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Laser‐induced fluorescence measurement of the dynamics of a pulsed planar sheath
Using laser‐induced fluorescence (LIF) the ion density near the edge of an expanding plasma sheath has been measured. These measurements utilized a transition of N+ 2 [the P12 component of the X 2Σ+ g (ν=0)→B 2Σ+ u (ν=0) band] in a N2 plasma. The strength of the laser‐induced fluorescence was used a...
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Published in: | Physics of plasmas 1994-04, Vol.1 (4), p.1064-1074 |
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description | Using laser‐induced fluorescence (LIF) the ion density near the edge of an expanding plasma sheath has been measured. These measurements utilized a transition of N+
2 [the P12 component of the X 2Σ+
g
(ν=0)→B 2Σ+
u
(ν=0) band] in a N2 plasma. The strength of the laser‐induced fluorescence was used as a measure of the temporally and spatially varying ion density. The expanding sheath was produced by applying a −5 kV pulse to a polished planar electrode in the plasma source ion implantation device [J. R. Conrad et
al., J. Vac. Sci. Technol. A 8, 3146 (1990)]. The laser beam was aligned normal to the surface and was reflected off the center of the electrode. The LIF diagnostic used here is nonperturbing whereas previous researchers have used Langmuir probes, which perturb the plasma, to make their measurements. As such, the data reported here represent a benchmark measurement of pulsed sheaths and allow a better comparison between experimental measurements and theoretical predictions. It has been found that the sheath edge moves approximately 16 times faster than the ion‐acoustic velocity during the early part of the pulse, t |
doi_str_mv | 10.1063/1.870924 |
format | article |
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2 [the P12 component of the X 2Σ+
g
(ν=0)→B 2Σ+
u
(ν=0) band] in a N2 plasma. The strength of the laser‐induced fluorescence was used as a measure of the temporally and spatially varying ion density. The expanding sheath was produced by applying a −5 kV pulse to a polished planar electrode in the plasma source ion implantation device [J. R. Conrad et
al., J. Vac. Sci. Technol. A 8, 3146 (1990)]. The laser beam was aligned normal to the surface and was reflected off the center of the electrode. The LIF diagnostic used here is nonperturbing whereas previous researchers have used Langmuir probes, which perturb the plasma, to make their measurements. As such, the data reported here represent a benchmark measurement of pulsed sheaths and allow a better comparison between experimental measurements and theoretical predictions. It has been found that the sheath edge moves approximately 16 times faster than the ion‐acoustic velocity during the early part of the pulse, t<1 μs, and then slows to approximately the ion‐acoustic velocity after 6 μs. In addition to the LIF measurements, a biased probe was used far from the cathode to determine the sheath edge location. Good agreement is found when the LIF and probe data are compared. The LIF data also are compared to the predictions of a simulation that is based on a time‐varying two‐fluid model of the sheath [G. A. Emmert and M. A. Henry, J. Appl. Phys. 71, 113 (1992)]. While the predictions of the model show moderate agreement with the data, substantial discrepancies are observed. These discrepancies are attributed to a number of physical phenomena that are not included in the present model.</description><identifier>ISSN: 1070-664X</identifier><identifier>EISSN: 1089-7674</identifier><identifier>DOI: 10.1063/1.870924</identifier><identifier>CODEN: PHPAEN</identifier><language>eng</language><publisher>United States</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; CHARGED PARTICLES ; COLLISIONLESS PLASMA ; ELECTRODES ; ELECTROMAGNETIC RADIATION ; EMISSION SPECTROSCOPY ; FLUORESCENCE SPECTROSCOPY ; ION ACOUSTIC WAVES ; ION DENSITY ; ION WAVES ; IONS ; LASER RADIATION ; NITROGEN IONS ; PLASMA ; PLASMA SHEATH ; PLASMA WAVES ; RADIATIONS ; SPECTROSCOPY 700350 -- Plasma Production, Heating, Current Drive, & Interactions-- (1992-) ; WALL EFFECTS</subject><ispartof>Physics of plasmas, 1994-04, Vol.1 (4), p.1064-1074</ispartof><rights>American Institute of Physics</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c354t-893bfdc2a0701f7a0a663ec215da8e21348450850ae0052cc04e0e0b544c41513</citedby><cites>FETCH-LOGICAL-c354t-893bfdc2a0701f7a0a663ec215da8e21348450850ae0052cc04e0e0b544c41513</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/pop/article-lookup/doi/10.1063/1.870924$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>230,314,780,782,784,795,885,27924,27925,76383</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/6685134$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Goeckner, M. J.</creatorcontrib><creatorcontrib>Malik, Shamim M.</creatorcontrib><creatorcontrib>Conrad, J. R.</creatorcontrib><creatorcontrib>Breun, R. A.</creatorcontrib><title>Laser‐induced fluorescence measurement of the dynamics of a pulsed planar sheath</title><title>Physics of plasmas</title><description>Using laser‐induced fluorescence (LIF) the ion density near the edge of an expanding plasma sheath has been measured. These measurements utilized a transition of N+
2 [the P12 component of the X 2Σ+
g
(ν=0)→B 2Σ+
u
(ν=0) band] in a N2 plasma. The strength of the laser‐induced fluorescence was used as a measure of the temporally and spatially varying ion density. The expanding sheath was produced by applying a −5 kV pulse to a polished planar electrode in the plasma source ion implantation device [J. R. Conrad et
al., J. Vac. Sci. Technol. A 8, 3146 (1990)]. The laser beam was aligned normal to the surface and was reflected off the center of the electrode. The LIF diagnostic used here is nonperturbing whereas previous researchers have used Langmuir probes, which perturb the plasma, to make their measurements. As such, the data reported here represent a benchmark measurement of pulsed sheaths and allow a better comparison between experimental measurements and theoretical predictions. It has been found that the sheath edge moves approximately 16 times faster than the ion‐acoustic velocity during the early part of the pulse, t<1 μs, and then slows to approximately the ion‐acoustic velocity after 6 μs. In addition to the LIF measurements, a biased probe was used far from the cathode to determine the sheath edge location. Good agreement is found when the LIF and probe data are compared. The LIF data also are compared to the predictions of a simulation that is based on a time‐varying two‐fluid model of the sheath [G. A. Emmert and M. A. Henry, J. Appl. Phys. 71, 113 (1992)]. While the predictions of the model show moderate agreement with the data, substantial discrepancies are observed. These discrepancies are attributed to a number of physical phenomena that are not included in the present model.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>CHARGED PARTICLES</subject><subject>COLLISIONLESS PLASMA</subject><subject>ELECTRODES</subject><subject>ELECTROMAGNETIC RADIATION</subject><subject>EMISSION SPECTROSCOPY</subject><subject>FLUORESCENCE SPECTROSCOPY</subject><subject>ION ACOUSTIC WAVES</subject><subject>ION DENSITY</subject><subject>ION WAVES</subject><subject>IONS</subject><subject>LASER RADIATION</subject><subject>NITROGEN IONS</subject><subject>PLASMA</subject><subject>PLASMA SHEATH</subject><subject>PLASMA WAVES</subject><subject>RADIATIONS</subject><subject>SPECTROSCOPY 700350 -- Plasma Production, Heating, Current Drive, & Interactions-- (1992-)</subject><subject>WALL EFFECTS</subject><issn>1070-664X</issn><issn>1089-7674</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1994</creationdate><recordtype>article</recordtype><recordid>eNp90M1KxDAQB_AgCq6r4CMUT3roOmmTNHuUxS9YEETBW8imE1rZpiVJhb35CD6jT2JLZS-Cp0yG3_wZhpBzCgsKIr-mC1nAMmMHZEZBLtNCFOxwrAtIhWBvx-QkhHcAYILLGXle64D--_OrdmVvsEzstm89BoPOYNKgDr3HBl1MWpvECpNy53RTmzD-ddL12zAMdVvttE9ChTpWp-TI6qF99vvOyevd7cvqIV0_3T-ubtapyTmLqVzmG1uaTA-bUVto0ELkaDLKSy0xozmTjIPkoBGAZ8YAQ0DYcMYMo5zmc3Ix5bYh1iqYOqKpTOscmqiEkANhA7qckPFtCB6t6nzdaL9TFNR4MEXVdLCBXk10jNKxbt3efrR-71RX2v_sn9wf_Lt5eQ</recordid><startdate>19940401</startdate><enddate>19940401</enddate><creator>Goeckner, M. J.</creator><creator>Malik, Shamim M.</creator><creator>Conrad, J. R.</creator><creator>Breun, R. A.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>19940401</creationdate><title>Laser‐induced fluorescence measurement of the dynamics of a pulsed planar sheath</title><author>Goeckner, M. J. ; Malik, Shamim M. ; Conrad, J. R. ; Breun, R. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c354t-893bfdc2a0701f7a0a663ec215da8e21348450850ae0052cc04e0e0b544c41513</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1994</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>CHARGED PARTICLES</topic><topic>COLLISIONLESS PLASMA</topic><topic>ELECTRODES</topic><topic>ELECTROMAGNETIC RADIATION</topic><topic>EMISSION SPECTROSCOPY</topic><topic>FLUORESCENCE SPECTROSCOPY</topic><topic>ION ACOUSTIC WAVES</topic><topic>ION DENSITY</topic><topic>ION WAVES</topic><topic>IONS</topic><topic>LASER RADIATION</topic><topic>NITROGEN IONS</topic><topic>PLASMA</topic><topic>PLASMA SHEATH</topic><topic>PLASMA WAVES</topic><topic>RADIATIONS</topic><topic>SPECTROSCOPY 700350 -- Plasma Production, Heating, Current Drive, & Interactions-- (1992-)</topic><topic>WALL EFFECTS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Goeckner, M. J.</creatorcontrib><creatorcontrib>Malik, Shamim M.</creatorcontrib><creatorcontrib>Conrad, J. R.</creatorcontrib><creatorcontrib>Breun, R. A.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Physics of plasmas</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Goeckner, M. J.</au><au>Malik, Shamim M.</au><au>Conrad, J. R.</au><au>Breun, R. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Laser‐induced fluorescence measurement of the dynamics of a pulsed planar sheath</atitle><jtitle>Physics of plasmas</jtitle><date>1994-04-01</date><risdate>1994</risdate><volume>1</volume><issue>4</issue><spage>1064</spage><epage>1074</epage><pages>1064-1074</pages><issn>1070-664X</issn><eissn>1089-7674</eissn><coden>PHPAEN</coden><abstract>Using laser‐induced fluorescence (LIF) the ion density near the edge of an expanding plasma sheath has been measured. These measurements utilized a transition of N+
2 [the P12 component of the X 2Σ+
g
(ν=0)→B 2Σ+
u
(ν=0) band] in a N2 plasma. The strength of the laser‐induced fluorescence was used as a measure of the temporally and spatially varying ion density. The expanding sheath was produced by applying a −5 kV pulse to a polished planar electrode in the plasma source ion implantation device [J. R. Conrad et
al., J. Vac. Sci. Technol. A 8, 3146 (1990)]. The laser beam was aligned normal to the surface and was reflected off the center of the electrode. The LIF diagnostic used here is nonperturbing whereas previous researchers have used Langmuir probes, which perturb the plasma, to make their measurements. As such, the data reported here represent a benchmark measurement of pulsed sheaths and allow a better comparison between experimental measurements and theoretical predictions. It has been found that the sheath edge moves approximately 16 times faster than the ion‐acoustic velocity during the early part of the pulse, t<1 μs, and then slows to approximately the ion‐acoustic velocity after 6 μs. In addition to the LIF measurements, a biased probe was used far from the cathode to determine the sheath edge location. Good agreement is found when the LIF and probe data are compared. The LIF data also are compared to the predictions of a simulation that is based on a time‐varying two‐fluid model of the sheath [G. A. Emmert and M. A. Henry, J. Appl. Phys. 71, 113 (1992)]. While the predictions of the model show moderate agreement with the data, substantial discrepancies are observed. These discrepancies are attributed to a number of physical phenomena that are not included in the present model.</abstract><cop>United States</cop><doi>10.1063/1.870924</doi><tpages>11</tpages><oa>free_for_read</oa></addata></record> |
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subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY CHARGED PARTICLES COLLISIONLESS PLASMA ELECTRODES ELECTROMAGNETIC RADIATION EMISSION SPECTROSCOPY FLUORESCENCE SPECTROSCOPY ION ACOUSTIC WAVES ION DENSITY ION WAVES IONS LASER RADIATION NITROGEN IONS PLASMA PLASMA SHEATH PLASMA WAVES RADIATIONS SPECTROSCOPY 700350 -- Plasma Production, Heating, Current Drive, & Interactions-- (1992-) WALL EFFECTS |
title | Laser‐induced fluorescence measurement of the dynamics of a pulsed planar sheath |
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