Abstract
The momentum operator for a particle in a box is represented by an infinite-order Hermitian matrix P. Its square P2 is well-defined (and diagonal), but its cube P3 is ill-defined, because P P2 not=P2 P. Truncating these matrices to a finite order restores the associative law, but leads to other curious results.
Original language | English |
---|---|
Article number | 027 |
Pages (from-to) | 1765-1769 |
Number of pages | 5 |
Journal | Journal of Physics A: Mathematical and General |
Volume | 28 |
Issue number | 6 |
DOIs | |
State | Published - 1995 |
Externally published | Yes |
ASJC Scopus subject areas
- Statistical and Nonlinear Physics
- Mathematical Physics
- General Physics and Astronomy