1992
DOI: 10.1103/physreva.45.3987
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Experimental investigation of radiation heat waves driven by laser-induced Planck radiation

Abstract: The propagation of a radiation heat wave through a thin foil of solid gold was investigated experimentally. The wave is driven by the intense thermal radiation in 1 -3-mm-diam gold cavities heated by an intense laser pulse (duration 0.8 -0.9 ns, wavelength 0.35 pm) to temperatures ranging from 80 to 240 eV.Evidence of the propagating wave was obtained from the delayed onset of thermal emission from the outer side of the foil. A detailed comparison of the results with the self-similar solution for the ablative … Show more

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Cited by 29 publications
(9 citation statements)
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“…The resulting velocity and depth of penetration of the radiatively driven ionization wave is 1 to 2 orders of magnitude greater than that observed at low intensity. Previous measurements of radiative transport effects have been largely composed of long pulse ͑ϳ1 ns͒ studies where the effects of radiative transport have been inferred by indirect means [7] or by direct measurement of radiative transport effects in thin foils [8,9] or foams [10] driven by a separate lasercreated x-ray source. In these experiments the drive laser pulse width was comparable to or longer than the time scale for the energy transport.…”
mentioning
confidence: 99%
“…The resulting velocity and depth of penetration of the radiatively driven ionization wave is 1 to 2 orders of magnitude greater than that observed at low intensity. Previous measurements of radiative transport effects have been largely composed of long pulse ͑ϳ1 ns͒ studies where the effects of radiative transport have been inferred by indirect means [7] or by direct measurement of radiative transport effects in thin foils [8,9] or foams [10] driven by a separate lasercreated x-ray source. In these experiments the drive laser pulse width was comparable to or longer than the time scale for the energy transport.…”
mentioning
confidence: 99%
“…The thick solid line represents a trajectory for a 1 ns square laser pulse drive, which is the "" standard ÏÏ implosion discussed in this paper. The X-ray Ñux created by this laser drive has been well characterized for inertial conÐnement fusion by X-ray diode and "" witness plate ÏÏ measurements which accurately measure temporal and spectral information of the Ñux (Kau †man et al 1994 ;Sigel et al 1990aSigel et al , 1990bSigel et al , 1992. The thin solid line is a curve for a shaped 1.7 ns laser drive often used in high convergence experiments similar to those described by Landen et al (1994).…”
Section: Introductionmentioning
confidence: 93%
“…There are various diffraction elements for dispersing soft X-rays, for example, crystal (Koenig et al, 1997;Arora et al, 2000), grazing grating (Chowdhury et al, 1999), or transmission grating (Fiedorowicz et al, 1996). In contrast, transmission grating spectrographs (TGS) operating at normal incidence are convenient to use and can be coupled to detectors such as microchannel plates (MCPs) and charge-coupled-device (CCD) cameras for online monitoring (Fiedorowicz et al, 1996;Alexandrov et al, 1988;Zeng et al, 1992) and streak cameras for temporally resolved measurements (Fiedorowicz et al, 1996;Bourgade et al, 1988;Sigel et al, 1992). In contrast, transmission grating spectrographs (TGS) operating at normal incidence are convenient to use and can be coupled to detectors such as microchannel plates (MCPs) and charge-coupled-device (CCD) cameras for online monitoring (Fiedorowicz et al, 1996;Alexandrov et al, 1988;Zeng et al, 1992) and streak cameras for temporally resolved measurements (Fiedorowicz et al, 1996;Bourgade et al, 1988;Sigel et al, 1992).…”
Section: Introductionmentioning
confidence: 99%
“…Although crystal spectrographs based on Bragg reflection and flat field grating spectrographs based on Rowland circle geometry can be used to achieve high spectral resolution, these are quite cumbersome in operation and require critical alignment. As a matter of fact, TGS have been widely used in laser-plasma studies requiring a wide spectral range (0.5 nm-20 nm), and a moderate resolution (Fiedorowicz et al, 1996;Alexandrov et al, 1988;Eidmann et al, 1986;Bourgade et al, 1988;Zeng et al, 1992;Sigel et al, 1992). As a matter of fact, TGS have been widely used in laser-plasma studies requiring a wide spectral range (0.5 nm-20 nm), and a moderate resolution (Fiedorowicz et al, 1996;Alexandrov et al, 1988;Eidmann et al, 1986;Bourgade et al, 1988;Zeng et al, 1992;Sigel et al, 1992).…”
Section: Introductionmentioning
confidence: 99%