Physics Notes: The action and the wave function

I read in volume III of Landau's and Lifshitz's Theoretical Physics that the action of classical mechanics can be seen as the complex phase of the wave function of quantum mechanics. I also read a reference somewhere else, that it was in a 1948 paper1 that Richard Feynman demonstrated this relationship. Landau and Lifshitz were not very informative, and I had no access to Feynman's old paper (I've since obtained a copy, but it's a Good Thing that I didn't have it earlier, as it gave me the motivation to do these calculations on my own), so I decided to work this out myself, at least in the simple case of a point particle in a potential field.

The Schrödinger equation of a point particle is well known:

 
φ
 = – 
ħ²
 
∂²φ
 +
t 2m q²

What if φ is expressed as ρeiS/ħ, where S is an arbitrary function of time, the coordinates, and perhaps momenta? Let's do the substitution, dropping the eiS/ħ part as it appears as a factor on both sides of the equation:

 
ρ
 – ρ 
S
 = – 
ħ²




∂²ρ
 + 
2i
 
ρ
 
S
 + 
 
∂²S
 – 
ρ



S



2 



 +
t t 2m q² ħ q q ħ q² ħ² q

Separating the real and imaginary parts yields two equations. The equation for the real part looks like this:

 – ρ 
S
 = – 
ħ²




∂²ρ
 – 
ρ



S



2 



 +
t 2m q² ħ² q

which, when divided by ρ, can be simplified as

 – 
S
 = 
1



S
2


 – 
ħ²
 
∂²ρ
 + V
t 2m q 2 q²

The smallness of ħ suggests that, at least for macroscopic systems, the second term on the right hand side can be eliminated, leaving us with the equation

 – 
S
 = 
1



S
2


 + V
t 2m q

which is the equation of motion for a point particle governed by the action S.

As a footnote of sorts, I now found that this relationship is also demonstrated in §§31-32 of Dirac's book2.


1R. P. Feynman: "Space-time Approach to Non-relativistic Quantum Mechanics", Rev. Mod. Physics, Vol 20, pp. 367-387, April 1948
2P. A. M. Dirac: "The Principles of Quantum Mechanics", Oxford University Press, 1958