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 h \rightarrow 0 limit of quantum mechanics(rather action >> \hbar,from path integral formulation),so should it be possible to argue from a path integral approach, that ray optics is the \lambda\rightarrow 0 limit of wave optics.What would such a path integral be?Here we go:-
The optical action may be written as
<br /> S=\int \frac{ds}{v(x,y,z)}=\int dt,
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
<br /> \begin{equation}<br /> P=\sum_{all paths}\exp{\iota S/T_0},<br /> \end{equation}<br />
where T_0 is the time period.
As long as S=\int dt is not very large compared to T_0,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
<br /> \begin{equation}<br /> \frac{1}{T_0}=\nu=\frac{E}{h}.<br /> \end{equation}<br />
Hence for a photon,prob. amplitude to go from one point to the other is given as
<br /> \begin{equation}<br /> P=\sum_{all paths}\exp{\iota ES/h},<br /> \end{equation}<br />
i.e.
<br /> \begin{equation}<br /> P=\sum_{all paths}\exp{\frac{\iota E\int dt}{h}}<br /> \end{equation}<br />
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!
Just as classical mechanics is the h \rightarrow 0 limit of quantum mechanics(rather action >> \hbar,from path integral formulation),so should it be possible to argue from a path integral approach, that ray optics is the \lambda\rightarrow 0 limit of wave optics.What would such a path integral be?Here we go:-
The optical action may be written as
<br /> S=\int \frac{ds}{v(x,y,z)}=\int dt,
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
<br /> \begin{equation}<br /> P=\sum_{all paths}\exp{\iota S/T_0},<br /> \end{equation}<br />
where T_0 is the time period.
As long as S=\int dt is not very large compared to T_0,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
<br /> \begin{equation}<br /> \frac{1}{T_0}=\nu=\frac{E}{h}.<br /> \end{equation}<br />
Hence for a photon,prob. amplitude to go from one point to the other is given as
<br /> \begin{equation}<br /> P=\sum_{all paths}\exp{\iota ES/h},<br /> \end{equation}<br />
i.e.
<br /> \begin{equation}<br /> P=\sum_{all paths}\exp{\frac{\iota E\int dt}{h}}<br /> \end{equation}<br />
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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