Abstract
The quantum statistical aspects of a simple classical order parameter equation will be discussed in view of a previously developed procedure for the quantization of dissipative systems in the Lagrange-Hamilton formalism. Regarding the lack of knowledge concerning the quantum nature of the physical interactions underlying the systems behaviour, however, one can of course only expect to obtain incomplete information about its quantum noise features. After quantising the classical equation of motion the density operator equation is derived.
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More From: Zeitschrift f�r Physik B Condensed Matter and Quanta
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