RESEARCH
QUANTUM CIRCUITS2026

Higher Josephson Harmonics in a Tunable Double-Junction Transmon Qubit

Ksenia Shagalov, David Feldstein-Bofill, Leo Uhre Jakobsen, Zhenhai Sun, Casper Wied, Amalie T. J. Paulsen, Johann Bock Severin, Malthe A. Marciniak, Clinton A. Potts, Anders Kringhøj, Jacob Hastrup, Karsten Flensberg, Svend Krøjer, Morten Kjaergaard

A flux-tunable superconducting circuit reveals higher Josephson harmonics, opening a route to tailored nonlinear quantum devices.

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Double-junction transmon circuit, device micrographs, and effective Josephson potential with higher harmonics
Figure 1. Qubit circuit and device design. (a) Circuit schematic of the tunable double-junction transmon with a single JJ (blue) and a SQUID loop (red) in series, shunted by a large capacitor (green). (b) SEM of the tunable double-junction transmon showing the large island that forms the capacitor (green). A quarter-wave resonator is capacitively coupled to the qubit for readout. A flux line threads magnetic flux through the SQUID loop, and the drive line facilitates the XY control. (c) SEM image of the single JJ (blue) and the SQUID loop (red) in series. (d) The potentials UU plotted for each SIS junction (blue, red), which in series effectively correspond to the potential from Eq. (2), shown for λ=1\lambda=1 (purple). (e) Harmonic content of the potential from Eq. (2) as a function of λ\lambda. (f) λ\lambda as a function of the ratio between the Josephson energies of the two junctions.Shagalov et al., Phys. Rev. Lett. 137, 057001 (2026), doi:10.1103/fr7x-555s. Original Figure 1 caption. Figure and caption reproduced under CC BY 4.0.

THE WORK

A conventional transmon is usually described by a Josephson potential dominated by a single cosine. This experiment builds a tunable alternative: a tunnel junction in series with a SQUID loop, allowing magnetic flux to change the shape of the potential and its higher harmonics.

The two elements share the superconducting phase across the circuit. Changing the effective Josephson energy of the SQUID adjusts their balance, producing a potential that departs from the familiar cosine. A large shunting capacitor allows the resulting device to operate as a transmon, with microwave control and resonator readout.

Spectroscopy follows the first four qubit transitions as the applied flux changes. A model fitted to the first two transitions also predicts the higher transitions, providing a check on the circuit description. Accounting for an internal mode associated with the island between the junction and SQUID is essential to capture the measured spectrum.

The measurements resolve a second harmonic reaching about 10% of the fundamental. They also identify a flux sweet spot where the qubit and internal-mode contributions to the ground-state dispersive shift cancel. This connects the additional circuit degree of freedom to an observable change in the resonator response.

The work establishes a fully superconducting circuit element for engineering nonlinear behavior in situ. Its significance is the ability to tune the potential within a fabricated device, offering a building block for customized microwave components and future protected-qubit designs. The experiment demonstrates that building block, with protected-qubit operation remaining a direction for further work.

Explore the full methods, measurements, and discussion in the paper.

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