2012
DOI: 10.1016/j.nuclphysb.2011.09.006
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From constrained stochastic processes to the nonlinear sigma model. Two old problems revisited

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“…[21], in which six non-Abelian Chern-Simon fields are necessary in order to reproduce the exponent e −iλτ 3 (C 1 ,C 2 ,C 3 ) , where τ 3 (C 1 , C 2 , C 3 ) is the Massey type invariant of Eq. (43). Moreover, in the present approach the introduction of non-local gauge invariant and metric independent operators like those of Ref.…”
Section: Discussionmentioning
confidence: 96%
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“…[21], in which six non-Abelian Chern-Simon fields are necessary in order to reproduce the exponent e −iλτ 3 (C 1 ,C 2 ,C 3 ) , where τ 3 (C 1 , C 2 , C 3 ) is the Massey type invariant of Eq. (43). Moreover, in the present approach the introduction of non-local gauge invariant and metric independent operators like those of Ref.…”
Section: Discussionmentioning
confidence: 96%
“…(1) and the Massey invariant of Eq. (43). The final field theoretical models are respectively given in Eq.…”
Section: Discussionmentioning
confidence: 99%
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