Note on Stochastic Quantization of Field Theories with Bottomless Actions : Particles and Fields
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概要
- 論文の詳細を見る
It is shown that the kerneled Langevin equation, which has recently been proposed by Tanaka et al. to quantize field theories with bottomless action, reproduces perturbation theory results independent of the initial conditions. The effective potential is approximately determined from the kerneled Langevin equation to be bounded from below. The evolution equation for the two-point correlation function also defines the effective potential for the propagator, which is given for the zero-dimensional "wrong-sign" -λφ^4 model under the assumption that all higher-moment cumulants than the second vanish.
- 理論物理学刊行会の論文
- 1993-07-25
著者
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Morita Katsusada
Department Of Physics Kyoto University
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Ito Masatoshi
Department Of Bioinformatics Soka University
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Ito Masatoshi
Department Of Applied Mathematics Faculty Of Science Science University Of Tokyo
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Morita Katsusada
Department Of Physics Dalhousie University Halifax : Nagoya University
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MORITA Katsusada
Department of Physics, Faculty of Science, Nagoya University
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