Nambu goto effect

The Nambu-Goto action ( English Nambu-Goto action , after Yōichirō Nambu and Tetsuo Gotō ) is the simplest possible effect of a conformal field theory on a two-dimensional manifold and the effect of the boson string theory .

${\displaystyle S=T\int _{\Sigma }d\sigma d\tau {\sqrt {-|h|}}}$.

It was introduced by Yōichirō Nambu in 1970 and by Tetsuo Gotō in 1971 .

It is equivalent to the Polyakov effect . Further see string theory .

Individual evidence

1. ^ Yōichirō Nambu, Lectures Copenhagen Symposium August 1970, published in Nambu, Selected Papers 1995
2. ↑ Tetsuo Gotō, Relativistic quantum mechanics of one dimensional mechanical continuum and subsidiary condition of dual resonance model, Progress Theoretical Physics, Volume 46, 1971, p. 1560