Instantons appear as classical solutions of Yang-Mills equation due to nontrivial topology of nonabelian gauge group. They may play some role in physics because of requirement of finiteness of vacuum energy. When we ask how explicitly instantons affect on physics, we must use quantum description: nontrivial homotopy group of nonabelian symmetry group and requirement of the finiteness of energy imply the statement that there are infinite number of different topological vacua which are labelled by discrete winding number n, and the true vacuum of theory is superposition of these vacua,
|vac⟩≡∑neinθ|n⟩
This is exactly quantum approach. Instantons then acquire as quasiclassical amplitude of tunneling between vacua when we include extended field configurations in path integral (this is required by principle of cluster decomposition of S-matrix),
⟨n−1|ˆS|n⟩≠0,
and the amplitude is exponent with degree
∼1ℏ. That's where
ℏ arises.
This post imported from StackExchange Physics at 2016-09-04 15:25 (UTC), posted by SE-user Name YYY