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Electron-scale turbulence characteristics with varying electron temperature gradient in LHD
Electron-scale turbulence, whose wavelength is the electron Larmor radius, is thought to have the potential to cause stiffness in an electron temperature gradient and degrade the confinement of future burning plasma in which the electron heating by alpha particles is dominant. The dependence of elec...
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Published in: | Nuclear fusion 2024-09, Vol.64 (9), p.96008 |
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creator | Nasu, T. Tokuzawa, T. Nakata, M. Ida, K. Inagaki, S. Nishiura, M. Yoshimura, Y. Yanai, R. Tanaka, K. Yoshinuma, M. Kobayashi, T. Ejiri, A. Watanabe, K.Y. Yamada, I. |
description | Electron-scale turbulence, whose wavelength is the electron Larmor radius, is thought to have the potential to cause stiffness in an electron temperature gradient and degrade the confinement of future burning plasma in which the electron heating by alpha particles is dominant. The dependence of electron-scale turbulence and electron heat flux on the electron temperature inverse gradient length R ax / L T e , were investigated. The electron temperature gradient was successfully varied in the range of − 3 < R ax / L T e < 12 by controlling the injection power of on/off-axis electron cyclotron heating. The results show a significant increase in the electron-scale turbulence with increasing R ax / L T e , especially in conditions where Electron Temperature Gradient (ETG) instability is linearly unstable, suggesting the presence of ETG turbulence at high R ax / L T e . The electron heat flux also increases steeply with increasing R ax / L T e . In addition, the electron-scale turbulence is observed even at R ax / L T e ∼ 0 , which is stable in linear GKV calculations. Finding the cause of this phenomenon is an interesting task for the future. |
doi_str_mv | 10.1088/1741-4326/ad5d7c |
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The dependence of electron-scale turbulence and electron heat flux on the electron temperature inverse gradient length R ax / L T e , were investigated. The electron temperature gradient was successfully varied in the range of − 3 < R ax / L T e < 12 by controlling the injection power of on/off-axis electron cyclotron heating. The results show a significant increase in the electron-scale turbulence with increasing R ax / L T e , especially in conditions where Electron Temperature Gradient (ETG) instability is linearly unstable, suggesting the presence of ETG turbulence at high R ax / L T e . The electron heat flux also increases steeply with increasing R ax / L T e . In addition, the electron-scale turbulence is observed even at R ax / L T e ∼ 0 , which is stable in linear GKV calculations. Finding the cause of this phenomenon is an interesting task for the future.</description><identifier>ISSN: 0029-5515</identifier><identifier>EISSN: 1741-4326</identifier><identifier>DOI: 10.1088/1741-4326/ad5d7c</identifier><identifier>CODEN: NUFUAU</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>fusion plasma ; magnetic confinement ; stiffness ; turbulence</subject><ispartof>Nuclear fusion, 2024-09, Vol.64 (9), p.96008</ispartof><rights>2024 The Author(s). 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Fusion</addtitle><description>Electron-scale turbulence, whose wavelength is the electron Larmor radius, is thought to have the potential to cause stiffness in an electron temperature gradient and degrade the confinement of future burning plasma in which the electron heating by alpha particles is dominant. The dependence of electron-scale turbulence and electron heat flux on the electron temperature inverse gradient length R ax / L T e , were investigated. The electron temperature gradient was successfully varied in the range of − 3 < R ax / L T e < 12 by controlling the injection power of on/off-axis electron cyclotron heating. The results show a significant increase in the electron-scale turbulence with increasing R ax / L T e , especially in conditions where Electron Temperature Gradient (ETG) instability is linearly unstable, suggesting the presence of ETG turbulence at high R ax / L T e . The electron heat flux also increases steeply with increasing R ax / L T e . In addition, the electron-scale turbulence is observed even at R ax / L T e ∼ 0 , which is stable in linear GKV calculations. Finding the cause of this phenomenon is an interesting task for the future.</description><subject>fusion plasma</subject><subject>magnetic confinement</subject><subject>stiffness</subject><subject>turbulence</subject><issn>0029-5515</issn><issn>1741-4326</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>DOA</sourceid><recordid>eNp9kD1PwzAYhC0EEqWwM3piItTfdkZUCq1UiQUmBsvxR-sqTSI7BfHvSWnVCTG90ume03sHwC1GDxgpNcGS4YJRIibGcSftGRidpHMwQoiUBeeYX4KrnDcIYYYpHYGPWe1tn9qmyNbUHva7VO1q31gP7dokY3ufYu6jzfAr9mv4adJ3bFbQHzHY-23nkxk4D1fJuOibHsYGLudP1-AimDr7m-Mdg_fn2dt0XixfXxbTx2VhKRN94VRFmJQYocoGSx0TFCtMjWR2OCV1plQCc0lcUIY44oMjoeSKMKokkYKOweKQ61qz0V2K2-FJ3Zqof4U2rbRJQ4Xaa-RVoKEMjJCKCcRUxR1yWBHJLXOKD1nokGVTm3Py4ZSHkd4Prfer6v2q-jD0gNwfkNh2etPuUjOU_c9-94e9CVowXWpUCoSU7lygP7IEjFs</recordid><startdate>20240901</startdate><enddate>20240901</enddate><creator>Nasu, T.</creator><creator>Tokuzawa, T.</creator><creator>Nakata, M.</creator><creator>Ida, K.</creator><creator>Inagaki, S.</creator><creator>Nishiura, M.</creator><creator>Yoshimura, Y.</creator><creator>Yanai, R.</creator><creator>Tanaka, K.</creator><creator>Yoshinuma, M.</creator><creator>Kobayashi, T.</creator><creator>Ejiri, A.</creator><creator>Watanabe, K.Y.</creator><creator>Yamada, I.</creator><general>IOP Publishing</general><scope>O3W</scope><scope>TSCCA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0003-2693-4859</orcidid><orcidid>https://orcid.org/0000-0002-7023-1539</orcidid><orcidid>https://orcid.org/0000-0001-5473-2109</orcidid><orcidid>https://orcid.org/0000-0002-4808-857X</orcidid><orcidid>https://orcid.org/0000-0002-0585-4561</orcidid><orcidid>https://orcid.org/0000-0001-5669-1937</orcidid><orcidid>https://orcid.org/0000-0002-9172-7381</orcidid><orcidid>https://orcid.org/0000-0001-6744-1829</orcidid><orcidid>https://orcid.org/0000-0002-4486-7437</orcidid></search><sort><creationdate>20240901</creationdate><title>Electron-scale turbulence characteristics with varying electron temperature gradient in LHD</title><author>Nasu, T. ; Tokuzawa, T. ; Nakata, M. ; Ida, K. ; Inagaki, S. ; Nishiura, M. ; Yoshimura, Y. ; Yanai, R. ; Tanaka, K. ; Yoshinuma, M. ; Kobayashi, T. ; Ejiri, A. ; Watanabe, K.Y. ; Yamada, I.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c346t-d8b2477100bcfc3d4631813a74c81393da9861572df8a2d2efd2f958243872763</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>fusion plasma</topic><topic>magnetic confinement</topic><topic>stiffness</topic><topic>turbulence</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nasu, T.</creatorcontrib><creatorcontrib>Tokuzawa, T.</creatorcontrib><creatorcontrib>Nakata, M.</creatorcontrib><creatorcontrib>Ida, K.</creatorcontrib><creatorcontrib>Inagaki, S.</creatorcontrib><creatorcontrib>Nishiura, M.</creatorcontrib><creatorcontrib>Yoshimura, Y.</creatorcontrib><creatorcontrib>Yanai, R.</creatorcontrib><creatorcontrib>Tanaka, K.</creatorcontrib><creatorcontrib>Yoshinuma, M.</creatorcontrib><creatorcontrib>Kobayashi, T.</creatorcontrib><creatorcontrib>Ejiri, A.</creatorcontrib><creatorcontrib>Watanabe, K.Y.</creatorcontrib><creatorcontrib>Yamada, I.</creatorcontrib><creatorcontrib>LHD Experiment Group</creatorcontrib><collection>IOP Publishing</collection><collection>IOPscience (Open Access)</collection><collection>CrossRef</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>Nuclear fusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nasu, T.</au><au>Tokuzawa, T.</au><au>Nakata, M.</au><au>Ida, K.</au><au>Inagaki, S.</au><au>Nishiura, M.</au><au>Yoshimura, Y.</au><au>Yanai, R.</au><au>Tanaka, K.</au><au>Yoshinuma, M.</au><au>Kobayashi, T.</au><au>Ejiri, A.</au><au>Watanabe, K.Y.</au><au>Yamada, I.</au><aucorp>LHD Experiment Group</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electron-scale turbulence characteristics with varying electron temperature gradient in LHD</atitle><jtitle>Nuclear fusion</jtitle><stitle>NF</stitle><addtitle>Nucl. Fusion</addtitle><date>2024-09-01</date><risdate>2024</risdate><volume>64</volume><issue>9</issue><spage>96008</spage><pages>96008-</pages><issn>0029-5515</issn><eissn>1741-4326</eissn><coden>NUFUAU</coden><abstract>Electron-scale turbulence, whose wavelength is the electron Larmor radius, is thought to have the potential to cause stiffness in an electron temperature gradient and degrade the confinement of future burning plasma in which the electron heating by alpha particles is dominant. The dependence of electron-scale turbulence and electron heat flux on the electron temperature inverse gradient length R ax / L T e , were investigated. The electron temperature gradient was successfully varied in the range of − 3 < R ax / L T e < 12 by controlling the injection power of on/off-axis electron cyclotron heating. The results show a significant increase in the electron-scale turbulence with increasing R ax / L T e , especially in conditions where Electron Temperature Gradient (ETG) instability is linearly unstable, suggesting the presence of ETG turbulence at high R ax / L T e . The electron heat flux also increases steeply with increasing R ax / L T e . In addition, the electron-scale turbulence is observed even at R ax / L T e ∼ 0 , which is stable in linear GKV calculations. 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title | Electron-scale turbulence characteristics with varying electron temperature gradient in LHD |
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