The 0.7 anomaly — an interaction-induced conductance shoulder near 0.7×(2e2/h)0.7\times(2e^2/h) that appears below the first quantized plateau of a quantum point contact — has resisted a unanimously accepted microscopic explanation since its observation. Smith et al. (Phys. Rev. B 90, 045426 (2014)) measured an ensemble of 98 clean devices defined from a 256-gate array and found that the conductance of the 0.7 structure, G0.7G_{0.7}, varies from device to device (0.63–0.84 in units of 2e2/h2e^2/h) without significant correlation with any extracted microscopic parameter, and identified the questions that ensemble statistics must answer: which parameters govern G0.7G_{0.7}, how to separate disorder from intrinsic many-body physics, whether the device-to-device spread survives thermal cycling, and whether reduced-disorder (undoped, high-mobility) platforms narrow it — jointly, whether any theoretical model of the anomaly can be validated or falsified by ensemble statistics. The objective is to determine, by ensemble statistics over nominally identical one-dimensional quantum wires, which microscopic parameters govern G0.7G_{0.7} and which candidate mechanism — spontaneous spin polarization, a quasi-bound Kondo-like state, Wigner/spin-incoherent strong correlations, or interaction-enhanced transmission via the 1D van Hove ridge — the ensemble data validate or falsify.

Background

A quantum point contact (QPC) is a short, narrow constriction connecting two reservoirs of a two-dimensional electron gas (2DEG), itself a layer of mobile electrons confined at a semiconductor heterointerface (typically GaAs/AlGaAs). When the constriction width is comparable to the electron wavelength, transverse modes are quantized, and the two-terminal conductance rises in steps of the conductance quantum 2e2/h2e^2/h as gate voltage opens successive modes (the Landauer picture of conductance as quantum transmission). Since the mid-1990s, an additional shoulder has repeatedly been observed at roughly 0.7×(2e2/h)0.7\times(2e^2/h), below the first plateau — the "0.7 anomaly" (also called the 0.7 structure; an early and widely cited report is Thomas et al., Phys. Rev. Lett. 77, 135 (1996)). It is strongest at elevated temperature and low carrier density, evolves with increasing magnetic field toward 0.5×(2e2/h)0.5\times(2e^2/h), and several incompatible microscopic explanations coexist: spontaneous spin polarization driven by the exchange-enhanced density of states near a smooth barrier; a quasi-bound Kondo-like state acting as a magnetic moment coupled to channel electrons; Wigner-crystal regimes (electrons arranging into an ordered array at very low density) or spin-incoherent regimes (charge moves coherently while the spin degrees of freedom remain disordered) of strong one-dimensional (1D) correlations; and, more recently, models in which the 1D van Hove ridge — the divergence of the density of states at the bottom of each 1D subband at the saddle point of the constriction potential — combined with short-range electron–electron interactions enhances transmission near the band edge without spin order. Single-device experiments have not discriminated among these mechanisms, because each model can be tuned to reproduce one device's phenomenology.

The source paper (Smith et al., Phys. Rev. B 90, 045426 (2014); arXiv:1407.7441) took a statistical approach: using on-chip cryogenic multiplexing (integrated switching circuits that let many devices be measured through a small number of cryostat wiring lines) to address a lithographically identical array of 256 one-dimensional quantum wires, each defined by a split gate — a pair of surface gate electrodes whose negative voltage depletes the electron gas beneath it, leaving a narrow channel — and screening disorder, it extracted per-device parameters: the barrier curvature ℏωx\hbar\omega_x (Ex=ℏωxE_x=\hbar\omega_x, the curvature of the saddle-shaped potential barrier in the transport direction, in harmonic units; the 1D subband spacing ΔE1,2\Delta E_{1,2} is a distinct measured quantity, set by the transverse confinement), 1D carrier density, the gate voltages at which the channel pinches off (pinch-off voltage) and first shows one-dimensional transport (1D-definition voltage), and features of the 0.7 structure. For the 36 devices with a resolvable 0.7 feature at 1.4 K and zero magnetic field, G0.7G_{0.7} ranged from 0.63 to 0.84 (in units of 2e2/h2e^2/h), and no significant correlation (∣r∣≤0.33|r|\le 0.33) was found with any extracted parameter — though the ℏωx\hbar\omega_x estimates carried lever-arm (αn\alpha_n) errors, computed from an average conversion between gate voltage and subband energy, that could mask intrinsic correlations. The paper's conclusion explicitly lists what ensemble statistics still must deliver: per-device dc-bias spectroscopy (measuring differential conductance versus source–drain bias voltage, whose nonlinear structure resolves the subband spacings and lever arms) to pin down the lever arms and barrier curvatures; magnetic-field- and temperature-dependent measurements on large ensembles to disentangle disorder from intrinsic many-body physics (disorder effects can be masked at the single operating temperature of 1.4 K); dedicated studies of reproducibility under thermal cycling, to separate stable device-to-device variations from thermally history-dependent ones; and measurements on higher-mobility or undoped heterostructures with electrostatically induced 2DEGs, to reduce dopant-induced potential fluctuations. The overarching goal is to determine whether any specific theoretical model of the 0.7 anomaly can be validated or falsified by ensemble statistics. A companion methodology line (e.g. Lesage et al., J. Appl. Phys. 117, 015704 (2015)) developed automated extraction of level spacings and lever arms from dc-bias spectroscopy, the per-device characterization the source paper called for.

Subsequent work has advanced and partly tested this program. Follow-up studies by the same collaboration established the barrier curvature ℏωx\hbar\omega_x as the primary governing parameter at zero field and 1.4 K, and demonstrated the measurement methodologies the source paper called for (per-device dc-bias spectroscopy, thermal-cycling reproducibility, and undoped architectures). Ma et al. (Chip 3, 100095 (2024)) executed the first large-scale ensemble model-discrimination study — 571 quantum point contacts measured at two temperatures across 12 cooldowns — reporting that the spontaneous-spin-polarization and Kondo-like models do not fit their data while some features largely agree with an interacting van-Hove-ridge model. That claim is single-group, lacks magnetic-field-resolved ensemble statistics, and is contested by continuing single-device and cross-platform experiments.

Problem Statement

Determine, by ensemble statistics over nominally identical one-dimensional quantum wires, which microscopic parameters or parameter combinations deterministically govern the conductance G0.7G_{0.7} of the 0.7 anomaly, and whether any proposed theoretical mechanism for the anomaly — spontaneous spin polarization, a quasi-bound Kondo-like state, Wigner/spin-incoherent strong correlations, or interaction-enhanced transmission via the 1D van Hove ridge — is validated or falsified by such statistics. Concretely, following the open issues stated by Smith et al. (Phys. Rev. B 90, 045426 (2014)) and the subsequent state of the art: (i) extract per-device lever arms, subband spacings, and barrier curvatures by per-device dc-bias spectroscopy rather than ensemble-averaged conversion, and test which parameters (including the barrier curvature ℏωx\hbar\omega_x and the curvature ratio Ey/ExE_y/E_x, the ratio of transverse to longitudinal confinement energies at the saddle point of the constriction) the 0.7 conductance and its strength correlate with; (ii) perform magnetic-field- and temperature-dependent measurements across large device ensembles to disentangle disorder effects from intrinsic many-body physics, using as discriminators the magnetic-field dependence (the spin gap splitting the rising flank of the conductance step toward 0.5×(2e2/h)0.5\times(2e^2/h) under spontaneous spin polarization, versus an orbital or interaction-driven field response) and the sign of the temperature dependence (Kondo-like growth at low temperature versus its opposite); (iii) establish by thermal-cycling studies which device-to-device variations are stable and which are cooldown-history dependent; and (iv) repeat the statistics on higher-mobility or undoped, electrostatically induced 2DEG platforms to test whether residual disorder or dopant-induced fluctuations dominate the spread in confinement parameters. These four components jointly serve the single objective of the source program: to decide, at the ensemble level, which model of the 0.7 anomaly — if any — the data sustain, including confirmation or refutation of the claim by Ma et al. (Chip 3, 100095 (2024)) that the ensemble data favor the interacting van-Hove-ridge model over the spin-polarization and Kondo alternatives. The single deliverable is that determination: components (i)–(iv) are the evidence axes on which it must be argued, not separately required experiments.

References

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