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American Journal of Physics -- February 2006 -- Volume 74, Issue 2, pp. 109
Quantum mechanics of the 1∕x2 potential
In quantum mechanics a localized attractive potential typically supports a (possibly infinite) set of bound states, characterized by a discrete spectrum of allowed energies, together with a continuum of scattering states, characterized (in one dimension) by an energy-dependent phase shift. The 1∕x2 potential on 0<x<∞ confounds all of our intuitions and expectations. Resolving its paradoxes requires sophisticated theoretical machinery: regularization, renormalization, anomalous symmetry-breaking, and self-adjoint extensions. Our goal is to introduce the essential ideas at a level accessible to advanced undergraduates.
© 2006 American Association of Physics Teachers
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Quantum mechanics
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Received Sep 2005
Accepted Dec 2005
Online Jan 2006
Accepted Dec 2005
Online Jan 2006
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