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Klein paradox of the second kind

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Lettere al Nuovo Cimento (1971-1985)

Summary

In this note we discuss how a nonrelativistically nonconfining potential gives confinement when it is used as a scalar in the Klein-Gordon or Dirac equation.

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References

  1. L. I. Schiff:Quantum Mechanics, 3rd Edition (McGraw-Hill, New York, N. Y. 1968), Chapt. 13.

  2. B. Ram:Am. J. Phys.,50, 549 (1982).

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  3. M. G. Olsson:Am. J. Phys.,51, 1042 (1983).

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  4. B. Ram:Lett. Nuovo Cimento,28, 476 (1980); andM. Plesset:Phys. Rev.,41, 278 (1932).

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  5. N. N. Bogolubov:Ann. Insi. Henri Poincaré,8, 163 (1968). It has since been used in the MIT bag model:A. Chodos, R. L. Jaffe, K. Johnson, C. B. Thorn andV. F. Weisskopf:Phys. Rev. D,12, 923 (1975);D. W. Fein:Nuovo Cimento A,38, 19 (1977);B. Ram:Lett. Nuovo Cimento,23, 321 (1978);28, 476 (1980);B. Ram andR. Leon: Lett.Nuovo Cimento,36, 205 (1983).

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Authors and Affiliations

  1. Physics Department, New Mexico State University, NM88003, Las Cruces

    B. Ram

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  1. B. Ram
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Ram, B. Klein paradox of the second kind. Lett. Nuovo Cimento 43, 199–202 (1985). https://doi.org/10.1007/BF02746979

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  • DOI: https://doi.org/10.1007/BF02746979

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