Your image of the space of finite-energy solutions is indeed wrong. It's not a vector space. Take, for example, a model with an energy functional
∫(12(∂tϕ)2+12(∂xϕ)2+λϕ4−14ϕ2+164λ)dxdt.
In this model, there are only two possible asymptotic values for a stationary finite-energy solution
ϕ(x,t):
limx→±∞ϕ(x,t) has to be either
1√8λ or
−1√8λ, otherwise the energy cannot be finite. This solution space is not a vector space:
ϕ+(x,t)=1√8λ is a finite-energy solution, but
2ϕ+ is not.
Rather, we observe indeed that the space of finite-energy solutions has four homotopy components: There are solutions which take the positive value at both spatial infinities, those that take the negative value, and those that take the positive at one infinity and the negative at the other. There are no continuous deformations which would deform one such class of solutions into the other while keeping the function as a finite-energy solution all along the way. Of course you could deform one solution into any other if you didn't care whether it remained a solution along the way, but that's not what we're talking about here.
This post imported from StackExchange Physics at 2017-08-19 14:49 (UTC), posted by SE-user ACuriousMind