- #1
Gezstarski
- 16
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Consider a Double Slits experiment in which the light source is monochromatic and each slit very narrow. There will be many fringes visible on either side of the axis.
1) If the light source is pulsed with very short, randomly spaced, pulses it will produce spectrally broadened radiation and so the number of fringes will be reduced. Effectively each component wavelength will produce fringes with a different pitch so at large off-axis distances they will blur together. Equivalently one can say that for large offsets the path difference for radiation passing through the two slits exceeds the coherence length of the radiation. Or that the difference in light travel time for radiation passing through one slit or the other exceeds the pulse duration so photons taking the two routes cannot interfere,
2) The same effect would arise with a continuous monochromatic source if a hypothetical ultra-fast (electro-optic?) shutter were used to modulate a monochromatic light source. If the shutter is only opened for very brief intervals, again the spectrum would be broadened and the number of visible fringes reduced.
3) Suppose the shutter were placed not before the slits but immediately in front of the detector – would the effect still be the same?
4) Now suppose that instead of the shutter, the detector is one that records images at a very high frame-rate. Taking a widely spaced subset of the frames would appear to be like using the shutter and so you might expect to see just a few fringes and beyond that a uniform mean level. But stacking all the frames would be expected to be equivalent to an unmodulated source and so fringes should be apparent, even far off-axis. So in the subset there will be photons in positions where nulls are seen in the full set !
(This sequence captures the same basic physics as another thread which was closed because of an unfortunately chosen header, but it is the physics behind the problem that interests me)
1) If the light source is pulsed with very short, randomly spaced, pulses it will produce spectrally broadened radiation and so the number of fringes will be reduced. Effectively each component wavelength will produce fringes with a different pitch so at large off-axis distances they will blur together. Equivalently one can say that for large offsets the path difference for radiation passing through the two slits exceeds the coherence length of the radiation. Or that the difference in light travel time for radiation passing through one slit or the other exceeds the pulse duration so photons taking the two routes cannot interfere,
2) The same effect would arise with a continuous monochromatic source if a hypothetical ultra-fast (electro-optic?) shutter were used to modulate a monochromatic light source. If the shutter is only opened for very brief intervals, again the spectrum would be broadened and the number of visible fringes reduced.
3) Suppose the shutter were placed not before the slits but immediately in front of the detector – would the effect still be the same?
4) Now suppose that instead of the shutter, the detector is one that records images at a very high frame-rate. Taking a widely spaced subset of the frames would appear to be like using the shutter and so you might expect to see just a few fringes and beyond that a uniform mean level. But stacking all the frames would be expected to be equivalent to an unmodulated source and so fringes should be apparent, even far off-axis. So in the subset there will be photons in positions where nulls are seen in the full set !
(This sequence captures the same basic physics as another thread which was closed because of an unfortunately chosen header, but it is the physics behind the problem that interests me)
