Transport through Andreev Bound States in a Superconductor-Quantum Dot-Graphene System

Transcription

1 Transport through Andreev Bound States in a Superconductor-Quantum Dot-Graphene System Nadya Mason Travis Dirk, Yung-Fu Chen, Cesar Chialvo Taylor Hughes, Siddhartha Lal, Bruno Uchoa Paul Goldbart University of Illinois at Urbana-Champaign

2 Outline Tunneling spectroscopy with a superconducting probe Fabrication of SC-QD-graphene system Data: Superconducting tunneling into QD-graphene system Analysis: Spectroscopy of Andreev bound states G V I S

3 Graphene electronics Dirac Cones in momentum space linear dispersion around Dirac point semi-metal, but gate tunable E k E ( p) =± v p + p =± v p 2 2 F x y F E p m m v v p m v ± (, ) =± F + F with = 0 F ± = 3 ta c/ à Simple devices show a large variety of electronic behavior: * room temperature quantum Hall effect * transistors * relativistic Klein tunneling Often, high-mobility, low-density of states, & gate-tunability more important than Dirac spectrum (surface accessible 2DEG)

4 Superconduc2vity in graphene Bipolar supercurrent (Heersche et al, Nature 2007) Andreev billiards (Miao et al, Science 2007) Current-phase relation (Chialvo et al, arxiv 2011)

5 à Tunneling spectroscopy with a superconducting probe on graphene: E V G I S 2Δ di/dv (µs) Δ e Birge, Michigan State Ag-Al V (mv) Δ e Metal superconductor - Sharp DOS of superconductor can map out features of graphene - Use subgap conductance to study Andreev reflections & proximity effect

6 à Tunneling spectroscopy with a superconducting probe: Previously, spectroscopy of carbon nanotubes Non-equilibrium tunneling à electron interactions in carbon nanotubes U V nanotube V bias CNT I S Cr/Au Cr/Au contact SC contact Pb/In SiO 2 Si V g Chen et al, PRL (2009)

7 à Tunneling spectroscopy with a superconducting probe: Measure proximity effect N V I S Blonder, Tinkham, Klapwijk (BTK), PRB (1982) Z=0, perfect transmission à enhanced conductance below gap (Δ) Z large, tunnel barrier à suppressed conductance below Δ

8 à Tunneling spectroscopy with a superconducting probe: Surface Andreev bound states in d-wave superconductors à Nodal, d-wave nature of high-tc See Deutscher, RMP (2005) point contact à Can superconducting tunneling spectroscopy be used to measure Andreev bound states in graphene-based system?

9 à Can superconducting tunneling spectroscopy be used to measure Andreev bound states in graphene-based system? Andreev Reflections N S Andreev Bound States (ABS) S N S Standing waves à ABS of discrete energies - Similar ABS in S-N systems if normal metal confined (e.g., superconductor-quantum dot systems) - In long superconducting junctions, supercurrent carried by ABS SC Relevant for characterizing & understanding long Josephson junctions, SNS systems; applications such as SC-SETs, qubits, etc

10 à Can superconducting tunneling spectroscopy be used to measure Andreev bound states in graphene-based system? Andreev Reflections N S Andreev Bound States (ABS) S N S Standing waves à ABS of discrete energies Renewed interest in utilizing ABS:

11 à Sharp spectra of individual Andreev bound states are difficult to measure: - In transport, ABS observed as supercurrent, measure contributions from many modes - In point-contact tunneling, ABS seen as zero-bias anomalies - Spectra of ABS in SNS systems not measured à ABS can be measured via quantum dot coupled to a superconductor:

12 à ABS can be measured via quantum dot coupled to a superconductor: E add = e 2 / C source drain QD is normal when occupied by single particle à ABS form on quantum dot energy levels Subgap features for Au-QD-Al system à need N lead to be weakly coupled to reduce smearing

13 à Can superconducting tunneling spectroscopy be used to measure Andreev bound states in graphene-based system? In Superconductor-graphene system: - Tunneling to obtain spectroscopy - Low density of states leads à few carriers, sharp spectra - Possibility of gate-tuning energy levels - ABS confined in quantum dot coupled to graphene and superconductor

14 Device fabrication graphene SC tunnel probe thin tunnel barrier V contact SiO 2 contact G I S Si SC tunnel probe (Pb) PbOx AlOx nanoparticle Cr/Au Cr/Au SiO 2 Si (gate electrode)

15 Device fabrication PbOx SC tunnel probe (Pb) AlOx nanoparticle Cr/Au Cr/Au SiO 2 Si (gate electrode) 1)Exfoliate graphene onto Si/SiO2 5 µm exfoliate with tape 10µm

16 Device fabrication PbOx SC tunnel probe (Pb) AlOx nanoparticle Cr/Au Cr/Au SiO 2 Si (gate electrode) 1)Exfoliate graphene onto Si/SiO2 2)Cr/Au (2nm/50nm) contacts to ends

17 Device fabrication 3) Deposit 1 nm AlOx via atomic layer deposition - nanoparticles form at graphene edges and defects Al 2 O 3 nanoparticles Graphene Cr/Au Contacts Si/SiO 2 substrate

18 Device fabrication 4) Pb probes à capped with In à ~ 200x200 nm 2 overlap with graphene edge; covers a few nanoparticles à oxidize Pb to attain desired tunnel resistance Cr/Au PbOx SC tunnel probe (Pb) SiO 2 Si (gate electrode) AlOx nanoparticle Cr/Au Room temperature resistances: Cr/Au R ends = 500 Ω R tunnel = kω Cr/Au 2 µm Pb/In

19 Measurement Setup Pb graphene 5 µm Cr/Au

20 Tunnel Conductance for Pb-AlOx-Graphene Similar data seen for 6 different samples, both single layer and multilayer graphene

21 Oscillations above the gap

22 Oscillations above the gap: geometric resonances 0.4 mev particles in a (graphene) box G (µs) V tunnel (mv) source lead (Pb/In) graphene cavity drain lead (Cr/Au) Cr/Au αv gate - V bias = πnv F /L Cr/Au 2 µm Pb/In For L = 3.5µm, v F ~ 6 evå πv F /L ~ 0.5 mev

23 Oscillations above the gap: geometric resonances G (µs) 0.4 mev particles in a (graphene) box αv gate - V bias = πnv F /L V tunnel (mv) Oscillations shift with V gate à extracted value of α consistent with other measurements V gate (mv)

24 Oscillations above the gap: geometric resonances particles in a (graphene) box αv gate - V bias = πnv F /L Simulations of geometric resonances consistent with data (coupling to discrete QD levels allows cavity energy levels to be observed)

25 Tunnel Conductance for Pb-AlOx-Graphene Two low-energy peaks appear inside the gap (ABS)

26 Subgap peaks have strong gate-voltage dependence

27 Data nearly identical to simulation of Andreev reflections in a superconductor-quantum dot-graphene system Calculation *See Nat. Phys. 7, 386, Supp. Info. Data

28 Behavior similar to recent work on Andreev reflections and bound states in quantum dots Subgap features

29 Behavior similar to recent work on Andreev reflections and bound states in quantum dots

30 Robust against temperature, magnetic field

31 ABS only seen when AlOx deposited on graphene ABS features With ALD Without ALD à QD states likely due to AlOx nanoparticles hybridizing with dangling bonds at graphene edge or defect sites

32 Transport through Andreev bound states in a superconductor-quantum dot-graphene system! Gate-tunable, sharp bound states To be discussed: -How do bound states form? - Can data be explained by spectra of bound states?

33 How do ABS form? electron-like U E F U normal quantum dot: single electron transport, separated by charging energy (even/odd spin filling for levels) hole-like Quantum dot coupled to superconductor: no singleparticle states, electron and hole (Andreev) levels

34 How do ABS form? ev b E F solid: electron-like dashed: hole-like ABS form on energy levels Resonant conduction when level within V b of Fermi energy U Levels can shift with gate voltage Discrete level à possibility of isolating individual ABS! Only resolve ABS as subgap peaks for charging energy U > Δ If U < Δ, form Cooper pairs on levels within gap; conductance suppressed (BTK-like)

35 How do ABS form? ev b E F solid: electron-like dashed: hole-like ABS form on energy levels Resonant conduction when level within V b of Fermi energy U Levels can shift with gate voltage Discrete level à possibility of isolating individual ABS! Role of graphene? - Low density lead à sharp spectra -Large range of gate tunability for QD -Single particle QD state from hybrid of AlOx & graphene

36 Spectroscopy of Andreev Bound States ev b U E F ε ~ QD single-particle energy ( or ), E shift = α(δv gate ), U ~ e 2 /κc, ABS Energy as function of gate voltage:

37 Spectroscopy of Andreev Bound States

38 Spectroscopy of Andreev Bound States: Ongoing Work: Correlate ABS spectra with number and size of QDs under superconducting probe 1 nm ALD AlOx 0.5 nm thermally evaporated Al Si/SiO2 substrate Al2O3 nanoparticles Graphene Graphene Si/SiO2 substrate Cr/Au Contacts

39 Spectroscopy of Andreev Bound States: Ongoing Work: Correlate ABS spectra with number and size of QDs under superconducting probe Simulation of ABS for 2 coupled dots

40 Spectroscopy of Andreev Bound States: Ongoing Work: Correlate ABS spectra with number and size of QDs under superconducting probe Simulation of ABS for 3 coupled dots à Controlled multiple-dot spectroscopy, systems of coupled ABS à Patterning QDs by patterning defects in graphene

41 Summary Transport through Andreev bound states in a superconductorgraphene quantum dot system In superconductor-insulator-graphene-normal metal system: Geometric resonances à conductance oscillations Quantum dot formed, likely due to nanoparticle-graphene hybridization Sharp, gate-tunable Andreev bound states formed in quantum dot *See Nat. Phys. 7, 386 *Superconducting tunneling spectroscopy fertile technique *Lots of new physics in hybrid superconducting systems nanostructure contact tunnel probe SiO 2 Si thin tunnel barrier contact

42 Acknowledgements Travis Dirks Yung-Fu Chen Cesar Chialvo Taylor Hughes Siddhartha Lal Bruno Uchoa Paul Goldbart Mason Group, Univ. of Illinois Work supported by the NSF under DMR and the DOE under DE-FG02-07ER46453 through the Frederick Seitz Materials Research Laboratory

43

44 Difficult to experimentally verify quantum dot (work in progress).. - Pillet et al find no evidence of Coulomb blockade when leads normal Seen Not Seen - We also find no evidence of Coulomb blockade when leads normal à Quantum dot can be well-coupled to leads, or in open regime, as long as charging energy significant

45 Effect of end-to-end bias

46 à Tunneling spectroscopy with a superconducting probe: Measure weak tunneling signals in quantum dots Enhanced conductance signals in carbon nanotube quantum dots Pd/In tunneling probe insulator Pd dot SiO 2 Si Pd N V I S -Elastic co-tunneling -Inelastic co-tunneling Dirks et al, APL (2009)

47 Sharp spectra of individual Andreev bound states are difficult to measure: In transport, ABS observed as supercurrent - measure contributions from many modes In point-contact tunneling, ABS seen as zero-bias anomalies à Can couple a superconductor to a quantum dot for individual states à Create tunnel junction to obtain spectra à Make S-QD-N junction to avoid other superconducting resonances à Use low density of states leads to get sharp spectra à Tuning QD energy levels with gate or bias tunes ABS S-QD-graphene system works well!

48 How does one get conductance inside a superconducting gap? - Leaky tunnel barrier - Kondo X - Andreev reflections X N S But, according to BTK, these should be exponentially suppressed inside gap for a tunnel barrier! (and don t see periodicity of MAR)

49 Oscillations above the gap: geometric resonances particles in a (graphene) box αv gate - V bias = πnv F /L Coupling to discrete QD levels allows cavity energy levels to be observed à Spectroscopy of low-energy resonant states!