1987
DOI: 10.1088/0022-3727/20/2/010
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Temporally resolved target potential measurements in laser-target interactions

Abstract: Rapid (100 ps) voltage oscillations have been observed in a capacitively coupled target irradiated with 3.5 ns pulses of Nd-YAG light at irradiances of between 5*1012 and 2*1015 W cm-2 on a 40 mu m spot. The measurements were made using a fast (40 ps rise-time) Pockels cell intercepting a diagnostic light pulse to a streak camera. The oscillations were found to depend on the spot size and the shape of the laser pulse. The oscillation frequencies found (up to 12 GHz) were too low to correspond to plasma instabi… Show more

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Cited by 17 publications
(8 citation statements)
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“…The ratio of the total positive target charge to the charge carried by positive ions observed with the FC is of the order of 10 −3 . In contrast with the experiments with nanoseconds to sub-picoseconds lasers (Benjamin et al, 1979;Borowitz et al, 1987), where the time of target charging was comparable with the laser pulse width, in our experiment the positive charge was balanced by a target current during a time period longer by a factor ∼100 in comparison with the laser pulse length. Moreover, a new phenomenon arising after t zero = 2.8 μs indicates that the target is being negatively charged.…”
Section: Resultscontrasting
confidence: 93%
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“…The ratio of the total positive target charge to the charge carried by positive ions observed with the FC is of the order of 10 −3 . In contrast with the experiments with nanoseconds to sub-picoseconds lasers (Benjamin et al, 1979;Borowitz et al, 1987), where the time of target charging was comparable with the laser pulse width, in our experiment the positive charge was balanced by a target current during a time period longer by a factor ∼100 in comparison with the laser pulse length. Moreover, a new phenomenon arising after t zero = 2.8 μs indicates that the target is being negatively charged.…”
Section: Resultscontrasting
confidence: 93%
“…The inset shows the corresponding time-resolved FC currents which were transformed to the ion fronts. multi-peak target current occurs (Ludmirsky et al, 1985;Borowitz et al, 1987). Thus, from Figure 3 we can deduce that each double layer reaches a maximum in the charge density ρ(x,t) = e(Zn i − n e ) at the ion front located at a critical distance, x cr from the target, where Z is the ion charge number, n i is the ion density, and n e is the electron density.…”
Section: Resultsmentioning
confidence: 93%
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“…In Figure 2b, we have represented the particle current evolution in time for various scale resolutions. We noticed that the particles present an oscillatory dynamic, as was previously reported by [23] and experimentally proven in [24] and [25]. The frequency changes with the scale resolution, thus we deduce that each component of the plasma might present a different oscillatory behavior dictated by the characteristics of the double layer formed in the area separating the structures.…”
Section: Plasma Modellingsupporting
confidence: 81%
“…Target current (TC) is a relatively unexplored phenomenum in the field of laser-matter interaction. The initial studies started in the late seventies [2,3] and continued in a patchy fashion across the following decades [4,5] until recently.…”
Section: Introductionmentioning
confidence: 99%