Plasma diagnostics in spherical tokamaks with silicon charged-particle detectors

Detection of charged fusion products, such as protons and tritons resulting from D(d, p) t reactions, can be used to determine the position and time dependent fusion reaction rate profile in spherical tokamak plasmas with neutral beam heating. We have developed a prototype instrument consisting of 6...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Review of scientific instruments 2016-11, Vol.87 (11), p.11D805-11D805
Hauptverfasser: Netepenko, A., Boeglin, W. U., Darrow, D. S., Ellis, R., Sibilia, M. J.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 11D805
container_issue 11
container_start_page 11D805
container_title Review of scientific instruments
container_volume 87
creator Netepenko, A.
Boeglin, W. U.
Darrow, D. S.
Ellis, R.
Sibilia, M. J.
description Detection of charged fusion products, such as protons and tritons resulting from D(d, p) t reactions, can be used to determine the position and time dependent fusion reaction rate profile in spherical tokamak plasmas with neutral beam heating. We have developed a prototype instrument consisting of 6 ion-implanted-silicon surface barrier detectors combined with collimators in such a way that each detector can accept 3 MeV protons and 1 MeV tritons and thus provides a curved view across the plasma cross section. The combination of the results from all six detectors will provide information on the spatial distribution of the fusion reaction rate. The expected time resolution of about 1 ms makes it possible to study changes in the reaction rate due to slow variations in the neutral beam density profile, as well as rapid changes resulting from MHD instabilities. Details of the new instrument, its data acquisition system, simulation results, and electrical noise testing results are discussed in this paper. First experimental data are expected to be taken during the current experimental campaign at NSTX-U.
doi_str_mv 10.1063/1.4955485
format Article
fullrecord <record><control><sourceid>proquest_pubme</sourceid><recordid>TN_cdi_pubmed_primary_27910355</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1845828131</sourcerecordid><originalsourceid>FETCH-LOGICAL-c481t-7174e5e0490c505ce61de09b6e4f843a5fd855db43813b59b2a9cfe07285b8a53</originalsourceid><addsrcrecordid>eNp90cFu1DAQBmALgehSOPACKBIXipTisT2JfawqCkiV6AHOluNMum6TONhZEG-PV7u0J_DFl8-_f3sYew38HHgjP8C5MohK4xO2Aa5N3TZCPmUbzqWqm1bpE_Yi5zteFgI8ZyeiNcAl4obd3IwuT67qg7udY16Dz1WYq7xsKQXvxmqN925y97n6FdZtlcMYfJwrv3Xplvp6cakcGanqaSW_xpRfsmeDGzO9Ou6n7PvVx2-Xn-vrr5--XF5c115pWOsWWkVIXBnukaOnBnripmtIDVpJh0OvEftOSQ2yQ9MJZ_xAvBUaO-1QnrK3h9x9aZt9KPdvS7W51LBCoGmw0UW9O6glxR87yqudQvY0jm6muMsWtEItyhXwGPhA7-IuzeUNVoCAliO2pqizg_Ip5pxosEsKk0u_LXC7H4YFexxGsW-Oibtuov5B_v39At4fwL6-W0Oc_5v2T_wzpkdol36QfwAJHZ7G</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2121705579</pqid></control><display><type>article</type><title>Plasma diagnostics in spherical tokamaks with silicon charged-particle detectors</title><source>AIP Journals Complete</source><source>Alma/SFX Local Collection</source><creator>Netepenko, A. ; Boeglin, W. U. ; Darrow, D. S. ; Ellis, R. ; Sibilia, M. J.</creator><creatorcontrib>Netepenko, A. ; Boeglin, W. U. ; Darrow, D. S. ; Ellis, R. ; Sibilia, M. J.</creatorcontrib><description>Detection of charged fusion products, such as protons and tritons resulting from D(d, p) t reactions, can be used to determine the position and time dependent fusion reaction rate profile in spherical tokamak plasmas with neutral beam heating. We have developed a prototype instrument consisting of 6 ion-implanted-silicon surface barrier detectors combined with collimators in such a way that each detector can accept 3 MeV protons and 1 MeV tritons and thus provides a curved view across the plasma cross section. The combination of the results from all six detectors will provide information on the spatial distribution of the fusion reaction rate. The expected time resolution of about 1 ms makes it possible to study changes in the reaction rate due to slow variations in the neutral beam density profile, as well as rapid changes resulting from MHD instabilities. Details of the new instrument, its data acquisition system, simulation results, and electrical noise testing results are discussed in this paper. First experimental data are expected to be taken during the current experimental campaign at NSTX-U.</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/1.4955485</identifier><identifier>PMID: 27910355</identifier><identifier>CODEN: RSINAK</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>Charged particles ; Collimation ; Collimators ; CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY ; DATA ACQUISITION ; DIAGRAMS ; Electrical noise ; HEAVY ION FUSION REACTIONS ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY ; ION IMPLANTATION ; IONS ; MAGNETOHYDRODYNAMICS ; MEV RANGE 01-10 ; Neutral beams ; NSTX DEVICE ; PLASMA DIAGNOSTICS ; PROTONS ; Radiation counters ; REACTION KINETICS ; Scientific apparatus &amp; instruments ; Sensors ; SILICON ; SPATIAL DISTRIBUTION ; SPHERICAL CONFIGURATION ; Spherical plasmas ; SURFACE BARRIER DETECTORS ; THERMONUCLEAR REACTIONS ; TIME DEPENDENCE ; TIME RESOLUTION ; Tokamak devices ; TRITONS ; TRITURUS</subject><ispartof>Review of scientific instruments, 2016-11, Vol.87 (11), p.11D805-11D805</ispartof><rights>Author(s)</rights><rights>2016 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c481t-7174e5e0490c505ce61de09b6e4f843a5fd855db43813b59b2a9cfe07285b8a53</citedby><cites>FETCH-LOGICAL-c481t-7174e5e0490c505ce61de09b6e4f843a5fd855db43813b59b2a9cfe07285b8a53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/rsi/article-lookup/doi/10.1063/1.4955485$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>230,314,780,784,794,885,4511,27923,27924,76255</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27910355$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/22596568$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Netepenko, A.</creatorcontrib><creatorcontrib>Boeglin, W. U.</creatorcontrib><creatorcontrib>Darrow, D. S.</creatorcontrib><creatorcontrib>Ellis, R.</creatorcontrib><creatorcontrib>Sibilia, M. J.</creatorcontrib><title>Plasma diagnostics in spherical tokamaks with silicon charged-particle detectors</title><title>Review of scientific instruments</title><addtitle>Rev Sci Instrum</addtitle><description>Detection of charged fusion products, such as protons and tritons resulting from D(d, p) t reactions, can be used to determine the position and time dependent fusion reaction rate profile in spherical tokamak plasmas with neutral beam heating. We have developed a prototype instrument consisting of 6 ion-implanted-silicon surface barrier detectors combined with collimators in such a way that each detector can accept 3 MeV protons and 1 MeV tritons and thus provides a curved view across the plasma cross section. The combination of the results from all six detectors will provide information on the spatial distribution of the fusion reaction rate. The expected time resolution of about 1 ms makes it possible to study changes in the reaction rate due to slow variations in the neutral beam density profile, as well as rapid changes resulting from MHD instabilities. Details of the new instrument, its data acquisition system, simulation results, and electrical noise testing results are discussed in this paper. First experimental data are expected to be taken during the current experimental campaign at NSTX-U.</description><subject>Charged particles</subject><subject>Collimation</subject><subject>Collimators</subject><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</subject><subject>DATA ACQUISITION</subject><subject>DIAGRAMS</subject><subject>Electrical noise</subject><subject>HEAVY ION FUSION REACTIONS</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>ION IMPLANTATION</subject><subject>IONS</subject><subject>MAGNETOHYDRODYNAMICS</subject><subject>MEV RANGE 01-10</subject><subject>Neutral beams</subject><subject>NSTX DEVICE</subject><subject>PLASMA DIAGNOSTICS</subject><subject>PROTONS</subject><subject>Radiation counters</subject><subject>REACTION KINETICS</subject><subject>Scientific apparatus &amp; instruments</subject><subject>Sensors</subject><subject>SILICON</subject><subject>SPATIAL DISTRIBUTION</subject><subject>SPHERICAL CONFIGURATION</subject><subject>Spherical plasmas</subject><subject>SURFACE BARRIER DETECTORS</subject><subject>THERMONUCLEAR REACTIONS</subject><subject>TIME DEPENDENCE</subject><subject>TIME RESOLUTION</subject><subject>Tokamak devices</subject><subject>TRITONS</subject><subject>TRITURUS</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp90cFu1DAQBmALgehSOPACKBIXipTisT2JfawqCkiV6AHOluNMum6TONhZEG-PV7u0J_DFl8-_f3sYew38HHgjP8C5MohK4xO2Aa5N3TZCPmUbzqWqm1bpE_Yi5zteFgI8ZyeiNcAl4obd3IwuT67qg7udY16Dz1WYq7xsKQXvxmqN925y97n6FdZtlcMYfJwrv3Xplvp6cakcGanqaSW_xpRfsmeDGzO9Ou6n7PvVx2-Xn-vrr5--XF5c115pWOsWWkVIXBnukaOnBnripmtIDVpJh0OvEftOSQ2yQ9MJZ_xAvBUaO-1QnrK3h9x9aZt9KPdvS7W51LBCoGmw0UW9O6glxR87yqudQvY0jm6muMsWtEItyhXwGPhA7-IuzeUNVoCAliO2pqizg_Ip5pxosEsKk0u_LXC7H4YFexxGsW-Oibtuov5B_v39At4fwL6-W0Oc_5v2T_wzpkdol36QfwAJHZ7G</recordid><startdate>20161101</startdate><enddate>20161101</enddate><creator>Netepenko, A.</creator><creator>Boeglin, W. U.</creator><creator>Darrow, D. S.</creator><creator>Ellis, R.</creator><creator>Sibilia, M. J.</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>20161101</creationdate><title>Plasma diagnostics in spherical tokamaks with silicon charged-particle detectors</title><author>Netepenko, A. ; Boeglin, W. U. ; Darrow, D. S. ; Ellis, R. ; Sibilia, M. J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c481t-7174e5e0490c505ce61de09b6e4f843a5fd855db43813b59b2a9cfe07285b8a53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Charged particles</topic><topic>Collimation</topic><topic>Collimators</topic><topic>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</topic><topic>DATA ACQUISITION</topic><topic>DIAGRAMS</topic><topic>Electrical noise</topic><topic>HEAVY ION FUSION REACTIONS</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><topic>ION IMPLANTATION</topic><topic>IONS</topic><topic>MAGNETOHYDRODYNAMICS</topic><topic>MEV RANGE 01-10</topic><topic>Neutral beams</topic><topic>NSTX DEVICE</topic><topic>PLASMA DIAGNOSTICS</topic><topic>PROTONS</topic><topic>Radiation counters</topic><topic>REACTION KINETICS</topic><topic>Scientific apparatus &amp; instruments</topic><topic>Sensors</topic><topic>SILICON</topic><topic>SPATIAL DISTRIBUTION</topic><topic>SPHERICAL CONFIGURATION</topic><topic>Spherical plasmas</topic><topic>SURFACE BARRIER DETECTORS</topic><topic>THERMONUCLEAR REACTIONS</topic><topic>TIME DEPENDENCE</topic><topic>TIME RESOLUTION</topic><topic>Tokamak devices</topic><topic>TRITONS</topic><topic>TRITURUS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Netepenko, A.</creatorcontrib><creatorcontrib>Boeglin, W. U.</creatorcontrib><creatorcontrib>Darrow, D. S.</creatorcontrib><creatorcontrib>Ellis, R.</creatorcontrib><creatorcontrib>Sibilia, M. J.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Netepenko, A.</au><au>Boeglin, W. U.</au><au>Darrow, D. S.</au><au>Ellis, R.</au><au>Sibilia, M. J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Plasma diagnostics in spherical tokamaks with silicon charged-particle detectors</atitle><jtitle>Review of scientific instruments</jtitle><addtitle>Rev Sci Instrum</addtitle><date>2016-11-01</date><risdate>2016</risdate><volume>87</volume><issue>11</issue><spage>11D805</spage><epage>11D805</epage><pages>11D805-11D805</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>Detection of charged fusion products, such as protons and tritons resulting from D(d, p) t reactions, can be used to determine the position and time dependent fusion reaction rate profile in spherical tokamak plasmas with neutral beam heating. We have developed a prototype instrument consisting of 6 ion-implanted-silicon surface barrier detectors combined with collimators in such a way that each detector can accept 3 MeV protons and 1 MeV tritons and thus provides a curved view across the plasma cross section. The combination of the results from all six detectors will provide information on the spatial distribution of the fusion reaction rate. The expected time resolution of about 1 ms makes it possible to study changes in the reaction rate due to slow variations in the neutral beam density profile, as well as rapid changes resulting from MHD instabilities. Details of the new instrument, its data acquisition system, simulation results, and electrical noise testing results are discussed in this paper. First experimental data are expected to be taken during the current experimental campaign at NSTX-U.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>27910355</pmid><doi>10.1063/1.4955485</doi><tpages>3</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0034-6748
ispartof Review of scientific instruments, 2016-11, Vol.87 (11), p.11D805-11D805
issn 0034-6748
1089-7623
language eng
recordid cdi_pubmed_primary_27910355
source AIP Journals Complete; Alma/SFX Local Collection
subjects Charged particles
Collimation
Collimators
CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
DATA ACQUISITION
DIAGRAMS
Electrical noise
HEAVY ION FUSION REACTIONS
INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY
ION IMPLANTATION
IONS
MAGNETOHYDRODYNAMICS
MEV RANGE 01-10
Neutral beams
NSTX DEVICE
PLASMA DIAGNOSTICS
PROTONS
Radiation counters
REACTION KINETICS
Scientific apparatus & instruments
Sensors
SILICON
SPATIAL DISTRIBUTION
SPHERICAL CONFIGURATION
Spherical plasmas
SURFACE BARRIER DETECTORS
THERMONUCLEAR REACTIONS
TIME DEPENDENCE
TIME RESOLUTION
Tokamak devices
TRITONS
TRITURUS
title Plasma diagnostics in spherical tokamaks with silicon charged-particle detectors
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-08T06%3A39%3A05IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_pubme&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Plasma%20diagnostics%20in%20spherical%20tokamaks%20with%20silicon%20charged-particle%20detectors&rft.jtitle=Review%20of%20scientific%20instruments&rft.au=Netepenko,%20A.&rft.date=2016-11-01&rft.volume=87&rft.issue=11&rft.spage=11D805&rft.epage=11D805&rft.pages=11D805-11D805&rft.issn=0034-6748&rft.eissn=1089-7623&rft.coden=RSINAK&rft_id=info:doi/10.1063/1.4955485&rft_dat=%3Cproquest_pubme%3E1845828131%3C/proquest_pubme%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2121705579&rft_id=info:pmid/27910355&rfr_iscdi=true