Overview of results from the 2023 DIII-D negative triangularity campaign
Negative triangularity (NT) is a potentially transformative configuration for tokamak-based fusion energy with its high-performance core, edge localized mode (ELM)-free edge, and low-field-side divertors that could readily scale to an integrated reactor solution. Previous NT work on the TCV and DIII...
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Veröffentlicht in: | Plasma physics and controlled fusion 2024-10, Vol.66 (10), p.105018 |
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creator | Thome, K E Austin, M E Hyatt, A Marinoni, A Nelson, A O Paz-Soldan, C Scotti, F Boyes, W Casali, L Chrystal, C Ding, S Du, X D Eldon, D Ernst, D Hong, R McKee, G R Mordijck, S Sauter, O Schmitz, L Barr, J L Burke, M G Coda, S Cote, T B Fenstermacher, M E Garofalo, A Khabanov, F O Kramer, G J Lasnier, C J Logan, N C Lunia, P McLean, A G Okabayashi, M Shiraki, D Stewart, S Takemura, Y Truong, D D Osborne, T Van Zeeland, M A Victor, B S Wang, H Q Watkins, J G Wehner, W P Welander, A S Wilks, T M Yang, J Yu, G Zeng, L |
description | Negative triangularity (NT) is a potentially transformative configuration for tokamak-based fusion energy with its high-performance core, edge localized mode (ELM)-free edge, and low-field-side divertors that could readily scale to an integrated reactor solution. Previous NT work on the TCV and DIII-D tokamaks motivated the installation of graphite-tile armor on the low-field-side lower outer wall of DIII-D. A dedicated multiple-week experimental campaign was conducted to qualify the NT scenario for future reactors. During the DIII-D NT campaign, high confinement (
H
98
y
,
2
≳
1), high current (
q
95
<
3), and high normalized pressure plasmas (
β
N
>
2.5) were simultaneously attained in strongly NT-shaped discharges with average triangularity
δ
avg
= −0.5 that were stably controlled. Experiments covered a wide range of DIII-D operational space (plasma current, toroidal field, electron density and pressure) and did not trigger an ELM in a single discharge as long as sufficiently strong NT was maintained; in contrast, to other high-performance ELM-suppression scenarios that have narrower operating windows. These strong NT plasmas had a lower outer divertor X-point shape and maintained a non-ELMing edge with an electron temperature pedestal, exceeding that of typical L-mode plasmas. Also, the following was achieved during the campaign: high normalized density (
n
e
/
n
GW
of at least 1.7), particle confinement comparable to energy confinement with
Z
eff
∼
2
, a detached divertor without impurity seeding, and a mantle radiation scenario using extrinsic impurities. These results are promising for a NT fusion pilot plant but further questions on confinement extrapolation and core-edge integration remain, which motivate future NT studies on DIII-D and beyond. |
doi_str_mv | 10.1088/1361-6587/ad6f40 |
format | Article |
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H
98
y
,
2
≳
1), high current (
q
95
<
3), and high normalized pressure plasmas (
β
N
>
2.5) were simultaneously attained in strongly NT-shaped discharges with average triangularity
δ
avg
= −0.5 that were stably controlled. Experiments covered a wide range of DIII-D operational space (plasma current, toroidal field, electron density and pressure) and did not trigger an ELM in a single discharge as long as sufficiently strong NT was maintained; in contrast, to other high-performance ELM-suppression scenarios that have narrower operating windows. These strong NT plasmas had a lower outer divertor X-point shape and maintained a non-ELMing edge with an electron temperature pedestal, exceeding that of typical L-mode plasmas. Also, the following was achieved during the campaign: high normalized density (
n
e
/
n
GW
of at least 1.7), particle confinement comparable to energy confinement with
Z
eff
∼
2
, a detached divertor without impurity seeding, and a mantle radiation scenario using extrinsic impurities. These results are promising for a NT fusion pilot plant but further questions on confinement extrapolation and core-edge integration remain, which motivate future NT studies on DIII-D and beyond.</description><identifier>ISSN: 0741-3335</identifier><identifier>EISSN: 1361-6587</identifier><identifier>DOI: 10.1088/1361-6587/ad6f40</identifier><identifier>CODEN: PLPHBZ</identifier><language>eng</language><publisher>United States: IOP Publishing</publisher><subject>confinement ; negative triangularity ; NT edge</subject><ispartof>Plasma physics and controlled fusion, 2024-10, Vol.66 (10), p.105018</ispartof><rights>2024 The Author(s). Published by IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c232t-692772c9c826c194c791033293d752d25c6607429bcdaf2f91681340c846f5de3</cites><orcidid>0000-0002-9612-1936 ; 0000-0002-1251-2922 ; 0000-0001-8537-4383 ; 0000-0001-6127-2825 ; 0000-0002-9577-2809 ; 0000-0003-1920-2799 ; 0000-0002-0196-9919 ; 0000-0001-7619-3724 ; 0000-0002-1452-6949 ; 0000-0002-0697-4397 ; 0000-0003-4750-8015 ; 0000-0002-8010-4971 ; 0000-0002-0099-6675 ; 0000-0003-1895-0648 ; 0000-0002-9675-678X ; 0000-0001-5069-4934 ; 0000-0002-1930-0439 ; 0000-0002-4801-3922 ; 0000-0002-8244-2448 ; 0000-0002-0017-8605 ; 0000-0003-1346-0914 ; 0000-0001-7768-5931 ; 0000-0003-2641-4597 ; 0000-0003-3049-8658 ; 0000-0002-2754-9816 ; 0000-0002-6020-7113 ; 0000-0003-3754-897X ; 0009-0005-5063-7047 ; 0000-0002-6930-4702 ; 0000-0002-0002-5342 ; 0000-0001-5105-8139 ; 0000-0002-9146-1544 ; 0000-0002-7911-2739 ; 0000-0003-3384-5280 ; 0000-0002-8573-2539 ; 0000-0003-1004-5782 ; 0000-0001-8422-8464 ; 0000-0002-7109-2278 ; 0000-0002-3268-7359 ; 0000-0001-5635-7330 ; 0000-0003-2924-3674 ; 0000000319202799 ; 0000000310045782 ; 0000000347508015 ; 0000000296121936 ; 0000000232687359 ; 0000000313460914 ; 0000000330498658 ; 0000000329243674 ; 0000000150694934 ; 0000000326414597 ; 0000000212512922 ; 0000000161272825 ; 000000033754897X ; 0000000318950648 ; 0000000227549816 ; 0000000248013922 ; 0000000200996675 ; 0000000200025342 ; 0000000260207113 ; 0000000291461544 ; 0000000280104971 ; 0000000156357330 ; 0000000151058139 ; 0000000282442448 ; 0000000219300439 ; 0000000177685931 ; 0000000271092278 ; 0000000269304702 ; 0000000279112739 ; 0000000184228464</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1361-6587/ad6f40/pdf$$EPDF$$P50$$Giop$$Hfree_for_read</linktopdf><link.rule.ids>230,314,777,781,882,27905,27906,53827,53874</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/2432530$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Thome, K E</creatorcontrib><creatorcontrib>Austin, M E</creatorcontrib><creatorcontrib>Hyatt, A</creatorcontrib><creatorcontrib>Marinoni, A</creatorcontrib><creatorcontrib>Nelson, A O</creatorcontrib><creatorcontrib>Paz-Soldan, C</creatorcontrib><creatorcontrib>Scotti, F</creatorcontrib><creatorcontrib>Boyes, W</creatorcontrib><creatorcontrib>Casali, L</creatorcontrib><creatorcontrib>Chrystal, C</creatorcontrib><creatorcontrib>Ding, S</creatorcontrib><creatorcontrib>Du, X D</creatorcontrib><creatorcontrib>Eldon, D</creatorcontrib><creatorcontrib>Ernst, D</creatorcontrib><creatorcontrib>Hong, R</creatorcontrib><creatorcontrib>McKee, G R</creatorcontrib><creatorcontrib>Mordijck, S</creatorcontrib><creatorcontrib>Sauter, O</creatorcontrib><creatorcontrib>Schmitz, L</creatorcontrib><creatorcontrib>Barr, J L</creatorcontrib><creatorcontrib>Burke, M G</creatorcontrib><creatorcontrib>Coda, S</creatorcontrib><creatorcontrib>Cote, T B</creatorcontrib><creatorcontrib>Fenstermacher, M E</creatorcontrib><creatorcontrib>Garofalo, A</creatorcontrib><creatorcontrib>Khabanov, F O</creatorcontrib><creatorcontrib>Kramer, G J</creatorcontrib><creatorcontrib>Lasnier, C J</creatorcontrib><creatorcontrib>Logan, N C</creatorcontrib><creatorcontrib>Lunia, P</creatorcontrib><creatorcontrib>McLean, A G</creatorcontrib><creatorcontrib>Okabayashi, M</creatorcontrib><creatorcontrib>Shiraki, D</creatorcontrib><creatorcontrib>Stewart, S</creatorcontrib><creatorcontrib>Takemura, Y</creatorcontrib><creatorcontrib>Truong, D D</creatorcontrib><creatorcontrib>Osborne, T</creatorcontrib><creatorcontrib>Van Zeeland, M A</creatorcontrib><creatorcontrib>Victor, B S</creatorcontrib><creatorcontrib>Wang, H Q</creatorcontrib><creatorcontrib>Watkins, J G</creatorcontrib><creatorcontrib>Wehner, W P</creatorcontrib><creatorcontrib>Welander, A S</creatorcontrib><creatorcontrib>Wilks, T M</creatorcontrib><creatorcontrib>Yang, J</creatorcontrib><creatorcontrib>Yu, G</creatorcontrib><creatorcontrib>Zeng, L</creatorcontrib><creatorcontrib>the DIII-D Team</creatorcontrib><creatorcontrib>Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)</creatorcontrib><creatorcontrib>General Atomics, San Diego, CA (United States)</creatorcontrib><title>Overview of results from the 2023 DIII-D negative triangularity campaign</title><title>Plasma physics and controlled fusion</title><addtitle>PPCF</addtitle><addtitle>Plasma Phys. Control. Fusion</addtitle><description>Negative triangularity (NT) is a potentially transformative configuration for tokamak-based fusion energy with its high-performance core, edge localized mode (ELM)-free edge, and low-field-side divertors that could readily scale to an integrated reactor solution. Previous NT work on the TCV and DIII-D tokamaks motivated the installation of graphite-tile armor on the low-field-side lower outer wall of DIII-D. A dedicated multiple-week experimental campaign was conducted to qualify the NT scenario for future reactors. During the DIII-D NT campaign, high confinement (
H
98
y
,
2
≳
1), high current (
q
95
<
3), and high normalized pressure plasmas (
β
N
>
2.5) were simultaneously attained in strongly NT-shaped discharges with average triangularity
δ
avg
= −0.5 that were stably controlled. Experiments covered a wide range of DIII-D operational space (plasma current, toroidal field, electron density and pressure) and did not trigger an ELM in a single discharge as long as sufficiently strong NT was maintained; in contrast, to other high-performance ELM-suppression scenarios that have narrower operating windows. These strong NT plasmas had a lower outer divertor X-point shape and maintained a non-ELMing edge with an electron temperature pedestal, exceeding that of typical L-mode plasmas. Also, the following was achieved during the campaign: high normalized density (
n
e
/
n
GW
of at least 1.7), particle confinement comparable to energy confinement with
Z
eff
∼
2
, a detached divertor without impurity seeding, and a mantle radiation scenario using extrinsic impurities. These results are promising for a NT fusion pilot plant but further questions on confinement extrapolation and core-edge integration remain, which motivate future NT studies on DIII-D and beyond.</description><subject>confinement</subject><subject>negative triangularity</subject><subject>NT edge</subject><issn>0741-3335</issn><issn>1361-6587</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><recordid>eNp1kM9PwjAUxxujiYjePTaenbSvW7cdDYgsIeGi56a-tVACK2kLhv_ekRlvnl7y8vm-Hx9CHjl74ayqJlxInsmiKie6lTZnV2T017omI1bmPBNCFLfkLsYtY5xXIEdksTqZcHLmm3pLg4nHXYrUBr-naWMoMBB01jRNNqOdWevkToam4HS3Pu50cOlMUe8P2q27e3Jj9S6ah986Jp_zt4_pIluu3pvp6zJDEJAyWUNZAtbYb0de51jWnAkBtWjLAlooUMr-Vqi_sNUWbM1lxUXOsMqlLVojxuRpmOtjciqiSwY36LvOYFKQCygE6yE2QBh8jMFYdQhur8NZcaYuutTFjbq4UYOuPvI8RJw_qK0_hq7_4n_8B2u9aOk</recordid><startdate>20241001</startdate><enddate>20241001</enddate><creator>Thome, K E</creator><creator>Austin, M 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of results from the 2023 DIII-D negative triangularity campaign</title><author>Thome, K E ; Austin, M E ; Hyatt, A ; Marinoni, A ; Nelson, A O ; Paz-Soldan, C ; Scotti, F ; Boyes, W ; Casali, L ; Chrystal, C ; Ding, S ; Du, X D ; Eldon, D ; Ernst, D ; Hong, R ; McKee, G R ; Mordijck, S ; Sauter, O ; Schmitz, L ; Barr, J L ; Burke, M G ; Coda, S ; Cote, T B ; Fenstermacher, M E ; Garofalo, A ; Khabanov, F O ; Kramer, G J ; Lasnier, C J ; Logan, N C ; Lunia, P ; McLean, A G ; Okabayashi, M ; Shiraki, D ; Stewart, S ; Takemura, Y ; Truong, D D ; Osborne, T ; Van Zeeland, M A ; Victor, B S ; Wang, H Q ; Watkins, J G ; Wehner, W P ; Welander, A S ; Wilks, T M ; Yang, J ; Yu, G ; Zeng, L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c232t-692772c9c826c194c791033293d752d25c6607429bcdaf2f91681340c846f5de3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>confinement</topic><topic>negative triangularity</topic><topic>NT edge</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Thome, K E</creatorcontrib><creatorcontrib>Austin, M E</creatorcontrib><creatorcontrib>Hyatt, A</creatorcontrib><creatorcontrib>Marinoni, A</creatorcontrib><creatorcontrib>Nelson, A O</creatorcontrib><creatorcontrib>Paz-Soldan, C</creatorcontrib><creatorcontrib>Scotti, F</creatorcontrib><creatorcontrib>Boyes, W</creatorcontrib><creatorcontrib>Casali, L</creatorcontrib><creatorcontrib>Chrystal, C</creatorcontrib><creatorcontrib>Ding, S</creatorcontrib><creatorcontrib>Du, X D</creatorcontrib><creatorcontrib>Eldon, D</creatorcontrib><creatorcontrib>Ernst, D</creatorcontrib><creatorcontrib>Hong, R</creatorcontrib><creatorcontrib>McKee, G R</creatorcontrib><creatorcontrib>Mordijck, S</creatorcontrib><creatorcontrib>Sauter, O</creatorcontrib><creatorcontrib>Schmitz, L</creatorcontrib><creatorcontrib>Barr, J L</creatorcontrib><creatorcontrib>Burke, M G</creatorcontrib><creatorcontrib>Coda, S</creatorcontrib><creatorcontrib>Cote, T B</creatorcontrib><creatorcontrib>Fenstermacher, M E</creatorcontrib><creatorcontrib>Garofalo, A</creatorcontrib><creatorcontrib>Khabanov, F O</creatorcontrib><creatorcontrib>Kramer, G J</creatorcontrib><creatorcontrib>Lasnier, C J</creatorcontrib><creatorcontrib>Logan, N C</creatorcontrib><creatorcontrib>Lunia, P</creatorcontrib><creatorcontrib>McLean, A G</creatorcontrib><creatorcontrib>Okabayashi, M</creatorcontrib><creatorcontrib>Shiraki, D</creatorcontrib><creatorcontrib>Stewart, S</creatorcontrib><creatorcontrib>Takemura, Y</creatorcontrib><creatorcontrib>Truong, D D</creatorcontrib><creatorcontrib>Osborne, T</creatorcontrib><creatorcontrib>Van Zeeland, M A</creatorcontrib><creatorcontrib>Victor, B S</creatorcontrib><creatorcontrib>Wang, H Q</creatorcontrib><creatorcontrib>Watkins, J G</creatorcontrib><creatorcontrib>Wehner, W P</creatorcontrib><creatorcontrib>Welander, A S</creatorcontrib><creatorcontrib>Wilks, T M</creatorcontrib><creatorcontrib>Yang, J</creatorcontrib><creatorcontrib>Yu, G</creatorcontrib><creatorcontrib>Zeng, L</creatorcontrib><creatorcontrib>the DIII-D Team</creatorcontrib><creatorcontrib>Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)</creatorcontrib><creatorcontrib>General Atomics, San Diego, CA (United States)</creatorcontrib><collection>IOP Publishing Free Content</collection><collection>IOPscience (Open Access)</collection><collection>CrossRef</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Plasma physics and controlled fusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Thome, K E</au><au>Austin, M E</au><au>Hyatt, A</au><au>Marinoni, A</au><au>Nelson, A O</au><au>Paz-Soldan, C</au><au>Scotti, F</au><au>Boyes, W</au><au>Casali, L</au><au>Chrystal, C</au><au>Ding, S</au><au>Du, X D</au><au>Eldon, D</au><au>Ernst, D</au><au>Hong, R</au><au>McKee, G R</au><au>Mordijck, S</au><au>Sauter, O</au><au>Schmitz, L</au><au>Barr, J L</au><au>Burke, M G</au><au>Coda, S</au><au>Cote, T B</au><au>Fenstermacher, M E</au><au>Garofalo, A</au><au>Khabanov, F O</au><au>Kramer, G J</au><au>Lasnier, C J</au><au>Logan, N C</au><au>Lunia, P</au><au>McLean, A G</au><au>Okabayashi, M</au><au>Shiraki, D</au><au>Stewart, S</au><au>Takemura, Y</au><au>Truong, D D</au><au>Osborne, T</au><au>Van Zeeland, M A</au><au>Victor, B S</au><au>Wang, H Q</au><au>Watkins, J G</au><au>Wehner, W P</au><au>Welander, A S</au><au>Wilks, T M</au><au>Yang, J</au><au>Yu, G</au><au>Zeng, L</au><aucorp>the DIII-D Team</aucorp><aucorp>Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)</aucorp><aucorp>General Atomics, San Diego, CA (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Overview of results from the 2023 DIII-D negative triangularity campaign</atitle><jtitle>Plasma physics and controlled fusion</jtitle><stitle>PPCF</stitle><addtitle>Plasma Phys. Control. Fusion</addtitle><date>2024-10-01</date><risdate>2024</risdate><volume>66</volume><issue>10</issue><spage>105018</spage><pages>105018-</pages><issn>0741-3335</issn><eissn>1361-6587</eissn><coden>PLPHBZ</coden><abstract>Negative triangularity (NT) is a potentially transformative configuration for tokamak-based fusion energy with its high-performance core, edge localized mode (ELM)-free edge, and low-field-side divertors that could readily scale to an integrated reactor solution. Previous NT work on the TCV and DIII-D tokamaks motivated the installation of graphite-tile armor on the low-field-side lower outer wall of DIII-D. A dedicated multiple-week experimental campaign was conducted to qualify the NT scenario for future reactors. During the DIII-D NT campaign, high confinement (
H
98
y
,
2
≳
1), high current (
q
95
<
3), and high normalized pressure plasmas (
β
N
>
2.5) were simultaneously attained in strongly NT-shaped discharges with average triangularity
δ
avg
= −0.5 that were stably controlled. Experiments covered a wide range of DIII-D operational space (plasma current, toroidal field, electron density and pressure) and did not trigger an ELM in a single discharge as long as sufficiently strong NT was maintained; in contrast, to other high-performance ELM-suppression scenarios that have narrower operating windows. These strong NT plasmas had a lower outer divertor X-point shape and maintained a non-ELMing edge with an electron temperature pedestal, exceeding that of typical L-mode plasmas. Also, the following was achieved during the campaign: high normalized density (
n
e
/
n
GW
of at least 1.7), particle confinement comparable to energy confinement with
Z
eff
∼
2
, a detached divertor without impurity seeding, and a mantle radiation scenario using extrinsic impurities. These results are promising for a NT fusion pilot plant but further questions on confinement extrapolation and core-edge integration remain, which motivate future NT studies on DIII-D and beyond.</abstract><cop>United States</cop><pub>IOP Publishing</pub><doi>10.1088/1361-6587/ad6f40</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-9612-1936</orcidid><orcidid>https://orcid.org/0000-0002-1251-2922</orcidid><orcidid>https://orcid.org/0000-0001-8537-4383</orcidid><orcidid>https://orcid.org/0000-0001-6127-2825</orcidid><orcidid>https://orcid.org/0000-0002-9577-2809</orcidid><orcidid>https://orcid.org/0000-0003-1920-2799</orcidid><orcidid>https://orcid.org/0000-0002-0196-9919</orcidid><orcidid>https://orcid.org/0000-0001-7619-3724</orcidid><orcidid>https://orcid.org/0000-0002-1452-6949</orcidid><orcidid>https://orcid.org/0000-0002-0697-4397</orcidid><orcidid>https://orcid.org/0000-0003-4750-8015</orcidid><orcidid>https://orcid.org/0000-0002-8010-4971</orcidid><orcidid>https://orcid.org/0000-0002-0099-6675</orcidid><orcidid>https://orcid.org/0000-0003-1895-0648</orcidid><orcidid>https://orcid.org/0000-0002-9675-678X</orcidid><orcidid>https://orcid.org/0000-0001-5069-4934</orcidid><orcidid>https://orcid.org/0000-0002-1930-0439</orcidid><orcidid>https://orcid.org/0000-0002-4801-3922</orcidid><orcidid>https://orcid.org/0000-0002-8244-2448</orcidid><orcidid>https://orcid.org/0000-0002-0017-8605</orcidid><orcidid>https://orcid.org/0000-0003-1346-0914</orcidid><orcidid>https://orcid.org/0000-0001-7768-5931</orcidid><orcidid>https://orcid.org/0000-0003-2641-4597</orcidid><orcidid>https://orcid.org/0000-0003-3049-8658</orcidid><orcidid>https://orcid.org/0000-0002-2754-9816</orcidid><orcidid>https://orcid.org/0000-0002-6020-7113</orcidid><orcidid>https://orcid.org/0000-0003-3754-897X</orcidid><orcidid>https://orcid.org/0009-0005-5063-7047</orcidid><orcidid>https://orcid.org/0000-0002-6930-4702</orcidid><orcidid>https://orcid.org/0000-0002-0002-5342</orcidid><orcidid>https://orcid.org/0000-0001-5105-8139</orcidid><orcidid>https://orcid.org/0000-0002-9146-1544</orcidid><orcidid>https://orcid.org/0000-0002-7911-2739</orcidid><orcidid>https://orcid.org/0000-0003-3384-5280</orcidid><orcidid>https://orcid.org/0000-0002-8573-2539</orcidid><orcidid>https://orcid.org/0000-0003-1004-5782</orcidid><orcidid>https://orcid.org/0000-0001-8422-8464</orcidid><orcidid>https://orcid.org/0000-0002-7109-2278</orcidid><orcidid>https://orcid.org/0000-0002-3268-7359</orcidid><orcidid>https://orcid.org/0000-0001-5635-7330</orcidid><orcidid>https://orcid.org/0000-0003-2924-3674</orcidid><orcidid>https://orcid.org/0000000319202799</orcidid><orcidid>https://orcid.org/0000000310045782</orcidid><orcidid>https://orcid.org/0000000347508015</orcidid><orcidid>https://orcid.org/0000000296121936</orcidid><orcidid>https://orcid.org/0000000232687359</orcidid><orcidid>https://orcid.org/0000000313460914</orcidid><orcidid>https://orcid.org/0000000330498658</orcidid><orcidid>https://orcid.org/0000000329243674</orcidid><orcidid>https://orcid.org/0000000150694934</orcidid><orcidid>https://orcid.org/0000000326414597</orcidid><orcidid>https://orcid.org/0000000212512922</orcidid><orcidid>https://orcid.org/0000000161272825</orcidid><orcidid>https://orcid.org/000000033754897X</orcidid><orcidid>https://orcid.org/0000000318950648</orcidid><orcidid>https://orcid.org/0000000227549816</orcidid><orcidid>https://orcid.org/0000000248013922</orcidid><orcidid>https://orcid.org/0000000200996675</orcidid><orcidid>https://orcid.org/0000000200025342</orcidid><orcidid>https://orcid.org/0000000260207113</orcidid><orcidid>https://orcid.org/0000000291461544</orcidid><orcidid>https://orcid.org/0000000280104971</orcidid><orcidid>https://orcid.org/0000000156357330</orcidid><orcidid>https://orcid.org/0000000151058139</orcidid><orcidid>https://orcid.org/0000000282442448</orcidid><orcidid>https://orcid.org/0000000219300439</orcidid><orcidid>https://orcid.org/0000000177685931</orcidid><orcidid>https://orcid.org/0000000271092278</orcidid><orcidid>https://orcid.org/0000000269304702</orcidid><orcidid>https://orcid.org/0000000279112739</orcidid><orcidid>https://orcid.org/0000000184228464</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0741-3335 |
ispartof | Plasma physics and controlled fusion, 2024-10, Vol.66 (10), p.105018 |
issn | 0741-3335 1361-6587 |
language | eng |
recordid | cdi_iop_journals_10_1088_1361_6587_ad6f40 |
source | IOP Publishing Journals; Institute of Physics (IOP) Journals - HEAL-Link |
subjects | confinement negative triangularity NT edge |
title | Overview of results from the 2023 DIII-D negative triangularity campaign |
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