Negative Ion Kinetics in RF Glow Discharges
Using temporally and spatially resolved laser spectroscopy, we have determined the identities, approximate concentrations, effects on the local field, and kinetics of formation and loss of negative ions in RF discharges. Cl- and BCl3- are the dominant negative ions found in low-frequency discharges...
Gespeichert in:
Veröffentlicht in: | IEEE Trans. Plasma Sci.; (United States) 1986-04, Vol.14 (2), p.92-102 |
---|---|
Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 102 |
---|---|
container_issue | 2 |
container_start_page | 92 |
container_title | IEEE Trans. Plasma Sci.; (United States) |
container_volume | 14 |
creator | Gottscho, Richard A. Gaebe, Carl E. |
description | Using temporally and spatially resolved laser spectroscopy, we have determined the identities, approximate concentrations, effects on the local field, and kinetics of formation and loss of negative ions in RF discharges. Cl- and BCl3- are the dominant negative ions found in low-frequency discharges through Cl2 and BCl3, respectively. The electron affinity for Cl is measured to be 3.6118 ± 0.0005 eV. Negative ion kinetics are strongly affected by application of the RF field. Formation of negative ions by attachment of slow electrons in RF discharges is governed by the extent and duration of electron energy relaxation. Similarly, destruction of negative ions by collisional detachment and field extraction is dependent upon ion energy modulation. Thus, at low frequency, the anion density peaks at the beginning of the anodic and cathodic half-cycles after electrons have attached but before detachment and extraction have had time to occur. At higher frequencies, electrons have insufficient time to attach before they are reheated and the instantaneous anion density in the sheath is greatly reduced. When the negative ion density is comparable to the positive ion density, the plasma potential is observed to lie below the anode potential, double layers form between sheath and plasma, and anions and electrons are accelerated by large sheath fields to electrode surfaces. |
doi_str_mv | 10.1109/TPS.1986.4316511 |
format | Article |
fullrecord | <record><control><sourceid>proquest_RIE</sourceid><recordid>TN_cdi_proquest_miscellaneous_24139740</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>4316511</ieee_id><sourcerecordid>24139740</sourcerecordid><originalsourceid>FETCH-LOGICAL-c395t-1c1ecd2f15860e5d56b85ebbb9f583c60d2941ce6e2932548a58a4495d6db9563</originalsourceid><addsrcrecordid>eNo9kE1Lw0AURQdRsFb3gpsg4kZS52U-OrOUamuxqGhdD5PJSzuSJjWTKv57U1K7eot37uVyCDkHOgCg-nb--j4AreSAM5AC4ID0QDMdazYUh6RHqWYxU8COyUkIn5QCFzTpkZtnXNjGf2M0rcroyZfYeBciX0Zv42hSVD_RvQ9uaesFhlNylNsi4Nnu9snH-GE-eoxnL5Pp6G4WO6ZFE4MDdFmSg1CSosiETJXANE11LhRzkmaJ5uBQYqJZIriyQlnOtchklmohWZ9cdr1VaLwJzjfolq4qS3SNEQrEMFEtdN1B67r62mBozKodikVhS6w2wSQcmB5y2oK0A11dhVBjbta1X9n61wA1W3WmVWe26sxOXRu52nXb4GyR17Z0PuxzSjLWTm-xiw7ziLj__pf8ARe5dBM</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>24139740</pqid></control><display><type>article</type><title>Negative Ion Kinetics in RF Glow Discharges</title><source>IEEE Electronic Library (IEL)</source><creator>Gottscho, Richard A. ; Gaebe, Carl E.</creator><creatorcontrib>Gottscho, Richard A. ; Gaebe, Carl E. ; AT and T Bell Laboratories, Murray Hill, NJ 07974</creatorcontrib><description>Using temporally and spatially resolved laser spectroscopy, we have determined the identities, approximate concentrations, effects on the local field, and kinetics of formation and loss of negative ions in RF discharges. Cl- and BCl3- are the dominant negative ions found in low-frequency discharges through Cl2 and BCl3, respectively. The electron affinity for Cl is measured to be 3.6118 ± 0.0005 eV. Negative ion kinetics are strongly affected by application of the RF field. Formation of negative ions by attachment of slow electrons in RF discharges is governed by the extent and duration of electron energy relaxation. Similarly, destruction of negative ions by collisional detachment and field extraction is dependent upon ion energy modulation. Thus, at low frequency, the anion density peaks at the beginning of the anodic and cathodic half-cycles after electrons have attached but before detachment and extraction have had time to occur. At higher frequencies, electrons have insufficient time to attach before they are reheated and the instantaneous anion density in the sheath is greatly reduced. When the negative ion density is comparable to the positive ion density, the plasma potential is observed to lie below the anode potential, double layers form between sheath and plasma, and anions and electrons are accelerated by large sheath fields to electrode surfaces.</description><identifier>ISSN: 0093-3813</identifier><identifier>EISSN: 1939-9375</identifier><identifier>DOI: 10.1109/TPS.1986.4316511</identifier><identifier>CODEN: ITPSBD</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>420800 - Engineering- Electronic Circuits & Devices- (-1989) ; AFFINITY ; ANODES ; BORON CHLORIDES ; BORON COMPOUNDS ; CATHODES ; CHARGED PARTICLES ; CHLORIDES ; CHLORINE COMPOUNDS ; CHLORINE IONS ; COLLISIONS ; ELECTRIC DISCHARGES ; ELECTRODES ; ELECTRONS ; ELEMENTARY PARTICLES ; ENERGY RANGE ; ENGINEERING ; EV RANGE ; EV RANGE 01-10 ; Exact sciences and technology ; FERMIONS ; GLOW DISCHARGES ; HALIDES ; HALOGEN COMPOUNDS ; ION COLLISIONS ; ION DENSITY ; ION MOBILITY ; IONS ; Kinetic theory ; LASER SPECTROSCOPY ; LEPTONS ; MOBILITY ; PARTICLE MOBILITY ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; PLASMA ; Plasma accelerators ; Plasma density ; Plasma sheaths ; Radio frequency ; RF SYSTEMS ; Spatial resolution ; SPECTROSCOPY</subject><ispartof>IEEE Trans. Plasma Sci.; (United States), 1986-04, Vol.14 (2), p.92-102</ispartof><rights>1986 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c395t-1c1ecd2f15860e5d56b85ebbb9f583c60d2941ce6e2932548a58a4495d6db9563</citedby><cites>FETCH-LOGICAL-c395t-1c1ecd2f15860e5d56b85ebbb9f583c60d2941ce6e2932548a58a4495d6db9563</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/4316511$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,885,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/4316511$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=8633293$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/5815728$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Gottscho, Richard A.</creatorcontrib><creatorcontrib>Gaebe, Carl E.</creatorcontrib><creatorcontrib>AT and T Bell Laboratories, Murray Hill, NJ 07974</creatorcontrib><title>Negative Ion Kinetics in RF Glow Discharges</title><title>IEEE Trans. Plasma Sci.; (United States)</title><addtitle>TPS</addtitle><description>Using temporally and spatially resolved laser spectroscopy, we have determined the identities, approximate concentrations, effects on the local field, and kinetics of formation and loss of negative ions in RF discharges. Cl- and BCl3- are the dominant negative ions found in low-frequency discharges through Cl2 and BCl3, respectively. The electron affinity for Cl is measured to be 3.6118 ± 0.0005 eV. Negative ion kinetics are strongly affected by application of the RF field. Formation of negative ions by attachment of slow electrons in RF discharges is governed by the extent and duration of electron energy relaxation. Similarly, destruction of negative ions by collisional detachment and field extraction is dependent upon ion energy modulation. Thus, at low frequency, the anion density peaks at the beginning of the anodic and cathodic half-cycles after electrons have attached but before detachment and extraction have had time to occur. At higher frequencies, electrons have insufficient time to attach before they are reheated and the instantaneous anion density in the sheath is greatly reduced. When the negative ion density is comparable to the positive ion density, the plasma potential is observed to lie below the anode potential, double layers form between sheath and plasma, and anions and electrons are accelerated by large sheath fields to electrode surfaces.</description><subject>420800 - Engineering- Electronic Circuits & Devices- (-1989)</subject><subject>AFFINITY</subject><subject>ANODES</subject><subject>BORON CHLORIDES</subject><subject>BORON COMPOUNDS</subject><subject>CATHODES</subject><subject>CHARGED PARTICLES</subject><subject>CHLORIDES</subject><subject>CHLORINE COMPOUNDS</subject><subject>CHLORINE IONS</subject><subject>COLLISIONS</subject><subject>ELECTRIC DISCHARGES</subject><subject>ELECTRODES</subject><subject>ELECTRONS</subject><subject>ELEMENTARY PARTICLES</subject><subject>ENERGY RANGE</subject><subject>ENGINEERING</subject><subject>EV RANGE</subject><subject>EV RANGE 01-10</subject><subject>Exact sciences and technology</subject><subject>FERMIONS</subject><subject>GLOW DISCHARGES</subject><subject>HALIDES</subject><subject>HALOGEN COMPOUNDS</subject><subject>ION COLLISIONS</subject><subject>ION DENSITY</subject><subject>ION MOBILITY</subject><subject>IONS</subject><subject>Kinetic theory</subject><subject>LASER SPECTROSCOPY</subject><subject>LEPTONS</subject><subject>MOBILITY</subject><subject>PARTICLE MOBILITY</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>PLASMA</subject><subject>Plasma accelerators</subject><subject>Plasma density</subject><subject>Plasma sheaths</subject><subject>Radio frequency</subject><subject>RF SYSTEMS</subject><subject>Spatial resolution</subject><subject>SPECTROSCOPY</subject><issn>0093-3813</issn><issn>1939-9375</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1986</creationdate><recordtype>article</recordtype><recordid>eNo9kE1Lw0AURQdRsFb3gpsg4kZS52U-OrOUamuxqGhdD5PJSzuSJjWTKv57U1K7eot37uVyCDkHOgCg-nb--j4AreSAM5AC4ID0QDMdazYUh6RHqWYxU8COyUkIn5QCFzTpkZtnXNjGf2M0rcroyZfYeBciX0Zv42hSVD_RvQ9uaesFhlNylNsi4Nnu9snH-GE-eoxnL5Pp6G4WO6ZFE4MDdFmSg1CSosiETJXANE11LhRzkmaJ5uBQYqJZIriyQlnOtchklmohWZ9cdr1VaLwJzjfolq4qS3SNEQrEMFEtdN1B67r62mBozKodikVhS6w2wSQcmB5y2oK0A11dhVBjbta1X9n61wA1W3WmVWe26sxOXRu52nXb4GyR17Z0PuxzSjLWTm-xiw7ziLj__pf8ARe5dBM</recordid><startdate>19860401</startdate><enddate>19860401</enddate><creator>Gottscho, Richard A.</creator><creator>Gaebe, Carl E.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>19860401</creationdate><title>Negative Ion Kinetics in RF Glow Discharges</title><author>Gottscho, Richard A. ; Gaebe, Carl E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c395t-1c1ecd2f15860e5d56b85ebbb9f583c60d2941ce6e2932548a58a4495d6db9563</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1986</creationdate><topic>420800 - Engineering- Electronic Circuits & Devices- (-1989)</topic><topic>AFFINITY</topic><topic>ANODES</topic><topic>BORON CHLORIDES</topic><topic>BORON COMPOUNDS</topic><topic>CATHODES</topic><topic>CHARGED PARTICLES</topic><topic>CHLORIDES</topic><topic>CHLORINE COMPOUNDS</topic><topic>CHLORINE IONS</topic><topic>COLLISIONS</topic><topic>ELECTRIC DISCHARGES</topic><topic>ELECTRODES</topic><topic>ELECTRONS</topic><topic>ELEMENTARY PARTICLES</topic><topic>ENERGY RANGE</topic><topic>ENGINEERING</topic><topic>EV RANGE</topic><topic>EV RANGE 01-10</topic><topic>Exact sciences and technology</topic><topic>FERMIONS</topic><topic>GLOW DISCHARGES</topic><topic>HALIDES</topic><topic>HALOGEN COMPOUNDS</topic><topic>ION COLLISIONS</topic><topic>ION DENSITY</topic><topic>ION MOBILITY</topic><topic>IONS</topic><topic>Kinetic theory</topic><topic>LASER SPECTROSCOPY</topic><topic>LEPTONS</topic><topic>MOBILITY</topic><topic>PARTICLE MOBILITY</topic><topic>Physics</topic><topic>Physics of gases, plasmas and electric discharges</topic><topic>Physics of plasmas and electric discharges</topic><topic>PLASMA</topic><topic>Plasma accelerators</topic><topic>Plasma density</topic><topic>Plasma sheaths</topic><topic>Radio frequency</topic><topic>RF SYSTEMS</topic><topic>Spatial resolution</topic><topic>SPECTROSCOPY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gottscho, Richard A.</creatorcontrib><creatorcontrib>Gaebe, Carl E.</creatorcontrib><creatorcontrib>AT and T Bell Laboratories, Murray Hill, NJ 07974</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>IEEE Trans. Plasma Sci.; (United States)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Gottscho, Richard A.</au><au>Gaebe, Carl E.</au><aucorp>AT and T Bell Laboratories, Murray Hill, NJ 07974</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Negative Ion Kinetics in RF Glow Discharges</atitle><jtitle>IEEE Trans. Plasma Sci.; (United States)</jtitle><stitle>TPS</stitle><date>1986-04-01</date><risdate>1986</risdate><volume>14</volume><issue>2</issue><spage>92</spage><epage>102</epage><pages>92-102</pages><issn>0093-3813</issn><eissn>1939-9375</eissn><coden>ITPSBD</coden><abstract>Using temporally and spatially resolved laser spectroscopy, we have determined the identities, approximate concentrations, effects on the local field, and kinetics of formation and loss of negative ions in RF discharges. Cl- and BCl3- are the dominant negative ions found in low-frequency discharges through Cl2 and BCl3, respectively. The electron affinity for Cl is measured to be 3.6118 ± 0.0005 eV. Negative ion kinetics are strongly affected by application of the RF field. Formation of negative ions by attachment of slow electrons in RF discharges is governed by the extent and duration of electron energy relaxation. Similarly, destruction of negative ions by collisional detachment and field extraction is dependent upon ion energy modulation. Thus, at low frequency, the anion density peaks at the beginning of the anodic and cathodic half-cycles after electrons have attached but before detachment and extraction have had time to occur. At higher frequencies, electrons have insufficient time to attach before they are reheated and the instantaneous anion density in the sheath is greatly reduced. When the negative ion density is comparable to the positive ion density, the plasma potential is observed to lie below the anode potential, double layers form between sheath and plasma, and anions and electrons are accelerated by large sheath fields to electrode surfaces.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TPS.1986.4316511</doi><tpages>11</tpages></addata></record> |
fulltext | fulltext_linktorsrc |
identifier | ISSN: 0093-3813 |
ispartof | IEEE Trans. Plasma Sci.; (United States), 1986-04, Vol.14 (2), p.92-102 |
issn | 0093-3813 1939-9375 |
language | eng |
recordid | cdi_proquest_miscellaneous_24139740 |
source | IEEE Electronic Library (IEL) |
subjects | 420800 - Engineering- Electronic Circuits & Devices- (-1989) AFFINITY ANODES BORON CHLORIDES BORON COMPOUNDS CATHODES CHARGED PARTICLES CHLORIDES CHLORINE COMPOUNDS CHLORINE IONS COLLISIONS ELECTRIC DISCHARGES ELECTRODES ELECTRONS ELEMENTARY PARTICLES ENERGY RANGE ENGINEERING EV RANGE EV RANGE 01-10 Exact sciences and technology FERMIONS GLOW DISCHARGES HALIDES HALOGEN COMPOUNDS ION COLLISIONS ION DENSITY ION MOBILITY IONS Kinetic theory LASER SPECTROSCOPY LEPTONS MOBILITY PARTICLE MOBILITY Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges PLASMA Plasma accelerators Plasma density Plasma sheaths Radio frequency RF SYSTEMS Spatial resolution SPECTROSCOPY |
title | Negative Ion Kinetics in RF Glow Discharges |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-21T14%3A46%3A30IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_RIE&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Negative%20Ion%20Kinetics%20in%20RF%20Glow%20Discharges&rft.jtitle=IEEE%20Trans.%20Plasma%20Sci.;%20(United%20States)&rft.au=Gottscho,%20Richard%20A.&rft.aucorp=AT%20and%20T%20Bell%20Laboratories,%20Murray%20Hill,%20NJ%2007974&rft.date=1986-04-01&rft.volume=14&rft.issue=2&rft.spage=92&rft.epage=102&rft.pages=92-102&rft.issn=0093-3813&rft.eissn=1939-9375&rft.coden=ITPSBD&rft_id=info:doi/10.1109/TPS.1986.4316511&rft_dat=%3Cproquest_RIE%3E24139740%3C/proquest_RIE%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=24139740&rft_id=info:pmid/&rft_ieee_id=4316511&rfr_iscdi=true |