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From local to collective superconductivity in proximitized graphene

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arxiv 2504.19620 v1 pith:WLSFJEOK submitted 2025-04-28 cond-mat.mes-hall cond-mat.supr-con

classification cond-mat.mes-hallcond-mat.supr-con
keywords superconductingcorrelationseffectgraphenecollectivedopinglengthpairing
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The superconducting proximity effect induces pairing correlations in metallic systems via Andreev scattering. This effect is particularly intriguing in graphene, as it enables two-dimensional superconductivity that is tunable through doping. Understanding how superconducting correlations propagate within the metal is crucial to unveiling the key factors behind this tunability. Here, we employ scanning tunneling microscopy to investigate the energy and length scales of the proximity effect induced by Pb islands on graphene. Using tip-induced manipulation, we assemble S/N/S junctions with tunable N-region spacing and explore the evolution of the proximitized state in the confined normal region. We find that different doping levels can lead to either localized or collective superconducting states. By combining our experimental results with quasiclassical theory, we demonstrate that interface conductance plays a key role in determining the strength and coherence length of pairing correlations and inter-island coupling. Our findings provide new insights into the design of novel superconducting states and the control of their properties.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Probing Cooper pair momentum by quasiparticle steering with planar Josephson junctions

    cond-mat.mes-hall 2026-07 accept novelty 6.0 of 10

    Quasiparticles eject from ballistic planar Josephson junctions at a phase-controlled angle scaling as √(Δ/μ), providing a kinematic probe of condensate momentum transfer.

  2. Local control of parity and charge in nanoscale superconducting lead islands

    cond-mat.mes-hall 2025-07 conditional novelty 6.0 of 10

    In lead islands smaller than about 12 nm radius, Coulomb charging energy exceeds the pairing gap, enabling stable odd-parity ground states that can be locally tuned with STM voltage pulses.

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