1960
DOI: 10.1088/0034-4885/23/1/303
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Photoelectric photometry

Abstract: T h e development of photoelectric devices has occasioned considerable changes in all types of instrument in which intensities are measured or compared. These devices are directly sensitive to flux and the optical systems used with them must be designed accordingly. At very low intensities the photomultiplier cell allows a light flux of only a few quanta per second to be measured and the theoretical limitations and practical arrangements are discussed. In the ultra-violet spectrum, the photoelectric technique … Show more

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Cited by 25 publications
(9 citation statements)
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“…With a large resting fluorescence, the noise in the measurements was predominantly due to random arrival of photons at the photodetector, and the signal-to-noise ratio was proportional to (i,)~/2 (Braddick, 1960). In this situation the signal-to-noise ratio depended upon the incident excitation intensity, the fraction of the emitted light reaching the detector, the quantum efficiency of the detector, as well as AI/I, (Cohen, Hille & Keynes, 1969).…”
Section: Resultsmentioning
confidence: 99%
“…With a large resting fluorescence, the noise in the measurements was predominantly due to random arrival of photons at the photodetector, and the signal-to-noise ratio was proportional to (i,)~/2 (Braddick, 1960). In this situation the signal-to-noise ratio depended upon the incident excitation intensity, the fraction of the emitted light reaching the detector, the quantum efficiency of the detector, as well as AI/I, (Cohen, Hille & Keynes, 1969).…”
Section: Resultsmentioning
confidence: 99%
“…The root mean square statistical noise in a light measurement made over a certain period is equal to the square root of the number of photons detected during that period (Braddick, 1960). Thus the percentage of noise is reduced by increasing the number of photons in each measurement.…”
Section: Optical Changes In Electric Organ 491 Methodsmentioning
confidence: 99%
“…With currently available light sources, there are random fluctuations in the number of photons emitted (and measured) per unit time; the root-mean-square (r.m.s.) deviation in the number measured is the square root of the average number (Braddick 1960;Malmstadt et al 1974). Thus, in a shot-noise-limited measurement, the signal-to-noise ratio is directly proportional to the square root of the number of measured photons and inversely proportional to the square root of the bandwidth of the photodetection system.…”
Section: Noise In Optical Measurementsmentioning
confidence: 99%