2009
DOI: 10.1109/tap.2009.2025674
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Propagation of Large Bandwidth Microwave Signals in Water

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Cited by 30 publications
(23 citation statements)
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“…(37) combined with Eq. (30) in the four cases considered in this paragraph. The optical thickness α c ℓ = 7 has been chosen in order that the main signal is dominated by the precursor but remains visible.…”
Section: Response To Sine-waves With Linearly Varying Amplitudementioning
confidence: 92%
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“…(37) combined with Eq. (30) in the four cases considered in this paragraph. The optical thickness α c ℓ = 7 has been chosen in order that the main signal is dominated by the precursor but remains visible.…”
Section: Response To Sine-waves With Linearly Varying Amplitudementioning
confidence: 92%
“…Propagation of waves in Debye media has been extensively studied in the past, with particular attention paid to the important case of water in the radio-frequency and microwave domains. For papers related to the present study, see, e.g., Refs [10,[22][23][24][25][26][27][28][29][30][31][32][33][34]. Albanese et al were the first to refer to the Brillouin precursors in Debye media [22].…”
Section: Introductionmentioning
confidence: 99%
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“…It has been demonstrated that the propagation of any kind of signal through any dispersive media can arise out the formation of signals named as Brillouin precursors [1][2][3][4][5]. This phenomenon depends on the dielectric properties of the underlying medium as well as on other parameters or settings; we can mention the input signal type and its configuration, the involved transmitted and/or received bandwidth, among the main of those parameters which additionally determine the formation of the Brillouin precursor [1,2,[6][7][8].…”
Section: Introductionmentioning
confidence: 99%
“…Of particular importance here is the fact that the peak amplitude point of the Brillouin precursor experiences zero exponential decay with propagation distance z Ͼ 0, decreasing algebraically as z −1/2 in the dispersive absorptive medium, with the peak values of both the energy density and Poynting vector then only decreasing algebraically as z −1 , thereby transmitting electromagnetic energy deeper into the dispersive attenuative dielectric [8,14] than that described by the Beer-Lambert-Bouger law [15]. This rather unique feature renders the Brillouin precursor as a powerful tool for imaging through a given obscuring dispersive material [8,16], a result that has been verified experimentally for large bandwidth microwave signals [17].…”
Section: Introductionmentioning
confidence: 99%