Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis
Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as wel...
Ausführliche Beschreibung
Autor*in: |
Batistoni, D. A. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2000 |
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Anmerkung: |
© Springer-Verlag Berlin Heidelberg 2000 |
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Übergeordnetes Werk: |
Enthalten in: Analytical and bioanalytical chemistry - Berlin : Springer, 2002, 366(2000), 3 vom: 01. Feb., Seite 221-227 |
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Übergeordnetes Werk: |
volume:366 ; year:2000 ; number:3 ; day:01 ; month:02 ; pages:221-227 |
Links: |
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DOI / URN: |
10.1007/s002160050044 |
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SPR002131285 |
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520 | |a Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. | ||
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700 | 1 | |a Rodríguez, R. E. |4 aut | |
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10.1007/s002160050044 doi (DE-627)SPR002131285 (SPR)s002160050044-e DE-627 ger DE-627 rakwb eng Batistoni, D. A. verfasserin aut Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis 2000 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2000 Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. Electron Number Density (dpeaa)DE-He213 Sodium Tetrahydroborate (dpeaa)DE-He213 Water Aerosol (dpeaa)DE-He213 Background Enhancement (dpeaa)DE-He213 Volatile Hydride (dpeaa)DE-He213 Garavaglia, R. N. aut Rodríguez, R. E. aut Enthalten in Analytical and bioanalytical chemistry Berlin : Springer, 2002 366(2000), 3 vom: 01. Feb., Seite 221-227 (DE-627)25372337X (DE-600)1459122-4 1618-2650 nnns volume:366 year:2000 number:3 day:01 month:02 pages:221-227 https://dx.doi.org/10.1007/s002160050044 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_120 GBV_ILN_121 GBV_ILN_150 AR 366 2000 3 01 02 221-227 |
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10.1007/s002160050044 doi (DE-627)SPR002131285 (SPR)s002160050044-e DE-627 ger DE-627 rakwb eng Batistoni, D. A. verfasserin aut Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis 2000 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2000 Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. Electron Number Density (dpeaa)DE-He213 Sodium Tetrahydroborate (dpeaa)DE-He213 Water Aerosol (dpeaa)DE-He213 Background Enhancement (dpeaa)DE-He213 Volatile Hydride (dpeaa)DE-He213 Garavaglia, R. N. aut Rodríguez, R. E. aut Enthalten in Analytical and bioanalytical chemistry Berlin : Springer, 2002 366(2000), 3 vom: 01. Feb., Seite 221-227 (DE-627)25372337X (DE-600)1459122-4 1618-2650 nnns volume:366 year:2000 number:3 day:01 month:02 pages:221-227 https://dx.doi.org/10.1007/s002160050044 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_120 GBV_ILN_121 GBV_ILN_150 AR 366 2000 3 01 02 221-227 |
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10.1007/s002160050044 doi (DE-627)SPR002131285 (SPR)s002160050044-e DE-627 ger DE-627 rakwb eng Batistoni, D. A. verfasserin aut Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis 2000 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2000 Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. Electron Number Density (dpeaa)DE-He213 Sodium Tetrahydroborate (dpeaa)DE-He213 Water Aerosol (dpeaa)DE-He213 Background Enhancement (dpeaa)DE-He213 Volatile Hydride (dpeaa)DE-He213 Garavaglia, R. N. aut Rodríguez, R. E. aut Enthalten in Analytical and bioanalytical chemistry Berlin : Springer, 2002 366(2000), 3 vom: 01. Feb., Seite 221-227 (DE-627)25372337X (DE-600)1459122-4 1618-2650 nnns volume:366 year:2000 number:3 day:01 month:02 pages:221-227 https://dx.doi.org/10.1007/s002160050044 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_120 GBV_ILN_121 GBV_ILN_150 AR 366 2000 3 01 02 221-227 |
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10.1007/s002160050044 doi (DE-627)SPR002131285 (SPR)s002160050044-e DE-627 ger DE-627 rakwb eng Batistoni, D. A. verfasserin aut Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis 2000 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2000 Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. Electron Number Density (dpeaa)DE-He213 Sodium Tetrahydroborate (dpeaa)DE-He213 Water Aerosol (dpeaa)DE-He213 Background Enhancement (dpeaa)DE-He213 Volatile Hydride (dpeaa)DE-He213 Garavaglia, R. N. aut Rodríguez, R. E. aut Enthalten in Analytical and bioanalytical chemistry Berlin : Springer, 2002 366(2000), 3 vom: 01. Feb., Seite 221-227 (DE-627)25372337X (DE-600)1459122-4 1618-2650 nnns volume:366 year:2000 number:3 day:01 month:02 pages:221-227 https://dx.doi.org/10.1007/s002160050044 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_120 GBV_ILN_121 GBV_ILN_150 AR 366 2000 3 01 02 221-227 |
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10.1007/s002160050044 doi (DE-627)SPR002131285 (SPR)s002160050044-e DE-627 ger DE-627 rakwb eng Batistoni, D. A. verfasserin aut Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis 2000 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2000 Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. Electron Number Density (dpeaa)DE-He213 Sodium Tetrahydroborate (dpeaa)DE-He213 Water Aerosol (dpeaa)DE-He213 Background Enhancement (dpeaa)DE-He213 Volatile Hydride (dpeaa)DE-He213 Garavaglia, R. N. aut Rodríguez, R. E. aut Enthalten in Analytical and bioanalytical chemistry Berlin : Springer, 2002 366(2000), 3 vom: 01. Feb., Seite 221-227 (DE-627)25372337X (DE-600)1459122-4 1618-2650 nnns volume:366 year:2000 number:3 day:01 month:02 pages:221-227 https://dx.doi.org/10.1007/s002160050044 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_120 GBV_ILN_121 GBV_ILN_150 AR 366 2000 3 01 02 221-227 |
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author |
Batistoni, D. A. |
spellingShingle |
Batistoni, D. A. misc Electron Number Density misc Sodium Tetrahydroborate misc Water Aerosol misc Background Enhancement misc Volatile Hydride Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis |
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Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis Electron Number Density (dpeaa)DE-He213 Sodium Tetrahydroborate (dpeaa)DE-He213 Water Aerosol (dpeaa)DE-He213 Background Enhancement (dpeaa)DE-He213 Volatile Hydride (dpeaa)DE-He213 |
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misc Electron Number Density misc Sodium Tetrahydroborate misc Water Aerosol misc Background Enhancement misc Volatile Hydride |
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misc Electron Number Density misc Sodium Tetrahydroborate misc Water Aerosol misc Background Enhancement misc Volatile Hydride |
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misc Electron Number Density misc Sodium Tetrahydroborate misc Water Aerosol misc Background Enhancement misc Volatile Hydride |
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(DE-627)25372337X (DE-600)1459122-4 |
title |
Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis |
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(DE-627)SPR002131285 (SPR)s002160050044-e |
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Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis |
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Batistoni, D. A. |
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Analytical and bioanalytical chemistry |
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2000 |
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Batistoni, D. A. Garavaglia, R. N. Rodríguez, R. E. |
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366 |
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Elektronische Aufsätze |
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Batistoni, D. A. |
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10.1007/s002160050044 |
title_sort |
evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-icp-atomic emission spectrometric analysis |
title_auth |
Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis |
abstract |
Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. © Springer-Verlag Berlin Heidelberg 2000 |
abstractGer |
Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. © Springer-Verlag Berlin Heidelberg 2000 |
abstract_unstemmed |
Abstract The simultaneous injection of volatile hydride species and hydrogen gas, originating in reagent decomposition, was monitored during the operation of a continuous hydride generation manifold employed for the determination of trace arsenic by HG-ICP-AES. Line and background intensities as well as the FWHM of the hydrogen Hγ and Hδ lines were measured, and electron number densities ($ n_{e} $) estimated from Stark broadening of the line profiles. Results were compared with those obtained by conventional pneumatic injection of aqueous solutions. Overlapping with atomic nitrogen lines at 410 nm and 411 nm tends to distort the Hδ line profile for the hydrogen-seeded plasma, rendering unreliable results. The N I lines seem to be quenched by the presence of water aerosol. More consistent results were obtained with the Hγ line. When no solutions are pumped through the hydride generation manifold (“dry” plasma), the measured $ n_{e} $ value was (1.57 ± 0.22) × $ 10^{15} %$ cm^{–3} $. Conversely, when the reducing reagent flow was replaced by pure water (corresponding to the injection of water vapor in equilibrium that is swept by the argon carrier gas passing through the phase separator), the electron concentration is 25% higher. In that case the $ n_{e} $ value agrees between the experimental error with that obtained for a plasma in which a water aerosol is introduced at a flow rate of 1 mL/min. An enhancement of 52% relative is observed in $ n_{e} $ when the system is operated under optimized conditions for arsine generation, employing sodium tetrahydroborate in acidic medium as reducing agent (i.e. hydrogen seeded plasma). It was also observed that the continuum emission near 410 nm for the hydrogen containing plasma correlates with the measured electron number density, suggesting that the background enhancement under hydride generation conditions may respond to the ion-electron recombination mechanism. © Springer-Verlag Berlin Heidelberg 2000 |
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Evaluation of hydrogen line emission and argon plasma electron concentrations resulting from the gaseous sample injection involved in hydride generation-ICP-atomic emission spectrometric analysis |
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