Garnet N. Ord

Department of Math, Physics and Computer Science


 

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  • Dr. L. Nottale (Fractal Space-time)
  • Dr. S. Goldstein (Foundations, Bohm)
  • Dr. D. Finklestein (Quantum Topology)
  • Schroedinger's Equation

    This section contains abstracts of representative papers:

    The Schroedinger and Diffusion Propagators Coexisting on a Lattice

     The Schroedinger and Diffusion Equations are normally related only through a formal analytic continuation. There are apparently no intermediary partial differential equations with physical interpretations that can form a conceptual bridge between the two. However if one starts off with a symmetric binary random walk on a lattice then it is possible to show that both equations occur as approximate descriptions of different aspects of the same classical probabilistic system. This suggests that lattice calculations may prove to be a useful intermediary between classical and quantum physics. The above figure shows the appearance of the diffusive and Feynman propagators at fixed time as the space-time lattice is refined. Both these functions are observable characteristics of the same physical system. (J. Phys. A. Lett. 7 March 1996) 
     

    Classical Spin in a Potential Field
     

    We consider an ensemble of restricted discrete random walks in 2+1 dimensions. The restriction on the walks is such as to give particles an intrinsic angular momentum. The walks are embedded in a field which affects the mean free path of the walks. We show that the dynamics of the walks are such that second order effects are described by a discrete form of Schroedinger's equation for particles in a potential field. This provides a classical context of the equation which is independent of its quantum context. 
     

    Random Walks, Continuum Limits and Schroedinger's Equation

    By considering the simple binary symmetric random walk on a discrete lattice in $1+1$ dimensions, we show that the discrete analog of Schroedinger's equation describes a simple counting problem involving the sample paths on the lattice. Schroedinger's equation is obtained in the continuum limit with the result that this equation is confirmed to have a classical as well as a quantum context. (G.N. Ord and A.S. Deakin, Phys. Rev. A v.54 #5 1996) 
     

    Schroedinger's Equation and Discrete Random Walks in a Potential Field 

    It has been recently noted that the free particle Schroedinger equation in 1+1 dimensions occurs naturally in the description of correlations in random walks. In this non-quantum context, wave function solutions describe features of ensembles of random walks on lattices and are as a consequence observable and easily interpreted. In this article we extend this result to show that the original random walk system may be modified to include a smooth temperature field which locally alters the walker's expected mean free path. This modification effects the correlations in such a way that Schroedinger's free particle equation aquires a potential term. (G.N. Ord Annals of Physics 250, August 1996) 
     

    Random Walks and Schroedinger's equation in 2+1 Dimensions

    We consider an ensemble of restricted discrete random walks in 2+1 dimensions. The restriction on the walks is such as to give particles an intrinsic angular momentum. The walks are embedded in a field which affects the mean free path of the walks. We show that the dynamics of the walks are such that second order effects are described by a discrete form of Schroedinger's equation for particles in a potential field. This provides a classical context of the equation which is independent of its quantum context.