Andreev bound states probed in three-terminal quantum dots
Andreev bound states (ABSs) are well-defined many-body quantum states that emerge from the hybridization of individual quantum dot (QD) states with a superconductor and exhibit very rich and fundamental phenomena. We demonstrate several electron transport phenomena mediated by ABSs that form on thre...
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description | Andreev bound states (ABSs) are well-defined many-body quantum states that emerge from the hybridization of individual quantum dot (QD) states with a superconductor and exhibit very rich and fundamental phenomena. We demonstrate several electron transport phenomena mediated by ABSs that form on three-terminal carbon nanotube (CNT) QDs, with one superconducting (S) contact in the center and two adjacent normal-metal (N) contacts. Three-terminal spectroscopy allows us to identify the coupling to the N contacts as the origin of the Andreev resonance (AR) linewidths and to determine the critical coupling strengths to S, for which a ground state (or quantum phase) transition in such S-QD systems can occur. In addition, we ascribe replicas of the lowest-energy ABS resonance to transitions between the ABS and odd-parity excited QD states, a process we call excited state ABS resonances. In the conductance between the two N contacts we find a characteristic pattern of positive and negative differential subgap conductance, which we explain by considering two nonlocal processes, the creation of Cooper pairs in S by electrons from both N terminals, and a transport mechanism we call resonant ABS tunneling, possible only in multiterminal QD devices. In the latter process, electrons are transferred via the ABS without effectively creating Cooper pairs in S. The three-terminal geometry also allows spectroscopy experiments with different boundary conditions, for example by leaving S floating. Surprisingly, we find that, depending on the boundary conditions and the device parameters, the experiments either show single-particle Coulomb blockade resonances, ABS characteristics, or both in the same measurements, seemingly contradicting the notion of ABSs replacing the single-particle states as eigenstates of the QD. We qualitatively explain these results as originating from the finite time scale required for the coherent oscillations between the superposition states after a single-electron tunneling event. These experiments demonstrate that three-terminal experiments on a single complex quantum object can also be useful to investigate charge dynamics otherwise not accessible due to the very high frequencies. |
doi_str_mv | 10.1103/PhysRevB.96.195418 |
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We demonstrate several electron transport phenomena mediated by ABSs that form on three-terminal carbon nanotube (CNT) QDs, with one superconducting (S) contact in the center and two adjacent normal-metal (N) contacts. Three-terminal spectroscopy allows us to identify the coupling to the N contacts as the origin of the Andreev resonance (AR) linewidths and to determine the critical coupling strengths to S, for which a ground state (or quantum phase) transition in such S-QD systems can occur. In addition, we ascribe replicas of the lowest-energy ABS resonance to transitions between the ABS and odd-parity excited QD states, a process we call excited state ABS resonances. In the conductance between the two N contacts we find a characteristic pattern of positive and negative differential subgap conductance, which we explain by considering two nonlocal processes, the creation of Cooper pairs in S by electrons from both N terminals, and a transport mechanism we call resonant ABS tunneling, possible only in multiterminal QD devices. In the latter process, electrons are transferred via the ABS without effectively creating Cooper pairs in S. The three-terminal geometry also allows spectroscopy experiments with different boundary conditions, for example by leaving S floating. Surprisingly, we find that, depending on the boundary conditions and the device parameters, the experiments either show single-particle Coulomb blockade resonances, ABS characteristics, or both in the same measurements, seemingly contradicting the notion of ABSs replacing the single-particle states as eigenstates of the QD. We qualitatively explain these results as originating from the finite time scale required for the coherent oscillations between the superposition states after a single-electron tunneling event. These experiments demonstrate that three-terminal experiments on a single complex quantum object can also be useful to investigate charge dynamics otherwise not accessible due to the very high frequencies.</description><identifier>ISSN: 2469-9950</identifier><identifier>EISSN: 2469-9969</identifier><identifier>DOI: 10.1103/PhysRevB.96.195418</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Boundary conditions ; Carbon nanotubes ; Cooper pairs ; Coupling ; Eigenvectors ; Electron transport ; Electron tunneling ; Experiments ; Phase transitions ; Quantum dots ; Resistance ; Spectroscopy ; Spectrum analysis ; Superposition (mathematics) ; Transport buildings, stations and terminals ; Transport phenomena ; Very high frequencies</subject><ispartof>Physical review. B, 2017-11, Vol.96 (19)</ispartof><rights>Copyright American Physical Society Nov 15, 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Gramich, J</creatorcontrib><creatorcontrib>Baumgartner, A</creatorcontrib><creatorcontrib>Schönenberger, C</creatorcontrib><title>Andreev bound states probed in three-terminal quantum dots</title><title>Physical review. B</title><description>Andreev bound states (ABSs) are well-defined many-body quantum states that emerge from the hybridization of individual quantum dot (QD) states with a superconductor and exhibit very rich and fundamental phenomena. We demonstrate several electron transport phenomena mediated by ABSs that form on three-terminal carbon nanotube (CNT) QDs, with one superconducting (S) contact in the center and two adjacent normal-metal (N) contacts. Three-terminal spectroscopy allows us to identify the coupling to the N contacts as the origin of the Andreev resonance (AR) linewidths and to determine the critical coupling strengths to S, for which a ground state (or quantum phase) transition in such S-QD systems can occur. In addition, we ascribe replicas of the lowest-energy ABS resonance to transitions between the ABS and odd-parity excited QD states, a process we call excited state ABS resonances. In the conductance between the two N contacts we find a characteristic pattern of positive and negative differential subgap conductance, which we explain by considering two nonlocal processes, the creation of Cooper pairs in S by electrons from both N terminals, and a transport mechanism we call resonant ABS tunneling, possible only in multiterminal QD devices. In the latter process, electrons are transferred via the ABS without effectively creating Cooper pairs in S. The three-terminal geometry also allows spectroscopy experiments with different boundary conditions, for example by leaving S floating. Surprisingly, we find that, depending on the boundary conditions and the device parameters, the experiments either show single-particle Coulomb blockade resonances, ABS characteristics, or both in the same measurements, seemingly contradicting the notion of ABSs replacing the single-particle states as eigenstates of the QD. We qualitatively explain these results as originating from the finite time scale required for the coherent oscillations between the superposition states after a single-electron tunneling event. These experiments demonstrate that three-terminal experiments on a single complex quantum object can also be useful to investigate charge dynamics otherwise not accessible due to the very high frequencies.</description><subject>Boundary conditions</subject><subject>Carbon nanotubes</subject><subject>Cooper pairs</subject><subject>Coupling</subject><subject>Eigenvectors</subject><subject>Electron transport</subject><subject>Electron tunneling</subject><subject>Experiments</subject><subject>Phase transitions</subject><subject>Quantum dots</subject><subject>Resistance</subject><subject>Spectroscopy</subject><subject>Spectrum analysis</subject><subject>Superposition (mathematics)</subject><subject>Transport buildings, stations and terminals</subject><subject>Transport phenomena</subject><subject>Very high frequencies</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNo9jlFLwzAURoMoOOb-gE8Bn1tzb5o08W0OncJAEX0eSXPDNrZ2a9KB_96C4tP54MDHYewWRAkg5P375jt90PmxtLoEqyowF2yClbaFtdpe_m8lrtkspZ0QArSwtbAT9jBvQ0905r4b2sBTdpkSP_adp8C3Lc-b0RaZ-sO2dXt-GlybhwMPXU437Cq6faLZH6fs6_npc_FSrN6Wr4v5qjgCyFwoNE2UISryMmpLDekKCBsV0FvXyFo3WKFBsCIiVdEEpxQ0HpVW0Qcpp-zu93esOg2U8nrXDf1Yk9YIKMGgqa38AbhgTDo</recordid><startdate>20171115</startdate><enddate>20171115</enddate><creator>Gramich, J</creator><creator>Baumgartner, A</creator><creator>Schönenberger, C</creator><general>American Physical Society</general><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20171115</creationdate><title>Andreev bound states probed in three-terminal quantum dots</title><author>Gramich, J ; Baumgartner, A ; Schönenberger, C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p113t-528cf3df5eb3f69ece641e2c5d2b9ac376c24282190f2e4f8da551cb2565fbd33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Boundary conditions</topic><topic>Carbon nanotubes</topic><topic>Cooper pairs</topic><topic>Coupling</topic><topic>Eigenvectors</topic><topic>Electron transport</topic><topic>Electron tunneling</topic><topic>Experiments</topic><topic>Phase transitions</topic><topic>Quantum dots</topic><topic>Resistance</topic><topic>Spectroscopy</topic><topic>Spectrum analysis</topic><topic>Superposition (mathematics)</topic><topic>Transport buildings, stations and terminals</topic><topic>Transport phenomena</topic><topic>Very high frequencies</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gramich, J</creatorcontrib><creatorcontrib>Baumgartner, A</creatorcontrib><creatorcontrib>Schönenberger, C</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gramich, J</au><au>Baumgartner, A</au><au>Schönenberger, C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Andreev bound states probed in three-terminal quantum dots</atitle><jtitle>Physical review. B</jtitle><date>2017-11-15</date><risdate>2017</risdate><volume>96</volume><issue>19</issue><issn>2469-9950</issn><eissn>2469-9969</eissn><abstract>Andreev bound states (ABSs) are well-defined many-body quantum states that emerge from the hybridization of individual quantum dot (QD) states with a superconductor and exhibit very rich and fundamental phenomena. We demonstrate several electron transport phenomena mediated by ABSs that form on three-terminal carbon nanotube (CNT) QDs, with one superconducting (S) contact in the center and two adjacent normal-metal (N) contacts. Three-terminal spectroscopy allows us to identify the coupling to the N contacts as the origin of the Andreev resonance (AR) linewidths and to determine the critical coupling strengths to S, for which a ground state (or quantum phase) transition in such S-QD systems can occur. In addition, we ascribe replicas of the lowest-energy ABS resonance to transitions between the ABS and odd-parity excited QD states, a process we call excited state ABS resonances. In the conductance between the two N contacts we find a characteristic pattern of positive and negative differential subgap conductance, which we explain by considering two nonlocal processes, the creation of Cooper pairs in S by electrons from both N terminals, and a transport mechanism we call resonant ABS tunneling, possible only in multiterminal QD devices. In the latter process, electrons are transferred via the ABS without effectively creating Cooper pairs in S. The three-terminal geometry also allows spectroscopy experiments with different boundary conditions, for example by leaving S floating. Surprisingly, we find that, depending on the boundary conditions and the device parameters, the experiments either show single-particle Coulomb blockade resonances, ABS characteristics, or both in the same measurements, seemingly contradicting the notion of ABSs replacing the single-particle states as eigenstates of the QD. We qualitatively explain these results as originating from the finite time scale required for the coherent oscillations between the superposition states after a single-electron tunneling event. These experiments demonstrate that three-terminal experiments on a single complex quantum object can also be useful to investigate charge dynamics otherwise not accessible due to the very high frequencies.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.96.195418</doi></addata></record> |
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subjects | Boundary conditions Carbon nanotubes Cooper pairs Coupling Eigenvectors Electron transport Electron tunneling Experiments Phase transitions Quantum dots Resistance Spectroscopy Spectrum analysis Superposition (mathematics) Transport buildings, stations and terminals Transport phenomena Very high frequencies |
title | Andreev bound states probed in three-terminal quantum dots |
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