{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,5,14]],"date-time":"2026-05-14T07:21:32Z","timestamp":1778743292310,"version":"3.51.4"},"reference-count":40,"publisher":"IOP Publishing","issue":"3","license":[{"start":{"date-parts":[[2023,9,11]],"date-time":"2023-09-11T00:00:00Z","timestamp":1694390400000},"content-version":"vor","delay-in-days":10,"URL":"http:\/\/creativecommons.org\/licenses\/by\/4.0"},{"start":{"date-parts":[[2023,9,11]],"date-time":"2023-09-11T00:00:00Z","timestamp":1694390400000},"content-version":"tdm","delay-in-days":10,"URL":"https:\/\/iopscience.iop.org\/info\/page\/text-and-data-mining"}],"funder":[{"DOI":"10.13039\/100010661","name":"Horizon 2020 Framework Programme","doi-asserted-by":"crossref","award":["871501"],"award-info":[{"award-number":["871501"]}],"id":[{"id":"10.13039\/100010661","id-type":"DOI","asserted-by":"crossref"}]}],"content-domain":{"domain":["iopscience.iop.org"],"crossmark-restriction":false},"short-container-title":["Neuromorph. Comput. Eng."],"published-print":{"date-parts":[[2023,9,1]]},"abstract":"<jats:title>Abstract<\/jats:title>\n               <jats:p>The frequency of vanadium dioxide (VO<jats:sub>2<\/jats:sub>) oscillators is a fundamental figure of merit for the realization of neuromorphic circuits called oscillatory neural networks (ONNs) since the high frequency of oscillators ensures low-power consuming, real-time computing ONNs. In this study, we perform electrothermal 3D technology computer-aided design (TCAD) simulations of a VO<jats:sub>2<\/jats:sub> relaxation oscillator. We find that there exists an upper limit to its operating frequency, where such a limit is not predicted from a purely circuital model of the VO<jats:sub>2<\/jats:sub> oscillator. We investigate the intrinsic physical mechanisms that give rise to this upper limit. Our TCAD simulations show that it arises a dependence on the frequency of the points of the curve current versus voltage across the VO<jats:sub>2<\/jats:sub> device corresponding to the insulator-to-metal transition (IMT) and metal-to-insulator transition (MIT) during oscillation, below some threshold values of <jats:inline-formula>\n                     <jats:tex-math\/>\n                     <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:msub>\n                           <mml:mi>C<\/mml:mi>\n                           <mml:mrow>\n                              <mml:mrow>\n                                 <mml:mi mathvariant=\"normal\">e<\/mml:mi>\n                                 <mml:mi mathvariant=\"normal\">x<\/mml:mi>\n                                 <mml:mi mathvariant=\"normal\">t<\/mml:mi>\n                              <\/mml:mrow>\n                           <\/mml:mrow>\n                        <\/mml:msub>\n                     <\/mml:math>\n                     <jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" xlink:href=\"nceacf2bfieqn1.gif\" xlink:type=\"simple\"\/>\n                  <\/jats:inline-formula>. This implies that the condition for the self-oscillatory regime may be satisfied by a given load-line in the low-frequency range but no longer at higher frequencies, with consequent suppression of oscillations. We note that this variation of the IMT\/MIT points below some threshold values of <jats:inline-formula>\n                     <jats:tex-math\/>\n                     <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:msub>\n                           <mml:mi>C<\/mml:mi>\n                           <mml:mrow>\n                              <mml:mrow>\n                                 <mml:mi mathvariant=\"normal\">e<\/mml:mi>\n                                 <mml:mi mathvariant=\"normal\">x<\/mml:mi>\n                                 <mml:mi mathvariant=\"normal\">t<\/mml:mi>\n                              <\/mml:mrow>\n                           <\/mml:mrow>\n                        <\/mml:msub>\n                     <\/mml:math>\n                     <jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" xlink:href=\"nceacf2bfieqn2.gif\" xlink:type=\"simple\"\/>\n                  <\/jats:inline-formula> is due to a combination of different factors: intermediate resistive states achievable by VO<jats:sub>2<\/jats:sub> channel and the interplay between frequency and heat transfer rate. Although the upper limit on the frequency that we extract is linked to the specific VO<jats:sub>2<\/jats:sub> device we simulate, our findings apply qualitatively to any VO<jats:sub>2<\/jats:sub> oscillator. Overall, our study elucidates the link between electrical and thermal behavior in VO<jats:sub>2<\/jats:sub> devices that sets a constraint on the upper values of the operating frequency of any VO<jats:sub>2<\/jats:sub> oscillator.<\/jats:p>","DOI":"10.1088\/2634-4386\/acf2bf","type":"journal-article","created":{"date-parts":[[2023,8,22]],"date-time":"2023-08-22T22:31:19Z","timestamp":1692743479000},"page":"034010","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":8,"title":["How fast can vanadium dioxide neuron-mimicking devices oscillate? Physical mechanisms limiting the frequency of vanadium dioxide oscillators"],"prefix":"10.1088","volume":"3","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-9271-1189","authenticated-orcid":true,"given":"S","family":"Carapezzi","sequence":"first","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0002-4979-6754","authenticated-orcid":false,"given":"A","family":"Plews","sequence":"additional","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0001-8830-3572","authenticated-orcid":false,"given":"G","family":"Boschetto","sequence":"additional","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0001-7656-5874","authenticated-orcid":false,"given":"A","family":"Nejim","sequence":"additional","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0001-9873-2717","authenticated-orcid":false,"given":"S","family":"Karg","sequence":"additional","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0001-8573-2910","authenticated-orcid":false,"given":"A","family":"Todri-Sanial","sequence":"additional","affiliation":[]}],"member":"266","published-online":{"date-parts":[[2023,9,11]]},"reference":[{"key":"nceacf2bfbib1","doi-asserted-by":"publisher","first-page":"3293","DOI":"10.1038\/s41598-020-60373-z","article-title":"Resistive switching studies in VO2 thin films","volume":"10","author":"Rana","year":"2020","journal-title":"Sci. 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Physical mechanisms limiting the frequency of vanadium dioxide oscillators","name":"article_title","label":"Article Title"},{"value":"Neuromorphic Computing and Engineering","name":"journal_title","label":"Journal Title"},{"value":"paper","name":"article_type","label":"Article Type"},{"value":"\u00a9 2023 The Author(s). Published by IOP Publishing Ltd","name":"copyright_information","label":"Copyright Information"},{"value":"2023-05-02","name":"date_received","label":"Date Received","group":{"name":"publication_dates","label":"Publication dates"}},{"value":"2023-08-22","name":"date_accepted","label":"Date Accepted","group":{"name":"publication_dates","label":"Publication dates"}},{"value":"2023-09-11","name":"date_epub","label":"Online publication date","group":{"name":"publication_dates","label":"Publication dates"}}]}}