The Momentum Eigenstates and the Lorentz-Invariant State

  • Lutz Castell
Chapter

Abstract

I have some difficulties about which topic in C.F. von Weizsäcker’s ur theory I should write. There are fascinating new developments in this area, which lead to a quantized form of time and space, but which may be too lengthy for this volume. So I want to report on an elegant derivation of a formula, in which C.F. von Weizsäcker has been most interested. This is the following: The eigenstates of the momentum operator of a mass 0, spin 0 particle (in the simplest case) can be interpreted as superpositions of many-ur and anti-ur states in a quite natural way [1].

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References

  1. 1.
    L. Castell: In L. Castell, M. Drieschner and C.F. von Weizsäcker (eds.): Quantum Theory and the Structures of Time and Space. Vol. 1, C. Hanser Verlag, München 1975, p. 147Google Scholar
  2. 2.
    L. Castell: In L. Castell, M. Drieschner and C.F. von Weizsäcker (eds.): Quantum Theory and the Structures of Time and Space. Vol. 2, C. Hanser Verlag, München 1977, p. 130Google Scholar
  3. 3.
    L. Castel: Phys. Rev. D6, 563 (1972)Google Scholar

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© Springer-Verlag Berlin Heidelberg 2003

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  • Lutz Castell

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