The first post in the "From Branes to Brains" series. For the introduction to the series see this post.
In this post, I will mostly follow the ideas from the classical book by Polyakov, as well as from this paper by Kleinert.
First of all, consider a classical particle with mass m in the one-dimensional potential V(x,t). If we know, that at the moment t1 the particle was in the point x1, and in the moment t2 the particle was in the point x2, the particle should have travelled between these two points along the path that minimizes the action
S[x(t),x1,x2,t1,t2]=∫t2t1dt(m2(dx(t)dt)2−V(x(t),t))
This is known as the minimal action principle. In quantum mechanics, instead, the particle travels along all the possible trajectories, according to the Feynman... (read 1010 more words →)
Ok, but what would negative probability then be?