Two-dimensional hydrodynamic viscous electron flow in annular Corbino rings
Pith reviewed 2026-05-24 00:38 UTC · model grok-4.3
The pith
Nonlocal voltages in annular Corbino rings indicate viscous hydrodynamic electron flow far from the source-drain region.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In concentric annular rings formed in high-mobility GaAs/AlGaAs 2DEGs, nonlocal electronic transport measurements strongly suggest that viscous hydrodynamic flow occurs far away from the source-drain current region. This is corroborated by Navier-Stokes equation simulations that agree with the data below 1 K temperature. The work emphasizes the key role played by viscosity via electron-electron interactions when hydrodynamic transport is restricted radially.
What carries the argument
The annular Corbino ring geometry, which confines electron flow radially and enables detection of nonlocal voltages to reveal viscosity effects distant from current injection.
If this is right
- Viscous flow can be detected through nonlocal signals even in regions without direct source-drain current.
- Electron viscosity via electron-electron interactions remains dominant under radial geometric restriction.
- Navier-Stokes simulations accurately capture the transport without geometry-specific fitting parameters below 1 K.
- Hydrodynamic behavior in 2DEGs extends to annular structures where radial confinement applies.
Where Pith is reading between the lines
- Similar nonlocal signatures might appear in other curved or ring-based 2D devices if viscosity dominates.
- The approach could be adapted to test radial confinement effects in higher-mobility samples or different materials.
- Device designs using annular electrodes might exploit viscosity for flow control in restricted geometries.
Load-bearing premise
The observed nonlocal voltages arise specifically from viscous hydrodynamic flow rather than from ballistic trajectories, impurity scattering, or other non-hydrodynamic mechanisms.
What would settle it
Nonlocal voltage data from the annular rings that match predictions from ballistic transport models while deviating from Navier-Stokes simulations below 1 K.
Figures
read the original abstract
The concept of fluidic viscosity is ubiquitous in our everyday life and for it to arise the fluidic medium must necessarily form a continuum where macroscopic properties can emerge. While a powerful concept for tangible liquids, hydrodynamic manifestation of collective flow in electronic systems such as two-dimensional electron gases (2DEGs) has only been shown recently to occur in graphene and GaAs/AlGaAs. Here, we present nonlocal electronic transport measurements in concentric annular rings formed in high-mobility GaAs/AlGaAs 2DEGs and the resulting data strongly suggest that viscous hydrodynamic flow can occur far away from the source-drain current region. Our conclusion of viscous electronic transport is further corroborated by simulations of the Navier-Stokes equations that are found to be in agreement with our measurements below 1K temperature. Most importantly, our work emphasizes the key role played by viscosity via electron-electron (e-e) interaction when hydrodynamic transport is restricted radially, and for which a priori should not have played a major role.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper reports nonlocal voltage measurements in concentric annular Corbino rings fabricated in high-mobility GaAs/AlGaAs 2DEGs. It claims that the observed nonlocal signals far from the source-drain current path indicate viscous hydrodynamic electron flow driven by electron-electron interactions, with the radial confinement playing a key role; this interpretation is supported by agreement between the data and Navier-Stokes simulations below 1 K.
Significance. If the hydrodynamic interpretation is uniquely established, the work would provide evidence that viscosity remains important even when transport is radially restricted in annular geometries, extending prior demonstrations of electron hydrodynamics in graphene and GaAs beyond standard Hall-bar or point-contact setups.
major comments (2)
- [Results and Discussion sections (comparison to simulations)] The central claim that the nonlocal voltages arise specifically from viscous flow (rather than ballistic trajectories or impurity scattering) rests on agreement with Navier-Stokes simulations below 1 K, yet the manuscript provides no side-by-side ballistic (Landauer-Büttiker or Monte-Carlo) calculation for the identical contact layout, mobility, and annular geometry. Without this comparison, the NS match is consistent with hydrodynamics but does not exclude non-viscous mechanisms, particularly given that the elastic mean free path in these 2DEGs often exceeds the ring radii.
- [Abstract and experimental results section] The abstract states agreement with Navier-Stokes simulations below 1 K, but the text supplies no quantitative details on data exclusion criteria, error bars, baseline subtraction, number of devices measured, or how the nonlocal voltages are extracted from raw data. This absence prevents independent verification of the claimed agreement and the temperature threshold.
minor comments (1)
- [Methods/Figure 1] Notation for the annular radii and contact placements should be defined explicitly with a diagram in the methods or results section to allow direct comparison with any future ballistic simulations.
Simulated Author's Rebuttal
We thank the referee for their thorough review and valuable feedback on our manuscript. Below we provide point-by-point responses to the major comments. We have revised the manuscript accordingly to strengthen the presentation of our results and address the concerns raised.
read point-by-point responses
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Referee: [Results and Discussion sections (comparison to simulations)] The central claim that the nonlocal voltages arise specifically from viscous flow (rather than ballistic trajectories or impurity scattering) rests on agreement with Navier-Stokes simulations below 1 K, yet the manuscript provides no side-by-side ballistic (Landauer-Büttiker or Monte-Carlo) calculation for the identical contact layout, mobility, and annular geometry. Without this comparison, the NS match is consistent with hydrodynamics but does not exclude non-viscous mechanisms, particularly given that the elastic mean free path in these 2DEGs often exceeds the ring radii.
Authors: We appreciate the referee highlighting the importance of distinguishing hydrodynamic from ballistic transport. Our interpretation relies on the temperature-dependent onset of the nonlocal signal below 1 K, coinciding with the regime where electron-electron interactions dominate (as indicated by the mobility and known scattering rates in GaAs 2DEGs). In the ballistic regime, the annular geometry with radial confinement would primarily support azimuthal flow or direct paths, but the observed radial nonlocal voltages are characteristic of viscous momentum diffusion. In the revised manuscript, we have added a discussion paragraph explaining this distinction and why impurity scattering alone cannot account for the signals far from the current path. A complete side-by-side Monte-Carlo simulation for the exact geometry is not included as it would require significant additional computational resources, but we believe the existing evidence supports the hydrodynamic claim. revision: partial
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Referee: [Abstract and experimental results section] The abstract states agreement with Navier-Stokes simulations below 1 K, but the text supplies no quantitative details on data exclusion criteria, error bars, baseline subtraction, number of devices measured, or how the nonlocal voltages are extracted from raw data. This absence prevents independent verification of the claimed agreement and the temperature threshold.
Authors: We regret the omission of these important experimental details in the initial submission. The revised manuscript now includes an expanded 'Methods' section and additional information in the 'Results' section. Specifically, we detail: the measurement of three devices; the extraction of nonlocal voltages using AC lock-in detection with subtraction of any DC offsets; error bars as the standard error from repeated measurements at each temperature; baseline subtraction performed by fitting and removing the high-temperature (above 4 K) background where viscous effects are absent; and exclusion criteria based on sample stability and contact quality. These additions enable independent verification of the data and the agreement with simulations below 1 K. revision: yes
Circularity Check
No circularity: experimental data compared to independent Navier-Stokes simulations
full rationale
The manuscript reports nonlocal voltage measurements in annular GaAs 2DEG rings and states that Navier-Stokes simulations agree with the data below 1 K. No derivation equations, fitted parameters, or self-citations are shown that reduce the reported voltages or the hydrodynamic interpretation to quantities extracted from the same dataset by construction. The central claim rests on direct experimental observation plus external simulation comparison rather than any self-definitional, fitted-input, or self-citation-load-bearing step. This is the most common honest finding for primarily experimental work with independent numerical validation.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Navier-Stokes equations apply to collective electron flow in high-mobility 2DEGs at low temperature
Lean theorems connected to this paper
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IndisputableMonolith/Foundation/ArithmeticFromLogic.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Navier-Stokes equation ... ν ∇²u + f ... ur ∝ 1/r, ϕ ∝ τ⁻¹ log(r)
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
viscosity ν = v_f ℓ_MC /4 ... Gurzhi effect ... Knudsen number ζ ≲ 1
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
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These two wafers have GaAs substrates that are 700 nm thick
Heterostructure The devices used in the manuscript were fabricated on two different wafers, each with a different heterostructure as shown in Fig.S1. These two wafers have GaAs substrates that are 700 nm thick. The heterostructure is deposited on top of the substrate, with spacer material acting as a buffer between layers. The distance between the dopant ...
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Measurement circuits 2.1. Local measurement Circuit The circuit in local transport measurements, depicted in Fig.S2, consists of an SR830 lock-in amplifier, a 10 MΩ resistor and a SR560 pre-amplifier. It is a basic resistance measurement setup, where a fixed current is applied and the voltage difference is measured across the device. In this setup, an AC ...
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Probe symmetry To further confirm the results presented in Fig.2 of the main text, we also conducted nonlocal transport measure- ments using different probe configurations. The data obtained for both CBM301 and CBM302 at base temperature and zero magnetic fields ( B = 0 T ) are shown in Fig.S4. The results show that all probe symmetries are respected in b...
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[41]
Navier-Stokes in hydrodynamics 4.1. Length scales As mentioned in the main text, the length scale conditions for hydrodynamic transport are ℓM C ≪ W ≪ ℓM R, where W is channel width, ℓM C is momentum conserving scattering mean-free path (in our case the e − e scattering), and lM R is momentum relaxing scattering mean-free path. At low temperatures (T < 1 ...
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[42]
Simulation Numerical simulations of Eq.S8-S9 were performed in Python via Finite-Difference Method (FDM) in the 2D polar coordinate system. In FDM, first-order and second-order spatial derivatives are discretized using the central difference approximation, ∂f ∂x ≈ f(x + h) − f(x − h) 2h + O(h2), (S17) ∂2f ∂x2 ≈ f(x + h) + f(x − h) − 2f(x) h2 + O(h2). (S18...
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In this regime, the output would be proportional to the root-mean-square value measured by our lock-in by the same factor. To confirm our quasi-DC model, we performed AC simulations by simulating uniformly spaced points in our signal period. We then performed a root-mean-square calculation of our AC data points, which yielded nearly identical results to t...
work page 2023
discussion (0)
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