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  1. On the energy-time uncertainty relation. Part II: Pragmatic time versus energy indeterminacy. [REVIEW]Paul Busch - 1990 - Foundations of Physics 20 (1):33-43.
    The discussion of a particular kind of interpretation of the energy-time uncertainty relation, the “pragmatic time” version of the ETUR outlined in Part I of this work [measurement duration (pragmatic time) versus uncertainty of energy disturbance or measurement inaccuracy] is reviewed. Then the Aharonov-Bohm counter-example is reformulated within the modern quantum theory of unsharp measurements and thereby confirmed in a rigorous way.
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  • On the energy-time uncertainty relation. Part I: Dynamical time and time indeterminacy. [REVIEW]Paul Busch - 1990 - Foundations of Physics 20 (1):1-32.
    The problem of the validity and interpretation of the energy-time uncertainty relation is briefly reviewed and reformulated in a systematic way. The Bohr-Einsteinphoton-box gedanken experiment is seen to illustrate the complementarity of energy andevent time. A more recent experiment with amplitude-modulated Mößbauer quanta yields evidence for the genuine quantum indeterminacy of event time. In this way, event time arises as a quantum observable.
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  • Lorentz deformation and the jet phenomenon.Y. S. Kim, Marilyn E. Noz & S. H. Oh - 1979 - Foundations of Physics 9 (11-12):947-954.
    It is shown that the Lorentz-deformation property discussed in previous papers is consistent with the hadronic jet phenomenon in high-energy production processes.
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  • Time-energy uncertainty and relativistic canonical commutation relations in quantum spacetime.Eduard Prugovečki - 1982 - Foundations of Physics 12 (6):555-564.
    It is shown that the time operatorQ 0 appearing in the realization of the RCCR's [Qμ,Pv]=−jhgμv, on Minkowski quantum spacetime is a self adjoint operator on Hilbert space of square integrable functions over Σ m =σ×v m , where σ is a timelike hyperplane. This result leads to time-energy uncertainty relations that match their space-momentum counterparts. The operators Qμ appearing in Born's metric operator in quantum spacetime emerge as internal spacetime operators for exciton states, and the condition that the metric (...)
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  • Lorentz deformation and the jet phenomenon. II. Explanation of the nearly constant average jet transverse momentum.S. H. Oh, Y. S. Kim & Marilyn E. Noz - 1980 - Foundations of Physics 10 (7-8):635-639.
    It is shown that the jet mechanism derivable from the Lorentz deformation picture leads to a nearly constant average jet transverse momentum. It is pointed out that this is consistent with the high-energy experimental data. It is pointed out further that this result strengthens the physical basis for the minimal time-energy uncertainty combined covariantly with Heisenberg's space-momentum uncertainty relation.
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  • Physical principles in quantum field theory and in covariant harmonic oscillator formalism.D. Han, Y. S. Kim & Marilyn E. Noz - 1981 - Foundations of Physics 11 (11-12):895-905.
    It is shown that both covariant harmonic oscillator formalism and quantum field theory are based on common physical principles which include Poincaré covariance, Heisenberg's space-momentum uncertainty relation, and Dirac's “C-number” time-energy uncertainty relation. It is shown in particular that the oscillator wave functions are derivable from the physical principles which are used in the derivation of the Klein-Nishina formula.
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  • Four-space formulation of Dirac's equation.A. B. Evans - 1990 - Foundations of Physics 20 (3):309-335.
    Dirac's equation is reviewed and found to be based on nonrelativistic ideas of probability. A 4-space formulation is proposed that is completely Lorentzinvariant, using probability distributions in space-time with the particle's proper time as a parameter for the evolution of the wave function. This leads to a new wave equation which implies that the proper mass of a particle is an observable, and is sharp only in stationary states. The model has a built-in arrow of time, which is associated with (...)
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