• 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