GP....hmmm.
Let's see.
Again assuming non-relativistic non-zero motion (v/c < 0.01, mv >> hf/c) and to first order:
We have the impetus delivered by the photon as 2hf/c, so original momentum is mv and the final momentum is mv + 2hf/c. Energy transfer is elastic (or so) so the change in energy of the probe is (pf^2)/2m - (pi^2)/2m
To first order again, the energy increment is 4hfv/c, therefore this is how much of the original energy the photon loses. Note that we can see why the constraints are necessary, since for v/c > 0.25 we have that the photon descends into a negative energy state with this approximation, and for v=0 we get "something for nothing" as the photon does not lose energy in the process.
Let's see.
Again assuming non-relativistic non-zero motion (v/c < 0.01, mv >> hf/c) and to first order:
We have the impetus delivered by the photon as 2hf/c, so original momentum is mv and the final momentum is mv + 2hf/c. Energy transfer is elastic (or so) so the change in energy of the probe is (pf^2)/2m - (pi^2)/2m
To first order again, the energy increment is 4hfv/c, therefore this is how much of the original energy the photon loses. Note that we can see why the constraints are necessary, since for v/c > 0.25 we have that the photon descends into a negative energy state with this approximation, and for v=0 we get "something for nothing" as the photon does not lose energy in the process.
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