2001
DOI: 10.1063/1.1342031
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Langmuir probe measurement of plasma splitting during pulsed laser deposition

Abstract: The properties of plasma formed during pulsed laser deposition from a Bi–Sr–Ca–Cu–O target were measured using a Langmuir probe in the electron accelerating region “Plasma splitting” was observed at pressures in the range of 1–5 Pa and distances of the probe from the target of 3–14 mm.

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Cited by 10 publications
(5 citation statements)
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“…The following differences were noted at 10 −2 mbar: (i) the current profile is delayed in time, (ii) the area under the current profile is higher and (iii) the number of multiple peaks was reduced. The ion current profile at 10 −2 mbar had a two-peak structure, which is in agreement with results obtained from LP measurements [24] and spectroscopic studies [6,7,25]. In the presence of background gas, the increase in time delay was due to the drag force whereas the enhancement in intensity was due to confinement of the plume.…”
Section: Measurement Of Electron Temperature and Density At Higher Ba...supporting
confidence: 88%
“…The following differences were noted at 10 −2 mbar: (i) the current profile is delayed in time, (ii) the area under the current profile is higher and (iii) the number of multiple peaks was reduced. The ion current profile at 10 −2 mbar had a two-peak structure, which is in agreement with results obtained from LP measurements [24] and spectroscopic studies [6,7,25]. In the presence of background gas, the increase in time delay was due to the drag force whereas the enhancement in intensity was due to confinement of the plume.…”
Section: Measurement Of Electron Temperature and Density At Higher Ba...supporting
confidence: 88%
“…These processes can be enhanced either by reducing the characteristic carbon ion energy or by increasing the background pressure, which results in a shorter mean free path for collisions involving buffer gas atoms, and also in a reduction of the characteristic ion energy by collisions. The observation of two characteristic C 2 -rich plasma fronts can be explained by the fact that at near vacuum or low pressure, two carbon ion plasma fronts are observed, as seen in figure 7, and reported previously [23,24]. The polar dependence of the C 2 emission observed in the second front, at later times in figure 7, might be related to the known polar distribution observed in the plasma ion energy spectrum, which exhibits a decrease in energy, as the polar angle with respect to the target normal increases [25].…”
Section: Discussionsupporting
confidence: 76%
“…Wild et. al has also observed this type of plasma splitting during PLD [14].On increasing distance from 40 mm to 60 mm, the second peak in electron TOF signal (slow) again splits in two parts, as indicated in figure 3(a). Thus a triple peak structure is observed at a distance of 50 mm.…”
Section: Electron and Ion Time-of-flight (Tof) Signalsmentioning
confidence: 55%