The Electron's Heel: What Dirac Knew and Pauli Missed ✛

Original: "Time inversion symmetry in the Dirac and Schrödinger-Pauli theories"
· R. Winkler, U. Zülicke
arXiv:2506.01292v2 · 2025-06-02 · CC BY 4.0 · 1 min
In a magnetized material, electrons always drift sideways — even if you ignore the spin’s effect on their trajectory.

In a chunk of magnet, an electron behaves like a ship with a heel: even in dead calm, its trajectory curves to the side. This is the anomalous Hall effect — motion with a transverse drift without an external magnetic field.

Previously, it was thought that it all came down to how the electron's own rotation (spin) affects its motion. But the theories of Schrödinger and Pauli missed a deeper reason. The full description by Dirac in fundamental physics shows that the electron itself possesses a built-in path curvature (Berry curvature). It’s as if a vessel had an asymmetric hull and couldn’t sail straight.

The magnitude of the heel is given by the constant 1/(2m²c²), where m is the electron mass, c is the speed of light. In magnetically ordered crystals, where all spin-"compasses" point the same way, time symmetry is broken. This creates an additional electric field: that very anomalous signal. Surprisingly, such curvature exists even for a stationary electron. Practically, it promises electronics without bulky magnets: current can be controlled using the material’s internal curvature.

Discovered over a century ago, the effect long remained a mystery; only recently was it found that the answer lies hidden in Dirac’s equations, and this "heel" is fundamental even for stationary particles.

\Omega = \frac{1}{2m^2c^2}
intrinsic Berry curvature for the electron: m is mass, c is the speed of light
Scientists
Paul DiracEmilio Gino SegrèPeter HiggsRichard FeynmanMarie CurieEnrico Fermi
Concepts
arrow of time time reversal symmetry Dirac equation anomalous magnetic moment Kepler's third law berry curvature CPT theorem magnetic monopole Schrödinger equation Faraday's law of electromagnetic induction spacetime curvature Lorentz Invariance Violation Penrose singularity theorem altermagnetism bohr magneton Noether's theorem Curie's law de Broglie formula proper time positron