Evidence of Coulomb liquid phase in a few-electron droplets

ORAL

Abstract

In physics, correlations in fluctuating microscopic observables can provide key information about collective states of matter, such as the quark-gluon plasma formed in heavy-ion collisions (Science 332, 1525, 2011) or expanding quantum degenerate gases (Science 296, 1703, 1999). Mesoscopic colliders, through shot-noise measurements, have provided smoking-gun evidence on the nature of exotic electronic excitations such as fractional charges, levitons and anyon statistics. Yet, bridging the gap between two-particle collisions and the emergence of collectivity as the number of interacting particles increases remains a challenging task at the microscopic level.

 In this presentation we demonstrate all-body correlations in the partitioning of electron droplets containing up to 5 electrons, driven by a moving potential well through a Y-junction in a semiconductor device. Analyzing the partitioning data using high-order multivariate cumulants and finite-size scaling towards the thermodynamic limit reveals distinctive fingerprints of a strongly-correlated Coulomb liquid  (Nature 642, 928, 2025) . These fingerprints agree well with a universal limit where the partitioning of a droplet is predicted by a single collective variable. Our electron-droplet collider reveals the intricate interplay between confinement and interaction effects in few-electron systems, establishing a novel approach to probe engineered states of matter. This platform opens new avenues to study strongly correlated and coherent many-body phenomena in mesoscopic systems.

*This work was supported by  EQUBITFLY project. 

Publication: J. Shaju et al., Nature 642, 928 (2025)

Presenters

  • JASHWANTH SHAJU

    • Institut Néel-CNRS & Université Grenoble Alpes

Authors

  • JASHWANTH SHAJU

    • Institut Néel-CNRS & Université Grenoble Alpes
  • Elina Pavlovska

    • Department of Physics, University of Latvia, Riga, LV-1004, Latvia
  • Ralfs Suba

    • Department of Physics, University of Latvia, Riga, LV-1004, Latvia
  • Junliang Wang

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
  • Seddik Ouacel

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
  • Thomas Vasselon

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
  • Matteo Aluffi

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
  • Lucas Mazzella

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
  • Clément Geffroy

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel
  • Arne Ludwig

    • Lehrstuhl für Angewandte Festkörperphysik, Ruhr-Universität Bochum, Universitätsstrasse 150, D-44780 Bochum, Germany
  • Andreas D Wieck

    • Lehrstuhl für Angewandte Festkörperphysik, Ruhr-Universität Bochum, Universitätsstrasse 150, D-44780 Bochum, Germany
  • Matias Urdampilleta

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
    • CNRS
    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel
    • Univ. Grenoble Alpes, CNRS, Grenoble INP, Néel Institut, 38000 Grenoble, France
  • Christopher Bäuerle

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France
  • Vyacheslavs Kashcheyevs

    • Department of Physics, University of Latvia, Riga, LV-1004, Latvia
  • Hermann Sellier

    • Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, F-38000 Grenoble, France