Light effective hole mass in undoped Ge/SiGe quantum wells
We report density-dependent effective hole mass measurements in undoped germanium quantum wells. We are able to span a large range of densities (\(2.0-11\times10^{11}\) cm\(^{-2}\)) in top-gated field effect transistors by positioning the strained buried Ge channel at different depths of 12 and 44 n...
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creator | Lodari, M Tosato, A Sabbagh, D Schubert, M A Capellini, G Sammak, A Veldhorst, M Scappucci, G |
description | We report density-dependent effective hole mass measurements in undoped germanium quantum wells. We are able to span a large range of densities (\(2.0-11\times10^{11}\) cm\(^{-2}\)) in top-gated field effect transistors by positioning the strained buried Ge channel at different depths of 12 and 44 nm from the surface. From the thermal damping of the amplitude of Shubnikov-de Haas oscillations, we measure a light mass of \(0.061m_e\) at a density of \(2.2\times10^{11}\) cm\(^{-2}\). We confirm the theoretically predicted dependence of increasing mass with density and by extrapolation we find an effective mass of \(\sim0.05m_e\) at zero density, the lightest effective mass for a planar platform that demonstrated spin qubits in quantum dots. |
doi_str_mv | 10.48550/arxiv.1905.08064 |
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We are able to span a large range of densities (\(2.0-11\times10^{11}\) cm\(^{-2}\)) in top-gated field effect transistors by positioning the strained buried Ge channel at different depths of 12 and 44 nm from the surface. From the thermal damping of the amplitude of Shubnikov-de Haas oscillations, we measure a light mass of \(0.061m_e\) at a density of \(2.2\times10^{11}\) cm\(^{-2}\). We confirm the theoretically predicted dependence of increasing mass with density and by extrapolation we find an effective mass of \(\sim0.05m_e\) at zero density, the lightest effective mass for a planar platform that demonstrated spin qubits in quantum dots.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1905.08064</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Damping ; Density ; Dependence ; Field effect transistors ; Germanium ; Physics - Materials Science ; Physics - Mesoscale and Nanoscale Physics ; Quantum dots ; Quantum wells ; Qubits (quantum computing) ; Semiconductor devices</subject><ispartof>arXiv.org, 2019-05</ispartof><rights>2019. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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We are able to span a large range of densities (\(2.0-11\times10^{11}\) cm\(^{-2}\)) in top-gated field effect transistors by positioning the strained buried Ge channel at different depths of 12 and 44 nm from the surface. From the thermal damping of the amplitude of Shubnikov-de Haas oscillations, we measure a light mass of \(0.061m_e\) at a density of \(2.2\times10^{11}\) cm\(^{-2}\). We confirm the theoretically predicted dependence of increasing mass with density and by extrapolation we find an effective mass of \(\sim0.05m_e\) at zero density, the lightest effective mass for a planar platform that demonstrated spin qubits in quantum dots.</description><subject>Damping</subject><subject>Density</subject><subject>Dependence</subject><subject>Field effect transistors</subject><subject>Germanium</subject><subject>Physics - Materials Science</subject><subject>Physics - Mesoscale and Nanoscale Physics</subject><subject>Quantum dots</subject><subject>Quantum wells</subject><subject>Qubits (quantum computing)</subject><subject>Semiconductor devices</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><sourceid>GOX</sourceid><recordid>eNotj8tOwzAURC0kJKrSD2CFJdZJ7Ws7cdmhCgJSJBZ0H_lJXeXVOCnw94SWzczmaDQHoTtKUi6FIGs1fIdTSjdEpESSjF-hBTBGE8kBbtAqxgMhBLIchGAL9FiGz_2InffOjOHk8L6rHW5UjDi0eGpt1zuLC7f-CIXDx0m149TgL1fX8RZde1VHt_rvJdq9PO-2r0n5Xrxtn8pECeAJ-Fx7QgVQK7TRlsyhLAjjgWWOGWmpMNZwKi2j2nO9UcZpIojKqTSesiW6v8yexap-CI0afqo_weosOBMPF6IfuuPk4lgdumlo508VAEg-M5yzX7PNUzM</recordid><startdate>20190520</startdate><enddate>20190520</enddate><creator>Lodari, M</creator><creator>Tosato, A</creator><creator>Sabbagh, D</creator><creator>Schubert, M A</creator><creator>Capellini, G</creator><creator>Sammak, A</creator><creator>Veldhorst, M</creator><creator>Scappucci, G</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PHGZM</scope><scope>PHGZT</scope><scope>PIMPY</scope><scope>PKEHL</scope><scope>PQEST</scope><scope>PQGLB</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20190520</creationdate><title>Light effective hole mass in undoped Ge/SiGe quantum wells</title><author>Lodari, M ; 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We are able to span a large range of densities (\(2.0-11\times10^{11}\) cm\(^{-2}\)) in top-gated field effect transistors by positioning the strained buried Ge channel at different depths of 12 and 44 nm from the surface. From the thermal damping of the amplitude of Shubnikov-de Haas oscillations, we measure a light mass of \(0.061m_e\) at a density of \(2.2\times10^{11}\) cm\(^{-2}\). We confirm the theoretically predicted dependence of increasing mass with density and by extrapolation we find an effective mass of \(\sim0.05m_e\) at zero density, the lightest effective mass for a planar platform that demonstrated spin qubits in quantum dots.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1905.08064</doi><oa>free_for_read</oa></addata></record> |
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subjects | Damping Density Dependence Field effect transistors Germanium Physics - Materials Science Physics - Mesoscale and Nanoscale Physics Quantum dots Quantum wells Qubits (quantum computing) Semiconductor devices |
title | Light effective hole mass in undoped Ge/SiGe quantum wells |
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