Dzierzega Krzysztof, Zawadzki Witold, Pokrzywka Bartłomiej, Pellerin Stephane
Instytut Fizyki im. M. Smoluchowskiego, Uniwersytet Jagielloński, ulica Reymonta 4, 30-059 Kraków, Poland.
Phys Rev E Stat Nonlin Soft Matter Phys. 2006 Aug;74(2 Pt 2):026404. doi: 10.1103/PhysRevE.74.026404. Epub 2006 Aug 25.
Time and space resolved measurements of Thomson scattering of 532 nm , 6 ns laser pulses were performed on argon thermal discharge plasma with electron temperature T(e)>10,000 K and electron density 8 x 10(22) m(-3)< n(e)<2 x 10(23) m(-3). From these measurements, variations of the electron density and temperature across the laser beam and their evolution during the laser pulse were determined. While the electron density is augmented by no more than a few percent the electron temperature is significantly increased along the axis of the laser beam due to laser heating. It is also shown that the higher initial electron density, the more disturbed is the plasma. The initial "undisturbed" electron density was derived by studying the spatial variations of n(e) within the laser beam. On the other hand, the initial electron temperature was determined by studying the temporal evolution of T(e) during the laser pulse and then by extrapolating the results to the origin of the pulse. Despite strong and nonlinear plasma heating by the Thomson scattered laser light, our study yields temperatures close to those obtained by modeling and time-resolved spectroscopic measurements.
在电子温度(T(e)>10000K)且电子密度(8×10^{22}m^{-3}<n(e)<2×10^{23}m^{-3})的氩热放电等离子体上,对532nm、6ns激光脉冲的汤姆逊散射进行了时间和空间分辨测量。通过这些测量,确定了激光束方向上电子密度和温度的变化及其在激光脉冲期间的演变。虽然电子密度增加不超过百分之几,但由于激光加热,电子温度沿激光束轴显著升高。研究还表明,初始电子密度越高,等离子体受干扰越大。通过研究激光束内(n(e))的空间变化得出初始“未受干扰”的电子密度。另一方面,通过研究激光脉冲期间(T(e))的时间演变,然后将结果外推到脉冲起始时刻来确定初始电子温度。尽管汤姆逊散射激光对等离子体有强烈的非线性加热作用,但我们的研究得到的温度与通过建模和时间分辨光谱测量得到的温度相近。