Velocity distribution function of electrons plasma produced by high power laser pulse interacting aluminum target

This paper presents the experimental results of studying the distribution function of electrons plasma produced by irradiating aluminum target by nanosecond pulsed laser in vacuum. The laser beam was provided by second harmonic of a Q-switched Nd:YAG pulsed laser with ~10 nsec pulse duration and energy of 70 mJ. A home made Faraday cup was used for detecting the current signal. From analyzing the time of flight (TOF) experimental distribution function was determined. Comparing the experimental distribution function with Maxwell-Boltzamnn and effusion distribution functions, the electron temperature was estimated. From the experimental results, the velocity of maximum electron flux was determined. In this study the influence of the probe position and biasing voltage was investigated. The results show that the velocity of maximum electron flux and associated temperature rises with distance from the target surface. The results also show that effusion distribution function is more appropriate for modeling such plasma.

[1]  A. Voevodin,et al.  In situ time of flight laser induced florescence spectroscopy of carbon by pulsed laser deposition , 1998 .

[2]  R. Short,et al.  Using an afterglow plasma to modify polystyrene surfaces in pulsed radio frequency (RF) argon discharges , 2003 .

[3]  C. Lewis,et al.  The Langmuir probe as a diagnostic of the electron component within low temperature laser ablated plasma plumes , 1999 .

[4]  Michael N. R. Ashfold,et al.  Investigations of the plume accompanying pulsed ultraviolet laser ablation of graphite in vacuum , 2001 .

[5]  P. Dyer Electrical characterization of plasma generation in KrF laser Cu ablation , 1989 .

[6]  S. Amoruso,et al.  Characterization of laser-ablation plasmas , 1999 .

[7]  Laser-induced decomposition and ablation dynamics studied by nanosecond interferometry. 4. A polyimide film , 2002 .

[8]  F. Belloni,et al.  Characterization of a nonequilibrium XeCl laser-plasma by a movable Faraday cup , 2004 .

[9]  V. P. N. Nampoori,et al.  Electron density and temperature measurements in a laser produced carbon plasma , 1997 .

[10]  R. Dreyfus Cu0, Cu+, and Cu2 from excimer‐ablated copper , 1991 .

[11]  John G. Jones,et al.  Characterization of ZrO2/Y2O3 laser ablation plasma in vacuum, oxygen, and argon environments , 2000 .

[12]  Hansen,et al.  Angular distribution of electron temperature and density in a laser-ablation plume , 2000, Physical review letters.

[13]  A. C. Gaeris,et al.  Internal structure and expansion dynamics of laser ablation plumes into ambient gases , 2003 .

[14]  Hammel,et al.  Accuracy of K-shell spectra modeling in high-density plasmas , 2000, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[15]  T. N. Hansen,et al.  Angular distributions of silver ions and neutrals emitted in vacuum by laser ablation , 1997 .