Hamiltonian Approach to Secondary Quantization


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Structures and objects used in Hamiltonian secondary quantization are discussed. By the secondary quantization of a Hamiltonian system ℋ, we mean the Schrödinger quantization of another Hamiltonian system ℋ1 for which the Hamiltonian equation is the Schrödinger one obtained by the quantization of the original Hamiltonian system ℋ. The phase space of ℋ1 is the realification ℍR of the complex Hilbert space ℍ of the quantum analogue of ℋ equipped with the natural symplectic structure. The role of a configuration space is played by the maximal real subspace of ℍ.

作者简介

V. Kozlov

Steklov Mathematical Institute

Email: smolyanov@yandex.ru
俄罗斯联邦, Moscow, 119991

O. Smolyanov

Faculty of Mechanics and Mathematics; Moscow Institute of Physics and Technology (State University)

编辑信件的主要联系方式.
Email: smolyanov@yandex.ru
俄罗斯联邦, Moscow, 119991; Dolgoprudnyi, Moscow oblast, 141700

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