by Lu, Xingye, McNally, D. E., Sala, M. Moretti, Terzic, J. and Upton, M. H., Casa, D., Ingold, G., Cao, G. and Schmitt, T.
Abstract:
We use resonant elastic and inelastic x-ray scattering at the Ir-L-3 edge to study the doping-dependent magnetic order, magnetic excitations, and spin-orbit excitons in the electron-doped bilayer iridate (Sr1-xLax)(3)Ir2O7 (0 <= x <= 0.065). With increasing doping x, the three-dimensional long range anti-ferromagnetic order is gradually suppressed and evolves into a three-dimensional short range order across the insulator-to-metal transition from x = 0 to 0.05, followed by a transition to two-dimensional short range order between x = 0.05 and 0.065. Because of the interactions between the J(eff) = 1/2 pseudospins and the emergent itinerant electrons, magnetic excitations undergo damping, anisotropic softening, and gap collapse, accompanied by weakly doping-dependent spin-orbit excitons. Therefore, we conclude that electron doping suppresses the magnetic anisotropy and interlayer couplings and drives (Sr1-xLax)(3)Ir2O7 into a correlated metallic state with two-dimensional short range antiferromagnetic order. Strong antiferromagnetic fluctuations of the J(eff) = 1/2 moments persist deep in this correlated metallic state, with the magnon gap strongly suppressed.
Reference:
Doping Evolution of Magnetic Order and Magnetic Excitations in (Sr1-xLax)(3)Ir2O7 (Lu, Xingye, McNally, D. E., Sala, M. Moretti, Terzic, J. and Upton, M. H., Casa, D., Ingold, G., Cao, G. and Schmitt, T.), In PHYSICAL REVIEW LETTERS, AMER PHYSICAL SOC, volume 118, 2017.
Bibtex Entry:
@article{ ISI:000391927700009,
Author = {Lu, Xingye and McNally, D. E. and Sala, M. Moretti and Terzic, J. and
Upton, M. H. and Casa, D. and Ingold, G. and Cao, G. and Schmitt, T.},
Title = {{Doping Evolution of Magnetic Order and Magnetic Excitations in
(Sr1-xLax)(3)Ir2O7}},
Journal = {{PHYSICAL REVIEW LETTERS}},
Year = {{2017}},
Volume = {{118}},
Number = {{2}},
Month = {{JAN 12}},
Abstract = {{We use resonant elastic and inelastic x-ray scattering at the Ir-L-3
edge to study the doping-dependent magnetic order, magnetic excitations,
and spin-orbit excitons in the electron-doped bilayer iridate
(Sr1-xLax)(3)Ir2O7 (0 <= x <= 0.065). With increasing doping x, the
three-dimensional long range anti-ferromagnetic order is gradually
suppressed and evolves into a three-dimensional short range order across
the insulator-to-metal transition from x = 0 to 0.05, followed by a
transition to two-dimensional short range order between x = 0.05 and
0.065. Because of the interactions between the J(eff) = 1/2 pseudospins
and the emergent itinerant electrons, magnetic excitations undergo
damping, anisotropic softening, and gap collapse, accompanied by weakly
doping-dependent spin-orbit excitons. Therefore, we conclude that
electron doping suppresses the magnetic anisotropy and interlayer
couplings and drives (Sr1-xLax)(3)Ir2O7 into a correlated metallic state
with two-dimensional short range antiferromagnetic order. Strong
antiferromagnetic fluctuations of the J(eff) = 1/2 moments persist deep
in this correlated metallic state, with the magnon gap strongly
suppressed.}},
Publisher = {{AMER PHYSICAL SOC}},
Address = {{ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA}},
Type = {{Article}},
Language = {{English}},
Affiliation = {{Lu, XY (Corresponding Author), Paul Scherrer Inst, Res Dept Synchrotron Radiat & Nanotechnol, CH-5232 Villigen, Switzerland.
Lu, Xingye; McNally, D. E.; Ingold, G.; Schmitt, T., Paul Scherrer Inst, Res Dept Synchrotron Radiat & Nanotechnol, CH-5232 Villigen, Switzerland.
Sala, M. Moretti, European Synchrotron Radiat Facil, BP 220, F-38043 Grenoble, France.
Terzic, J.; Cao, G., Univ Kentucky, Dept Phys & Astron, Lexington, KY 40506 USA.
Terzic, J.; Cao, G., Univ Colorado Boulder, Dept Phys, Boulder, CO 80309 USA.
Upton, M. H.; Casa, D., Argonne Natl Lab, Adv Photon Source, Argonne, IL 60439 USA.
Ingold, G., Paul Scherrer Inst, SwissFEL, CH-5232 Villigen, Switzerland.}},
DOI = {{10.1103/PhysRevLett.118.027202}},
Article-Number = {{027202}},
ISSN = {{0031-9007}},
EISSN = {{1079-7114}},
Keywords-Plus = {{FERMI ARCS; SPIN; PHYSICS}},
Research-Areas = {{Physics}},
Web-of-Science-Categories = {{Physics, Multidisciplinary}},
Author-Email = {{xingye.lu@psi.ch
thorsten.schmitt@psi.ch}},
ResearcherID-Numbers = {{Lu, Xingye/Q-4184-2019
Moretti, Marco/AAF-9255-2019
Schmitt, Thorsten/A-7025-2010
Sala, Marco Moretti/H-1034-2014
}},
ORCID-Numbers = {{Lu, Xingye/0000-0002-0409-1240
Moretti, Marco/0000-0002-9744-9976
Sala, Marco Moretti/0000-0002-9744-9976
Lu, Xingye/0000-0001-7526-3145
McNally, Daniel/0000-0003-3872-4306}},
Funding-Acknowledgement = {{Swiss National Science FoundationSwiss National Science Foundation
(SNSF); NCCR-MARVEL; European CommunityEuropean Community (EC)
{[}290605]; US National Science FoundationNational Science Foundation
(NSF) {[}DMR-1265162, DMR-1712101]; DOE Office of Science by Argonne
National LaboratoryUnited States Department of Energy (DOE)
{[}DE-AC02-06CH11357]}},
Funding-Text = {{We thank Matteo Rossi (ESRF) for helpful discussions. The work at PSI is
supported by the Swiss National Science Foundation through its Sinergia
network Mott Physics Beyond the Heisenberg Model (MPBH) and the
NCCR-MARVEL. Xingye Lu acknowledges financial support from the European
Community's Seventh Framework Programme (FP7/2007-2013) under Grant
agreement No. 290605 (COFUND: PSI-FELLOW). G. Cao acknowledges support
by the US National Science Foundation via Grants No. DMR-1265162 and No.
DMR-1712101. The work used Sector 27 of the Advanced Photon Source, a
U.S. Department of Energy (DOE) Office of Science User Facility operated
for the DOE Office of Science by Argonne National Laboratory under
Contract No. DE-AC02-06CH11357.}},
Number-of-Cited-References = {{56}},
Times-Cited = {{17}},
Usage-Count-Last-180-days = {{1}},
Usage-Count-Since-2013 = {{47}},
Journal-ISO = {{Phys. Rev. Lett.}},
Doc-Delivery-Number = {{EH7BL}},
Unique-ID = {{ISI:000391927700009}},
OA = {{Green Published, Bronze}},
DA = {{2020-12-22}},
}
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