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Annals of Physics

Variational approach to the Schrödinger dynamics in the Klauder's continuous representations

M. Ploszajczak. Niels Bohr Institute

Published Jul 1, 1986• 0 citations
Publisher
DOI
10.1016/0003-4916(86)90180-6

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Klauder's continuous representation naturally allows a basic length scale. It is assumed to be fundamental for continuous dynamical variables Q and P in a general quantum theory. We explore new properties of a particle's coordinates at short distances by constructing continuous base states in the coordinate space rather than in the phase space. The results show that the position operator Q has neither eigenvalues nor eigenvectors. There emerges a picture of ``fuzzy point particles''---point particles whose positions can never be measured with an accuracy smaller than \ensuremath{\Delta}qmin=R{q}_{\mathrm{min}=\mathrm{R}}qmin=R​, where R is a very small length scale for the coordinate variable. In the limit R\ensuremath{\rightarrow}0, Klauder's continuous representation reduces to Dirac's eigenbras and kets. The property \ensuremath{\Delta}q\ensuremath{\ge}R implies that waves with arbitrarily short wavelengths do not exist in the physical world.
Based on Klauder's continuous representations in Hilbert space, we discuss a fundamental fuzziness of the coordinate and momentum variables for a quantum particle. These fuzzy dynamical variables are intimately related to a very small radical length R(\ensuremath{\lesssim}${10}^{\mathrm{\ensuremath{-}}18}$ cm) and a very large cosmological length S (\ensuremath{\gtrsim}1010{10}^{10}1010 light years). The uncertainty \ensuremath{\Delta}q for the measurement of a particle's position alone is assumed to be restricted by S\ensuremath{\gtrsim}\ensuremath{\Delta}q\ensuremath{\gtrsim}R. Physical properties of fuzzy base states (p\ensuremath{\Vert} and (q\ensuremath{\Vert} and their general cosmological and very-high-energy implications are discussed. In particular, a new density of states and its possible effects on decay rates and scattering cross sections at large momenta p\ensuremath{\gtrsim}\ensuremath{\Elzxh}/R\ensuremath{\sim}104{10}^{4}104 GeV/c (c is the velocity of light) are considered. We also discuss the superposition of waves in the presence of R and S.