Suppression of toroidal Alfvén eigenmodes by the electron cyclotron current drive in KSTAR plasmas
Advanced operation scenarios such as high poloidal beta ( β P ) or high q min are promising concepts to achieve the steady-state high-performance fusion plasmas. However, those scenarios are prone to substantial Alfvénic activity, causing fast-ion transport and losses. Recent experiments with the ad...
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creator | Kim, J. Kang, J. Rhee, T. Jo, J. Han, H. Podestà, M. Lee, J.H. Lee, S. Bak, J.G. Choi, M.J. Nazikian, R. Jhang, H. Ko, J. Joung, M. Jeon, Y.-M. Na, Y.-S. Shinohara, K. Cheng, C.Z. |
description | Advanced operation scenarios such as high poloidal beta (
β
P
) or high
q
min
are promising concepts to achieve the steady-state high-performance fusion plasmas. However, those scenarios are prone to substantial Alfvénic activity, causing fast-ion transport and losses. Recent experiments with the advanced operation scenario on KSTAR tokamak have shown that the electron cyclotron current drive (ECCD) is able to mitigate and suppress the beam-ion driven toroidal Alfvén eigenmodes (TAEs) for over several tens of global energy confinement time. Co-current directional intermediate off-axis ECCD lowers the central safety factor slightly and tilts the central
q
-profile shape so that the continuum damping in the core region increases. Besides, the rise of central plasma pressure and increased thermal-ion Landau damping contribute to TAE stabilization. While the TAEs are suppressed, neutron emission rate and total stored energy increase by approximately 45% and 25%, respectively. Fast-ion transport estimated by TRANSP calculations approaches the classical level during the TAE suppression period. Substantial reduction in fast-ion loss and neutron deficit is also observed. Enhancement of fast-ion confinement by suppressing the TAEs leads to an increase of non-inductive current fraction and will benefit the sustainment of the long-pulse high-performance discharges. |
doi_str_mv | 10.1088/1741-4326/ac3e39 |
format | Article |
fullrecord | <record><control><sourceid>iop_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1088_1741_4326_ac3e39</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>nfac3e39</sourcerecordid><originalsourceid>FETCH-LOGICAL-c380t-1c6703e4af39d7b96ebdfa441226b541ec81b1f4d931079b737b6d8c5490c7cd3</originalsourceid><addsrcrecordid>eNp1kE1LxDAQhoMouH7cPQYPnqybadKkPS6LXygI7noObT7cSDcpSXdhf5K_wz9ml4onPc0wPO8w8yB0AeQGSFlOQTDIGM35tFbU0OoATX5Hh2hCSF5lRQHFMTpJ6YMQYEDpBKnFpuuiSckFj4PFfYjB6brFs9Zuvz49Nu7d-HXQJuFmh_uVwaY1qo8DrnaqDWO3idH4HuvotgY7j58Wy9kr7to6ret0ho5s3SZz_lNP0dvd7XL-kD2_3D_OZ8-ZoiXpM1BcEGpYbWmlRVNx02hbMwZ5zpuCgVElNGCZrigQUTWCiobrUhWsIkooTU_R5bg3pN7JpFxv1EoF74d7JZQFh1IMEBkhFUNK0VjZRbeu404CkXuTcq9N7rXJ0eQQuRojLnTyI2yiH76Q3kqey1ySnA9uZaftAF7_Af679xvbAoLw</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Suppression of toroidal Alfvén eigenmodes by the electron cyclotron current drive in KSTAR plasmas</title><source>IOP Publishing Journals</source><source>Institute of Physics (IOP) Journals - HEAL-Link</source><creator>Kim, J. ; Kang, J. ; Rhee, T. ; Jo, J. ; Han, H. ; Podestà, M. ; Lee, J.H. ; Lee, S. ; Bak, J.G. ; Choi, M.J. ; Nazikian, R. ; Jhang, H. ; Ko, J. ; Joung, M. ; Jeon, Y.-M. ; Na, Y.-S. ; Shinohara, K. ; Cheng, C.Z.</creator><creatorcontrib>Kim, J. ; Kang, J. ; Rhee, T. ; Jo, J. ; Han, H. ; Podestà, M. ; Lee, J.H. ; Lee, S. ; Bak, J.G. ; Choi, M.J. ; Nazikian, R. ; Jhang, H. ; Ko, J. ; Joung, M. ; Jeon, Y.-M. ; Na, Y.-S. ; Shinohara, K. ; Cheng, C.Z. ; Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)</creatorcontrib><description>Advanced operation scenarios such as high poloidal beta (
β
P
) or high
q
min
are promising concepts to achieve the steady-state high-performance fusion plasmas. However, those scenarios are prone to substantial Alfvénic activity, causing fast-ion transport and losses. Recent experiments with the advanced operation scenario on KSTAR tokamak have shown that the electron cyclotron current drive (ECCD) is able to mitigate and suppress the beam-ion driven toroidal Alfvén eigenmodes (TAEs) for over several tens of global energy confinement time. Co-current directional intermediate off-axis ECCD lowers the central safety factor slightly and tilts the central
q
-profile shape so that the continuum damping in the core region increases. Besides, the rise of central plasma pressure and increased thermal-ion Landau damping contribute to TAE stabilization. While the TAEs are suppressed, neutron emission rate and total stored energy increase by approximately 45% and 25%, respectively. Fast-ion transport estimated by TRANSP calculations approaches the classical level during the TAE suppression period. Substantial reduction in fast-ion loss and neutron deficit is also observed. Enhancement of fast-ion confinement by suppressing the TAEs leads to an increase of non-inductive current fraction and will benefit the sustainment of the long-pulse high-performance discharges.</description><identifier>ISSN: 0029-5515</identifier><identifier>EISSN: 1741-4326</identifier><identifier>DOI: 10.1088/1741-4326/ac3e39</identifier><identifier>CODEN: NUFUAU</identifier><language>eng</language><publisher>United States: IOP Publishing</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; Alfv´en eigenmode ; Alfvén eigenmode ; ECCD ; energetic particle ; fusion plasma ; KSTAR ; tokamak</subject><ispartof>Nuclear fusion, 2022-02, Vol.62 (2), p.26029</ispartof><rights>2022 IAEA, Vienna</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c380t-1c6703e4af39d7b96ebdfa441226b541ec81b1f4d931079b737b6d8c5490c7cd3</citedby><cites>FETCH-LOGICAL-c380t-1c6703e4af39d7b96ebdfa441226b541ec81b1f4d931079b737b6d8c5490c7cd3</cites><orcidid>0000-0003-1923-8441 ; 0000-0002-7374-3759 ; 0000-0001-7792-3581 ; 0000-0002-5501-3939 ; 0000-0001-6618-7806 ; 0000-0003-0435-2436 ; 0000-0002-2825-6484 ; 0000-0002-1552-0426 ; 0000-0002-9845-4646 ; 0000-0003-4975-0585 ; 0000-0001-6506-9824 ; 0000-0001-7270-3846 ; 0000-0003-2406-4239 ; 0000-0002-0852-8817 ; 0000-0001-6235-6692 ; 0000000166187806 ; 0000000324064239 ; 0000000304352436 ; 0000000255013939 ; 0000000298454646 ; 0000000172703846 ; 0000000165069824 ; 0000000273743759 ; 0000000208528817 ; 0000000228256484 ; 0000000177923581 ; 0000000319238441 ; 0000000162356692 ; 0000000349750585 ; 0000000215520426</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1741-4326/ac3e39/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>230,314,776,780,881,27901,27902,53821,53868</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/1856187$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Kim, J.</creatorcontrib><creatorcontrib>Kang, J.</creatorcontrib><creatorcontrib>Rhee, T.</creatorcontrib><creatorcontrib>Jo, J.</creatorcontrib><creatorcontrib>Han, H.</creatorcontrib><creatorcontrib>Podestà, M.</creatorcontrib><creatorcontrib>Lee, J.H.</creatorcontrib><creatorcontrib>Lee, S.</creatorcontrib><creatorcontrib>Bak, J.G.</creatorcontrib><creatorcontrib>Choi, M.J.</creatorcontrib><creatorcontrib>Nazikian, R.</creatorcontrib><creatorcontrib>Jhang, H.</creatorcontrib><creatorcontrib>Ko, J.</creatorcontrib><creatorcontrib>Joung, M.</creatorcontrib><creatorcontrib>Jeon, Y.-M.</creatorcontrib><creatorcontrib>Na, Y.-S.</creatorcontrib><creatorcontrib>Shinohara, K.</creatorcontrib><creatorcontrib>Cheng, C.Z.</creatorcontrib><creatorcontrib>Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)</creatorcontrib><title>Suppression of toroidal Alfvén eigenmodes by the electron cyclotron current drive in KSTAR plasmas</title><title>Nuclear fusion</title><addtitle>NF</addtitle><addtitle>Nucl. Fusion</addtitle><description>Advanced operation scenarios such as high poloidal beta (
β
P
) or high
q
min
are promising concepts to achieve the steady-state high-performance fusion plasmas. However, those scenarios are prone to substantial Alfvénic activity, causing fast-ion transport and losses. Recent experiments with the advanced operation scenario on KSTAR tokamak have shown that the electron cyclotron current drive (ECCD) is able to mitigate and suppress the beam-ion driven toroidal Alfvén eigenmodes (TAEs) for over several tens of global energy confinement time. Co-current directional intermediate off-axis ECCD lowers the central safety factor slightly and tilts the central
q
-profile shape so that the continuum damping in the core region increases. Besides, the rise of central plasma pressure and increased thermal-ion Landau damping contribute to TAE stabilization. While the TAEs are suppressed, neutron emission rate and total stored energy increase by approximately 45% and 25%, respectively. Fast-ion transport estimated by TRANSP calculations approaches the classical level during the TAE suppression period. Substantial reduction in fast-ion loss and neutron deficit is also observed. Enhancement of fast-ion confinement by suppressing the TAEs leads to an increase of non-inductive current fraction and will benefit the sustainment of the long-pulse high-performance discharges.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>Alfv´en eigenmode</subject><subject>Alfvén eigenmode</subject><subject>ECCD</subject><subject>energetic particle</subject><subject>fusion plasma</subject><subject>KSTAR</subject><subject>tokamak</subject><issn>0029-5515</issn><issn>1741-4326</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp1kE1LxDAQhoMouH7cPQYPnqybadKkPS6LXygI7noObT7cSDcpSXdhf5K_wz9ml4onPc0wPO8w8yB0AeQGSFlOQTDIGM35tFbU0OoATX5Hh2hCSF5lRQHFMTpJ6YMQYEDpBKnFpuuiSckFj4PFfYjB6brFs9Zuvz49Nu7d-HXQJuFmh_uVwaY1qo8DrnaqDWO3idH4HuvotgY7j58Wy9kr7to6ret0ho5s3SZz_lNP0dvd7XL-kD2_3D_OZ8-ZoiXpM1BcEGpYbWmlRVNx02hbMwZ5zpuCgVElNGCZrigQUTWCiobrUhWsIkooTU_R5bg3pN7JpFxv1EoF74d7JZQFh1IMEBkhFUNK0VjZRbeu404CkXuTcq9N7rXJ0eQQuRojLnTyI2yiH76Q3kqey1ySnA9uZaftAF7_Af679xvbAoLw</recordid><startdate>20220201</startdate><enddate>20220201</enddate><creator>Kim, J.</creator><creator>Kang, J.</creator><creator>Rhee, T.</creator><creator>Jo, J.</creator><creator>Han, H.</creator><creator>Podestà, M.</creator><creator>Lee, J.H.</creator><creator>Lee, S.</creator><creator>Bak, J.G.</creator><creator>Choi, M.J.</creator><creator>Nazikian, R.</creator><creator>Jhang, H.</creator><creator>Ko, J.</creator><creator>Joung, M.</creator><creator>Jeon, Y.-M.</creator><creator>Na, Y.-S.</creator><creator>Shinohara, K.</creator><creator>Cheng, C.Z.</creator><general>IOP Publishing</general><general>IOP Science</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OIOZB</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0003-1923-8441</orcidid><orcidid>https://orcid.org/0000-0002-7374-3759</orcidid><orcidid>https://orcid.org/0000-0001-7792-3581</orcidid><orcidid>https://orcid.org/0000-0002-5501-3939</orcidid><orcidid>https://orcid.org/0000-0001-6618-7806</orcidid><orcidid>https://orcid.org/0000-0003-0435-2436</orcidid><orcidid>https://orcid.org/0000-0002-2825-6484</orcidid><orcidid>https://orcid.org/0000-0002-1552-0426</orcidid><orcidid>https://orcid.org/0000-0002-9845-4646</orcidid><orcidid>https://orcid.org/0000-0003-4975-0585</orcidid><orcidid>https://orcid.org/0000-0001-6506-9824</orcidid><orcidid>https://orcid.org/0000-0001-7270-3846</orcidid><orcidid>https://orcid.org/0000-0003-2406-4239</orcidid><orcidid>https://orcid.org/0000-0002-0852-8817</orcidid><orcidid>https://orcid.org/0000-0001-6235-6692</orcidid><orcidid>https://orcid.org/0000000166187806</orcidid><orcidid>https://orcid.org/0000000324064239</orcidid><orcidid>https://orcid.org/0000000304352436</orcidid><orcidid>https://orcid.org/0000000255013939</orcidid><orcidid>https://orcid.org/0000000298454646</orcidid><orcidid>https://orcid.org/0000000172703846</orcidid><orcidid>https://orcid.org/0000000165069824</orcidid><orcidid>https://orcid.org/0000000273743759</orcidid><orcidid>https://orcid.org/0000000208528817</orcidid><orcidid>https://orcid.org/0000000228256484</orcidid><orcidid>https://orcid.org/0000000177923581</orcidid><orcidid>https://orcid.org/0000000319238441</orcidid><orcidid>https://orcid.org/0000000162356692</orcidid><orcidid>https://orcid.org/0000000349750585</orcidid><orcidid>https://orcid.org/0000000215520426</orcidid></search><sort><creationdate>20220201</creationdate><title>Suppression of toroidal Alfvén eigenmodes by the electron cyclotron current drive in KSTAR plasmas</title><author>Kim, J. ; Kang, J. ; Rhee, T. ; Jo, J. ; Han, H. ; Podestà, M. ; Lee, J.H. ; Lee, S. ; Bak, J.G. ; Choi, M.J. ; Nazikian, R. ; Jhang, H. ; Ko, J. ; Joung, M. ; Jeon, Y.-M. ; Na, Y.-S. ; Shinohara, K. ; Cheng, C.Z.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c380t-1c6703e4af39d7b96ebdfa441226b541ec81b1f4d931079b737b6d8c5490c7cd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>Alfv´en eigenmode</topic><topic>Alfvén eigenmode</topic><topic>ECCD</topic><topic>energetic particle</topic><topic>fusion plasma</topic><topic>KSTAR</topic><topic>tokamak</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kim, J.</creatorcontrib><creatorcontrib>Kang, J.</creatorcontrib><creatorcontrib>Rhee, T.</creatorcontrib><creatorcontrib>Jo, J.</creatorcontrib><creatorcontrib>Han, H.</creatorcontrib><creatorcontrib>Podestà, M.</creatorcontrib><creatorcontrib>Lee, J.H.</creatorcontrib><creatorcontrib>Lee, S.</creatorcontrib><creatorcontrib>Bak, J.G.</creatorcontrib><creatorcontrib>Choi, M.J.</creatorcontrib><creatorcontrib>Nazikian, R.</creatorcontrib><creatorcontrib>Jhang, H.</creatorcontrib><creatorcontrib>Ko, J.</creatorcontrib><creatorcontrib>Joung, M.</creatorcontrib><creatorcontrib>Jeon, Y.-M.</creatorcontrib><creatorcontrib>Na, Y.-S.</creatorcontrib><creatorcontrib>Shinohara, K.</creatorcontrib><creatorcontrib>Cheng, C.Z.</creatorcontrib><creatorcontrib>Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (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>Kim, J.</au><au>Kang, J.</au><au>Rhee, T.</au><au>Jo, J.</au><au>Han, H.</au><au>Podestà, M.</au><au>Lee, J.H.</au><au>Lee, S.</au><au>Bak, J.G.</au><au>Choi, M.J.</au><au>Nazikian, R.</au><au>Jhang, H.</au><au>Ko, J.</au><au>Joung, M.</au><au>Jeon, Y.-M.</au><au>Na, Y.-S.</au><au>Shinohara, K.</au><au>Cheng, C.Z.</au><aucorp>Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Suppression of toroidal Alfvén eigenmodes by the electron cyclotron current drive in KSTAR plasmas</atitle><jtitle>Nuclear fusion</jtitle><stitle>NF</stitle><addtitle>Nucl. Fusion</addtitle><date>2022-02-01</date><risdate>2022</risdate><volume>62</volume><issue>2</issue><spage>26029</spage><pages>26029-</pages><issn>0029-5515</issn><eissn>1741-4326</eissn><coden>NUFUAU</coden><abstract>Advanced operation scenarios such as high poloidal beta (
β
P
) or high
q
min
are promising concepts to achieve the steady-state high-performance fusion plasmas. However, those scenarios are prone to substantial Alfvénic activity, causing fast-ion transport and losses. Recent experiments with the advanced operation scenario on KSTAR tokamak have shown that the electron cyclotron current drive (ECCD) is able to mitigate and suppress the beam-ion driven toroidal Alfvén eigenmodes (TAEs) for over several tens of global energy confinement time. Co-current directional intermediate off-axis ECCD lowers the central safety factor slightly and tilts the central
q
-profile shape so that the continuum damping in the core region increases. Besides, the rise of central plasma pressure and increased thermal-ion Landau damping contribute to TAE stabilization. While the TAEs are suppressed, neutron emission rate and total stored energy increase by approximately 45% and 25%, respectively. Fast-ion transport estimated by TRANSP calculations approaches the classical level during the TAE suppression period. Substantial reduction in fast-ion loss and neutron deficit is also observed. Enhancement of fast-ion confinement by suppressing the TAEs leads to an increase of non-inductive current fraction and will benefit the sustainment of the long-pulse high-performance discharges.</abstract><cop>United States</cop><pub>IOP Publishing</pub><doi>10.1088/1741-4326/ac3e39</doi><tpages>21</tpages><orcidid>https://orcid.org/0000-0003-1923-8441</orcidid><orcidid>https://orcid.org/0000-0002-7374-3759</orcidid><orcidid>https://orcid.org/0000-0001-7792-3581</orcidid><orcidid>https://orcid.org/0000-0002-5501-3939</orcidid><orcidid>https://orcid.org/0000-0001-6618-7806</orcidid><orcidid>https://orcid.org/0000-0003-0435-2436</orcidid><orcidid>https://orcid.org/0000-0002-2825-6484</orcidid><orcidid>https://orcid.org/0000-0002-1552-0426</orcidid><orcidid>https://orcid.org/0000-0002-9845-4646</orcidid><orcidid>https://orcid.org/0000-0003-4975-0585</orcidid><orcidid>https://orcid.org/0000-0001-6506-9824</orcidid><orcidid>https://orcid.org/0000-0001-7270-3846</orcidid><orcidid>https://orcid.org/0000-0003-2406-4239</orcidid><orcidid>https://orcid.org/0000-0002-0852-8817</orcidid><orcidid>https://orcid.org/0000-0001-6235-6692</orcidid><orcidid>https://orcid.org/0000000166187806</orcidid><orcidid>https://orcid.org/0000000324064239</orcidid><orcidid>https://orcid.org/0000000304352436</orcidid><orcidid>https://orcid.org/0000000255013939</orcidid><orcidid>https://orcid.org/0000000298454646</orcidid><orcidid>https://orcid.org/0000000172703846</orcidid><orcidid>https://orcid.org/0000000165069824</orcidid><orcidid>https://orcid.org/0000000273743759</orcidid><orcidid>https://orcid.org/0000000208528817</orcidid><orcidid>https://orcid.org/0000000228256484</orcidid><orcidid>https://orcid.org/0000000177923581</orcidid><orcidid>https://orcid.org/0000000319238441</orcidid><orcidid>https://orcid.org/0000000162356692</orcidid><orcidid>https://orcid.org/0000000349750585</orcidid><orcidid>https://orcid.org/0000000215520426</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY Alfv´en eigenmode Alfvén eigenmode ECCD energetic particle fusion plasma KSTAR tokamak |
title | Suppression of toroidal Alfvén eigenmodes by the electron cyclotron current drive in KSTAR plasmas |
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