A new form of path integral for the coherent states representation and its semiclassical limit
A new form of path integral for the coherent states representation and its semiclassical limit
复制标题
相干态表示的一种新的路径积分形式及其半经典极限
DOI:
10.1590/s0103-97332005000100015
复制
发表时间:
2004
影响因子:
1.6
通讯作者:
M. D. Aguiar
中科院分区:
文献类型:
--
作者:
Luis Santos;M. D. Aguiar
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 [1] for the two corresponding path integral forms suggested by Klauder and Skagerstan in [2]. 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.
DOI:
--
发表时间:
2007
期刊:
影响因子:
--
作者:
N.;Kumano-go・D.;Fujiwara;Akihiro Shimomura;T.Suzuki;Naoto Kumano-go;T.Suzuki;Naoto Kumanogo;Naoyasu Kita;T.Suzuki;Jun-ichi Segata;Naoto Kumano-go;T.Suzuki;T.Suzuki;熊ノ郷直人;Jun-ichi Segata and Akihiro Shimomura;Akihiro Shimomura and Yoshio Tsutsumi;T.Suzuki;Naoto Kumano-go;Akihiro Shimomura;T. Suzuki;熊ノ郷直人;T. Suzuki;Akihiro Shimomura;T. Suzuki;Akihiro Shimomura;熊ノ郷直人;Naoto Kumano-go
通讯作者:
Naoto Kumano-go