Optimal emission enhancement in orthogonal double-pulse laser-induced breakdown spectroscopy

被引:20
作者
Sangines, R. [1 ,2 ]
Contreras, V. [3 ]
Sobral, H. [1 ]
Robledo-Martinez, A. [4 ]
机构
[1] Univ Nacl Autonoma Mexico CCADET UNAM, Ctr Ciencias Aplicadas & Desarrollo Tecnol, Mexico City 04510, DF, Mexico
[2] Univ Nacl Autonoma Mexico, Ctr Nanociencias & Nanotecnol, Catedra CONACyT, Ensenada 22800, BC, Mexico
[3] Tampere Univ Technol, Dept Phys, FI-33101 Tampere, Finland
[4] Univ Autonoma Metropolitana, Unidad Azcapotzalco, Mexico City 02200, DF, Mexico
关键词
LIBS; Double-pulse; Emission enhancement; PRE-ABLATION SPARK; 2ND PULSE; PLASMA; TIME; MECHANISMS; LIBS; ALUMINUM; GEOMETRY; TARGET; DELAY;
D O I
10.1016/j.sab.2015.06.012
中图分类号
O433 [光谱学];
学科分类号
0703 ; 070302 ;
摘要
Orthogonal double-pulse (DP) laser-induced breakdown spectroscopy (LIBS) was performed using reheating and pre-ablative configurations. The ablation pulse power density was varied by two orders of magnitude and the DP experiments were carried out for a wide range of interpulse delays. For both DP-LIBS schemes, the signal enhancement was evaluated with respect to the corresponding single-pulse (SP) LIBS as a function of the interpulse delay. The reheating scheme shows a sharp maximum signal enhancement of up to 200-fold for low ablative power densities (0.4 GW cm(-2)); however, for power densities larger than 10 GW cm(-2) this configuration did not improve the SP outcome. On the other hand, a more uniform signal enhancement of about 4-6 was obtained for the pre-ablative scheme nearly independently of the used ablative power density. In terms of the signal-to-noise ratio (SNR) the pre-ablative scheme shows a monotonic increment with the ablative power density. Whereas the reheating configuration reaches a maximum at 2.2 GW cm(-2), its enhancement effect collapses markedly for fluencies above 10 GW cm(-2). (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:139 / 145
页数:7
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