Inhomogeneous electronic states in superconductors (Chapelier, Ioffe) How to disentangle the unavoidable atomic level inhomogeneity of real materials from the electronic inhomogeneity discussion-session
Maud Vinet Walter Escoffier Benjamin Sacépé Thomas Dubouchet Charlène Tonnoir Claude Chapelier CEA INAC-SPSMS-LaTEQS, Grenoble Very Low Temperature STM: a powerful probe for inhomogeneous superconducting states (tutorial)
Very Low Temperature STM: a powerful probe for inhomogeneous superconducting states (tutorial) I.STM/STS and usual inhomogeneous superconducting states II.Highly disordered superconductors III.Discussion
Coarse approach motor Coarse positioning X-Y table Sample holder Tip Piezo tube 10 cm Scanning Tunneling Microscopy Michael Schmid, TU Wien
P.Mallet et al., J. Vac. Sci. Technol. B 14, 1070 (1996) Michael Schmid, TU Wien NbSe 2 Scanning Tunneling Microscopy
P.Mallet et al., J. Vac. Sci. Technol. B 14, 1070 (1996) D. Roditchev’s group, Michael Schmid, TU Wien NbSe 2 Scanning Tunneling Microscopy
Scanning Tunneling Spectroscopy P.Mallet et al., J. Vac. Sci. Technol. B 14, 1070 (1996) I V dI/dV NbSe 2 D. Roditchev’s group,
Scanning Tunneling Spectroscopy P.Mallet et al., J. Vac. Sci. Technol. B 14, 1070 (1996) I V dI/dV NbSe 2 D. Roditchev’s group, H. Hess et al., Physica B 169, 422 (1991)
I V dI/dV Scanning Tunneling Spectroscopy P.Mallet et al., J. Vac. Sci. Technol. B 14, 1070 (1996) NbSe 2 D. Roditchev’s group, H. Hess et al., Physica B 169, 422 (1991)
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Vortex NbSe 2 Sachdev & Zhang, Science
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Vortex H. Hess et al., Phys. Rev. Lett.. 62, 214 (1989) NbSe 2
Vortex NbSe 2 H. Hess et al., Physica B 169, 422 (1991)
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Very Low Temperature STM: a powerful probe for inhomogeneous superconducting states (tutorial) I.STM/STS and usual inhomogeneous superconducting states II.Highly disordered superconductors III.Discussion
Superconductor-Insulator Transition Granular systemsHomogeneously disordered materials H.M. Jaeger, et al., Phys. Rev. B 34, (1986) D.B. Haviland, et al., Phys. Rev. Lett. 62, 2180 (1989) Gallium Bismuth
Superconductor-Insulator Transition TiN Reactive sputter deposition of TiN films Homogeneously disordered ? N. Hadaceket al., Phys. Rev. B 69, (2004) 100 nm 10 nm
Superconductor-Insulator Transition TiN 100 nm 10 nm T (K) R (Ohms) Reactive sputter deposition of TiN films Granular ? Homogeneously disordered ? N. Hadaceket al., Phys. Rev. B 69, (2004)
Superconductor-Insulator Transition TiN T (K) R (Ohms) Reactive sputter deposition of TiN films Granular ? Homogeneously disordered ? N. Hadaceket al., Phys. Rev. B 69, (2004) ≈ 80 × 80 × 2 nm ≈ 400 × 400 × 3 nm W. Escoffier et al.,Phys. Rev. Lett. 93, (2004) 100 nm 10 nm
Superconductor-Insulator Transition TiN Reactive sputter deposition of TiN films Homogeneously disordered ? N. Hadaceket al., Phys. Rev. B 69, (2004) ≈ 80 × 80 × 2 nm ≈ 400 × 400 × 3 nm W. Escoffier et al.,Phys. Rev. Lett. 93, (2004) 100 nm 10 nm
M. Baklanov and A. Satta (IMEC) Superconductor-Insulator Transition TiN Atomic layer deposition of 5 nm thick TiN films
Increasing disorder Superconductor-Insulator transition Sacépé et al., Phys. Rev. Lett. 101, (2008) TiN
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Pseudogap B. Sacépé, et al., Nature Communications 1:140 (2010)
Superconducting fluctuations correction to the DOS Short-lived Cooper pairs above Tc A. Varlamov and V. Dorin, Sov. Phys. JETP 57, 1089, (1983) Pseudogap B. Sacépé, et al., Nature Communications 1:140 (2010)
Superconducting fluctuations correction to the DOS Short-lived Cooper pairs above Tc A. Varlamov and V. Dorin, Sov. Phys. JETP 57, 1089, (1983) Pseudogap B. Sacépé, et al., Nature Communications 1:140 (2010) R □ [kΩ] T c (R □ ) [K] T c (DOS) [K] An extreme sensitivity to Tc
Very Low Temperature STM: a powerful probe for inhomogeneous superconducting states (tutorial) I.STM/STS and usual inhomogeneous superconducting states II.Highly disordered superconductors III.Discussion How to disentangle the unavoidable atomic level inhomogeneity of real materials from the electronic inhomogeneity ? Which inhomogeneities ? Down to which scale a real material must be considered granular or not ? What is a homogeneously disordered material ? How can we relate global macroscopic behavior (transport) and local signatures (STS) ?
Dilution fridge setup
Anomalous proximity effect Superconducting granular TiN films d S,N W. Escoffier et al., Phys. Rev. Lett. (2004) ≈ 80 × 80 × 2 nm ≈ 400 × 400 × 3 nm Theory : Zhang & Xiong, Physica C (2006)
Anomalous proximity effect Superconducting granular TiN films B. Sacépé (unpublished) 1500 nm x 1500 nm
Superconducting fluctuations quantum corrections
T c [K] One parameter fit : T c Superconducting fluctuations quantum corrections