1997
DOI: 10.1103/physreva.56.1938
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Levinson theorem in two dimensions

Abstract: A two-dimensional analogue of Levinson's theorem for nonrelativistic quantum mechanics is established, which relates the phase shift at threshold(zero momentum) for the $m$th partial wave to the total number of bound states with angular momentum $m\hbar(m=0,1,2,...)$ in an attractive central field.Comment: LaTeX, no figur

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Cited by 30 publications
(37 citation statements)
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“…(41), one can obtain the Levinson theorem in the form (10). However, the method of the Green functions in the form proposed by Lin [23] does not work for singular potentials. The reason is that the difference of Green functions (41) has a singularity at the origin, hence it is not integrable.…”
Section: The Levinson Theoremmentioning
confidence: 99%
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“…(41), one can obtain the Levinson theorem in the form (10). However, the method of the Green functions in the form proposed by Lin [23] does not work for singular potentials. The reason is that the difference of Green functions (41) has a singularity at the origin, hence it is not integrable.…”
Section: The Levinson Theoremmentioning
confidence: 99%
“…The 2D Levinson theorem was established for different models, too: for the Schrödinger equation [23,24], the Klein-Gordon equation [25], and the Dirac equation [26]. Moreover there exists an extension of the Levinson theorem for the Schrödinger equation in D dimensions.…”
Section: Introductionmentioning
confidence: 99%
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“…Most of works mainly studied the Levinson theorem in the three-dimensional space. With the wide interest in lower-dimensional field theories recently, the two-dimensional Levinson theorem has been studied numerically [18] as well as theoretically [19][20][21][22][23][24][25]. …”
Section: Introductionmentioning
confidence: 99%