**Optics and Photonics Journal**

Vol.05 No.03(2015), Article ID:54857,11 pages

10.4236/opj.2015.53007

Self-Absorption Effects on Electron Temperature-Measurements Utilizing Laser Induced Breakdown Spectroscopy (LIBS)-Techniques

Shawqi A. M. Mansour

Ministry of Education and Higher Education, Accreditation and Quality Authority, Gaza, Palestine

Email: dr_shmansour@yahoo.com

Copyright © 2015 by author and Scientific Research Publishing Inc.

This work is licensed under the Creative Commons Attribution International License (CC BY).

Received 4 March 2015; accepted 19 March 2015; published 20 March 2015

ABSTRACT

In the present work, we have studied the temporal evolution of aluminum alloy plasma produced by the fundamental (1064 nm) of a Q-switched Nd:YAG laser by placing the target material in air at atmospheric pressure. The four Al I-neutral lines at 308.21, 309.27, 394.40 and 369.15 nm as well as Al II-ionic lines at 281.61, 385.64 and 466.30 nm are used for the determination of the electron temperature T_{e} using Saha-Boltzmann plot method. The neutral aluminum lines were found to suffer from optical thickness which manifested itself on the form of scattered points around the Saha-Boltzmann line. The isolated optically thin hydrogen H_{α}-line at 656.27 nm appeared in the spectra under the same experimental conditions was used to correct the Al I-lines which contained some optical thickness. The measurements were repeated at different delay times ranging from 1 to 5 µs. The comparison between the deduced electron temperatures from aluminum neutral lines before correction against the effect self-absorption to that after correction revealed a precise value in temperature. The results sure that, in case of the presence of self-absorption effect the temperature varies from (1.4067 - 1.2548 eV) as the delay time is varied from 0 to 5 µs. Whereas, in the case of repairing against the effect, it varies from (1.2826 - 0.8961 eV) for the same delay time variation.

**Keywords:**

Laser Induces Breakdown Spectroscopy (LIBS), Self-Absorption (SA), Saha-Boltzmann Plot, Delay Time (T_{d}), Electron Number Density (N_{e}), Plasma Temperature (T_{e})

1. Introduction

The laser induced breakdown spectroscopy (LIBS) is a useful technique for elemental analysis of the materials in the form of solids, liquids and gases. It has a variety of applications like material analysis, environmental monitoring, determination of soil contamination, and biomedical studies, etc. [1] -[3] . It employs a low-energy pulsed laser and a focusing lens to generate plasma on the surface of a target. The spectrum of the plasma plume is the signature of the chemical species in the sample, and its analysis yields their composition and relative abundance. It depends on several parameters, including target features (physical and chemical), ambient medium properties (plus-width), wavelength, spot size, and laser energy [4] [5] . In general, aluminum metal is the most coast-effective and widely used in various industries. It is the third most common element after oxygen and alloyed with other material, usually iron, silicon, zinc and magnesium, to create metals with different properties. Due to its importance and wide utility, aluminum has become the material of choice for a diverse range of applications and remained a subject of interest for many researchers [6] -[12] . Recently, Sun and Yu [13] proposed a simplified procedure for correcting self-absorption effect by laser-ablated aluminum target in air. El Sherbini et al. [14] utilized the diode laser atomic absorption spectroscopy (DLAAS) technique to assess the degree of optical opacity of plasmas at the wavelength of the H_{α}-line by focusing a 6 ns Nd:YAG laser pulse at 1064 nm on different solid targets material including aluminum target.

In this paper, we report the spectroscopic studies of the plasma generated at the surface of alumina (Al) by the fundamental (1064 nm) of a Q-switched Nd:YAG laser. We have studied the transitions at 256.87, 257.59, 265.32, 266.12, and 394.51 nm, and the resonance line at 396.26 nm of neutral aluminum. These transitions have been used to study the temporal behavior by estimating the plasma temperature T_{e} and the electron number density N_{e}.

2. Experimental Setup

The experimental setup is shown in Figure 1. Briefly we used a Q-Switched Nd:YAG (Quintal, model Brilliant B) pulsed laser having a pulse duration of 6ns and a 10-Hz repetition rate which capable of delivering 600 mJ at 1064 nm. An absolutely calibrated power-meter (Ophier, model 1z02165) was used in measuring the fraction of the laser light reflected from a quartz beam splitter to monitor the incident laser energy. The laser beam was focused on the target (certified aluminum based alloy with traces of Mg 1.16%) using a convex lens with a 10cm focal length. The target was mounted on a 3-D sample stage, which was rotated to avoid the non-uniform pitting of the target. The distance between the focusing lens and the sample was kept less than the focal length of the lens to prevent any breakdown of the ambient air in the front of the target. The spectra were obtained by aver- aging three data of single shot under identical experimental conditions. The radiation emitted by the plasma was

Figure 1. Schematic diagram of the experimental set up.

collected by a quarts fiber optics (25 µm diameter) positioned at a distance of 12.5 mm and normal to the direction of the laser beam. The optical fiber was connected with Echelle type spectrograph (type catalina, model SE 200) with resolving power of 2400 and equipped with a time gated ICCD Camera (1064 × 1064 pix with 13 µm × 13 µm pixel size at a binning mode of 1 × 1 (type Andor, model iStar DH 737-18F). The wavelength scale was calibrated using a low pressure Hg-lamp (type Ocean optics). The instrumental bandwidth was measured from the FWHM of the Hg lines and was found to be 0.12 ± 0.02 nm. The experimental setup was absolutely calibrated using a deuterium tungsten halogen lamp (type Ocean optics, model DH 2000 Cal.). The gain of the camera was kept at constant level of 200. The gate time was adjusted at a gate time of 2 µs while we have scanned the different delay times from 1 to 5 µs to measure the temporal variation of the plasma parameters at different delay times after the laser pulse.

3. Results and Discussions

3.1. Emission Studies

In the first set of this experimental work, we have recorded the plasma emission generated by the fundamental (1064 nm) of a Nd:YAG laser. The laser was focused by a quarts lens with a focal length of 10 cm. Aluminum plasma was recorded at different delay times ranging from 1 to 5 µs along the direction of the propagation of the plasma. Figure 2 represents the window of emission spectrum of aluminum plasma covering the spectrum region from 200 to 400 nm which consists of the neutral aluminum spectral lines that we used for the determination of the electron temperature, while the small window in the same diagram shows the whole spectrum. The ionic aluminum emission spectral lines at 281.61, 358.64, 466.30 nm and the neutral lines at 308.21, 309.27, 394.40, 396.15 nm were selected for the determination of electron number density (N_{e}) and the electron temperature (T_{e}) respectively, and are listed with related details [15] in Table 1. A couple of lines belonging to magnesium lines (Mg II, I) at 285.21, 279.54 and 280.26 nm respectively have also been detected in the emission spectra. We can observed clearly that the lines spectra are superimposed on a large continuum component. This continuum is mainly results from free-free (Bremsstrahuling process) and the free-bound transitions. This continuum should be removed before proceeding in the spectral line shape analysis.

3.2. Determination of the Electron Density

During the evaluation of laser induced plasma (LIP), excitation and ionization of the evaporated material occur. It is important to determine the thermodynamic parameters of LIP such as the electron number density and the

Figure 2. The emission spectrum of neutral aluminum plasma produced by 1064 nm wavelength of the Nd:YAG laser target whereas, the small window represents the whole spectra including the H_{α}-line at the wavelength 656.27 nm.

Table 1. Spectroscopic parameters of the spectral lines used for estimating electron temperature.

electron temperature. One of the most reliable techniques to determine the electron number density is from the measured Stark broadened line profile of an isolated line of either neutral atom or single charge ion. The electron number density (N_{e}), related to the full width at half of maximum (FWHM) of the Stark broadening lines given by the following relation [16] :

(1)

where, is the electron impact width parameter, A is the ion broadening parameter, N_{e} is the electron number density and N_{D} is the number of particles in the Debye sphere. The first term in Equation (1) refers to the broadening due to the electron contribution while, the second term is attributed to the ion broadening. Since the contribution of the ionic broadening is normally very small, therefore, it can be neglected. The electron number densities have been determined from the line profiles of the isolated aluminum neutral lines using Equation (1) by neglecting the contribution of the ion impact broadening and Doppler broadening to become in a new Equation:

(2)

where, Δλ is the Lorentzian FWHM of the line, and is the Stark broadening parameter, which can be found in [17] , N_{r} is the reference electron density which equal to 10^{16} (cm^{−3}) for neutral atoms and 10^{17} (cm^{−3}) for singly charged ions [18] [19] .

In the special case of the hydrogen H_{α}-line, the electron density can be related to the Lorentzian half width at the half of the maximum Δλ_{1/2} through the relation [20] :

(3)

where, Δλ_{s} is the intrinsic full width at half of maximum (FWHM) of the spectral line in Angstrom, and α_{1/2} is the half width of the reduced Stark profiles in Angstrom. Precise values of α_{1/2} for the Balmer series can be found in [17] . However, when the laser beam is focused on the target, the ablation of the target takes place, and due to the density gradient, the plasma rapidly expands. Figure 3 shows the results of the best fitting to the different spectral lines at an arbitrary delay times of 1, 3, 5 µs and at a fixed gate time of 2 µs. The full width half maximum (FWHM) of the spectra are used to estimate the electron number density. The temporal behavior of the electron number density in the plume is determined using Equation (2) for Al II, I lines and Equation (3) for hydrogen line at the wavelength 656.27 nm. It is evident that, the deviation of the measured electron density calculated from the aluminum resonance lines with respect to that estimated from the optically thin H_{α}-line indicates the existence of self-absorption while, the aluminum ionic lines exhibits a good agreement with H_{α}-line reminiscent of free from self-absorption as shown in Figure 4 and Figure 5 respectively.

3.3. Determination of Self-Absorption Coefficients

The process of re-absorption of the plasma to the light photons in their path to outside the plasma active volume

T_{d} = 1 µs T_{d} = 2 µs T_{d} = 3 µs

Figure 3. Represents examples of the Voigt fitting to different arbitrary spectral lines at 656.27 nm (H_{α}-line), 281.61 nm (Al II), 308.21 nm (Al I), and the Al I at 394.40 nm at three different delay times of 1, 3, 5 µs, respectively.

is called the self-absorption. It is well known that this process affecting the spectral line shape i.e. the line intensity decreases and its full width at half maximum (FWHM) increases [21] -[24] . El Sherbini et al. [25] have been developed a new method in order to quantify the effect of self-absorption to the emitted lines in terms of what is known as the coefficient of self-absorption, depending on the suggestion of Kunze [26] in the definition of the coefficient of self-absorption that given by the expression:

(4)

where, k(λ_{o})l is the optical depth of the plasma at the line center. Similarly, they suggested that the same amount (SA) can be expressed on the form of relative spectral line widths of Lorentzian components of the same line in a two different situations of self-absorbed line given by [25] :

Figure 4. Represents the temporal variation of the measured electron density using the H_{α}-line (Black solid squares) and the Al I lines at 308.21 nm, (red solid diamond), 309.27 nm, (blue solid triangles), 394.40 nm (magenta solid circle), and 396.15 nm (cyan solid pentagram).

Figure 5. Represents the temporal variation of the measured electron density using the H_{α}-line (Black solid squares) and the Al II lines at 281.61 nm, (red solid right triangle), 309.27 nm, (blue solid triangles), 394.40 nm (green solid diamond).

(5)

where, α = 0.56, Δλ_{o} is the intrinsic FWHM of the Lorentzian component of the spectral line if the line is optically thin and Δλ is the distorted Lorentizian of the same line which resulted from the effect of the self-absorp- tion. The Equation (5) can be modified to expressed in terms of the ratio of two electron density values as [25] :

(6)

where, n_{e} (line) is the electron density of the line which suffering from self-absorption effect and n_{e}(H_{α}) is the electron density of H_{α}-line free from self-absorption. Hence, we utilized Equation (6) in order to calculate the amount of absorption (SA), and then used Equation (4) to get the corrected value of the spectral line intensity I_{o}(λ_{o}). The self-absorption coefficients were calculated using Equation (6) to the four resonance aluminum lines (Al I) at 308.21, 309.27, 394.40 and 396.15 nm. Figure 6 shows algorithmic decreases in the SA values, indicating an increase of the optical depth of the lines with delay time. This means that as the plasma became cooler with the delay time (as a result of expansion) the population of the atoms in the lower state becomes higher and hence the more the absorption.

3.4. Determination of the Electron Temperature

The excitation temperature (T) of a given species is in general retrieved using the well known Boltzmann plot method [27] . Assuming the LTE is established within the plasma, the population in different levels governed by the Boltzmann distribution. The line intensity I_{ji} (of a transition from an upper level j to a lower level i) is thus related to the energy of the upper level E_{j} by the relation:

(7)

where, λ is the wavelength of the transition, A_{ji} and g_{j} are the transition probability and the statistical weight of the upper level, k and h are the Boltzmann and Plank constants, c is the velocity of the light, N and U(T) are the number density and the partition function of the considered species, respectively. This relation leads to a linear plot against E_{j} if several transitions of the same species are considered. The temperature of this species can thus be deduced from the slope of such a plot. In order to increase the accuracy of the calculation, the range of E_{j} should be as large as possible. For this reason, a more precise method consists of representing the emissions from the different ionized states of the same element in the same plot. This method, called the Saha-Boltzmann plot allows a significant extension of the range of E_{j} and therefore an increase in the accuracy of the temperature determination [28] . The validation of this method implies however that the species of different ionization degrees of a given element are in thermodynamic equilibrium with the same temperature. In this way, the Boltz- mann and Saha equations are supposed to be verified with a single temperature. We get in this case an expression similar to case of the Boltzmann plot [27] :

Figure 6. A demonstration to the variation of the coefficients of self- absorption for the Al I lines at 308.21 nm, (red solid diamond), 309.27 nm, (blue solid triangles), 394.40 nm (magenta solid circle), and 396.15 nm (cyan solid pentagram).

(8)

where the superscript z represents the type of species (z = 0 for neutral atom, z = 1 for single ionized specie, etc). This relation is similar to Equation (7) as mentioned. However for ionized species (z ≥ 1) the quantities marked with the superscript ^{*} must be replaced by the following expressions (only z = 1 is considered in our work for simplicity):

(9)

(10)

Obviously for z = 0, Equation (8) become identical to Equation (7). In Equation (9), m refers to the mass of electron. In Equation (10), E_{ion} and refer to the ionization energy and the energy of the upper ion state, respectively. We specify that for ionized species, the quantity in the right side of Equation (9) depends on the temperature T, which needs to be determined. Hence, to calculate the electron temperature and to study its temporal behavior, we have used Saha-Boltzmann plot. A correction to the aluminum resonance spectral lines were carried out according to Equation (4). Saha-Boltzmann were constructed [27] with the result as shown in Figure 7, utilizing the Al I,II lines intensities both before and after correction against self-absorption effect. We can notice the scattering of the points corresponding to the emission wavelengths of 308.21, 309.27, 394.40 and 396.15 nm before correction against self-absorption effect while, after the application of correction procedures and re- construction of Saha-Boltzmann plot, the points are tending to coincide with the line of forming a straight line with ionic lines. This figure primarily indicates the effectiveness of the correction process. However, errors are bound to present in the determination of the plasma temperature by this method especially, before correction of intensities of the absorbed lines and was around »10% uncertainty, while diminished to ~1.0% after the correction the intensities of the absorbed lines against self-absorption effect. Errors coming mainly from the transition probabilities and the measurement of the integrated intensities of the spectral lines. The variation in electron temperature (before and after the correction against self-absorption effect) as a function of delay time for the plasma produced by the 1064nm is show in Figure 8. The region near the surface of the target material constantly absorbs radiation during the time interval of the laser pulse, causing a higher temperature near the target. This higher value of the temperature is due to the absorption of the laser radiation by the electrons via the inverse bremsstrahuling absorption process. A decrease in the temperature may be attributed to the thermal energy which is rapidly converted into kinetic energy when the plasma is attaining maximum expansion velocities, causing the temperature to drop for the expanding plasma.

3.5. Validity of the Local Thermodynamic Equilibrium (LTE)

The use of the emission spectroscopy for the determination of the plasma temperature and the electron number density requires optically thin plasma spectral lines. The self-absorption depends on the oscillator strength, level energies degeneracy, broadening parameters and also on the plasma parameters. The condition that the atomic states should be populated and depopulated predominantly by electron collisions, rather than by radiation, requires an electron density which is sufficient to ensure the high collision rate. The corresponding lower limit of the electron density is given by McWhirter criterion, which is the necessary (but not sufficient condition) for attaining the minimum number density to check the validity of LTE [29] :

(11)

where, ΔE_{ji} is the largest energy transition for which the condition holds and T_{e} is the plasma temperature in electron volts [30] . At T ~12421 K, Equation (11) yields:. The electron number density in our experiment are in the order 10^{17}, which higher than required number density to satisfy the LTE condition. In this condition, the collisionally contribution dominates the radiative contribution in the plasma. The electron densities determined in our experiment within the range to satisfy the LTE condition.

Before correction against (SA) After correction against (SA)

Figure 7. Saha-Boltzmann plot for the neutral aluminum lines at 308.21 nm, (red solid diamond), 309.27 nm, (blue solid triangles), 394.40 nm (magenta solid circle), and 396.15 nm (cyan solid pentagram) as well as ionized lines (Black solid square) emitted by the laser induced plasma from the target at a delay times ranging from 1 to 5 µs (from top to bottom) respectively, and a gate time of 2 µs before and after the correction against self-absorption.

Figure 8. Variation of the electron temperature with delay time utilizing Saha-Boltzmann (black solid circle-before correction) and (red solid square-after the correction against self-absorption effect).

4. Conclusion

The LIBS method has been successfully applied as an analytical technique for the analysis of aluminum plasma using the fundamental (1064 nm) Nd:YAG laser. The optical emission spectrum of the aluminum plasma reveals transitions of neutral and singly ionized spectral lines. The effects of the self-absorption on Al lines at 308.21, 309.27, 394.40 and 396.15 nm were quantified utilizing simple formulas based on the measurement of the ratio of the apparent electron density from the lines of interest to that derived from the optically thin H_{α}-line. The spectral line intensities were then corrected. In the comparative study of the effect self-absorption, we have observed enhanced temperatures in the case of correction against self-absorption as compare to that before correction. The results show that the atomic aluminum lines (Al I) appeared in LIBS spectrum are good candidate for measuring the temperature of the plasma in LIBS experiments, especially after correction against self-absorption effect.

Acknowledgements

The author is thankful to laboratory of lasers and new materials (LINM) in Cairo University in Egypt for the encouragement in terms of provision of time and moral support to carryout research work. Beside, express his gratitude to the valuable discussions with Prof. Th. M. El Sherbini, Prof. S. H. Allam and Dr. A. M. El Sherbini.

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