- #1
gptejms
- 386
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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}
P=\sum_{all paths}\exp{\iota S/T_0},
\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}
\frac{1}{T_0}=\nu=\frac{E}{h}.
\end{equation}
[/tex]
Hence for a photon,prob. amplitude to go from one point to the other is given as
[tex]
\begin{equation}
P=\sum_{all paths}\exp{\iota ES/h},
\end{equation}
[/tex]
i.e.
[tex]
\begin{equation}
P=\sum_{all paths}\exp{\frac{\iota E\int dt}{h}}
\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!
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}
P=\sum_{all paths}\exp{\iota S/T_0},
\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}
\frac{1}{T_0}=\nu=\frac{E}{h}.
\end{equation}
[/tex]
Hence for a photon,prob. amplitude to go from one point to the other is given as
[tex]
\begin{equation}
P=\sum_{all paths}\exp{\iota ES/h},
\end{equation}
[/tex]
i.e.
[tex]
\begin{equation}
P=\sum_{all paths}\exp{\frac{\iota E\int dt}{h}}
\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!
Last edited: