1990
DOI: 10.1017/s0263034600008077
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Plasma evolution in laser-irradiated hollow microcylinders

Abstract: Hollow microcylinder targets, 200–300 μm in diameter, have been internally irradiated at up to 5 · 1014 W/cm2 with Nd:glass laser pulses directed through an axial entrance slit. The plasma evolution in the interior of the cavities was diagnosed with a pinhole imaging X-ray streak camera and a Nomarski-type interferometer. Plasma collision near the center of the cylinder is observed about 300 ps after the irradiating laser pulse. The experimental results are confirmed by a one-dimensional Eulerian fluid code.

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Cited by 17 publications
(8 citation statements)
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“…This scheme has also been found useful in increasing the gain of the lasing medium of X-ray laser (Suckewer & Fishman 1980;Suckewer et al 1985) when operated in recombination regime as a result of increase in particle confinement, because in this case particle confinement time remains much larger than the electron temperature decay time and the plasma is cooled through the radiation losses. Enhancement in UV and visible emission from beryllium plasma in the presence of magnetic field have also been reported (Begimaculov et al 1992). An enhancement of ~ 100 in stimulated emission (along magnetic field) over spontaneous emission (perpendicular to magnetic field) of C vi 182 A line has been measured in the presence of 90 kG magnetic field.…”
Section: Introductionmentioning
confidence: 75%
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“…This scheme has also been found useful in increasing the gain of the lasing medium of X-ray laser (Suckewer & Fishman 1980;Suckewer et al 1985) when operated in recombination regime as a result of increase in particle confinement, because in this case particle confinement time remains much larger than the electron temperature decay time and the plasma is cooled through the radiation losses. Enhancement in UV and visible emission from beryllium plasma in the presence of magnetic field have also been reported (Begimaculov et al 1992). An enhancement of ~ 100 in stimulated emission (along magnetic field) over spontaneous emission (perpendicular to magnetic field) of C vi 182 A line has been measured in the presence of 90 kG magnetic field.…”
Section: Introductionmentioning
confidence: 75%
“…It was observed that the X-ray signals from copper plasma were enhanced 2-3 times when the magnetic field was increased from 0.1 to 0.6 T. However no change was observed in X-ray intensity in the absence or presence of 0.01 T magnetic field. Generally the value of a has been reported to be ranging from 1.5 to 2.5 in the absence of magnetic field (Bleach & Nagel 1978;Rai et al 1995b). In this case X-ray detector with zapon filter was sensitive for soft as well as hard X-ray energy.…”
Section: Study Of X-ray Emissionmentioning
confidence: 99%
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“…The collision and subsequent interaction of dense plasmas created by intense laser irradiation of cylindrical cavities are of interest for fundamental and practical reasons [1][2][3]. We have recently reported the study of semi-cylindrical cavity plasmas using soft X-ray laser interferometry and hydrodynamic simulations [4].…”
Section: Introductionmentioning
confidence: 99%