Quantum Gas Breaks the Textbook Rules express

Original: "Observation of anyonic thermodynamics and generalized Pauli principle"
arXiv:2606.19009 · 2026-06-17 · CC BY 4.0 · 1 min
Physicists have directly measured the 'wrong' thermodynamics of particles that refuse to be together or apart.

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Textbooks divide particles into two camps: bosons love to crowd into the same state, fermions absolutely refuse. But nature allows a third option. Anyons are quasiparticles whose behavior lies somewhere in between. They can 'remember' how they were exchanged and obey a nonstandard exclusion principle.

Anyons with unusual memory have been observed in experiments before. But their thermal behavior, how they fill energy levels and carry heat, remained a mystery.

A team of physicists took a one-dimensional quantum gas of strongly interacting atoms and turned it into an anyonic thermodynamic ensemble. In one dimension, the dynamical interaction between particles can be recast as a statistical one — a well-known mathematical trick. By varying the repulsion strength and temperature, the authors measured the gas's equation of state. The plots showed clear departures from the Bose–Einstein and Fermi–Dirac statistics.

These departures fell exactly on the curves of generalized exclusion statistics: that extended version of the Pauli principle. Additional measurements of pressure and Tan's contact confirmed the picture. The researchers now have a platform where particle statistics can be tuned with the turn of a knob.

The one-dimensional world is much friendlier to anyons: in two or three dimensions, creating such tunable statistics via interactions is far more difficult.

Scientists
Satyendra Nath BoseAlbert EinsteinWolfgang PauliJohn BardeenAndrey Markov
Concepts
anyon Fermi–Dirac statistics quantum statistics Pauli exclusion principle non abelian anyons fermion partition function topological quantum computing ensemble average exchange interaction boson spin–statistics theorem thermal state Boltzmann equation braiding temperature boltzmann constant efficiency cryogenic temperature zeroth law of thermodynamics