| |
Title of Thesis
PLASMA DIAGNOSTICS OF Zn, Cd, AND Hg USING LASER-INDUCED BREAKDOWN SPECTROSCOPY |
Author(s)
Nek Muhammad Shaikh |
Institute/University/Department Details
Department of Physics/ Quaid-i-Azam University Islamabad |
Session
2006 |
Subject
Physics |
Number of Pages
109 |
Keywords (Extracted from title, table of contents and abstract of thesis)
plasma diagnostics, laser-induced breakdown spectroscopy, cadmium plasma, laser ablation, laser induced zinc plasma |
Abstract Laser-induced breakdown spectroscopy (LIBS) is a technique that can provide qualitative and quantitative measurement of metals in various environments. In the present work, we have studied the spatial and temporal evolution of the plasma parameters of the zinc (Zn), cadmium (Cd) and mercury (Hg) plasma, produced by the fundamental (1064 nm), second (532 nm) and third(355 nm) harmonics of a Q-switched pulsed Nd:Y AG laser. The experimentally observed line profiles of several atomic and ionic species have been used to extract the excitation temperature and electron number density. The excitation temperature is estimated from the intensity ratio method and from the Boltzmann plot method. The electron temperature of the zinc plasma has determined using the transitions 4s4d 3D3→ 4s4p 3P2 at 334.5 nm and 4s5s 3S1→ 4s4p 3P2 at 481.0 nm of neutral zinc. In the case of cadmium plasma, eight transition lines 228.80 nm (5p 1P1 → 5s2 1S0), 283.74 nm (6d 3D1→ 5p 3p0), 298.06 nm (6d 3D3→5p 3P2), 346.78 nm (5d 3D2 → 5p 3p1), 361.05 nm (5d 3D3 →5p 3P2), 467.81 nm (6s 3S1 → 5p 3p0), 479.99 nm (6s 3S1 → 5p 3p1), and 508.58 nm (6s 3S1 → 5p 3P2) of neutral cadmium have used in the Boltzmann plot method. The ion temperature is estimated from the relative intensity ratio method of the ionic and atomic transitions using the Saha equation. In the case of mercury plasma, six transition lines at, 296.72 nm (6s6d 3D1→ 6s6p 3p0), 365.01 nm (6s6p 3D3 → 6s6p 3P2), 404.66 nm (6s7s 3S1 → 6s6p 3p0), 435.83 nm (6s7s 3S1 → 6s6p 3Pl), 576.96 nm (6s6d 3D2 → 6s6p 1p1) and 579.07 nm (6s6d 1D2 →6s6p 1pl) have been used for the determination of the excitation temperature. Stark broadened profiles of the neutral and singly ionized species have been utilized for the electron number density measurements. The electron number density of the Zn, Cd and Hg plasma has been deduced from the Zn (I) line at 334.5 nm, Cd (II) line at 226.50 nm and Hg (II) line at 398.39 run respectively. The experiments have been performed in air at atmospheric pressure as well as in the presence of different ambient gases (Ar, Ne and He) to investigate the effect ambient gas environments on the emission intensity of the atomic and ionic transition lines and on the plasma parameters. Besides, we present experimental relative transition probabilities of the Zn (4s5s 3S1 →4s4p 3p0,1,2) and Cd (5s6s 3S1 → 5s5p 3p0,1,2) triplets and compare our data with that listed in the NIST data base. In addition we have studied the variation of the excitation temperature and electron number density as a function of laser irradiance at atmospheric pressure and estimated the inverse bremstrahlung (IB) absorption and photo ionization (PI) absorption coefficients. The validity of the assumption of local thermodynamic equilibrium is discussed in the light of the results obtained.
|
 |
 |
 |
 |
 |
| S. No. |
Chapter |
Title of the Chapters |
Page |
Size (KB) |
 |
 |
 |
 |
 |
| 1 |
0 |
Contents |
|
 281.05 KB |
 |
 |
 |
 |
 |
| 2 |
1 |
Introduction |
11 |
 633.52 KB |
| |
1.1 |
Laser Induced Breakdown Spectroscopy (LIBS ) |
11 |
| |
1.2 |
Advantages And Disadvantages Of LIBS |
12 |
| |
1.3 |
LIBS Plasma Precipitation Mechanism |
13 |
| |
1.4 |
Effect Of Physical Variables LIBS |
17 |
| |
1.5 |
Laser Absorption In The Plasma |
21 |
| |
1.6 |
Line Broadening Mechanism LIBS |
23 |
| |
1.7 |
Determination Of Electron Number Density From Stark Broadening Of Spectral Lines |
27 |
| |
1.8 |
Determination Of Excitation / Electron Temperature |
28 |
| |
1.9 |
Local Thermodynamic Equilibrium |
30 |
| |
1.10 |
Self Absorption |
31 |
| |
1.11 |
Zinc |
31 |
| |
1.12 |
Cadmium |
32 |
| |
1.13 |
Mercury |
33 |
 |
 |
 |
 |
 |
| 3 |
2 |
Experimental Setup |
35 |
 192.25 KB |
| |
2.1 |
N d : Yag Laser |
37 |
| |
2.2 |
LIBS 2000+Spectrometer |
38 |
| |
2.3 |
Hr2000 High Resolution Spectrometer |
39 |
| |
2.4 |
Optics Fiber |
40 |
| |
2.5 |
Measurements Of Error In The Electron Number Density And The Excitation Temperature |
41 |
 |
 |
 |
 |
 |
| 4 |
3 |
Measurement Of Electron Density And Temperature Of The Laser Induced Zinc Plasma |
42 |
 584.07 KB |
| |
3.1 |
Summary Of The Work |
42 |
| |
3.2 |
Historical Background |
42 |
| |
3.3 |
Results And Discussion |
43 |
 |
 |
 |
 |
 |
| 5 |
4 |
Diagnostics Of Cadmium Plasma Produced By Laser Ablation |
66 |
 523.14 KB |
| |
4.1 |
Summary Of The Work |
66 |
| |
4.2 |
Historical Background |
66 |
| |
4.3 |
Results And Discussion |
67 |
 |
 |
 |
 |
 |
| 6 |
5 |
Optical Emission Studies Of The Mercury Plasma Generated By The Fundamental Second And Third Harmonics Of The N d Yag Lasers |
87 |
 405.23 KB |
| |
5.1 |
Summary Of The Work |
87 |
| |
5.2 |
Historical Background |
87 |
| |
5.3 |
Results And Discussion |
89 |
 |
 |
 |
 |
 |
| 7 |
6 |
Conclusions |
103 |
 208.86 KB |
| |
6.2 |
Future Plan : |
105 |
| |
6.3 |
References |
106 |
 |
 |
 |
 |
 |