The breakthrough was made possible not by a new microscope, but by a concept borrowed from quantum information theory: quantum Fisher information (QFI). Originally developed by quantum physicist Peter Zoller and his group at the University of Innsbruck, QFI quantifies how sensitively a quantum system responds to a small perturbation. If a system's response exceeds a well-defined classical limit—meaning it reacts more strongly than the sum of its independent parts—that sensitivity can only arise from quantum entanglement , .
By applying this framework, the team could for the first time extract a direct entanglement measure from a bulk solid, a stark departure from traditional experiments that rely on careful state preparation and isolation.
The researchers, led by Prof. Silke Bühler-Paschen at TU Wien, did not attempt to place the entire crystal into a superposition—a practical impossibility for such a large object. Instead, they used inelastic neutron scattering at the Institut Laue–Langevin (ILL) in Grenoble, France, to measure the material's dynamical spin correlation function, S(q, ω, T). In simpler terms, they bombarded the crystal with neutrons and watched how the spins of the material's particles moved and fluctuated together as a function of energy, momentum, and temperature .
When they applied the QFI formalism to the scattering data, the results were striking. The crystal's collective response was far too strong to be explained by independent particles. The QFI density reached f_Q = 8.2 ± 0.9 at the lowest measured temperature, a value that mathematically corresponds to a group of at least nine quantum-entangled entities acting together. The entanglement peaked at the experiment's coldest temperature of 60 mK (millikelvin) and near a magnetic field of roughly 1.73 Tesla, exactly at the quantum critical point where Kondo destruction takes place. When the crystal was cooled from 10 K down to 60 mK, the QFI density surged nearly 40-fold with no sign of saturation, suggesting even stronger entanglement could exist at even lower temperatures , .
The results offer a compelling new narrative for one of the biggest puzzles in condensed matter physics. Strange metals do not conduct electricity like ordinary metals. Their electrons seem to lose their individual identity, forming a collective quantum soup. This experiment directly links the breakdown of quasiparticles at a Kondo destruction quantum critical point to a surge in multipartite entanglement , . The linear-in-temperature resistivity that defines strange metals may not be the fingerprint of disorder or simple scattering, but rather a signature of a highly entangled, collective quantum state.
Beyond explaining strange metals, the work carves a practical path forward for quantum technology. Quantum Fisher information is not just a detector of entanglement; it is also the central quantity in quantum metrology, the science of ultra-precise measurement. A material that exhibits strong, stable internal entanglement is a natural platform for a highly sensitive sensor. If such entanglement can be maintained at higher, more practical temperatures, these materials could be used for everything from magnetic field sensing to detecting gravitational waves. The study opens the door to using QFI-based techniques to systematically screen other quantum materials, potentially including high-temperature superconductors, for macroscopic entanglement , .
The study was an international collaboration. The experimental work was led by Silke Bühler-Paschen's group at TU Wien with PhD student Federico Mazza conducting the neutron scattering at ILL Grenoble. The theoretical foundation was built by Peter Zoller's team at the University of Innsbruck, with additional contributions from Qimiao Si at Rice University, whose group has long studied the Kondo destruction mechanism in Ce₃Pd₂₀Si₆.
By uniting the abstract tools of quantum information with the messy reality of a bulk solid, the team has built a bridge between two previously distant fields. They have given physicists a new way to witness the "spooky action" that Einstein famously doubted, not in a controlled vacuum chamber, but inside a small, glittering crystal sitting in plain sight.