Abstract
It is observed that the in and out states of a particle of energy k 2/2m, entering or leaving a Coulomb field along the +z direction, are eigenstates of L3 with eigenvalue 0, and of A3, the third component of the Runge-Lenz vector, with eigenvalues ±αx+ik/m, respectively. From this characterization and the commutation relations of the symmetry group, the phase shifts are easily obtained algebraically.
Original language | English (US) |
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Pages (from-to) | 1858-1860 |
Number of pages | 3 |
Journal | Journal of Mathematical Physics |
Volume | 8 |
Issue number | 9 |
DOIs | |
State | Published - 1967 |
ASJC Scopus subject areas
- Statistical and Nonlinear Physics
- Mathematical Physics