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Seventy years of the Klein paradox
The Klein paradox is examined. Its explanation in terms of electron–positron production is reassessed. It is shown that a potential well or barrier in the Dirac equation can produce positron or electron emission spontaneously if the potential is strong enough. The vacuum charge and lifetime of the w...
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Published in: | Physics reports 1999-07, Vol.315 (1), p.41-58 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that cite this one |
Online Access: | Get full text |
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Summary: | The Klein paradox is examined. Its explanation in terms of electron–positron production is reassessed. It is shown that a potential well or barrier in the Dirac equation can produce positron or electron emission spontaneously if the potential is strong enough. The vacuum charge and lifetime of the well/barrier are calculated. If the well is wide enough, a seemingly constant current is emitted. These phenomena are transient whereas the tunnelling first calculated by Klein is time-independent. Furthermore, tunnelling without exponential suppression occurs when an electron is incident on a high barrier, even when it is not high enough to radiate. Klein tunnelling is therefore a property of relativistic wave equations and not necessarily connected to particle emission. The Coulomb potential is investigated in this context: it is shown that a heavy nucleus of sufficiently large
Z will bind positrons. Correspondingly, it is expected that as
Z increases the Coulomb barrier will become increasingly transparent to positrons. This is an example of Klein tunnelling. |
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ISSN: | 0370-1573 1873-6270 |
DOI: | 10.1016/S0370-1573(99)00023-X |