Nonlocal transport properties due to Andreev scattering
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1 Charles Univ. in Prague, 5 X 2015 Nonlocal transport properties due to Andreev scattering Tadeusz Domański Marie Curie-Skłodowska University, Lublin, Poland
2 Outline
3 Outline A few questions:
4 Outline A few questions: how can we obtain nano-superconductivity / proximity effect /
5 Outline A few questions: how can we obtain nano-superconductivity / proximity effect / how can we observe nano-superconductivity / spectroscopic signatures /
6 Outline A few questions: how can we obtain nano-superconductivity / proximity effect / how can we observe nano-superconductivity / spectroscopic signatures / where can we use nano-superconductors / practical aspects /
7 1. Nano-superconductivity: how to obtain it?
8 Superconducting state of bulk materials
9 Superconducting state of bulk materials ideal d.c. conductance
10 Superconducting state of bulk materials ideal d.c. conductance ideal diamagnetism /perfect screening of the d.c. magnetic field/ T > T c T < T c
11 Superconducting state of bulk materials ideal d.c. conductance (vanishing resistance) ideal diamagnetism (Meissner effect) are caused by the superfluid electron pairs n s (T) 1/λ 2 that move coherently over macroscopic distances.
12 Superconducting state of bulk materials The pairing mechanisms originate from: 1. phonon-exchange / classical superconductors, MgB 2,... / 2. magnon-exchange / heavy fermion compounds / 3. strong correlations / spin exchange 2t2 ij U in the high T c superconductors /.. other exotic processes / ultracold atoms, nuclei, gluon-quark plasma /
13 Superconducting state of bulk materials The pairing mechanisms originate from: 1. phonon-exchange / classical superconductors, MgB 2,... / 2. magnon-exchange / heavy fermion compounds / 3. strong correlations / spin exchange 2t2 ij U in the high T c superconductors /.. other exotic processes / ultracold atoms, nuclei, gluon-quark plasma / Onset of the fermion pairing often goes hand in hand with appearance of the superconductivity/superfluidity, but it doesn t have to be a rule.
14 Proximity effect induced superconductivity
15 Proximity effect induced superconductivity Any material brought in contact with superconductor
16 Proximity effect induced superconductivity Any material brought in contact with superconductor absorbs the paired electrons up to distances ξ n.
17 Proximity effect induced superconductivity Any material brought in contact with superconductor absorbs the paired electrons up to distances ξ n. Spatial size L of nanoscopic objects is L ξ n!
18 2. Nano-superconductivity: how can we observe it?
19 Superconductivity in nanosystems specific issues
20 Superconductivity in nanosystems specific issues 1. Quantum Size Effect discrete energy spectrum normal state superconductor
21 Superconductivity in nanosystems specific issues 1. Quantum Size Effect discrete energy spectrum normal state superconductor Anderson criterion: superconductivity only for > ε i+1 ε i
22 Superconductivity in nanosystems specific issues 2. Coulomb blockade (electron pairing vs repulsion) The odd / even electron number plays the important and qualitative role!
23 Superconductivity in nanosystems specific issues 2. Coulomb blockade (electron pairing vs repulsion) The odd / even electron number plays the important and qualitative role! Coulomb potential U C is usually much smaller than, therefore its influence can be in practice observed only indirectly, via : u 0 v ( quantum phase transition )
24 Superconductivity in nanosystems specific issues 2. Coulomb blockade (electron pairing vs repulsion) The odd / even electron number plays the important and qualitative role! Coulomb potential U C is usually much smaller than, therefore its influence can be in practice observed only indirectly, via : u 0 v ( quantum phase transition ) Physical consequences: inversion of the Josephson current (in S-QD-S junctions) activation/blocking of the Kondo effect (in N-QD-S junctions)
25 Superconductivity in nanosystems specific issues 3. Pairing vs Kondo state ( to screen or not to screen ) R. Maurand, Ch. Schönenberger, Physics 6, 75 (2013).
26 Superconductivity in nanosystems specific issues 3. Pairing vs Kondo state ( to screen or not to screen ) R. Maurand, Ch. Schönenberger, Physics 6, 75 (2013). states near the Fermi level are depleted electron pairing vs the Kondo state (nontrivial relation)
27 Josephson junctions / 0 π transition /
28 Josephson junctions / 0 π transition / Theory and experiment on 0 π transition D. Luitz, F.F. Assad, T. Novotný, C. Karasch, and V. Meden, Phys. Rev. Lett. 108, (2012).
29 Josephson junctions / 0 π transition / Phase boundaries obtained by several methods M. Žonda, V. Pokorný, V. Janiš, and T. Novotný, Sci. Rep. 5, 8821 (2015).
30 3. Nano-superconductivity: some practical aspects
31 Andreev reflections possible applications
32 Andreev reflections possible applications Schematic illustration of the Andreev-type scattering
33 Andreev reflections possible applications Andreev-type scattering can be also considered in more complex junctions P. Cadden-Zimansky, Ph.D. thesis, Northwestern University (2008).
34 Andreev reflections possible applications Andreev-type scattering can be also considered in more complex junctions incident electron P. Cadden-Zimansky, Ph.D. thesis, Northwestern University (2008).
35 Andreev reflections possible applications Andreev-type scattering can be also considered in more complex junctions incident electron elastic tunelling P. Cadden-Zimansky, Ph.D. thesis, Northwestern University (2008).
36 Andreev reflections possible applications Andreev-type scattering can be also considered in more complex junctions incident electron elastic tunelling crossed Andreev refl. P. Cadden-Zimansky, Ph.D. thesis, Northwestern University (2008).
37 Non-local transport planar junctions
38 Non-local transport planar junctions These ET/CAR processes have first considered in the planar junctions A, B normal electrodes, S superconducting material G. Falci, D. Feinberg, F. Hekking, Europhys. Lett. 54, 255 (2001).
39 Non-local transport planar junctions Experimental realization (Delft group) S. Russo, M. Kroug, T. M. Klapwijk & A.F. Morpurgo, Phys. Rev. Lett. 95, (2005).
40 Non-local transport planar junctions Experimental realization S. Russo, M. Kroug, T. M. Klapwijk & A.F. Morpurgo, Phys. Rev. Lett. 95, (2005).
41 Non-local transport planar junctions Experimental realization (Karlsruhe group) J. Brauer, F. Hübler, M. Smetanin, D. Beckman, D. & H. von Löhneysen, Phys. Rev. B 81, (2010).
42 Non-local transport planar junctions Experimental realization (Karlsruhe group) J. Brauer, F. Hübler, M. Smetanin, D. Beckman, D. & H. von Löhneysen, Phys. Rev. B 81, (2010).
43 3-terminal junctions with quantum dots
44 3-terminal junctions with quantum dots Cooper pairs are split, preserving entanglement of individual electrons. L. Hofstetter, S. Csonka, J. Nygård, C. Schönenberger, Nature 461, 960 (2009). J. Schindele, A. Baumgartner, C. Schönenberger, Phys. Rev. Lett. 109, (2012).... and many other groups.
45 3-terminal junctions with quantum dots Possible channels of the Cooper pair splitting L.G. Herrmann et al, Phys. Rev. Lett. 104, (2010).
46 3-terminal junctions with quantum dots These processes are similar to the crossed Andreev scattering and cause the strong non-local transport properties.
47 Non-local transport crossed Andreev refelections
48 Non-local transport crossed Andreev refelections Quantum impurity in the 3-terminal configuration L, R normal electrodes, S superconducting reservoir, QD quantum dot G. Michałek, T. Domański, B.R. Bułka & K.I. Wysokiński, Scientific Reports 5, (2015).
49 Non-local transport crossed Andreev refelections Transmittance of the non-local transport channels T(E) 1 CAR ET ε 0 = E / Γ L Γ S / Γ L 1 0 ET single electron transfer, CAR crossed Andreev reflection
50 Non-local transport crossed Andreev refelections Non-local resistance in the linear response limit. 2R RS,LS /D R [e 2 /h] max: 2e 2 /h e 0 =0 G R =G L G S =G L +G R G S =(G L +G R ) 3 min: -1/4e 2 /h k B T/G L R RS,LS V RS /I LS G S /G L Negative resistance for strong enough coupling Γ S!
51 Non-local transport crossed Andreev refelections Transmittance of the non-local transport channels T(E) CAR ET ε 0 = 3Γ L E / Γ L ε0 / Γ L 1 2 ET single electron transfer, CAR crossed Andreev reflection
52 Non-local transport crossed Andreev refelections Non-local resistance in the linear response limit. 1 2R RS,LS /D R [e 2 /h] k B T/G L GS/G L =3 G S /G L =1 G S /G L =2 G R =G L R RS,LS V RS /I LS e 0 / L Negative resistance for strong enough coupling Γ S and ε 0 0!
53 Non-local transport crossed Andreev refelections Beyond the linear response regime. ev R / L k B T/G L G S /G L =2 G S /G L =4 G S /G L =6 e 0 =0 G R =G L ev L / L Inverse sign of the non-local voltage for strong enough coupling Γ S.
54 Andreev reflections other perspectives
55 Andreev reflections other perspectives Crossed Andreev reflections enable the separation of charge from heat currents F. Mazza, S. Valentini, R. Bosisio, G. Benenti, V. Giovannetti, R. Fazio and F. Tadddei, Phys. Rev. B 91, (2015).
56 Andreev reflections other perspectives On-chip nanoscopic thermometer operating down to 7 mk. A.V. Feshchenko, L. Casparis,..., J.P. Pekola & D.M. Zumbühl, Phys. Rev. Appl. 4, (2015). T. Faivre, D.S. Golubev and J.P. Pekola, Appl. Phys. Lett. 106, (2015). Virtues of a device: is almost free of any self-heating operates at cryogenic temperatures can thermally-monitor the qubits
57 Summary
58 Summary Nanoscopic superconductors:
59 Summary Nanoscopic superconductors: can be induced by the proximity effect
60 Summary Nanoscopic superconductors: can be induced by the proximity effect are manifested via the in-gap (Andreev/Shiba) quasiparticles
61 Summary Nanoscopic superconductors: can be induced by the proximity effect are manifested via the in-gap (Andreev/Shiba) quasiparticles The anomalous (subgap) tunneling can reveal:
62 Summary Nanoscopic superconductors: can be induced by the proximity effect are manifested via the in-gap (Andreev/Shiba) quasiparticles The anomalous (subgap) tunneling can reveal: strong non-local properties (e.g. negative resistance)
63 Summary Nanoscopic superconductors: can be induced by the proximity effect are manifested via the in-gap (Andreev/Shiba) quasiparticles The anomalous (subgap) tunneling can reveal: strong non-local properties (e.g. negative resistance) separation of the charge from heat currents
64 Summary Nanoscopic superconductors: can be induced by the proximity effect are manifested via the in-gap (Andreev/Shiba) quasiparticles The anomalous (subgap) tunneling can reveal: strong non-local properties (e.g. negative resistance) separation of the charge from heat currents realization of exotic quasiparticles (e.g. Majorana-type)
65 Summary Nanoscopic superconductors: can be induced by the proximity effect are manifested via the in-gap (Andreev/Shiba) quasiparticles The anomalous (subgap) tunneling can reveal: strong non-local properties (e.g. negative resistance) separation of the charge from heat currents realization of exotic quasiparticles (e.g. Majorana-type)
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