Noise as an X-ray: How Hidden Triplet Superconductivity Emerged at a Superconductor-Iron Interface ✛ ✎

Original: "Giant shot noise in superconductor/ferromagnet junctions with orbital-symmetry-controlled spin-orbit coupling"
arXiv:2509.15983 · 2025-09-19 · arXiv non-exclusive · independent analysis · 2 min
In a superconductor-ferromagnet contact, shot noise exceeded the theoretical limit by a factor of one hundred, revealing induced triplet superconductivity.

Run a current through a contact between a superconductor and a ferromagnet, and you will hear the whisper of the quantum world. In the lab at 0.3 K, that whisper turned into a roar: the shot noise—electrical noise due to the discreteness of charge—was a hundred times louder than theory allows for ordinary contacts. Such a surge is unmistakable: it betrays the presence of something not directly visible, namely induced triplet superconductivity in the iron layer.

The effective charge estimated from the noise exceeds 100 electrons, as if not a single electron but a whole "clump" of a hundred charges passed through the barrier, even though only Cooper pairs are physically transferred.

Shot noise acts like an X-ray for hidden quantum states. In a normal tunnel junction, electrons cross the barrier one by one, randomly, and the noise is strictly predictable: the Fano factor (the ratio of measured noise to the Poissonian value) equals one. In a superconducting contact, it doubles due to Andreev reflection, where an electron converts into a hole at the interface. But here, in the vanadium/magnesium oxide/iron structure, the Fano factor soared above 100, and in one sample to nearly 200. This is possible only if an induced superconducting gap with parallel spins, that is, triplet rather than ordinary singlet, arises in the ferromagnet. Spin-orbit coupling at the interface, which links the electron's spin to its motion, acts as an interpreter that helps Cooper pairs penetrate the magnetic layer.

Magnetic field confirmed the hunch. It suppressed the noise anisotropically: most strongly for out-of-plane fields, but differently for the [100] and [110] in-plane directions. Such sensitivity to orientation is incompatible with ordinary singlet superconductivity and directly points to triplet correlations. Previously, giant shot noise was considered the privilege of structures with two superconductors, where multiple Andreev reflections accumulate effective charge. Now it is clear: a single superconductor and a suitable interface suffice.

This discovery changes the rules of the game for superconducting spintronics and the search for Majorana states needed for topological quantum computing. Noise spectroscopy becomes a simple and reliable tool: measure the noise and you see whether triplet superconductivity is present. Next steps include testing other hybrid systems, from half-metals to topological insulators. The X-ray is already on, and new physics is emerging in the image.

The effective charge estimated from the noise exceeds 100 electrons, as if not a single electron but a whole "clump" of a hundred charges passed through the barrier, even though only Cooper pairs are physically transferred.

The idea of hidden quantum states that manifest only through noise echoes Peter Watts's novel "Blindsight," where characters try to understand the nature of invisible entities through indirect clues.

F = \frac{S_I}{2eI}
The Fano factor F is the ratio of the measured spectral density of shot noise S_I to the Poissonian value 2eI, where e is the electron charge and I is the average current. For ordinary contacts F=1, for superconducting contacts it is 2, and here it exceeds 100, indicating collective charge transfer.
q_{\mathrm{eff}} = F \cdot e
The effective charge q_eff equals the Fano factor multiplied by the elementary charge. With F=100–200, this yields a charge of 100–200 electrons, even though only Cooper pairs are actually transferred. This results from multiple Andreev reflections that amplify the noise.
Scientists
Wolfgang PauliLeo EsakiFelix BlochSatyendra Nath BoseAlbert EinsteinJohn Bardeen
Concepts
proximity effect Josephson effect shot noise measurement noise magnetic superconductivity coupling magnetic superconductivity antiferromagnetic order josephson current spin curvature coupling phonon magnetism flux pinning flux quantization superconducting quantum interference device moiré pattern effects aluminum oxide resonance superconducting loop exoplanetary orbital resonance critical transition quantum synchronization