{"id":10966,"date":"2025-12-18T09:56:28","date_gmt":"2025-12-18T00:56:28","guid":{"rendered":"https:\/\/unit.nifs.ac.jp\/research\/?post_type=report&#038;p=10966"},"modified":"2025-12-18T09:59:28","modified_gmt":"2025-12-18T00:59:28","slug":"report-10968_en","status":"publish","type":"report","link":"https:\/\/unit.nifs.ac.jp\/research\/archives\/report\/report-10968_en","title":{"rendered":"Energy exchange between electrons and ions driven by ITG-TEM turbulence"},"content":{"rendered":"\n<p>Tetsuji Kato et al. summarized their research as &#8220;Energy exchange between electrons and ions driven by ITG-TEM turbulence,\u201d and their paper has been published in Issue 12 of Physics of Plasmas. In addition, this paper has been selected as a Featured Article.<\/p>\n\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<p>\u3010Abstract\u3011<\/p>\n\n\n\n<p>\u3000\u3000In this study, the energy exchange between electrons and ions in trapped-electron-mode (TEM) and mixed ion temperature gradient (ITG)\u2013TEM turbulence is investigated using gyrokinetic simulations. The energy exchange in TEM turbulence is primarily composed of the cooling of electrons associated with perpendicular&nbsp;grad-B curvature drift and the heating of ions moving parallel to magnetic field lines. TEM turbulence facilitates energy transfer from electrons to ions, which is opposite to the direction observed in ITG turbulence. In mixed ITG\u2013TEM turbulence, the relative magnitudes of parallel heating and perpendicular cooling for each species determine the overall direction and magnitude of energy exchange. From the viewpoint of entropy balance, it is further confirmed that energy flows from the species with larger entropy production, caused by particle and heat fluxes, to the other species in ITG\u2013TEM turbulence. The predictability of turbulent energy exchange in ITG\u2013TEM turbulence by the quasilinear model is examined. In addition, an alternative method based on the correlation between energy flux and energy exchange is developed, and its validity is demonstrated.<\/p>\n\n\n\n<p>\u3000\u3000The numerical simulations were performed on Plasma Simulator of NIFS.<\/p>\n\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"985\" height=\"698\" src=\"http:\/\/unit.nifs.ac.jp\/research\/wp-content\/uploads\/2025\/12\/Highlight.jpg\" alt=\"\" class=\"wp-image-10970\" style=\"width:720px\" srcset=\"https:\/\/unit.nifs.ac.jp\/research\/wp-content\/uploads\/2025\/12\/Highlight.jpg 985w, https:\/\/unit.nifs.ac.jp\/research\/wp-content\/uploads\/2025\/12\/Highlight-300x213.jpg 300w, https:\/\/unit.nifs.ac.jp\/research\/wp-content\/uploads\/2025\/12\/Highlight-768x544.jpg 768w, https:\/\/unit.nifs.ac.jp\/research\/wp-content\/uploads\/2025\/12\/Highlight-180x128.jpg 180w, https:\/\/unit.nifs.ac.jp\/research\/wp-content\/uploads\/2025\/12\/Highlight-500x354.jpg 500w\" sizes=\"auto, (max-width: 985px) 100vw, 985px\" \/><figcaption class=\"wp-element-caption\">Figure: Turbulent energy exchange as a function of electron and ion temperature gradients. Blue squares indicate the turbulent energy exchange between electrons and ions obtained from nonlinear simulations. Circles represent the turbulent energy exchange predicted by the quasilinear model, where the saturation rule is taken from the nonlinear simulation results. Green squares show the quantity, (Difference between the turbulent energy fluxes of electrons and ions)\/(Major radius), evaluated from the nonlinear simulations, while triangles denote the same quantity calculated using the turbulent energy fluxes predicted by the quasilinear model.<\/figcaption><\/figure>\n<\/div>\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<p>\u3010Information\u3011<\/p>\n\n\n\n<p>\u3000\u3000T. Kato, H. Sugama, and T.-H. Watanabe, &#8220;Energy exchange between electrons and ions driven by ITG-TEM turbulence,\u201d Phys. Plasmas 32, 122303 (2025).<\/p>\n\n\n\n<p>\u3000\u3000DOI: <a href=\"https:\/\/doi.org\/10.1063\/5.0291372\" data-type=\"link\" data-id=\"https:\/\/doi.org\/10.1063\/5.0291372\" target=\"_blank\">10.1063\/5.0291372<\/a><\/p>\n\n\n\n<div style=\"height:80px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n","protected":false},"author":9,"featured_media":10970,"menu_order":0,"template":"","meta":{"_acf_changed":false,"footnotes":""},"ppma_author":[347],"class_list":["post-10966","report","type-report","status-publish","has-post-thumbnail","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/report\/10966","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/report"}],"about":[{"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/types\/report"}],"author":[{"embeddable":true,"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/users\/9"}],"version-history":[{"count":6,"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/report\/10966\/revisions"}],"predecessor-version":[{"id":10983,"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/report\/10966\/revisions\/10983"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/media\/10970"}],"wp:attachment":[{"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/media?parent=10966"}],"wp:term":[{"taxonomy":"author","embeddable":true,"href":"https:\/\/unit.nifs.ac.jp\/research\/wp-json\/wp\/v2\/ppma_author?post=10966"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}