Use of operator wave functions to construct a refined correspondence principle via the quantum mechanics of Wigner and Moyal
We represent the momentum operator p by p+(h//2i)(∂/∂p) and the position operator q by q−(h//2i)(∂/∂p). We then apply each resulting operator that appears in the nonrelativistic quantum mechanics of Schrödinger and Heisenberg to the constant 1. What results is a Wigner–Moyal theory which is as compl...
Saved in:
Published in: | American journal of physics Vol. 48; no. 11; pp. 964 - 970 |
---|---|
Main Author: | |
Format: | Journal Article |
Language: | English |
Published: |
01-11-1980
|
Subjects: | |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Summary: | We represent the momentum operator p by p+(h//2i)(∂/∂p) and the position operator q by q−(h//2i)(∂/∂p). We then apply each resulting operator that appears in the nonrelativistic quantum mechanics of Schrödinger and Heisenberg to the constant 1. What results is a Wigner–Moyal theory which is as complete as the usual Schrödinger–Heisenberg theory. Replacing Planck’s constant h/ by zero in the Wigner–Moyal theory results in the classical physics of Newton. We thereby obtain a refined correspondence principle. |
---|---|
ISSN: | 0002-9505 1943-2909 |
DOI: | 10.1119/1.12197 |