Measurement and simulation of passive fast-ion D-alpha emission from the DIII-D tokamak
Spectra of passive fast-ion D-alpha (FIDA) light from beam ions that charge exchange with background neutrals are measured and simulated. The fast ions come from three sources: ions that pass through the diagnostic sightlines on their first full orbit, an axisymmetric confined population, and ions t...
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Veröffentlicht in: | Nuclear fusion 2016-11, Vol.56 (11), p.112023 |
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creator | Bolte, Nathan G. Heidbrink, William W. Pace, David Van Zeeland, Michael Chen, Xi |
description | Spectra of passive fast-ion D-alpha (FIDA) light from beam ions that charge exchange with background neutrals are measured and simulated. The fast ions come from three sources: ions that pass through the diagnostic sightlines on their first full orbit, an axisymmetric confined population, and ions that are expelled into the edge region by instabilities. A passive FIDA simulation (P-FIDASIM) is developed as a forward model for the spectra of the first-orbit fast ions and consists of an experimentally-validated beam deposition model, an ion orbit-following code, a collisional-radiative model, and a synthetic spectrometer. Model validation consists of the simulation of 86 experimental spectra that are obtained using 6 different neutral beam fast-ion sources and 13 different lines of sight. Calibrated spectra are used to estimate the neutral density throughout the cross-section of the tokamak. The resulting 2D neutral density shows the expected increase toward each X-point with average neutral densities of 8×109 cm−3 at the plasma boundary and 1×1011 cm−3 near the wall. Fast ions that are on passing orbits are expelled by the sawtooth instability more readily than trapped ions. In a sample discharge, approximately 1% of the fast-ion population is ejected into the high neutral density region per sawtooth crash. |
doi_str_mv | 10.1088/0029-5515/56/11/112023 |
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The fast ions come from three sources: ions that pass through the diagnostic sightlines on their first full orbit, an axisymmetric confined population, and ions that are expelled into the edge region by instabilities. A passive FIDA simulation (P-FIDASIM) is developed as a forward model for the spectra of the first-orbit fast ions and consists of an experimentally-validated beam deposition model, an ion orbit-following code, a collisional-radiative model, and a synthetic spectrometer. Model validation consists of the simulation of 86 experimental spectra that are obtained using 6 different neutral beam fast-ion sources and 13 different lines of sight. Calibrated spectra are used to estimate the neutral density throughout the cross-section of the tokamak. The resulting 2D neutral density shows the expected increase toward each X-point with average neutral densities of 8×109 cm−3 at the plasma boundary and 1×1011 cm−3 near the wall. Fast ions that are on passing orbits are expelled by the sawtooth instability more readily than trapped ions. In a sample discharge, approximately 1% of the fast-ion population is ejected into the high neutral density region per sawtooth crash.</description><identifier>ISSN: 0029-5515</identifier><identifier>EISSN: 1741-4326</identifier><identifier>DOI: 10.1088/0029-5515/56/11/112023</identifier><identifier>CODEN: NUFUAU</identifier><language>eng</language><publisher>United States: IOP Publishing</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; edge light ; fast ion losses ; FIDA ; FIDASIM ; neutral density ; passive FIDA ; sawtooth crash</subject><ispartof>Nuclear fusion, 2016-11, Vol.56 (11), p.112023</ispartof><rights>2016 IAEA, Vienna</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c405t-919af095ffb49da481dcc547f9020260b35f5cadc73dbaff9af8227967a86e593</citedby><cites>FETCH-LOGICAL-c405t-919af095ffb49da481dcc547f9020260b35f5cadc73dbaff9af8227967a86e593</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/0029-5515/56/11/112023/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>230,314,780,784,885,27915,27916,53837,53884</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/1371906$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Bolte, Nathan G.</creatorcontrib><creatorcontrib>Heidbrink, William W.</creatorcontrib><creatorcontrib>Pace, David</creatorcontrib><creatorcontrib>Van Zeeland, Michael</creatorcontrib><creatorcontrib>Chen, Xi</creatorcontrib><creatorcontrib>General Atomics, San Diego, CA (United States)</creatorcontrib><title>Measurement and simulation of passive fast-ion D-alpha emission from the DIII-D tokamak</title><title>Nuclear fusion</title><addtitle>NF</addtitle><addtitle>Nucl. Fusion</addtitle><description>Spectra of passive fast-ion D-alpha (FIDA) light from beam ions that charge exchange with background neutrals are measured and simulated. The fast ions come from three sources: ions that pass through the diagnostic sightlines on their first full orbit, an axisymmetric confined population, and ions that are expelled into the edge region by instabilities. A passive FIDA simulation (P-FIDASIM) is developed as a forward model for the spectra of the first-orbit fast ions and consists of an experimentally-validated beam deposition model, an ion orbit-following code, a collisional-radiative model, and a synthetic spectrometer. Model validation consists of the simulation of 86 experimental spectra that are obtained using 6 different neutral beam fast-ion sources and 13 different lines of sight. Calibrated spectra are used to estimate the neutral density throughout the cross-section of the tokamak. The resulting 2D neutral density shows the expected increase toward each X-point with average neutral densities of 8×109 cm−3 at the plasma boundary and 1×1011 cm−3 near the wall. Fast ions that are on passing orbits are expelled by the sawtooth instability more readily than trapped ions. In a sample discharge, approximately 1% of the fast-ion population is ejected into the high neutral density region per sawtooth crash.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>edge light</subject><subject>fast ion losses</subject><subject>FIDA</subject><subject>FIDASIM</subject><subject>neutral density</subject><subject>passive FIDA</subject><subject>sawtooth crash</subject><issn>0029-5515</issn><issn>1741-4326</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqFkF9LwzAUxYMoOKdfQYIvPsUlTZM2j7L5p6D4ovgY7tKEZVub0mSC396WiiAIwoUL5_7OhXMQumT0htGyXFCaKSIEEwshF4wNk9GMH6EZK3JGcp7JYzT7gU7RWYxbSlnOOJ-h92cL8dDbxrYJQ1vj6JvDHpIPLQ4OdxCj_7DYQUxk1FYE9t0GsG38cBkE14cGp43Fq6qqyAqnsIMGdufoxME-2ovvPUdv93evy0fy9PJQLW-fiMmpSEQxBY4q4dw6VzXkJauNEXnhFB1CSLrmwgkDtSl4vQbnBrrMskLJAkppheJzdDX9DTF5HY1P1mxMaFtrkma8YIrKAZITZPoQY2-d7nrfQP-pGdVjh3qsR4_1aCE1Y3rqcDBmk9GHTm_DoW-HLP-brv8wte4Xpbva8S-3Cn_H</recordid><startdate>20161101</startdate><enddate>20161101</enddate><creator>Bolte, Nathan G.</creator><creator>Heidbrink, William W.</creator><creator>Pace, David</creator><creator>Van Zeeland, Michael</creator><creator>Chen, Xi</creator><general>IOP Publishing</general><general>IOP Science</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>20161101</creationdate><title>Measurement and simulation of passive fast-ion D-alpha emission from the DIII-D tokamak</title><author>Bolte, Nathan G. ; Heidbrink, William W. ; Pace, David ; Van Zeeland, Michael ; Chen, Xi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c405t-919af095ffb49da481dcc547f9020260b35f5cadc73dbaff9af8227967a86e593</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>edge light</topic><topic>fast ion losses</topic><topic>FIDA</topic><topic>FIDASIM</topic><topic>neutral density</topic><topic>passive FIDA</topic><topic>sawtooth crash</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bolte, Nathan G.</creatorcontrib><creatorcontrib>Heidbrink, William W.</creatorcontrib><creatorcontrib>Pace, David</creatorcontrib><creatorcontrib>Van Zeeland, Michael</creatorcontrib><creatorcontrib>Chen, Xi</creatorcontrib><creatorcontrib>General Atomics, San Diego, CA (United States)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Nuclear fusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bolte, Nathan G.</au><au>Heidbrink, William W.</au><au>Pace, David</au><au>Van Zeeland, Michael</au><au>Chen, Xi</au><aucorp>General Atomics, San Diego, CA (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measurement and simulation of passive fast-ion D-alpha emission from the DIII-D tokamak</atitle><jtitle>Nuclear fusion</jtitle><stitle>NF</stitle><addtitle>Nucl. Fusion</addtitle><date>2016-11-01</date><risdate>2016</risdate><volume>56</volume><issue>11</issue><spage>112023</spage><pages>112023-</pages><issn>0029-5515</issn><eissn>1741-4326</eissn><coden>NUFUAU</coden><abstract>Spectra of passive fast-ion D-alpha (FIDA) light from beam ions that charge exchange with background neutrals are measured and simulated. The fast ions come from three sources: ions that pass through the diagnostic sightlines on their first full orbit, an axisymmetric confined population, and ions that are expelled into the edge region by instabilities. A passive FIDA simulation (P-FIDASIM) is developed as a forward model for the spectra of the first-orbit fast ions and consists of an experimentally-validated beam deposition model, an ion orbit-following code, a collisional-radiative model, and a synthetic spectrometer. Model validation consists of the simulation of 86 experimental spectra that are obtained using 6 different neutral beam fast-ion sources and 13 different lines of sight. Calibrated spectra are used to estimate the neutral density throughout the cross-section of the tokamak. The resulting 2D neutral density shows the expected increase toward each X-point with average neutral densities of 8×109 cm−3 at the plasma boundary and 1×1011 cm−3 near the wall. Fast ions that are on passing orbits are expelled by the sawtooth instability more readily than trapped ions. In a sample discharge, approximately 1% of the fast-ion population is ejected into the high neutral density region per sawtooth crash.</abstract><cop>United States</cop><pub>IOP Publishing</pub><doi>10.1088/0029-5515/56/11/112023</doi><tpages>19</tpages><oa>free_for_read</oa></addata></record> |
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subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY edge light fast ion losses FIDA FIDASIM neutral density passive FIDA sawtooth crash |
title | Measurement and simulation of passive fast-ion D-alpha emission from the DIII-D tokamak |
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