From Zee's Quantum Theory in a Nutshell he explains how the classical limit of quantum mechanics can be recovered from the path integral formalism.
It can be shown that the path integral formalism is:
$$ \langle q_F | e^{-iHT} | q_I \rangle = \int Dq(t)e^{i \int_0^T dt L(\dot{q},q)}$$
He then restores Planck's constant to get
$$\langle q_F | e^{-i/\hbar HT} | q_I \rangle = \int Dq(t)e^{(i/\hbar) \int_0^T dt L(\dot{q},q)}$$
I do not understand what he means by restoring Planck's constant, why he wants to do this and why he is allowed to do this.
Then he says to take the limit $\hbar \rightarrow 0$.
What is the motivation for taking this limit?? I just cannot see what the intuition for doing this is.
Moreover, once you have done this they obtain $e^{(i/\hbar) \int_0^T dt L(\dot{q_c},q_c)}$ where $q_c(t)$ is the classical path.
What does he mean by the classical path? I really dont remember this in my course on Quantum Mechanics so I must be missing something here.