In a world striving for chaos, rhythm sometimes arises. The Belousov–Zhabotinsky reaction has amazed for decades: in a test tube, color waves run on their own, as if a living organism breathing matter. Something similar lurks in crystals where iron atoms balance between two magnetic states — high-spin and low-spin. This entropic standoff can evolve into self-oscillations when thermodynamics meets collective exchange interaction. In a sense, the tiny crystal becomes a desktop pulsar — a radiator of a strictly periodic magnetic signal.
To understand how the magnetic rhythm is born, physicists turned to numerical simulation, drawing on the formalism of Roy Glauber for spin dynamics and the methods of Lev Landau for phase transitions. The key role is played by exchange interaction — an invisible spring binding the spins of neighboring ions. In the mean-field approximation, equilibrium is given by an equation where the order parameter resembles the tension of a string, sensitively responding to the slightest changes in the Boltzmann distribution. It was Ludwig Boltzmann who showed how microscopic reversibility gives way to the macroscopic flow of time — and here this transition takes visible form.
Numerical experiments revealed two scenarios. When elastic interaction dominates, the pendulum of magnetic moment swings only under constant external illumination. But if exchange interaction prevails, the system finds its own voice: at temperatures around 75 K and a relaxation rate of 4.5 s⁻¹, oscillations with an amplitude of about 1.3 Bohr magnetons appear on the iron ions. This is reminiscent of fast radio bursts — mysterious pulses from distant neutron stars. Similar self-organization principles might be at work there, too. Analogies with Bose–Einstein condensates and lasers suggest: collective coherence arises where the system gently tricks the second law of thermodynamics — not violating, but riding the flow of entropy. Astonishingly, the rhythm persists over a wide range of parameters — the crystal “remembers” its frequency, almost like a living neuron.
The predicted mechanism opens a new chapter in spintronics. Non-volatile memory cells switched by a short heat pulse, neuromorphic networks where artificial neurons communicate via magnetic spikes — all this ceases to be fantasy. The next step is to grow a perfect FeBO3 crystal and make it sing a magneto-optical aria. And then, perhaps, we will hear, in the laboratory silence, a tiny heartbeat echoing the rhythm of the Universe.
The spin crossover effect was discovered back in 1931 by Italian chemists L. Cambi and L. Szegő, but its non-equilibrium manifestations continue to amaze researchers to this day.