DocumentCode
972208
Title
Triple correlations
Author
Lohmann, Adolf W. ; Wirnitzer, Bernhard
Author_Institution
Physikalisches Institute der Universität Erlangen-Nürnberg, Erlangen, Federal Republic of Germany
Volume
72
Issue
7
fYear
1984
fDate
7/1/1984 12:00:00 AM
Firstpage
889
Lastpage
901
Abstract
The (auto)triple correlation l(3)(t1 , t2 ) is defined as the triple function integral, applied to the signal l(t) l(3)(t1 , t2 ) = ∫ l(t)l(t + t1 )l(t + t2 ) dt. The triple correlation l(3)(t1 , t2 ) is less popular than the standard (double) correlation l(2)(t1 ) for several reasons: l(2)is sometimes easier to observe and to process, l(3)is small for many bipolar or complex signals, the mathematics associated with l(2)is better known. On the other hand, the triple correlation l(3)knows more about the signal l than does the ordinary autocorrelation l(2). Also l(3)is in some ways more sensitive, in other ways less sensitive to noise, to bias drifts, etc. Hence, there are situations, where it is quite favorable to evaluate one-dimensional signals or two-dimensional pictures by means of their triple correlations. We will review the underlying mathematical tools and report on our projects where triple correlations were employed for studying laser pulse shapes, sound quality, halftone print statistics, mobility of bacteria, and astronomical speckle interferometry. We will mention also how others have used the triple correlation for ocean waves, engine noises, intensity interferometry, and other optical signal processing tasks.
Keywords
Acoustic noise; Autocorrelation; Integral equations; Laser noise; Mathematics; Noise shaping; Optical interferometry; Optical pulse shaping; Shape; Signal processing;
fLanguage
English
Journal_Title
Proceedings of the IEEE
Publisher
ieee
ISSN
0018-9219
Type
jour
DOI
10.1109/PROC.1984.12946
Filename
1457214
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