1957
DOI: 10.1007/bf03157612
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The interference phenomena of light at very low intensities

Abstract: An interference pattern is obtained with a Michelson interferometer; the intensity distribution in the pattern is determined by counting the tate of photons by means of a photomultiplier. It is shown that the pattern obtained for very low intensities of light does not differ outside the margin of experimental error from the pattern obtained for normal intensities. At low intensities about 106 photons enter the interferometer per sec ; thus for these low intensities in average at any time much less than one pho… Show more

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Cited by 38 publications
(4 citation statements)
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“…After the second world war, this type of experiments has been resumed again in the mid 1950s by Jánossy and Náray [23]. The interference apparatus was a Michelson interferometer, the spectroscopic line was mercury's green line at 546.1 nm, the detector a photomultiplier tube.…”
Section: Photons Interference and First 'Which Path Measurement'mentioning
confidence: 99%
“…After the second world war, this type of experiments has been resumed again in the mid 1950s by Jánossy and Náray [23]. The interference apparatus was a Michelson interferometer, the spectroscopic line was mercury's green line at 546.1 nm, the detector a photomultiplier tube.…”
Section: Photons Interference and First 'Which Path Measurement'mentioning
confidence: 99%
“…The first attempt to investigate the question experimentally [26] consisted of registering on a photographic plate the diffraction pattern of a needle illuminated with extremely attenuated light, so that the energy flux expressed in the number of photons per second would correspond to an average distance between the photons much larger than the size of the apparatus. This pioneering experiment was followed by a long series of diffraction [27] and interference [28][29][30][31][32][33] experiments with light emitted by strongly attenuated ordinary light sources, mostly discharge lamps, so that the average rate of photons entering the interferometric device, estimated as the power divided by the energy of a photon, ranged between 10 2 and 10 7 s −1 . Even at the largest of these rates, the average distance between photons was more than 10 m, much larger than the size of the interferometric device used in the corresponding experiment.…”
Section: In Search Of Feeble Light's Wave-like Properties: a Short Himentioning
confidence: 99%
“…Young's experiment has been performed using an ultraweak source. (23~ The two slits of Young have also been replaced by a beam splitter (24) and by a pair of independently tuned laser sources. (25) For someone like Schr6dinger, or the present authors, all this evidence is unremarkable.…”
Section: Light--waves or Particles?mentioning
confidence: 99%