a careful analysis of what is a truly self-adjoint operator. We then describe the self-adjoint extensions and their spectra for the momentum and the Hamiltonian operators in different settings. Additional physical requirements such as parity, time reversal, and positivity are used to restrict the large class of self-adjoint extensions of the Hamiltonian.

Publication:

American Journal of Physics

Pub Date:

March 2001

DOI:

10.1119/1.1328351

10.48550/arXiv.quant-ph/0103153

arXiv:

arXiv:quant-ph/0103153

Bibcode:

2001AmJPh..69..322B

Keywords:

E-Print:

25 pages, Latex file, extended version of Am. J. Phys. 69 (2001) 322