Path integral formulation of wave-optics

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gptejms
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A few years back,I stumbled upon a nice idea which I am reporting below:-

Just as classical mechanics is the [tex]h \rightarrow 0[/tex] limit of quantum mechanics(rather action >> [tex]\hbar[/tex],from path integral formulation),so should it be possible to argue from a path integral approach, that ray optics is the [tex]\lambda\rightarrow 0[/tex] limit of wave optics.What would such a path integral be?Here we go:-

The optical action may be written as
[tex] S=\int \frac{ds}{v(x,y,z)}=\int dt,[/tex]
where the symbols are self-explanatory.So the prob. amplitude for light/sound(or photon/..) to go from point A to point B may be written as
[tex] \begin{equation}<br /> P=\sum_{all paths}\exp{\iota S/T_0},<br /> \end{equation}[/tex]
where [tex]T_0[/tex] is the time period.

As long as [tex]S=\int dt[/tex] is not very large compared to [tex]T_0[/tex],all conceivable ray paths between any two fixed points are possible,so that there is an uncertainty in the ray path taken by light/sound in going from one point to the other.

Specially interesting is the case of a photon.For a photon
[tex] \begin{equation}<br /> \frac{1}{T_0}=\nu=\frac{E}{h}.<br /> \end{equation}[/tex]
Hence for a photon,prob. amplitude to go from one point to the other is given as
[tex] \begin{equation}<br /> P=\sum_{all paths}\exp{\iota ES/h},<br /> \end{equation}[/tex]
i.e.
[tex] \begin{equation}<br /> P=\sum_{all paths}\exp{\frac{\iota E\int dt}{h}}<br /> \end{equation}[/tex]

P.S. I am not able to see the latex graphics that I've generated in my browser--hope others are able to view it!
 
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i think it should be correct..but the action would come from the Eikonal equation:

[tex](\nabla{S})^{2}=n^{2}[/tex] where n is the refraction index as a function of x,y,z,t...then the path integral for optics would be:

[tex]\int{D[r,t]e^{iS(r,t)/\hbar}[/tex]
 
The beauty about the form that I suggest is that for a photon using E=h\nu,we arrive naturally at the particle action(starting with the optical lagrangian/action).
My quick impression is that your S(phase I believe) is nothing but my S(modulo T_0)/T_0*2\pi---don't know where you get the \hbar from.
 
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Eikonal equation should follow easily from my optical action S .[tex]\delta S=0[/tex] i.e. Fermat's principle should easily lead to the eikonal equation.
The nice thing would be to show that the wave equation follows from this sum over paths approach.