REVIEW 1 major objections 1 cited by
A single electron on solid neon forms a charge qubit with coherent microwave control at Rabi frequencies up to 76 MHz.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
2026-07-02 22:54 UTC pith:OMUXFSZP
load-bearing objection The 76 MHz Rabi frequency and NbTiN resonator are the clear new pieces; the single-electron claim rests on differential coupling without direct charge counting. the 1 major comments →
Fast coherent control of a charge qubit on solid neon with a spin-qubit-compatible resonator
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We couple a single electron on solid neon to a magnetic-field-compatible superconducting NbTiN nanowire resonator. We realize a charge qubit and demonstrate microwave readout and coherent control, with Rabi frequencies up to 76 MHz, an order of magnitude larger than in previous studies. Under strong driving, we observe a qubit frequency shift from nonlinear interactions with the intense microwave field. Deterministic electron trapping at an intended position remains challenging due to solid neon surface roughness; we characterize the electron's position from its differential coupling to distinct electrodes. Although not trapped at an intended position, our estimates indicate that spin-qubit
What carries the argument
The charge qubit formed by the two possible positions of a single electron on the neon surface, whose state is read out and driven through coupling to the NbTiN superconducting resonator.
Load-bearing premise
The microwave signals arise from a single electron whose position can be reliably inferred from differential electrode coupling despite surface roughness.
What would settle it
A direct position measurement or multi-electron signature that contradicts the inferred single-electron location while still producing the reported Rabi oscillations at 76 MHz.
If this is right
- Microwave readout becomes available for the electron charge state on solid neon.
- Coherent control reaches Rabi frequencies of 76 MHz, supporting faster operations.
- Nonlinear frequency shifts occur under strong microwave driving.
- Estimates show spin-qubit demonstrations on this platform remain feasible.
Where Pith is reading between the lines
- The same resonator architecture could support combined charge and spin control in one device.
- Surface preparation methods might be tested to achieve deterministic single-electron placement.
- Coupling the charge degree of freedom to spin could create hybrid qubits with tunable properties.
- Multi-electron versions of the platform could explore interactions without material defects.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports coupling a single electron on solid neon to a magnetic-field-compatible NbTiN nanowire resonator to realize a charge qubit. It demonstrates microwave readout and coherent control with Rabi frequencies reaching 76 MHz (an order of magnitude above prior work), observes a nonlinear qubit frequency shift under strong driving, and characterizes the electron position via differential electrode coupling despite challenges with deterministic trapping due to surface roughness. The authors conclude that spin-qubit demonstrations remain feasible based on their estimates.
Significance. If the single-electron assignment and position characterization hold, the work represents a meaningful advance for the solid-neon electron platform by delivering substantially faster coherent control and resonator compatibility with spin-qubit requirements. The nonlinear shift observation under strong driving is a notable experimental detail. The platform's isolation from material defects and potential for long coherence times would be strengthened by these results.
major comments (1)
- The headline claim of a single-electron charge qubit with quantified Rabi frequency and nonlinear shift rests on the resonator response arising from exactly one electron whose location is sufficiently known. The text states that deterministic trapping fails due to surface roughness and that position is inferred only from differential coupling to distinct electrodes. No independent charge-counting observable (e.g., discrete frequency jumps upon sequential loading) is described to exclude multi-electron configurations or a single electron in an unintended local minimum. This is load-bearing for interpreting the reported 76 MHz Rabi frequency and other extracted parameters as single-qubit properties. (See the sections on electron trapping, position characterization, and experimental results.)
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for identifying the key issue of single-electron assignment. We respond to the major comment below and indicate where revisions will be made.
read point-by-point responses
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Referee: The headline claim of a single-electron charge qubit with quantified Rabi frequency and nonlinear shift rests on the resonator response arising from exactly one electron whose location is sufficiently known. The text states that deterministic trapping fails due to surface roughness and that position is inferred only from differential coupling to distinct electrodes. No independent charge-counting observable (e.g., discrete frequency jumps upon sequential loading) is described to exclude multi-electron configurations or a single electron in an unintended local minimum. This is load-bearing for interpreting the reported 76 MHz Rabi frequency and other extracted parameters as single-qubit properties. (See the sections on electron trapping, position characterization, and experimental results.)
Authors: We agree that confirming single-electron occupancy is central to the claims. The manuscript infers single-electron trapping from the magnitude of the resonator frequency shift upon loading, which matches the expected capacitive shift for one electron, combined with the measured differential coupling to the two electrodes that constrains the position to a local minimum. The observed Rabi oscillations up to 76 MHz and the nonlinear frequency shift under strong driving are characteristic signatures of a driven two-level system; multi-electron states would be expected to produce additional spectral features or altered coupling strengths not seen in the data. We acknowledge that an independent charge-counting method such as discrete jumps during sequential loading is absent, as the surface roughness precludes deterministic sequential trapping. In the revised manuscript we will expand the discussion of electron trapping and position characterization to explicitly address possible multi-electron interpretations and explain why the observed parameters remain most consistent with a single electron. revision: partial
Circularity Check
No circularity: purely experimental measurements with no derivation chain
full rationale
The manuscript reports experimental realization of a charge qubit on solid neon, including microwave readout, coherent control with Rabi frequencies up to 76 MHz, and observation of nonlinear frequency shifts. Position is inferred from differential electrode coupling, but this is a direct measurement characterization rather than a fitted prediction or self-referential derivation. No equations, ansatzes, uniqueness theorems, or self-citations are invoked to derive results from inputs by construction. The work is self-contained against external benchmarks (measured Rabi rates, resonator responses) and contains no load-bearing theoretical steps that reduce to the paper's own fitted values or prior self-citations.
Axiom & Free-Parameter Ledger
Cite this review
Pith. "Pith review of Fast coherent control of a charge qubit on solid neon with a spin-qubit-compatible resonator." pith.science (2026). https://pith.science/paper/OMUXFSZP
@misc{pith2026260531185,
author = {Pith},
title = {Pith review of: Fast coherent control of a charge qubit on solid neon with a spin-qubit-compatible resonator},
year = {2026},
howpublished = {\url{https://pith.science/paper/OMUXFSZP}},
note = {Machine review of arXiv:2605.31185}
}
read the original abstract
Electrons floating in vacuum provide a clean platform for quantum information processing owing to their isolation from material defects. In particular, electrons on solid neon have emerged as a promising qubit platform because of their potentially long coherence times. Here, toward spin-qubit realization, we couple a single electron on solid neon to a magnetic-field-compatible superconducting NbTiN nanowire resonator. We realize a charge qubit and demonstrate microwave readout and coherent control, with Rabi frequencies up to 76 MHz, an order of magnitude larger than in previous studies. Under strong driving, we observe a qubit frequency shift from nonlinear interactions with the intense microwave field. Deterministic electron trapping at an intended position remains challenging due to solid neon surface roughness; we characterize the electron's position from its differential coupling to distinct electrodes. Although not trapped at an intended position, our estimates indicate that spin-qubit demonstrations remain feasible.
Figures
Forward citations
Cited by 1 Pith paper
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Deterministic single-electron trapping on solid neon using engineered dielectric surface geometry
Engineering a smooth dielectric layer with shallow etched wells can create deterministic single-electron traps on solid neon while keeping the qubit orbital splitting near the experimental value, per Schrödinger–Poiss...
Reference graph
Works this paper leans on
-
[1]
Dispersive coupling In the dispersive regime, i.e., g ≪ ∆qr with ∆qr = ωq − ωr being the qubit–resonator detuning, the interac- tion can be treated perturbatively. In the rotating frame of the driving frequency ωd, the Hamiltonian is given by [40]: H = ( ωr − ωd)a†a + 1 2 ( ωq − ωd + g2(2a†a + 1) ∆qr ) σz + εd(a† + a) + gεd ∆qr σx. (17) The term 2g2a†a/∆q...
-
[2]
Ponderomotive effect The ponderomotive effect is generated by an inho- mogeneous microwave driving field acting on a moving charged particle. Since we assume that the electron moves only along the x′ axis connecting the two poten- tial minima, the relevant spatial dependence reduces to the one-dimensional coordinate x′. Here, E(x′) denotes the magnitude o...
-
[3]
Y. Monarkha and K. Kono, Two-dimensional coulomb liquids and solids , Springer Series in Solid-State Sciences (Springer, Berlin, Germany, 2004)
work page 2004
-
[4]
E. Y. Andrei, Two-Dimensional Electron Systems : on Helium and other Cryogenic Substrates (Springer Nether- lands, 1997)
work page 1997
-
[5]
W. Guo, D. Konstantinov, and D. Jin, Quantum elec- tronics on quantum liquids and solids, Progress in Quan- tum Electronics 99, 100552 (2025)
work page 2025
-
[6]
P. M. Platzman and M. I. Dykman, Quantum Computing with Electrons Floating on Liquid Helium, Science 284, 1967 (1999)
work page 1967
-
[7]
M. Lea, P. Frayne, and Y. Mukharsky, Could we Quan- tum Compute with Electrons on Helium?, Fortschr. Phys. 48, 1109 (2000)
work page 2000
-
[8]
S. A. Lyon, Spin-based quantum computing using elec- trons on liquid helium, Phys. Rev. A 74, 052338 (2006)
work page 2006
-
[9]
D. I. Schuster, A. Fragner, M. I. Dykman, S. A. Lyon, and R. J. Schoelkopf, Proposal for Manipulating and De- tecting Spin and Orbital States of Trapped Electrons on Helium Using Cavity Quantum Electrodynamics, Phys. Rev. Lett. 105, 040503 (2010)
work page 2010
-
[10]
E. Kawakami, J. Chen, M. Benito, and D. Konstantinov, Blueprint for quantum computing using electrons on he- lium, Phys. Rev. Appl. 20, 054022 (2023)
work page 2023
-
[11]
A. Jennings, X. Zhou, I. Grytsenko, and E. Kawakami, Quantum computing using floating electrons on cryogenic substrates: Potential and challenges, Appl. Phys. Lett. 124, 120501 (2024)
work page 2024
-
[12]
G. Koolstra, G. Yang, and D. I. Schuster, Coupling a single electron on superfluid helium to a superconducting resonator, Nat. Commun. 10, 5323 (2019)
work page 2019
-
[13]
G. Koolstra, E. Glen, N. Beysengulov, H. Byeon, K. Cas- toria, M. Sammon, B. Dizdar, C. Wang, D. Schuster, S. Lyon, J. Pollanen, and D. Rees, High-impedance res- onators for strong coupling to an electron on helium, Phys. Rev. Appl. 23, 024001 (2025)
work page 2025
-
[14]
Strong coupling of a microwave photon to an electron on helium
G. Koolstra, E. O. Glen, N. R. Beysengulov, H. Byeon, K. E. Castoria, M. Sammon, S. A. Lyon, D. G. Rees, and J. Pollanen, Strong coupling of a microwave photon to an electron on helium, (2025), arXiv:2509.14506
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[15]
X. Zhou, G. Koolstra, X. Zhang, G. Yang, X. Han, B. Dizdar, X. Li, R. Divan, W. Guo, K. W. Murch, D. I. Schuster, and D. Jin, Single electrons on solid neon as a solid-state qubit platform, Nature 605, 46 (2022)
work page 2022
-
[16]
X. Zhou, X. Li, Q. Chen, G. Koolstra, G. Yang, B. Diz- dar, Y. Huang, C. S. Wang, X. Han, X. Zhang, D. I. Schuster, and D. Jin, Electron charge qubit with 0.1 mil- lisecond coherence time, Nat. Phys. 20, 116 (2024)
work page 2024
-
[17]
X. Li, C. S. Wang, B. Dizdar, Y. Huang, Y. Wen, W. Guo, X. Zhang, X. Han, X. Zhou, and D. Jin, Solid neon as a noise-resilient host for electron qubits above 100 mk, Nat. Electron. , 1 (2026)
work page 2026
- [18]
- [19]
-
[20]
Q. Chen, I. Martin, L. Jiang, and D. Jin, Electron spin coherence on a solid neon surface, Quantum Sci. Technol. 7, 045016 (2022)
work page 2022
-
[21]
N. Samkharadze, A. Bruno, P. Scarlino, G. Zheng, D. P. DiVincenzo, L. DiCarlo, and L. M. K. Vandersypen, High-kinetic-inductance superconducting nanowire res- onators for circuit qed in a magnetic field, Phys. Rev. Appl. 5, 044004 (2016)
work page 2016
-
[22]
N. Samkharadze, G. Zheng, N. Kalhor, D. Brousse, A. Sammak, U. C. Mendes, A. Blais, G. Scappucci, and L. M. K. Vandersypen, Strong spin-photon coupling in silicon., Science 359, 1123 (2018)
work page 2018
-
[23]
J. G. Kroll, F. Borsoi, K. L. van der Enden, W. Uilhoorn, D. de Jong, M. Quintero-Pérez, D. J. van Woerkom, A. Bruno, S. R. Plissard, D. Car, E. P. A. M. Bakkers, M. C. Cassidy, and L. P. Kouwenhoven, Magnetic-field- resilient superconducting coplanar-waveguide resonators for hybrid circuit quantum electrodynamics experiments, Phys. Rev. Appl. 11, 064053 (2019)
work page 2019
-
[24]
Y. Tian, I. Grytsenko, A. Jennings, J. Wang, H. Ikegami, X. Zhou, S. Tamate, H. Terai, H. Kutsuma, D. Jin, M. Benito, and E. Kawakami, Nb-ti-n nanowire res- onators and prospects for spin-photon coupling with elec- trons on solid neon, Phys. Rev. Appl. 25, 024011 (2025)
work page 2025
- [25]
- [26]
-
[27]
M. Pioro-Ladrière, T. Obata, Y. Tokura, Y.-S. Shin, T. Kubo, K. Yoshida, T. Taniyama, and S. Tarucha, Elec- trically driven single-electron spin resonance in a slanting Zeeman field, Nat. Phys. 4, 776 (2008)
work page 2008
-
[28]
D. J. Ibberson, T. Lundberg, J. A. Haigh, L. Hutin, B. Bertrand, S. Barraud, C.-M. Lee, N. A. Stelmashenko, G. A. Oakes, L. Cochrane, J. W. A. Robinson, M. Vinet, M. F. Gonzalez-Zalba, and L. A. Ibberson, Large disper- sive interaction between a cmos double quantum dot and microwave photons, PRX Quantum 2, 020315 (2021)
work page 2021
-
[29]
T. Hayashi, T. Fujisawa, H. D. Cheong, Y. H. Jeong, and Y. Hirayama, Coherent manipulation of electronic States in a double quantum dot., Phys. Rev. Lett. 91, 226804 (2003)
work page 2003
-
[30]
W. G. van der Wiel, S. De Franceschi, J. M. Elzerman, T. Fujisawa, S. Tarucha, and L. P. Kouwenhoven, Elec- tron transport through double quantum dots, Reviews of Modern Physics 75, 1 (2002)
work page 2002
-
[31]
I. I. Rabi, S. Millman, P. Kusch, and J. R. Zacharias, The molecular beam resonance method for measuring nuclear magnetic moments. the magnetic moments of 3Li6, 3Li7 and 9F19, Phys. Rev. 55, 526 (1939)
work page 1939
-
[32]
N. F. Ramsey, A molecular beam resonance method with separated oscillating fields, Phys. Rev. 78, 695 (1950)
work page 1950
-
[33]
Hahn, Spin Echoes, Physical Review 80, 580 (1950)
E. Hahn, Spin Echoes, Physical Review 80, 580 (1950)
work page 1950
-
[34]
S. Duthaluru, K. Zheng, E. A. Henriksen, and K. W. Murch, Real-time Monitoring of Neon Film Growth for Electron-on-Neon Qubits, Physical Review Applied 25, 044065 (2025)
work page 2025
-
[35]
M. Pioro-Ladrière, Y. Tokura, T. Obata, T. Kubo, and S. Tarucha, Micromagnets for coherent control of spin- charge qubit in lateral quantum dots, App. Phys. Lett. 15 90, 024105 (2007)
work page 2007
- [36]
- [37]
-
[38]
K. D. Petersson, L. W. McFaul, M. D. Schroer, M. Jung, J. M. Taylor, A. A. Houck, and J. R. Petta, Circuit quan- tum electrodynamics with a spin qubit., Nature 490, 380 (2012)
work page 2012
-
[39]
J. Dijkema, X. Xue, P. Harvey-Collard, et al. , Cavity- mediated iswap oscillations between distant spins, Nat. Phys. 21, 168 (2025)
work page 2025
-
[40]
X. Mi, J. V. Cady, D. M. Zajac, J. Stehlik, L. F. Edge, and J. R. Petta, Circuit quantum electrodynamics archi- tecture for gate-defined quantum dots in silicon, Applied Physics Letters 110, 043502 (2017)
work page 2017
-
[41]
M. Braik, I. Sow, J. Nelayah, A. Belkhir, M. Faustini, S. Mercone, S. Nowak, P. Decorse, J.-Y. Piquemal, and N. Félidj, Introducing cobalt as a potential plasmonic candidate combining optical and magnetic functionali- ties within the same nanostructure, Nanoscale 13, 2639 (2021)
work page 2021
-
[42]
A. Blais, R.-S. Huang, A. Wallraff, S. M. Girvin, and R. J. Schoelkopf, Cavity quantum electrodynamics for superconducting electrical circuits: An architecture for quantum computation, Phys. Rev. A 69, 062320 (2004)
work page 2004
-
[43]
T. W. B. Kibble, Mutual refraction of electrons and pho- tons, Phys. Rev. 150, 1060 (1966)
work page 1966
-
[44]
P. H. Bucksbaum, R. R. Freeman, M. Bashkansky, and T. J. McIlrath, Role of the ponderomotive potential in above-threshold ionization, J. Opt. Soc. Am. B 4, 760 (1987)
work page 1987
This paper was first reviewed by grok-4.3 on July 2, 2026.
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