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Electron-Phonon Decoupling in Two Dimensions

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George McArdle, Igor V. Lerner

Mesoscale and Nanoscale Physics · Submitted 26 Jan 2022

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We show that such an electron-phonon decoupling may happen in suspended films and it manifests itself via a bistability in the electron temperature.

how it is stated · hedged possibility 0.91 read the record →

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arXiv ID2201.10882 (version 1)
Pith IDIWFDWB56, Pith's permanent record of this paper and its review
CitationGeorge McArdle, Igor V. Lerner. "Electron-Phonon Decoupling in Two Dimensions." arXiv:2201.10882 (2022). https://pith.science/paper/IWFDWB56
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The compiled record

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 3,740 input tokens.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.82 · human participants 0.01 · controlled comparison 0.09 · randomized assignment 0.01 · states quantitative result 0.13 · compares with prior results 0.22 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

In order to observe many-body localisation in electronic systems, decoupling from the lattice phonons is required, which is possible only in out-of-equilibrium systems. We show that such an electron-phonon decoupling may happen in suspended films and it manifests itself via a bistability in the electron temperature. By studying the electron-phonon cooling rate in disordered, suspended films with two-dimensional phonons, we derive the conditions needed for such a bistability, which can be observed experimentally through hysteretic jumps of several orders of magnitude in the nonlinear current-voltage characteristics. We demonstrate that such a regime is achievable in systems with an Arrhenius form of the equilibrium conductivity, while practically unreachable in materials with Mott or Efros-Shklovskii hopping.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 In order to observe many-body localisation in electronic systems, decoupling from the lattice phonons is required, which is possible only in out-of-equilibrium systems. background 1.00 0.07 0.08 asserted 0.99
s1 We show that such an electron-phonon decoupling may happen in suspended films and it manifests itself via a bistability in the electron temperature. result 0.78 0.85 0.63 hedged possibility 0.91
s2 By studying the electron-phonon cooling rate in disordered, suspended films with two-dimensional phonons, we derive the conditions needed for such a bistability, which can be observed experimentally through hysteretic jumps of several orders of magnitude in the nonlinear current-voltage characteristics. contribution 0.52 0.95 0.34 asserted 0.99
s3 We demonstrate that such a regime is achievable in systems with an Arrhenius form of the equilibrium conductivity, while practically unreachable in materials with Mott or Efros-Shklovskii hopping. result 0.92 0.84 0.27 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.99.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

In order to observe many-body localisation in electronic systems, decoupling from the lattice phonons is required, which is possible only in out-of-equilibrium systems. We show that such an electron-phonon decoupling may happen in suspended films and it manifests itself via a bistability in the electron temperature. By studying the electron-phonon cooling rate in disordered, suspended films with two-dimensional phonons, we derive the conditions needed for such a bistability, which can be observed experimentally through hysteretic jumps of several orders of magnitude in the nonlinear current-voltage characteristics. We demonstrate that such a regime is achievable in systems with an Arrhenius form of the equilibrium conductivity, while practically unreachable in materials with Mott or Efros-Shklovskii hopping.

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