Pith. sign in

REVIEW 1 major objections 2 minor 26 references

Tomography of Transport Pathways in Selective-Area-Grown Nanowires Using Angle-Resolved Conductance Fluctuations

T0 review · 1 major / 2 minor · reviewed 2026-06-26 · grok-4.3

Challenge this review Re-run · record.json Download PDF Read on arXiv ↗ Review JSON

Pith's one-line read Conductance fluctuations show transport in InAs nanowires is dominated by a near-surface accumulation layer.

desk verdict The paper shows conductance fluctuation tomography can map phase-coherent paths in selective-area InAs nanowires, with data favoring near-surface accumulation layer transport over bulk or single-facet pictures. read the letter →

arxiv 2606.23053 v1 pith:RHVLTWIR submitted 2026-06-22 cond-mat.mes-hall

Christian E. N. Petersen , Damon J. Carrad , Daria Beznasyuk , Thomas S. Jespersen This is my paper · ORCID
classification cond-mat.mes-hall
keywords InAsnanowiresselectiveareagrowthconductancefluctuationstransporttomographynear-surfaceaccumulationphase-coherentnanowiredevicesmagneticfieldorientation
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

The paper applies conductance fluctuation tomography to planar selective-area-grown InAs nanowires in normal-normal and normal-superconductor geometries. By tracking how interference features evolve with magnetic field strength and orientation, the work maps the geometry of phase-coherent carrier paths. Data match a picture in which carriers concentrate in a thin near-surface layer rather than the wire bulk. Normal-contact devices display coherent crossing of the apex while hybrid devices show more facet-specific signatures. This matters because carrier location directly shapes how nanoscale devices conduct and interfere.

What carries the argument

Conductance fluctuation tomography, which extracts transport geometry from the evolution of conductance-interference features versus magnetic-field strength and orientation.

What would settle it

Conductance fluctuation patterns that instead match bulk-transport predictions across multiple field orientations and strengths would falsify the near-surface accumulation claim.

Watch

Extended reading notes

Core claim

Using theory to distinguish between bulk-dominated transport, coherent near-surface transport across facets, and transport confined to individual facets, the measurements are consistent with transport dominated by a near-surface accumulation layer in InAs. Devices with normal contacts show behavior consistent with coherent transport across the nanowire apex, whereas hybrid normal-superconductor devices exhibit signatures of more facet-dependent transport. These results demonstrate how universal conductance fluctuations can be used as a tomographic probe of phase-coherent transport pathways in semiconductor nanostructures.

Load-bearing premise

Theoretical modeling of conductance-interference evolution with magnetic-field strength and orientation can reliably distinguish bulk-dominated transport from coherent near-surface transport across facets and from transport confined to individual facets.

Editorial extensions

If this is right

  • Transport in these InAs nanowires occurs mainly through a near-surface accumulation layer.
  • Normal-contact devices permit coherent transport that crosses the nanowire apex.
  • Hybrid normal-superconductor devices display transport signatures tied more closely to individual facets.
  • Universal conductance fluctuations function as a tomographic probe of phase-coherent pathways in semiconductor nanostructures.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The same angle-resolved method could be tested on nanowires of other materials to check whether surface-layer dominance is general.
  • Facet dependence observed in hybrid devices suggests surface engineering may be needed to control interference in topological setups.
  • The technique offers a contact-based way to characterize internal transport geometry without requiring direct spatial imaging.
Share X Bluesky LinkedIn Reddit HN

Signed reviews

No signed human review yet.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

1 major / 2 minor

Summary. The manuscript applies conductance fluctuation tomography to selective-area-grown InAs nanowires in normal-normal and normal-superconductor geometries. By tracking the evolution of interference features versus magnetic-field strength and orientation, the authors use theory to distinguish bulk-dominated, coherent near-surface (across facets), and facet-confined transport, concluding that a near-surface accumulation layer dominates. NN devices are interpreted as showing apex-coherent transport while NS devices show more facet-dependent behavior.

Significance. If the theoretical mapping from fluctuation patterns to geometry is robust, the work offers a tomographic probe of phase-coherent pathways that could be useful for characterizing carrier distributions in semiconductor nanowires without invasive imaging. The dual NN/NS comparison provides an internal consistency check on the interpretation.

major comments (1)
  1. [Theory and comparison sections] The central claim that the data support near-surface accumulation-layer transport (rather than bulk or single-facet confinement) rests on the theoretical modeling of interference evolution with B-field strength and orientation. The manuscript must demonstrate that this mapping is unique by showing explicit theory curves, parameter sensitivity, or goodness-of-fit metrics that rule out alternative geometries for the selective-area-grown cross-section; without such evidence the distinction remains under-determined.
minor comments (2)
  1. Clarify the precise definition of 'angle-resolved' conductance fluctuations and how the magnetic-field orientation is controlled experimentally.
  2. Include error bars or statistical measures on the extracted interference features to allow assessment of the robustness of the regime distinctions.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their detailed review and constructive criticism. The point raised about demonstrating the uniqueness of the theoretical mapping is well taken, and we will strengthen the manuscript accordingly.

read point-by-point responses

  1. Referee: [Theory and comparison sections] The central claim that the data support near-surface accumulation-layer transport (rather than bulk or single-facet confinement) rests on the theoretical modeling of interference evolution with B-field strength and orientation. The manuscript must demonstrate that this mapping is unique by showing explicit theory curves, parameter sensitivity, or goodness-of-fit metrics that rule out alternative geometries for the selective-area-grown cross-section; without such evidence the distinction remains under-determined.

    Authors: We agree that the current presentation of the theoretical modeling would benefit from more explicit comparisons to establish uniqueness. The manuscript already contains calculations distinguishing bulk, near-surface, and single-facet regimes, but we acknowledge that additional figures showing full theory curves for each geometry, parameter sensitivity analysis, and quantitative goodness-of-fit metrics are needed to rigorously rule out alternatives. In the revised version we will add these elements to the theory and comparison sections, including supplementary material with the requested plots and metrics for the selective-area-grown cross-section. revision: yes

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity; experimental claims rest on data-theory comparison without self-referential reduction.

full rationale

The paper is an experimental study of conductance fluctuations in selective-area-grown InAs nanowires. It reports measurements in NN and NS device geometries and states that theory is used to interpret the evolution of interference features with magnetic field strength and orientation, leading to the conclusion of near-surface accumulation layer transport. No equations, fitted parameters renamed as predictions, or self-citations are present in the abstract or described text that would make the central claims equivalent to their inputs by construction. The distinction between bulk, near-surface, and facet-confined transport is presented as arising from external theoretical modeling applied to the data, rendering the derivation self-contained.

Assumptions & free parameters 0 free parameters · 0 assumptions · 0 invented entities

Abstract-only review provides no explicit free parameters, axioms, or invented entities; all such elements remain unknown.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Tomography of Transport Pathways in Selective-Area-Grown Nanowires Using Angle-Resolved Conductance Fluctuations." pith.science (2026). https://pith.science/paper/RHVLTWIR

@misc{pith2026260623053,
  author       = {Pith},
  title        = {Pith review of: Tomography of Transport Pathways in Selective-Area-Grown Nanowires Using Angle-Resolved Conductance Fluctuations},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/RHVLTWIR}},
  note         = {Machine review of arXiv:2606.23053}
}
read the original abstract

Understanding the spatial distribution of carriers is important for interpreting transport in nanoscale devices. Here, we apply conductance fluctuation tomography to planar selective-area-grown InAs nanowires in both normal-normal and normal-superconductor device geometries. By tracking the evolution of conductance-interference features as a function of magnetic-field strength and orientation, we extract information about the geometry of phase-coherent transport pathways. Using theory to distinguish between bulk-dominated transport, coherent near-surface transport across facets, and transport confined to individual facets. The measurements are consistent with transport dominated by a near-surface accumulation layer in InAs. Devices with normal contacts show behavior consistent with coherent transport across the nanowire apex, whereas hybrid normal-superconductor devices exhibit signatures of more facet-dependent transport. These results demonstrate how universal conductance fluctuations can be used as a tomographic probe of phase-coherent transport pathways in semiconductor nanostructures.

Figures

Figures reproduced from arXiv: 2606.23053 by the authors.

Figure 1
Figure 1. b defines the angles φ1, φ2, φ3 used to describe [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. FIG. 2. Differential conductance for Device NS ( [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. FIG. 3. Differential conductance for Device NN ( [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

26 extracted references

  1. [1]

    Krizek, J

    F. Krizek, J. E. Sestoft, P. Aseev, S. Marti-Sanchez, S. Vaitiek˙ enas, L. Casparis, S. A. Khan, Y. Liu, T. c. v. Stankeviˇ c, A. M. Whiticar, A. Fursina, F. Boekhout, R. Koops, E. Uccelli, L. P. Kouwenhoven, C. M. Mar- cus, J. Arbiol, and P. Krogstrup, Phys. Rev. Mater.2, 093401 (2018)

    2018

  2. [3]

    Olˇ steins, G

    D. Olˇ steins, G. Nagda, D. J. Carrad, D. V. Beznasyuk, C. E. Petersen, S. Mart´ ı-S´ anchez, J. Arbiol, and T. S. Jespersen, Nature communications14, 7738 (2023)

    2023

  3. [4]

    Olsteins, G

    D. Olsteins, G. Nagda, D. J. Carrad, D. V. Beznasyuk, C. E. N. Petersen, S. Mart´ ı-S´ anchez, J. Arbiol, and T. S. Jespersen, Nano Letters24, 6553–6559 (2024)

    2024

  4. [5]

    Alicea, Y

    J. Alicea, Y. Oreg, G. Refael, F. Von Oppen, and M. P. Fisher, Nature Physics7, 412 (2011)

    2011

  5. [6]

    Nadj-Perge, S

    S. Nadj-Perge, S. M. Frolov, E. P. A. M. Bakkers, and L. P. Kouwenhoven, Nature468, 1084–1087 (2010)

    2010

  6. [7]

    W. Peng, Z. Aksamija, S. A. Scott, J. J. Endres, D. E. Savage, I. Knezevic, M. A. Eriksson, and M. G. Lagally, Nature Communications4, 1339 (2013)

    2013

  7. [8]

    J. W. W. van Tilburg, R. E. Algra, G. Immink, M. A. Verheijen, E. P. A. M. Bakkers, and L. P. Kouwenhoven, Semiconductor Science and Technology 25, 024011 (2010)

    2010

  8. [9]

    Wang and M

    J. Wang and M. S. Gudiksen, Nanotechnology24, 375202 (2013)

    2013

Show all 26 references
  1. [10]

    L. O. Olsson, C. B. M. Andersson, M. C. H˚ akansson, J. Kanski, L. Ilver, and U. O. Karlsson, Phys. Rev. Lett. 76, 3626 (1996)

    1996

  2. [11]

    Dayeh, D

    S. Dayeh, D. P. Aplin, X. Zhou, P. K. Yu, E. Yu, and D. Wang, Small3, 326 (2007)

    2007

  3. [12]

    A. C. Ford, J. C. Ho, Y.-L. Chueh, Y.-C. Tseng, Z. Fan, J. Guo, J. Bokor, and A. Javey, Nano Letters9, 360 (2009)

    2009

  4. [13]

    V. E. Degtyarev, S. V. Khazanova, and N. V. Demarina, Scientific Reports7, 3411 (2017)

    2017

  5. [14]

    Gupta, IEEE Transactions on Electron Devices41, 2093 (1994)

    M. Gupta, IEEE Transactions on Electron Devices41, 2093 (1994)

  6. [15]

    P. A. Lee and A. D. Stone, Physical Review Letters55, 1622 (1985), publisher: American Physical Society

    1985

  7. [16]

    Imry, Europhysics Letters1, 249 (1986)

    Y. Imry, Europhysics Letters1, 249 (1986)

    1986

  8. [17]

    P. A. Mello, Physical Review Letters60, 1089 (1988), publisher: American Physical Society

    1988

  9. [18]

    P. A. Lee, A. D. Stone, and H. Fukuyama, Physical Re- view B35, 1039 (1987), publisher: American Physical Society

    1987

  10. [19]

    C. W. J. Beenakker, Reviews of Modern Physics69, 731 (1997), publisher: American Physical Society

    1997

  11. [20]

    Scheer, H

    E. Scheer, H. von L¨ ohneysen, A. D. Mirlin, P. W¨ olfle, and H. Hein, Physical Review Letters78, 3362 (1997)

    1997

  12. [21]

    Liang, J

    D. Liang, J. Du, and X. P. A. Gao, Phys. Rev. B81, 153304 (2010)

    2010

  13. [22]

    F. Haas, T. Wenz, P. Zellekens, N. Demarina, T. Rieger, M. Lepsa, D. Gr¨ utzmacher, H. L¨ uth, and T. Sch¨ apers, Scientific Reports6, 24573 (2016)

    2016

  14. [23]

    T. S. Jespersen, J. R. Hauptmann, C. B. Sørensen, and J. Nyg˚ ard, Phys. Rev. B91, 041302 (2015)

    2015

  15. [24]

    D. V. Beznasyuk, S. Mart´ ı-S´ anchez, J.-H. Kang, R. Tanta, M. Rajpalke, T. c. v. Stankeviˇ c, A. W. Chris- tensen, M. C. Spadaro, R. Bergamaschini, N. N. Maka, C. E. N. Petersen, D. J. Carrad, T. S. Jespersen, J. Ar- biol, and P. Krogstrup, Phys. Rev. Mater.6, 034602 (2022)

    2022

  16. [25]

    Trevisan, P

    A. Trevisan, P. D. Hodgson, F. Alvarado-C´ esar, M. Hayne, R. Beanland, and P. M. Koenraad, Journal of Applied Physics137, 195702 (2025)

    2025

  17. [26]

    M. E. n. Cachaza, A. W. Christensen, D. Beznasyuk, T. Særkjær, M. H. Madsen, R. Tanta, G. Nagda, S. Schuwalow, and P. Krogstrup, Phys. Rev. Mater.5, 094601 (2021)

    2021

  18. [27]

    C. W. J. Beenakker, Physical Review B47, 15763 (1993), publisher: American Physical Society. Supplemental Material for: Tomography of Transport Pathways in Selective-Area-Grown Nanowires Using Angle-Resolved Conductance Fluctuations Christian E. N. Petersen, 1,∗ Damon J. Carra...

    1993

Pith tools

Reviewed June 26, 2026 · model on record in the stance chip above.