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Langmuir Probe Measurements of Nd-YAG Laser-Produced Copper Plasmas
17
Citations
11
References
2011
Year
EngineeringLaser-plasma InteractionLaser MaterialPlasma ScienceLaser Plasma PhysicPlasma PhysicsLangmuir Probe TheoryIon DensityLaser Plasma PhysicsPlasma TheoryLangmuir Probe MeasurementsPlasma PhotonicsInstrumentationPlasma DiagnosticsPhysicsNatural SciencesSpectroscopyLaser-induced BreakdownApplied PhysicsLaser Irradiance
The plasma was produced by focusing Nd-YAG laser pulses of 1064-nm wavelength and 10-ns duration onto a copper target. A time-resolving plane Langmuir probe was used to record the electron and ion currents during the plasma expansion in vacuum. The Langmuir probe theory was used to determine the temporal variation of the plasma potential, electron temperature, and ion density. At the time of maximum ion current, the estimated plasma potential, electron temperature, and ion density were 2.42 V, 3.28 eV, and 2.30 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">12</sup> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> , respectively. In addition, a time-of-flight signal was used to determine the ion density and velocity of the various ion components as a function of laser irradiance and probe angle w.r.t. target surface normal. For the range of laser irradiance, 4-13 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">8</sup> W/cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> , we found an ion density in the range of 6.88 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">10</sup> -2.64 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">12</sup> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> and an ion velocity in the range of 2.2-4.6 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">6</sup> cm s <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-1</sup> at the time of maximum ion current. In particular, the velocity of the fastest plume component was most affected by the irradiance. The estimated threshold irradiance for the onset of plasma was 3.95 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">8</sup> W/cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> . The experimental scaling laws for the variation of ion velocity and ion charge with the laser irradiance and probe angle were proposed.
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