1977
DOI: 10.1146/annurev.pc.28.100177.002025
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Laser-Induced Fluorescence

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Cited by 273 publications
(75 citation statements)
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“…In this study, the MCS states are numerically solved based on the R-matrix Floquet theory (RFT) [34], and we attempt to find a complete solution, namely, a non-approximated solution, for the single electron DWSL problem within numerical round-off inaccuracy. By evaluating the excess density of state (DOS) [35][36][37][38] of DWSL, it is demonstrated that the DL band (1, 0) is really unstable in a certain region of THz intensity, as shown later. The excess DOS is an important physical quantity because it is associated with the lifetime of the concerned resonance state, and further, it provides the initial characterization for understanding a more complicated problem, for instance, the problem of the transient interband coherent dynamics of a THz-driven semiconductor DWSL.…”
Section: Introductionmentioning
confidence: 76%
“…In this study, the MCS states are numerically solved based on the R-matrix Floquet theory (RFT) [34], and we attempt to find a complete solution, namely, a non-approximated solution, for the single electron DWSL problem within numerical round-off inaccuracy. By evaluating the excess density of state (DOS) [35][36][37][38] of DWSL, it is demonstrated that the DL band (1, 0) is really unstable in a certain region of THz intensity, as shown later. The excess DOS is an important physical quantity because it is associated with the lifetime of the concerned resonance state, and further, it provides the initial characterization for understanding a more complicated problem, for instance, the problem of the transient interband coherent dynamics of a THz-driven semiconductor DWSL.…”
Section: Introductionmentioning
confidence: 76%
“…This paper reviews solid-liquid and solid-liquid-liquid refractive-index-matched systems employed in different fields, e.g., multiphase flows, turbomachinery, bio-fluid flows, with an emphasis on liquid-liquid systems. The refractive indices of various aqueous and organic phases found in the literature span the range 1.330-1.620 and 1.251-1.637, respectively, allowing the identification of appropriate combinations to match selected transparent or translucent plastics/polymers, glasses, or custom materials (i) Laser-induced fluorescence (LIF), as described by Kinsey (1977), Liu et al (1977), Walker (1987) and Crimaldi (2008), has been used to provide phenomenological insight as well as quantitative information on the distribution and other key characteristics of the fluid phases, including phase fraction, wave amplitude and frequency, bubble size distribution and frequency, etc. LIF has been utilized in RIM systems by Diez et al (2005), Ovdat and Berkowitz (2006), Liu et al (2006a, b), Ravelet et al (2007), Wu et al (2011), , , amongst others.…”
Section: Introductionmentioning
confidence: 99%
“…For the characterization of constituent materials and degradation forms Laser Induced Fluorescence (LIF) and Raman spectroscopy were used [5,6]. For the latter, a portable i-Raman spectrometer (B&W TEK Inc., USA) provided with a 785 nm excitation laser source and a CCD detector thermoelectrically cooled at 10 °C was chosen.…”
Section: Techniquesmentioning
confidence: 99%