Consider a double-well potential V(x)=λ(x2−a2)2.
(a) Find the instanton solution in imaginary time that connects the two minima x=±a.
(b) Compute the classical action SE of the instanton.
(c) Show that the instanton contribution to the tunneling amplitude between the two wells goes as e−SE/ℏ and relate this to the energy splitting between the ground and first excited states.