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 |
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Hauptverfasser: | , , , |
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. |
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ISSN: | 0531-7479 1432-1092 |
DOI: | 10.1051/epn/2015105 |