Analysis of aluminum alloys by resonance-enhanced laser-induced breakdown spectroscopy: How the beam profile of the ablation laser and the energy of the dye laser affect analytical performance

Abstract In resonance-enhanced laser-induced breakdown spectroscopy, the sample was ablated by a laser pulse and the expanding plume was photoresonantly rekindled by a dye laser pulse. By sampling aluminum alloys for Mg, Pb, Si, and Cu, we showed that for the ablation step, Gaussian beams gave 2 to 3× better signal-to-noise ratio (SNR) than non-uniform beams. For the rekindling step, if no further sample destruction was allowed, dye laser pulses that intercepted the plume transversely gave 6 to 12× higher SNR than the longitudinal case. By combining Gaussian beams and transverse rekindling, the mass limit-of-detection for Mg was about 100 amol while non-resonant analysis was 10× more destructive. Sub-monolayer of oxides grown on laser-cleaned aluminum surfaces was detected by monitoring the AlO emissions of rekindled plumes; without resonant enhancements, they were not detectable no matter how destructive was the analysis. Time resolved studies showed that the Gaussian beam produced less dispersed plumes and that a stronger dye laser beam directed transversely heated up a bigger plume mass without over-heating the plume core. The analyte emissions were sustained while the continuum background remained low.

[1]  J. Laserna,et al.  Angle-Resolved Laser-Induced Breakdown Spectrometry for Depth Profiling of Coated Materials , 2000 .

[2]  Nai‐Ho Cheung,et al.  Pulsed laser‐induced damage threshold studies of thin aluminum films on quartz: Simultaneous monitoring of optical and acoustic signals , 1993 .

[3]  N. Cheung,et al.  ArF Laser-Induced Plasma Spectroscopy for Part-per-Billion Analysis of Metal Ions in Aqueous Solutions , 2002 .

[4]  F. P. Fehlner,et al.  Low-Temperature Oxidation: The Role of Vitreous Oxides , 1986 .

[5]  K. Niemax,et al.  Spatial distributions of electron density in microplasmas produced by laser ablation of solids , 1992 .

[6]  S. Lui,et al.  Resonance-enhanced laser-induced plasma spectroscopy for sensitive elemental analysis: Elucidation of enhancement mechanisms , 2002 .

[7]  Ng Cw,et al.  Detection of sodium and potassium in single human red blood cells by 193-nm laser ablative sampling: a feasibility demonstration. , 2000 .

[8]  Cheung Nh,et al.  Analysis of solids by laser ablation and resonance-enhanced laser-induced plasma spectroscopy , 2000 .

[9]  E. Yeung,et al.  High-repetition-rate laser ablation for elemental analysis in an inductively coupled plasma with acoustic wave normalization , 1991 .

[10]  J. Weiner,et al.  Fundamentals and applications , 2003 .

[11]  Israel Schechter,et al.  Laser-induced breakdown spectroscopy (LIBS) : fundamentals and applications , 2006 .

[12]  Patrick Mauchien,et al.  Evaluation of laser ablation optical emission spectrometry for microanalysis in aluminium samples , 1996 .

[13]  Reinhard Noll,et al.  Online coating thickness measurement and depth profiling of zinc coated sheet steel by laser-induced breakdown spectroscopy , 2005 .

[14]  Patrick Mauchien,et al.  Correction of Matrix Effects in Quantitative Elemental AnalysisWith Laser Ablation Optical Emission Spectrometry , 1997 .

[15]  Resonance-Enhanced Laser-Induced Plasma Spectroscopy for Multielement Analysis in Laser Ablative Sampling , 2001 .

[16]  Cheung Nh,et al.  Minimally destructive analysis of aluminum alloys by resonance-enhanced laser-induced plasma spectroscopy. , 2005 .