Journal of Spectroscopy

Journal of Spectroscopy / 2013 / Article

Research Article | Open Access

Volume 2013 |Article ID 198420 |

S. Nomura, T. Kaneko, G. Ito, K. Komurasaki, Y. Arakawa, "Diode-Laser Induced Fluorescence Spectroscopy of an Optically Thick Plasma in Combination with Laser Absorption Spectroscopy", Journal of Spectroscopy, vol. 2013, Article ID 198420, 5 pages, 2013.

Diode-Laser Induced Fluorescence Spectroscopy of an Optically Thick Plasma in Combination with Laser Absorption Spectroscopy

Academic Editor: Lorenzo Giuffrida
Received13 Nov 2012
Revised11 Jan 2013
Accepted21 Jan 2013
Published21 Feb 2013


Distortion of laser-induced fluorescence profiles attributable to optical absorption and saturation broadening was corrected in combination with laser absorption spectroscopy in argon plasma flow. At high probe-laser intensity, saturated absorption profiles were measured to correct probe-laser absorption. At low laser intensity, nonsaturated absorption profiles were measured to correct fluorescence reabsorption. Saturation broadening at the measurement point was corrected using a ratio of saturated to non-saturated broadening. Observed LIF broadening and corresponding translational temperature without correction were, respectively,  GHz and  K and corrected broadening and temperature were, respectively,  GHz and  K. Although this correction is applicable only at the center of symmetry, the deduced temperature agreed well with that obtained by LAS with Abel inversion.

1. Introduction

Diode laser-induced fluorescence (DLIF) has a feature of high wavelength resolution on the order of picometers, which makes it useful to obtain translational temperature by measuring Doppler broadening of an atomic line of gases [1, 2] to the same degree as diode laser absorption spectroscopy (DLAS) [3, 4]. The advantage of DLIF over DLAS, which is a line-of-sight measurement, is the possibility of point measurements. However, in optically thick plasma, absorption of the excitation laser and reabsorption (or self-absorption) of fluorescence can broaden the fluorescence profile. The temperature deduced from observed fluorescence tends to be overestimated. Hertz-corrected DLIF profiles in flame consider the laser absorption effect by solving a nonsymmetric 1D distribution of the depleting laser using an iterative procedure [5], although fluorescence reabsorption was not corrected.

Although intense lasers with substantial fluorescence that can achieve a high signal-to-noise ratio are preferred, intense lasers are known to cause additional broadening, termed as saturation broadening or power broadening [6]. Moreover, their saturation regime is usually avoided. Instead, the linear region is used in LIF temperature measurements [7]. In contrast, in low-pressure plasma, the saturation intensity is low and the fluorescence profile is easily saturated. The saturation effect in LIF was investigated in earlier studies [810], in which the laser spectral width was comparable to Doppler broadening, and in which the spectral wing of laser was able to induce substantial fluorescence, causing additional broadening. In DLIF, however, the laser spectral width is about 1 MHz and three others of magnitude narrower than the absorption profile broadening. The mechanism of broadening differs, but with identical broadening to that of LAS [1113].

Correction methods for optical absorption and saturation broadening are demonstrated in an arc-heated argon plasma wind tunnel [14]. The wavelengths of both fluorescence and excitation are 772.42 nm (Ar I, 4s2[1/2]°−4p2[1/2]). The measured point is on the axis of the axisymmetric flow and the measured temperature is compared with the result of LAS with Abel inversion.

2. Theoretical

2.1. Absorption of the Exciting Laser

Taking laser absorption into consideration, the fluorescence is written as [5] where , , , and , respectively, denote the fluorescence intensity without reabsorption, experimental factor, incident spectral laser irradiance, and saturated absorption coefficient. The coordinate system is presented in Figure 1. The -axis is the laser pass and the center of the flow is the origin point. is the saturated absorption coefficient at . It is noteworthy that the laser absorption is saturated because of its high irradiance. In the axisymmetric plasma, absorbance from the incident edge to the center is half of that from the incident edge to the edge, as where is the laser frequency. The factor of 1/2 in (2) is valid only for the axisymmetric plasma. In accordance with the Beer-Lambert law, integration of the right term in (2) is where , respectively, denote the transmitted spectral laser irradiance. Consequently the laser absorption can be corrected by monitoring the transmitted spectral laser irradiance.

2.2. Reabsorption of the Fluorescence

The fluorescence intensity is much lower than the saturation intensity, and the absorption of fluorescence is not saturated. Consequently correction for the reabsorption must be done with the nonsaturated absorption, which is measured at low intensity. The measured fluorescence is expressed as where and , respectively, denote the measured fluorescence and nonsaturated absorption coefficient. In the same manner as the correction for the absorption of laser, the absorption can be evaluated: Although fluorescence may diffuse before it reaches the detector, this effect does not alter the profile shape because the diffusion is not a function of laser frequency in this spectral range. Thus diffusion is not considered here.

2.3. Saturation Effect

When intense laser illumination is used for excitation, the optical pumping rate exceeds the relaxation rate and the number density of the lower state atoms is depleted. The saturated integrated absorption coefficient is where , , and , respectively signify the saturated, nonsaturated integrated absorption coefficient, and saturation intensity. is integration over the frequency and has a unit of GHz/mm. A series of is obtained using LAS by varying the laser power. By fitting the measured with (6), and are obtainable. According to an earlier report [11], the true Doppler broadening is obtainable when the saturation parameter, (=), is less than 0.1. With a ratio of saturated broadening to the true Doppler broadening, the saturation effect is corrected.

3. Experimental

Figure 2 shows the experimental setup. An external cavity diode laser (Velocity Model 6300; New Focus Inc.), with linewidth of about 300 kHz, was used as the light source. The laser wavelength was swept at the repetitive frequency of 0.5 Hz with sweeping width of 20 GHz. The relative laser wavelength was monitored using an etalon with free spectral range of 0.75 GHz. The laser was modulated using an acoustooptic modulator (1205C; Isomet Corp.). The laser power at the output of the fiber was 1.0 mW and the laser spatial width at the measurement point was 0.4 mm, at which the intensity decreases to of the peak. During saturation measurements, the laser power was attenuated with neutral density filters. The fluorescence was collected with lenses and detected with a photomultiplier tube (H8249; Hamamatsu Photonics K.K.). A band-pass filter was mounted in front of the detector and the fluorescence signal was measured by phase sensitive detection using a lock-in amplifier (SR830; Stanford Research Systems Inc.). The plasma emission is negligibly small in comparison to the fluorescence signal. The output from the lock-in amplifier was recorded with an oscilloscope (DSOX2004A; Agilent Technologies Inc.).

The argon plasma flow was generated with an arc-heated plasma generator and expanded with a nozzle. The throat diameter was 2 mm. The nozzle exit was 30 mm. The input power was 1.2 kW with current of 50 A. The volume flow rate of argon was 4 slm. The chamber pressure was 20 Pa.

4. Results and Discussion

Saturated LAS was conducted with varying laser power from 1 μW to 0.97 mW. Figure 3 shows the saturated integrated absorption coefficient with the fitting curve. The saturation intensity was estimated at μW. The nonsaturated absorbance was at the peak and the nonsaturated broadening was  GHz. The broadening was evaluated by using full width at half maximum (FWHM). The most saturated absorption profile was obtained with laser power of 0.97 mW. At this power the saturated absorbance is at the peak; saturated broadening was  GHz. Consequently, the ratio of saturated broadening to true broadening was .

The LIF profile was obtained with maximum laser power of 0.97 mW. Broadening of the observed fluorescence was  GHz. The broadening effect by optical absorption was corrected using (1) and (4). Figure 4 shows the measured fluorescence profile and the corrected profiles. After correction for optical reabsorption, the broadening was deduced as  GHz. As described above, the ratio of saturated broadening to the true broadening is . Consequently, Doppler broadening and translational temperature were, respectively, deduced as  GHz and  K. Broadening and temperature of distorted and true profiles are shown in Table 1.

FWHM, GHzTemperature, KRatio of estimated temperature to true temperature

Profile distorted by reabsorption2.0421501.08
Profile distorted by absorption1.9820301.02
Profile distorted by saturation2.1123101.16

Observed profile2.2025101.26
True profile1.9619901

Figure 5 presents the ratio of estimated temperature to true temperature as a function of . The contribution of three effects to the distortion is shown there. The peak absorbance was 0.4, which corresponds to the optical thickness-to-plasma diameter ratio of 0.007 mm−1. The reabsorption of fluorescence was not saturated. It was independent of the spectral laser irradiance. As the spectral laser irradiance increased, the absorption of the laser became saturated and the distortion effect became minor. In the region where is higher than unity, saturation broadening is the most dominant among distortion effects. The three effects are independent of each other, and the true temperature is obtainable by dividing the measured temperature by the ratio in Figure 5. Thus, the error propagates linearly.

For the validation of this correction method, the temperature distribution was obtained using LAS with Abel inversion, as shown in Figure 6. The laser power was attenuated to 2.5 μW to avoid saturation. At the center, the temperature was estimated at  K. The present result shows good agreement with that obtained by LAS as shown in Table 2.

LIF1990 ± 150 K
LAS2050 ± 20 K

5. Conclusion

The distorted LIF profile attributable to optical absorption and saturation was corrected using LAS. For laser absorption and fluorescence reabsorption correction, saturated and nonsaturated line-of-sight absorbance was measured using the LAS setup. Saturation broadening was corrected with the ratio of saturated broadening to the nonsaturated broadening in LAS. The results obtained for arc-heated argon plasma show that the Doppler broadening was corrected as  GHz, and the translational temperature was  K. Instead, broadening without correction was  GHz, which corresponds to  K. This value showed good agreement with the result of LAS, which was spatially resolved with Abel inversion. The contribution of the three effects to distorted LIF profile was estimated theoretically as a function of , showing that in the region where is higher than unity, saturation broadening is the most dominant. Although the present correction method is applicable only to the center measurement of axisymmetric plasma, this method is a powerful tool for the measurements of the temperature distribution along the flow axis.

Conflict of Interests

The authors do not have any conflict of interests.


This work was partly supported by Research Fellowships of the Japan Society for the Promotion of Science for Young Scientists.


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Copyright © 2013 S. Nomura et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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