HEARING OVERCOMES UNCERTAINTY RELATION AND MEASURES DURATION OF ULTRASHORT PULSES

The acoustic pressure of such a signal is p(t) = p sub(0)exp(-t super(2)/2( Delta t) super( 2))cos(2[pi] [functionof] sub(1)t), where [functionof] sub(1) is the underlying frequency. The spectrum of the signal is also Gaussian, p([functionof]) = p sub(0)exp(-([functionof]-[functionof] sub(1)) super(...

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Veröffentlicht in:Europhysics news 2015-01, Vol.46 (1), p.27-31
Hauptverfasser: Majka, Marcin, Sobieszczyk, Pawel, Gebarowski, Robert, Zielinski, Piotr
Format: Artikel
Sprache:eng
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Zusammenfassung:The acoustic pressure of such a signal is p(t) = p sub(0)exp(-t super(2)/2( Delta t) super( 2))cos(2[pi] [functionof] sub(1)t), where [functionof] sub(1) is the underlying frequency. The spectrum of the signal is also Gaussian, p([functionof]) = p sub(0)exp(-([functionof]-[functionof] sub(1)) super(2)/2( Delta [ function of]) super(2)) and the widths of the two Gaussian functions are inversely proportional to one another.
ISSN:0531-7479
1432-1092
DOI:10.1051/epn/2015105