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Runge-Lenz operators

We will find the following shorthand for part of the Runge-Lenz operators helpful. Set... [Pg.271]

The same is true for two more special cases, namely the relativistic particle with spin (yielding the correct Dirac energy levels), and a relativistic particle without fine structure. In these cases, the Runge-Lenz vector is no longer a constant of motion, and the O4 symmetry of the nonrelativistic problem is broken. It is, however, not seriously broken, and an analogue of the Runge-Lenz vector, the so-called Johnson-Lippman operator [10]... [Pg.11]

See other pages where Runge-Lenz operators is mentioned: [Pg.12]    [Pg.267]    [Pg.268]    [Pg.388]    [Pg.12]    [Pg.267]    [Pg.268]    [Pg.388]    [Pg.295]    [Pg.295]    [Pg.43]    [Pg.103]    [Pg.295]   
See also in sourсe #XX -- [ Pg.12 , Pg.267 ]



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