Optics – How Is Momentum Conserved in Diffraction?

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Sigh. Approaching retirement age and still deeply confused about something I first encountered in highschool 40 years ago.

Consider the usual double slit experiment. Make the light source be a laser with a beam 1 mm wide. And put it 5 meters away from the slits.

On the other side of the slits the photon shows the well known diffraction pattern, alternating dark and light bands. Good, very tidy. But consider that single photons can diffract.

So a single photon comes down the beam. The beam is 1mm wide with very little scatter, and 5 m long. So the momentum of a single photon is very tightly bounded. And moving objects near but not in the beam don't change things on the other side of the slits. Objects such as students doing the experiment in highschool, for example. If you don't get any red on you, you won't change the pattern or the brightness.

On ther other side of the screen the photon can turn quite a corner, for example 30 degrees. The energy does not change very much, since it is still the same pretty red color from the laser.

How does it manage to turn this corner and conserve momentum?

Best Answer

The slits themselves receive a tiny impulse from each photon. If a photon is diffracted to the left, the slits get nudged to the right. Every time a photon changes direction, it requires something else to gain momentum in the opposite direction, whether a solar sail or a star bending light by gravity. Since the slits are usually anchored to the ground and the impulse is so small, the effect is not observable.

Your question actually came up in a series of debates between Albert Einstein and Niels Bohr on whether quantum mechanics made any sense. Einstein argued that the impulse of a photon on the slits would allow the measurement of the photon's position and momentum at the same time, contrary to quantum theory. Bohr replied that the necessary precision of the slit momentum measurement would--through Heisenberg's Uncertainty Principle--make the slit's position uncertain enough to destroy the interference pattern, negating any measurement of the photon's position.

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