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Title: Multiple Coulomb phase in the fluoride pyrochlore CsNiCrF6

Abstract

The Coulomb phase is an idealized state of matter whose properties are determined by factors beyond conventional considerations of symmetry, including global topology, conservation laws and emergent order. In theory, Coulomb phases occur in ice-type systems such as water ice and spin ice; in dimer models; and in certain spin liquids. Yet, apart from ice-type systems, more general experimental examples are very scarce. Here we study the partly disordered material CsNiCrF6 and show that this material is a multiple Coulomb phase with signature correlations in three degrees of freedom: charge configurations, atom displacements and spin configurations. We use neutron and X-ray scattering to separate these correlations and to determine the magnetic excitation spectrum. Our results reveal how the structural and magnetic properties of apparently disordered materials may inherit, and be dictated by, a hidden symmetry—the local gauge symmetry of an underlying Coulomb phase.

Authors:
ORCiD logo [1];  [2]; ORCiD logo [3];  [1];  [4];  [4];  [4];  [1];  [1];  [5]
  1. Paul Scherrer Inst. (PSI), Villigen (Switzerland)
  2. Univ. of Edinburgh, Scotland (United Kingdom)
  3. Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
  4. Inst. Laue-Langevin (ILL), Grenoble (France)
  5. Univ. College London (UCL), London (United Kingdom)
Publication Date:
Research Org.:
Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Basic Energy Sciences (BES)
OSTI Identifier:
1506794
Grant/Contract Number:  
AC05-00OR22725
Resource Type:
Accepted Manuscript
Journal Name:
Nature Physics
Additional Journal Information:
Journal Volume: 15; Journal Issue: 1; Journal ID: ISSN 1745-2473
Publisher:
Nature Publishing Group (NPG)
Country of Publication:
United States
Language:
English
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS

Citation Formats

Fennell, T., Harris, M. J., Calder, S., Ruminy, M., Boehm, M., Steffens, P., Lemée-Cailleau, M. -H., Zaharko, O., Cervellino, A., and Bramwell, S. T. Multiple Coulomb phase in the fluoride pyrochlore CsNiCrF6. United States: N. p., 2018. Web. doi:10.1038/s41567-018-0309-3.
Fennell, T., Harris, M. J., Calder, S., Ruminy, M., Boehm, M., Steffens, P., Lemée-Cailleau, M. -H., Zaharko, O., Cervellino, A., & Bramwell, S. T. Multiple Coulomb phase in the fluoride pyrochlore CsNiCrF6. United States. https://doi.org/10.1038/s41567-018-0309-3
Fennell, T., Harris, M. J., Calder, S., Ruminy, M., Boehm, M., Steffens, P., Lemée-Cailleau, M. -H., Zaharko, O., Cervellino, A., and Bramwell, S. T. Mon . "Multiple Coulomb phase in the fluoride pyrochlore CsNiCrF6". United States. https://doi.org/10.1038/s41567-018-0309-3. https://www.osti.gov/servlets/purl/1506794.
@article{osti_1506794,
title = {Multiple Coulomb phase in the fluoride pyrochlore CsNiCrF6},
author = {Fennell, T. and Harris, M. J. and Calder, S. and Ruminy, M. and Boehm, M. and Steffens, P. and Lemée-Cailleau, M. -H. and Zaharko, O. and Cervellino, A. and Bramwell, S. T.},
abstractNote = {The Coulomb phase is an idealized state of matter whose properties are determined by factors beyond conventional considerations of symmetry, including global topology, conservation laws and emergent order. In theory, Coulomb phases occur in ice-type systems such as water ice and spin ice; in dimer models; and in certain spin liquids. Yet, apart from ice-type systems, more general experimental examples are very scarce. Here we study the partly disordered material CsNiCrF6 and show that this material is a multiple Coulomb phase with signature correlations in three degrees of freedom: charge configurations, atom displacements and spin configurations. We use neutron and X-ray scattering to separate these correlations and to determine the magnetic excitation spectrum. Our results reveal how the structural and magnetic properties of apparently disordered materials may inherit, and be dictated by, a hidden symmetry—the local gauge symmetry of an underlying Coulomb phase.},
doi = {10.1038/s41567-018-0309-3},
journal = {Nature Physics},
number = 1,
volume = 15,
place = {United States},
year = {Mon Oct 22 00:00:00 EDT 2018},
month = {Mon Oct 22 00:00:00 EDT 2018}
}

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Cited by: 12 works
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Figures / Tables:

Fig. 1 Fig. 1: Illustration of mappings and structural features of CsNiCrF6. A: The pyrochlore lattice (medial) consists of corner-sharing tetrahedra, on which a Coulomb phase can be established by ensuring that local degrees of freedom can be represented by a non-divergent field that is derived from lattice fluxes on the diamondmore » lattice (parent) (I). A non-divergent configuration of flux variables (blue arrows) around a diamond lattice point is equivalent to the ice rule for spins in a spin ice (two-in-two-out). Antiferromagnetic pseudo-spins are related to the flux variables and configured two-up-two-down in a Coulomb phase ground state (green and orange arrows). B: Two cations occupying the pyrochlore lattice form a charge ice, with cation configurations directly related to the pseudo-spins (green and orange spheres). C: Vector spins coupled antiferromagnetically on the pyrochlore lattice (i.e. a pyrochlore Heisenberg antiferromagnet) must satisfy the condition that the total magnetization of every tetrahedron is zero (black arrows), which can be ensured if the $S$x,y,z vector components are each represented by a family of pseudospins that each obey the ice rule (blue, green and orange arrows). D: In the structure of CsNiCrF6, F- anions (small blue spheres) are coordinated to two cations. The bond valence sum requirements of the cations can be satisfied by displacing anions shared by a pair of unlike cations towards the cation with larger charge (Cr3+). Anions shared between a pair of like cations are not displaced. The edges with non-displaced cations can be identified as a fully packed loop model (FPL) on the diamond lattice, in which loops cover every link of the lattice, every site is visited by exactly two loops, and a given loop is occupied only by one of the cation species (green and orange lines). E: The structure of CsNiCrF6 is composed of the pyrochlore lattice of cations, coordinated by octahedra of F- ions. The octahedra share each of their vertices with one other octahedron, forming tetraheda of tilted octahedra. Extended sections of the FPL are shown, but the octahedra are drawn undistorted. F: The structure contains large cages in which the Cs+ ions reside. The cage coordination is by 18 F- ions, forming an octahedron that is truncated and capped with rectangular pyramids.« less

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