Electron on Helium Captures a Microwave Photon for the First Time ✛ ✎

Original: "Strong coupling of a microwave photon to an electron on helium"
arXiv:2509.14506 · 2025-09-18 · arXiv non-exclusive · independent analysis · 3 min
A single electron levitating above superfluid helium has been strongly coupled to a photon in a superconducting resonator.

Context

Quantum computing with electrons floating above superfluid helium promises long spin coherence times and a clean substrate free of charge traps. However, until now, a single electron in this system had not been strongly coupled to a microwave field, which is necessary for reading out and manipulating spin states. This work joins recent efforts to integrate electrons on helium with superconducting circuits: control of single electrons and their coupling to resonators had been demonstrated previously, but the strong coupling regime remained out of reach. This work closes that gap by using a compact quantum dot and a high-impedance resonator.

Methods

The electron is held in a quantum dot of size 1.4×1.4 μm², formed by electrostatic potentials above superfluid helium in a microfluidic channel. A titanium nitride resonator with high kinetic impedance (Z = 3.8 kΩ) enhances the coupling to the electron's motion by a factor of 20 compared to previous designs. The coupling was measured via resonator transmission spectroscopy: when the electron's motion frequency matched the resonator frequency, vacuum Rabi splitting was observed. Additionally, two-tone spectroscopy was used to directly probe the electron's energy levels and measure the relaxation time T1.

Results

Vacuum Rabi splitting was observed with a coupling strength g/2π = 118 ± 3 MHz, exceeding the resonator linewidth κ/2π = 23 MHz and the electron decoherence rate Γ2/2π = 61 MHz (under optimal conditions). The single-photon cooperativity was C ≈ 32. Voltage control of the electrodes allowed tuning the electron's motion frequency from 5.5 to 10 GHz and reducing decoherence by applying a negative bias. The energy relaxation time T1 reached 0.76 μs and was limited by Purcell emission into the resonator at small detunings. Decoherence Γ2 increased with temperature following a power law $T^0$.5, indicating coupling to low-frequency excitations of the helium surface or fluctuating charges.

Implications

This work for the first time brings electrons on helium into the strong coupling regime with a microwave photon, placing this platform on par with semiconductor quantum dots, where this regime has already enabled spin readout. The difference from related works in the archive is the use of a high-impedance resonator and a compact dot, which yielded a record coupling strength for this system. This opens the way to hybridizing charge and spin states via a magnetic field gradient, and thus to reading out spin qubits in microseconds.

Future development

The next step will be to introduce a magnetic field gradient to couple the electron's spin state to its motion, and through it, to the resonator. This would enable spin readout and possibly two-qubit operations. It also remains to understand the nature of the residual decoherence and find ways to suppress it, for example by improving shielding from charge fluctuations. In the long term, the architecture could be scaled to arrays of qubits on a shared helium film.

Impact

The result will impact the development of quantum computers based on electrons in superfluid helium, as well as fundamental studies of circuit quantum electrodynamics with single particles.

Next steps

Integrate a magnetic gradient into the device and demonstrate spin-resonator coupling; study decoherence sources at low temperatures.

Key open problems

For the electron-on-helium platform, the key unresolved problem remains reading out the spin state within a time shorter than the decoherence time. This work solves the first half of the problem: strong coupling of charge motion to a photon, but it does not solve the problem of spin control and protection from noise.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

This study reports the first realization of strong coupling between the motion of a single electron on superfluid helium and a microwave photon in a superconducting resonator. A compact quantum dot and a high-impedance titanium nitride resonator were used, achieving a coupling strength of g/2π = 118 MHz, which exceeds both the decoherence rate and the resonator linewidth. Vacuum Rabi splitting, voltage tuning of the electron frequency, and measurement of the relaxation time T1, limited by Purcell emission, were demonstrated.

Where its strength is

Strong coupling in the electron-on-helium system opens a direct path to reading out spin states via the microwave field. The high resonator impedance and compact dot geometry yield record cooperativity for this platform, making hybridization of charge and spin degrees of freedom possible.

Where it could go next

  • It might be interesting to see how single-spin readout via a resonator is implemented in a nearby paper: they may have used circuits that could be adapted for electrons on helium, especially regarding signal amplification and noise suppression.based on: A Resonator That Catches a Single Spin arXiv:2603.25258
  • A related paper on electric control of erbium spins is nearby; similar electric-field control methods might apply to spin states of electrons on helium if a magnetic field gradient is added, enabling single-qubit gates.based on: An electric steering wheel for an erbium spin arXiv:2608.07929v1
  • There is an analysis in the archive on charge noise; in the context of this work, it would be interesting to investigate how fluctuating charges on the helium surface affect decoherence, and possibly use noise characterization methods to improve coherence times.based on: The Noise That Gives Away the Charge arXiv:2603.22145

Worth trying

  • Try applying the readout technique from the paper on a resonator trapping a single spin to improve the signal-to-noise ratio when measuring the spin state of an electron on helium.
  • Use the electric control approaches from the erbium paper to modulate the spin transition frequency and implement fast single-qubit operations.
  • Perform charge noise correlation measurements similar to those described in the paper on charge noise to identify decoherence sources and optimize dot parameters.

The electron is held above the helium thanks to its image charge: it is repelled from the surface but cannot enter the liquid due to a barrier of about 1 eV. The depth of the potential well for the electron in the dot is approximately 1000 GHz, which is hundreds of times larger than the energy of its motion.

g/2\pi = 118 \text{ МГц}
The rate of energy exchange between the electron's motion and the microwave field of the resonator.
C = 4g^2/(\kappa \Gamma_2) \approx 32
A dimensionless measure of how much the coupling exceeds resonator losses and electron decoherence.
\Gamma_2/2\pi = 61 \text{ МГц}
The characteristic rate at which the electron's motion loses quantum coherence.

Key numbers

  • coupling strength: 118 MHz
  • resonator linewidth: 23 MHz
  • decoherence rate: 61 MHz
  • relaxation time T1: 0.76 μs
  • temperature: 7 mK
Scientists
Fred HoyleMargaret BurbidgeJohannes RydbergSatyendra Nath BoseDaniel BernoulliLev Landau
Concepts
coupling strength cavity qed superconducting resonator strong coupling quantum electrodynamics cryogenic microwave measurement microwave photon quantum liquid hybrid system cms detector charge qubit superconducting qubit kiloelectronvolt single spin manipulation cms collaboration electron pairs electric field sensor milliwatt helium atom photon