by Sala, M. Moretti, Schnells, V., Boseggia, S., Simonelli, L. and Al-Zein, A., Vale, J. G., Paolasini, L., Hunter, E. C. and Perry, R. S., Prabhakaran, D., Boothroyd, A. T., Krisch, M. and Monaco, G., Ronnow, H. M., McMorrow, D. F. and Mila, F.
Abstract:
The magnetic excitation spectrum in the bilayer iridate Sr3Ir2O7 has been investigated using high-resolution resonant inelastic x-ray scattering (RIXS) performed at the iridium L-3 edge and theoretical techniques. A study of the systematic dependence of the RIXS spectrum on the orientation of the wave-vector transfer Q, with respect to the iridium-oxide bilayer, has revealed that the magnon dispersion is comprised of two branches well separated in energy and gapped across the entire Brillouin zone. Our results contrast with those of an earlier study which reported the existence of a single dominant branch. While these earlier results were interpreted as two overlapping modes within a spin-wave model of weakly coupled iridium-oxide planes, our results are more reminiscent of those expected for a system of weakly coupled dimers. In this latter approach, the lower-and higher-energy modes find a natural explanation as those corresponding to transverse and longitudinal fluctuations, respectively. We have therefore developed a bond-operator theory which describes the magnetic dispersion in Sr3Ir2O7 in terms of quantum dimer excitations. In our model, dimerization is produced by the leading Heisenberg exchange J(c), which couples iridium ions in adjacent planes of the bilayer. The Hamiltonian also includes in-plane exchange J, as well as further neighbor couplings and relevant anisotropies. The bond-operator theory provides an excellent account of the dispersion of both modes, while the measured Q dependence of the RIXS intensities is in reasonable qualitative accord with the spin-spin correlation function calculated from the theory. We discuss our results in the context of the quantum criticality of bilayer dimer systems in the presence of anisotropic interactions derived from strong spin-orbit coupling.
Reference:
Evidence of quantum dimer excitations in Sr3Ir2O7 (Sala, M. Moretti, Schnells, V., Boseggia, S., Simonelli, L. and Al-Zein, A., Vale, J. G., Paolasini, L., Hunter, E. C. and Perry, R. S., Prabhakaran, D., Boothroyd, A. T., Krisch, M. and Monaco, G., Ronnow, H. M., McMorrow, D. F. and Mila, F.), In PHYSICAL REVIEW B, AMER PHYSICAL SOC, volume 92, 2015.
Bibtex Entry:
@article{ ISI:000357485100009,
Author = {Sala, M. Moretti and Schnells, V. and Boseggia, S. and Simonelli, L. and
Al-Zein, A. and Vale, J. G. and Paolasini, L. and Hunter, E. C. and
Perry, R. S. and Prabhakaran, D. and Boothroyd, A. T. and Krisch, M. and
Monaco, G. and Ronnow, H. M. and McMorrow, D. F. and Mila, F.},
Title = {{Evidence of quantum dimer excitations in Sr3Ir2O7}},
Journal = {{PHYSICAL REVIEW B}},
Year = {{2015}},
Volume = {{92}},
Number = {{2}},
Month = {{JUL 6}},
Abstract = {{The magnetic excitation spectrum in the bilayer iridate Sr3Ir2O7 has
been investigated using high-resolution resonant inelastic x-ray
scattering (RIXS) performed at the iridium L-3 edge and theoretical
techniques. A study of the systematic dependence of the RIXS spectrum on
the orientation of the wave-vector transfer Q, with respect to the
iridium-oxide bilayer, has revealed that the magnon dispersion is
comprised of two branches well separated in energy and gapped across the
entire Brillouin zone. Our results contrast with those of an earlier
study which reported the existence of a single dominant branch. While
these earlier results were interpreted as two overlapping modes within a
spin-wave model of weakly coupled iridium-oxide planes, our results are
more reminiscent of those expected for a system of weakly coupled
dimers. In this latter approach, the lower-and higher-energy modes find
a natural explanation as those corresponding to transverse and
longitudinal fluctuations, respectively. We have therefore developed a
bond-operator theory which describes the magnetic dispersion in Sr3Ir2O7
in terms of quantum dimer excitations. In our model, dimerization is
produced by the leading Heisenberg exchange J(c), which couples iridium
ions in adjacent planes of the bilayer. The Hamiltonian also includes
in-plane exchange J, as well as further neighbor couplings and relevant
anisotropies. The bond-operator theory provides an excellent account of
the dispersion of both modes, while the measured Q dependence of the
RIXS intensities is in reasonable qualitative accord with the spin-spin
correlation function calculated from the theory. We discuss our results
in the context of the quantum criticality of bilayer dimer systems in
the presence of anisotropic interactions derived from strong spin-orbit
coupling.}},
Publisher = {{AMER PHYSICAL SOC}},
Address = {{ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA}},
Type = {{Article}},
Language = {{English}},
Affiliation = {{Sala, MM (Corresponding Author), European Synchrotron Radiat Facil, BP 220, F-38043 Grenoble, France.
Sala, M. Moretti; Simonelli, L.; Al-Zein, A.; Paolasini, L.; Krisch, M.; Monaco, G., European Synchrotron Radiat Facil, F-38043 Grenoble, France.
Schnells, V., Univ Wurzburg, Inst Theoret Phys & Astrophys, D-97074 Wurzburg, Germany.
Boseggia, S.; Vale, J. G.; Perry, R. S.; McMorrow, D. F., UCL, London Ctr Nanotechnol, London WC1E 6BT, England.
Boseggia, S.; Vale, J. G.; Perry, R. S.; McMorrow, D. F., UCL, Dept Phys & Astron, London WC1E 6BT, England.
Boseggia, S., Diamond Light Source Ltd, Didcot OX11 0DE, Oxon, England.
Simonelli, L., CELLS ALBA Synchrotron Radiat Facil, Barcelona 08290, Spain.
Hunter, E. C., Ctr Sci Extreme Condit, Edinburgh EH9 3FD, Midlothian, Scotland.
Prabhakaran, D.; Boothroyd, A. T., Univ Oxford, Dept Phys, Clarendon Lab, Oxford OX1 3PU, England.
Monaco, G., Univ Trento, Dipartimento Fis, I-38123 Povo, TN, Italy.
Ronnow, H. M., Ecole Polytech Fed Lausanne, Lab Quantum Magnetism, CH-1015 Lausanne, Switzerland.
Ronnow, H. M., Univ Tokyo, Inst Solid State Phys, Neutron Sci Lab, Kashiwa, Chiba 2778581, Japan.
Mila, F., Ecole Polytech Fed Lausanne, Inst Theoret Phys, CH-1015 Lausanne, Switzerland.}},
DOI = {{10.1103/PhysRevB.92.024405}},
Article-Number = {{024405}},
ISSN = {{2469-9950}},
EISSN = {{2469-9969}},
Keywords-Plus = {{SPIN GAPS; FRUSTRATION; STATES}},
Research-Areas = {{Materials Science; Physics}},
Web-of-Science-Categories = {{Materials Science, Multidisciplinary; Physics, Applied; Physics,
Condensed Matter}},
ResearcherID-Numbers = {{Zein, Ali Al/F-4393-2019
Moretti, Marco/AAF-9255-2019
Krisch, Michael H/U-5662-2018
Ronnow, Henrik M/A-4953-2009
McMorrow, Desmond Francis/M-9036-2019
Simonelli, Laura/I-1963-2015
Mila, Frederic/R-4871-2019
McMorrow, Desmond/C-2655-2008
Vale, James/A-1475-2016
Monaco, Giulio/AAW-4387-2020
Sala, Marco Moretti/H-1034-2014
}},
ORCID-Numbers = {{Moretti, Marco/0000-0002-9744-9976
Krisch, Michael H/0000-0001-7423-1715
Ronnow, Henrik M/0000-0002-8832-8865
McMorrow, Desmond Francis/0000-0002-4947-7788
Mila, Frederic/0000-0003-4306-7996
McMorrow, Desmond/0000-0002-4947-7788
Vale, James/0000-0002-9148-3575
Monaco, Giulio/0000-0003-2497-6422
Sala, Marco Moretti/0000-0002-9744-9976
Giles, Emily/0000-0001-9880-1102}},
Funding-Acknowledgement = {{Swiss National Science FoundationSwiss National Science Foundation
(SNSF); ERC starters grant TOPOLECTRICS {[}ERC-StG-TOPOLECTRICS-336012];
Sinergia network Mott Physics Beyond the Heisenberg Model;
EPSRCEngineering & Physical Sciences Research Council (EPSRC);
Engineering and Physical Sciences Research CouncilEngineering &
Physical Sciences Research Council (EPSRC) {[}EP/J017124/1,
EP/G007357/1, EP/J016713/1, 1268395, 1745233] Funding Source:
researchfish}},
Funding-Text = {{We gratefully thank C. Henriquet and R. Verbeni for technical assistance
during the experiments and B. Normand, O. Syljuaasen, and B. Dalla
Piazza for insightful discussions. The work in Lausanne was supported by
the Swiss National Science Foundation and its Sinergia network Mott
Physics Beyond the Heisenberg Model, in London by the EPSRC, and in
Wurzburg by the ERC starters grant TOPOLECTRICS under
ERC-StG-TOPOLECTRICS-336012.}},
Number-of-Cited-References = {{40}},
Times-Cited = {{31}},
Usage-Count-Last-180-days = {{0}},
Usage-Count-Since-2013 = {{87}},
Journal-ISO = {{Phys. Rev. B}},
Doc-Delivery-Number = {{CM2BR}},
Unique-ID = {{ISI:000357485100009}},
OA = {{Green Published}},
DA = {{2020-12-22}},
}
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