Abstract

A new solution of the Euclidean equations of motion is found for the quantum-mechanical double-well potential with a four-fermion term. It extends the usual kink-instanton solution in which both the kink field and the fermionic fields contain a finite number of new terms which are polynomial in the fermionic collective coordinates. The solution has finite action, S=− m 3 3λ + 9 140 m g ϵ ijklξ iξ jξ kξ l , where ξ i,i=1,… ,4 , are fermionic collective coordinates and g, m and λ are coupling constants. We explain why in general the instanton action can depend on collective coordinates.

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