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Continuum of quantum fluctuations in a three-dimensional S = 1 Heisenberg magnet

Conventional crystalline magnets are characterized by symmetry breaking and normal modes of excitation called magnons, with quantized angular momentum ħ . Neutron scattering correspondingly features extra magnetic Bragg diffraction at low temperatures and dispersive inelastic scattering associated w...

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Bibliographic Details
Published in:Nature physics 2019-01, Vol.15 (1), p.54-59
Main Authors: Plumb, K. W., Changlani, Hitesh J., Scheie, A., Zhang, Shu, Krizan, J. W., Rodriguez-Rivera, J. A., Qiu, Yiming, Winn, B., Cava, R. J., Broholm, C. L.
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Language:English
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Summary:Conventional crystalline magnets are characterized by symmetry breaking and normal modes of excitation called magnons, with quantized angular momentum ħ . Neutron scattering correspondingly features extra magnetic Bragg diffraction at low temperatures and dispersive inelastic scattering associated with single magnon creation and annihilation. Exceptions are anticipated in so-called quantum spin liquids, as exemplified by the one-dimensional spin-1/2 chain, which has no magnetic order and where magnons accordingly fractionalize into spinons with angular momentum ħ /2. This is spectacularly revealed by a continuum of inelastic neutron scattering associated with two-spinon processes. Here, we report evidence for these key features of a quantum spin liquid in the three-dimensional antiferromagnet NaCaNi 2 F 7 . We show that despite the complication of random Na 1+ –Ca 2+ charge disorder, NaCaNi 2 F 7 is an almost ideal realization of the spin-1 antiferromagnetic Heisenberg model on a pyrochlore lattice. Magnetic Bragg diffraction is absent and 90% of the neutron spectral weight forms a continuum of magnetic scattering with low-energy pinch points, indicating NaCaNi 2 F 7 is in a Coulomb-like phase. Our results demonstrate that disorder can act to freeze only the lowest-energy magnetic degrees of freedom; at higher energies, a magnetic excitation continuum characteristic of fractionalized excitations persists. Despite of the charge disorder, the three-dimensional antiferromagnet NaCaNi 2 F 7 is an almost ideal realization of the spin-1 antiferromagnetic Heisenberg model on a pyrochlore lattice, showing key features of quantum spin liquid.
ISSN:1745-2473
1745-2481
DOI:10.1038/s41567-018-0317-3