A Magnetic Knob for a Superconducting Orchestra ✛

Original: "Magnetic contacts on freestanding superconducting LaAlO$$_3$$/SrTiO$$_3$$ micromembranes"
arXiv:2608.29771v1 · 2026-08-30 · CC BY 4.0 · 3 min
Superconductivity survives contact with ferromagnetic nickel, and the magnetic history of the contacts tunes the superconducting state.

A superconductor is like an orchestra that plays without a single wrong note, until the conductor turns a tuning knob. In this new work, that knob turned out to be the magnetic history of nickel contacts. The researchers created superconducting micromembranes from the oxides LaAlO3 and SrTiO3, where a thin layer of free electrons forms at the interface between the two materials: a two-dimensional electron gas. Ferromagnetic nickel contacts were attached to this buried layer through the sidewall, something previously thought nearly impossible.

All three devices transitioned to the superconducting state at temperatures between 100 and 200 millikelvins, just above absolute zero. Current flows through such a conductor without resistance, like water through a perfectly smooth pipe. But magnetized nickel contacts lie nearby, and their magnetic field interferes with the electrons' paired motion. It turned out that an external magnetic field can precisely compensate for this influence: the resistance dropped to zero not at zero field, but at a shift of about 45 millitesla in either direction.

The key surprise: the same external field could produce either a superconducting or a normal state, depending on which side you approached it from. This is hysteresis: a memory of magnetic history, as if the orchestra played differently after a morning rehearsal than after an evening one.

The magnetic field from the contacts acts on the electrons like a crosswind on a runner. With the field directed along the plane of the membrane, the critical current was about five times larger than with a perpendicular field. The reason is simple: the stray field from the thin nickel films is weaker in the plane, so the electrons can more easily maintain their paired dance. The researchers built a model linking the external field, the magnetization of the contacts, and the effective field felt by the superconductor. The coupling coefficient was 1.69×10⁻⁷ henries per meter, which allowed them to reconstruct the magnetization loop of nickel directly from transport measurements.

Previously, it was unclear whether ferromagnetic contacts could be attached to a superconducting two-dimensional gas at a buried interface without destroying superconductivity. Now it has been shown that it is possible. Moreover, the magnetic state of the contacts acts as a tuning knob: by turning it, we change the effective field in the two-dimensional gas and control the critical current. This is the first time a superconductor and a ferromagnet coexist in a single oxide micromembrane with a side contact.

The practical benefits are already visible. Such a platform could become the basis for superconducting memory, where logical states are set by magnetic history rather than by electric charge. The sensitivity of the superconducting response to magnetic history turns the device into an internal magnetometer for the contacts.

The orchestra from the opening sentence now sounds different. We are not just listening to its performance; we can turn the tuning knob, knowing that each note depends on how the knob was turned before. The next step is to learn to control two contacts independently, to obtain a ferromagnet–superconductor–ferromagnet transition and test whether triplet Cooper pairs are born there. Then superconducting spintronics will cease to be a promise and become a working tool.

The compensation field of ±45 mT corresponds to a nickel magnetization of about 2.5×10⁵ A/m, which is close to saturation of thin nickel films. This means that at such a field the contacts are still fully magnetized, and their stray field can be precisely compensated by an external field.

B_{2DEG}(B_z) = B_z - \alpha M_z(B_z)
The field experienced by the superconductor equals the external field minus the field from the magnetized contacts, proportional to the magnetization with coefficient α.
Scientists
Wolfgang PauliLeo EsakiFelix BlochSatyendra Nath BoseAlbert EinsteinJohn Bardeen
Concepts
magnetic superconductivity coupling superconducting magnet magnetic interaction superconducting electronics magnetic superconductivity