Electrothermal enhancement of β-(AlxGa1-x)2O3/Ga2O3 heterostructure field-effect transistors via back-end-of-line sputter-deposited AlN layer

dc.contributor.authorLundh, James Spenceren
dc.contributor.authorCress, Coryen
dc.contributor.authorJacobs, Alan G.en
dc.contributor.authorCheng, Zheen
dc.contributor.authorMasten, Hannah N.en
dc.contributor.authorSpencer, Joseph A.en
dc.contributor.authorSasaki, Koheien
dc.contributor.authorGallagher, Jamesen
dc.contributor.authorKoehler, Andrew D.en
dc.contributor.authorKonishi, Keitaen
dc.contributor.authorGraham, Samuelen
dc.contributor.authorKuramata, Akitoen
dc.contributor.authorAnderson, Travis J.en
dc.contributor.authorTadjer, Marko J.en
dc.contributor.authorHobart, Karl D.en
dc.contributor.authorMastro, Michael A.en
dc.date.accessioned2025-10-09T14:58:52Zen
dc.date.available2025-10-09T14:58:52Zen
dc.date.issued2024-12-14en
dc.description.abstractThe electrothermal device performance of beta-(Al0.21Ga0.79)(2)O-3/Ga2O3 heterostructure field-effect transistors (HFETs) was enhanced by incorporating a 400 nm thick AlN capping layer via back-end-of-line room-temperature reactive sputter deposition. The AlN-capped HFETs demonstrated DC power densities >5 W/mm, higher than any previous report on lateral beta-Ga2O3 transistors on native substrates. The breakdown voltage (V-B) of the uncapped HFETs was 569 +/- 250 V with a maximum V-B of 947 V. For the AlN-capped HFETs, V-B increased to 1210 +/- 351 V with a maximum V-B of 1868 V. The AlN-capped HFETs demonstrated a 27% reduction in device-level thermal resistance (R-TH) as measured from the gate electrode. The combined use of electrical and thermal simulation helped elucidate the coupled electrothermal contributions to the measured reduction in the temperature rise for the AlN-capped HFETs. Although the measured AlN film thermal conductivity (13.3 +/- 1.3 W/mK) was comparable to that of bulk beta-Ga2O3, the capping layer still reduced the simulated peak channel temperature rise by similar to 4% due to heat spreading only. Electrical simulation revealed that electric field spreading was an additional mechanism that contributed to the majority of the simulated 18% reduction in the peak channel temperature rise through delocalization and redistribution of the heat generation in the channel. Thermal modeling was used to evaluate further improvements in thermal performance that can be realized by optimizing the sputter deposition process to achieve thicker and higher thermal conductivity AlN.en
dc.description.sponsorshipOffice of Naval Research10.13039/100000006; National Research Council (NRC) postdoctoral fellowship program; Office of Naval Research (ONR); ONR Globalen
dc.format.mimetypeapplication/pdfen
dc.identifier.doihttps://doi.org/10.1063/5.0225896en
dc.identifier.eissn1089-7550en
dc.identifier.issn0021-8979en
dc.identifier.issue22en
dc.identifier.urihttps://hdl.handle.net/10919/138113en
dc.identifier.volume136en
dc.language.isoenen
dc.publisherAIP Publishingen
dc.rightsCreative Commons Attribution 4.0 Internationalen
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/en
dc.titleElectrothermal enhancement of β-(AlxGa1-x)2O3/Ga2O3 heterostructure field-effect transistors via back-end-of-line sputter-deposited AlN layeren
dc.title.serialJournal of Applied Physicsen
dc.typeArticle - Refereeden
dc.type.dcmitypeTexten

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