Abstract
With many Hamiltonians one can naturally associate a |Ψ|2-distributed Markov process. For nonrelativistic quantum mechanics, this process is in fact deterministic, and is known as Bohmian mechanics. For the Hamiltonian of a quantum field theory, it is typically a jump process on the configuration space of a variable number of particles. We define these processes for regularized quantum field theories, thereby generalizing previous work of John S. Bell [3] and of ourselves [11]. We introduce a formula expressing the jump rates in terms of the interaction Hamiltonian, and establish a condition for finiteness of the rates.
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Communicated by A. Connes
Acknowledgement We thank Ovidiu Costin, Avraham Soffer, and James Taylor of Rutgers University, Stefan Teufel of Technische Universität München, and Gianni Cassinelli and Alessandro Toigo of Università di Genova for helpful discussions. R.T. gratefully acknowledges support by the German National Science Foundation (DFG). N.Z. gratefully acknowledges support by INFN and DFG. Finally, we appreciate the hospitality that some of us have enjoyed, on more than one occasion, at the Mathematisches Institut of Ludwig-Maximilians-Universität München, at the Dipartimento di Fisica of Università di Genova, and at the Mathematics Department of Rutgers University.
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Dürr, D., Goldstein, S., Tumulka, R. et al. Quantum Hamiltonians and Stochastic Jumps. Commun. Math. Phys. 254, 129–166 (2005). https://doi.org/10.1007/s00220-004-1242-0
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DOI: https://doi.org/10.1007/s00220-004-1242-0