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Light scattering measurements of the repetitive supersonic implosion of a sonoluminescing bubble
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Resolving the picosecond characteristics of synchronous sonoluminescence
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0028518611
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Effect of noble gas doping in single bubble sonoluminescence
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Comparison of multibubble and single-bubble sonoluminescence spectra
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Direct observations of single sonoluminescence pulses
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Moran, M.J.1
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Hydrodynamic simulations of bubble collapse and picosecond sonoluminescence
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Moss, W.C.1
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Bubble Dynamics and Interface Phenomena
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edited by J. R. Blake, J. M. Boulton-Stone, and N. H. Thomas Kluwer, Boston
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T. Lepoint, N. Voglet, L. Faille, and F. Mullie, "Bubble Dynamics and Interface Phenomena," in Proceedings of an IUTAM Symposium, edited by J. R. Blake, J. M. Boulton-Stone, and N. H. Thomas (Kluwer, Boston, 1993), pp. 321-333; F. Mullie and D. De Pauw and T. Lepoint, "Nature of the 'extreme conditions' in single sonoluminescing bubbles," submitted to J. Phys. Chem.
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Nature of the 'extreme conditions' in single sonoluminescing bubbles
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J. Phys. Chem.
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A theoretical study of sonoluminescence
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Some comments on mechanisms of sonoluminescence
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Vaughan, P.W.1
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Study of the mechanism of sonoluminescence. II. Form of the light pulse in sonoluminescence
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Timing of sonoluminescence flash
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27
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33744701713
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5 for an applied voltage of -800 Vdc
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5 for an applied voltage of -800 Vdc.
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28
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33744648479
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The analog bandwidth refers to the input amplifiers of the scope, and is the limiting factor in the speed of this 9362. The sampling rate of 10 GHz refers to the digitizing rate only
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The analog bandwidth refers to the input amplifiers of the scope, and is the limiting factor in the speed of this 9362. The sampling rate of 10 GHz refers to the digitizing rate only.
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29
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0037802264
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-
McGraw-Hill, New York
-
cτ= 0.35. See, e.g., A. P. Malvino, Electronic Principles (McGraw-Hill, New York, 1984), pp. 426-428.
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Electronic Principles
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Malvino, A.P.1
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30
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33744598598
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The relationship between the FWHM and rise-time of a Gaussian signal can easily be determined by applying the equation for a Gaussian to the FWHM and rise-time, respectively. The common parameter of the Gaussian width can then be used to relate the FWHM and rise-time
-
The relationship between the FWHM and rise-time of a Gaussian signal can easily be determined by applying the equation for a Gaussian to the FWHM and rise-time, respectively. The common parameter of the Gaussian width can then be used to relate the FWHM and rise-time.
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