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ferromagnetism

(2 articles)

"The Earlier Transition"

# The Earlier Transition Europium oxide is a ferromagnetic semiconductor with a Curie temperature of 69 kelvin. Below that temperature, the electron spins align and the material becomes magnetic. Above it, the spins are disordered. This is a standard Hermitian phase transition — a change in what the material is. Researchers illuminated EuO with optical pulses and measured how it returned to equilibrium. Below the exceptional point at 84 kelvin, the relaxation is bi-exponential — the signal decays along two real timescales. Above 84 kelvin, the relaxation becomes single-exponential with a complex decay rate. The mathematical structure of the relaxation, not just its speed, changes qualitatively at this temperature. This is a non-Hermitian phase transition — a change in how the material behaves. The two critical temperatures are fifteen kelvin apart. As the material cools from above, it first passes through the exceptional point at 84 K, where the character of its dynamics changes. Then, fifteen degrees later, it passes through the Curie point at 69 K, where the static magnetic order sets in. The system's behavior reorganizes before its identity does. This ordering is not accidental. The non-Hermitian transition depends on the coupling between charge carriers and magnetic order. As temperature drops toward the Curie point, magnetic fluctuations grow, and the coupling strengthens enough to split the relaxation into two channels. The dynamic transition is a precursor — not in the sense of a warning sign, but in the sense that the way a system responds to perturbation is a more sensitive indicator of approaching order than the order parameter itself. The material changes how it relaxes before it changes what it is. Dynamics are the leading edge.

The Ferromagnetic Pair

# The Ferromagnetic Pair Superconductivity and ferromagnetism are conventionally antagonistic. Cooper pairs in standard superconductors form between electrons with opposite spins — singlet pairing. A ferromagnetic exchange field aligns spins in the same direction, breaking the singlet and destroying superconductivity. Materials are usually either superconducting or ferromagnetic, not both. Zhang and colleagues (arXiv:2603.25807, March 2026) directly image the Meissner effect in rhombohedral graphene and find superconductivity emerging during a continuous transition to a canted spin ferromagnetic state. The material is simultaneously ferromagnetic and superconducting. The superconductivity does not fight the ferromagnetism — it arises from it. The imaging reveals that the superconductivity screens only approximately 100 parts per million of the applied magnetic field — extraordinarily weak diamagnetism, far below what conventional superconductors produce. The superfluid stiffness — the energy cost of a phase twist in the superconducting order parameter — is linearly proportional to Tc, not following the BCS expectation where stiffness scales with the gap squared divided by the Fermi energy. The linear scaling indicates that the pairing mechanism is intrinsically different from the phonon-mediated pairing of conventional superconductors. The zero-temperature superfluid stiffness being proportional to Tc (rather than much larger) means the superconductor is in an extreme strong-coupling or low-density regime where all the available spectral weight is used for pairing. There is no "overhead" — the superconducting condensate is as weak as the critical temperature allows, and strengthening one strengthens the other in lockstep. The structural observation: a superconductor born from a ferromagnetic state violates the conventional antagonism between the two orders because the pairing symmetry accommodates the magnetism rather than competing with it. The canted spin state provides a compromise — the spins are partially aligned (ferromagnetic) but canted enough to permit triplet pairing (superconducting). The weakness of the Meissner screening and the linear stiffness-Tc scaling are signatures of a pairing mechanism that is intimately tied to the magnetic order rather than independent of it.