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    A New Form of Path Integral for the Coherent States Representation and its Semiclassical Limit

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    The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feynman's path integral. These different representations, although equivalent quantum mechanically, lead to different semiclassical limits. Two such semiclassical formulas were derived in \cite{Bar01} for the two corresponding path integral forms suggested by Klauder and Skagerstan in \cite{Klau85}. Each of these formulas involve trajectories governed by a different classical representation of the Hamiltonian operator: the P representation in one case and the Q representation in other. In this paper we construct a third representation of the path integral whose semiclassical limit involves directly the Weyl representation of the Hamiltonian operator, i.e., the classical Hamiltonian itself.Comment: 16 pages, no figure

    EUROPEAN UNION 1997 SEAFOOD-SAFETY BAN: THE ECONOMIC IMPACT ON BANGLADESH SHRIMP PROCESSING

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    Major markets for Bangladesh frozen shrimp are the European Union, the United States, and Japan. Bangladesh frozen shrimp imports into the EU and the United States have experienced safety and quality problems. The 1997 European Commission ban on Bangladesh seafood imports into the EU cost the Bangladesh frozen shrimp processing industry US$14.665 million in lost revenues.Resource /Energy Economics and Policy,

    Coherent State Path Integrals in the Weyl Representation

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    We construct a representation of the coherent state path integral using the Weyl symbol of the Hamiltonian operator. This representation is very different from the usual path integral forms suggested by Klauder and Skagerstan in \cite{Klau85}, which involve the normal or the antinormal ordering of the Hamiltonian. These different representations, although equivalent quantum mechanically, lead to different semiclassical limits. We show that the semiclassical limit of the coherent state propagator in Weyl representation is involves classical trajectories that are independent on the coherent states width. This propagator is also free from the phase corrections found in \cite{Bar01} for the two Klauder forms and provides an explicit connection between the Wigner and the Husimi representations of the evolution operator.Comment: 23 page
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