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arXiv:2604.23768 · Physics Letters A

Entanglement and reciprocal dynamics of the Barnett and Einstein-de Haas responses in a quantum spin-rotor model

Saikat Banerjee, Holger Fehske

quant-phcond-mat.str-elSubmitted Apr 26, 2026• Announced Apr 28, 2026• 0 citations• Revised Oct 25, 2026 (v3)
v1 · Apr 26, 2026v2 · Sep 14, 2026v3 · Oct 25, 2026
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Abstract

We study the reciprocal Barnett and Einstein--de Haas effects in an exactly solvable quantum spin--rotor model that conserves the total angular momentum. For a single spin-$1/2$, the model describes rotation-dependent spin polarization, coherent transfer of angular momentum between the spin and the rotor, and the accompanying spin--rotor entanglement. At a recoil-compensation point, all angular-momentum sectors become synchronized, allowing complete spin reversal and a one-quantum shift of an arbitrary rotor wave packet. We then extend the model to two spins coupled to the same rotor, where the shared rotational degree of freedom participates dynamically in the generation of spin--spin entanglement. The singlet forms a dark state, while the triplet sector remains coupled to the mechanical motion. At a special parameter point, the rotor returns to its original dynamical branch and disentangles from the spins, leaving behind a maximally entangled two-spin state locally equivalent to a Bell state.

Journal reference
Phys. Lett. A 600, 132285 (2026)
DOI
10.1016/j.physleta.2026.132285
Comments
9 pages, 3 figures. Final version

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We study the reciprocal Barnett and Einstein--de Haas effects in an exactly solvable quantum spin--rotor model that conserves the total angular momentum. For a single spin-1/21/21/2, the model describes rotation-dependent spin polarization, coherent transfer of angular momentum between the spin and the rotor, and the accompanying spin--rotor entanglement. At a recoil-compensation point, all angular-momentum sectors become synchronized, allowing complete spin reversal and a one-quantum shift of an arbitrary rotor wave packet. We then extend the model to two spins coupled to the same rotor, where the shared rotational degree of freedom participates dynamically in the generation of spin--spin entanglement. The singlet forms a dark state, while the triplet sector remains coupled to the mechanical motion. At a special parameter point, the rotor returns to its original dynamical branch and disentangles from the spins, leaving behind a maximally entangled two-spin state locally equivalent to a Bell state.
A theoretical framework is developed to study a magnetically levitated nanomagnet in the quantum regime. The system is very rich due to the interaction between its degrees of freedom: position, orientation, and magnetization. In particular, the Einstein--de Haas effect, namely the coupling between the magnetization and the angular momentum of the object, plays a dramatic role. This work sheds new light on one of the few unsolved problem in quantum mechanics, the rigid rotor with a spin. At the same time, it opens up the possibility to model the dynamics of a single magnetic domain nanoparticle in a magnetic trap, an interesting new scenario for future experiments.
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The Einstein-de Haas effect is a phenomenon in which angular momentum is transferred from microscopic spins to mechanical rotation of a macroscopic rigid body. We report an observation of the Einstein-de Haas effect in a spinor-dipolar Bose-Einstein condensate, in which the intrinsic magnetic dipole-dipole interaction mediates coherent transfer of angular momentum from atomic spins to collective circulation of a quantum fluid. The depolarized spinor components displayed ring-shaped density distributions that were confirmed as quantized vortices through matter-wave interferometry, revealing a coherent conversion between spin and orbital angular momentum. This observation opens a pathway to exploring ground-state phases with broken chiral symmetry, spin textures, and mass circulation, as well as the Barnett effect in dipolar quantum gases.
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What is the shortest possible timescale of the Einstein--de Haas effect? Addressing this problem theoretically poses a monumental challenge, for it involves an infinite number of coupled quantum angular momenta. Here, the authors formulate for the first time the problem in a rotationally invariant way, thereby enabling its solution in terms of angulon quasiparticles. Intriguingly, the first calculations reveal already that transfer between electron spin, orbital, and lattice degrees of freedom can occur on the femtosecond time scale.