57 research outputs found

    Van Vleck excitons in Ca2RuO4

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    A framework is presented for modeling and understanding magnetic excitations in localized, intermediate coupling magnets where the interplay between spin-orbit coupling, magnetic exchange, and crystal field effects are known to create a complex landscape of unconventional magnetic behaviors and ground states. A spin-orbit exciton approach for modeling these excitations is developed based upon a Hamiltonian which explicitly incorporates single-ion crystalline electric field and spin exchange terms. This framework is then leveraged to understand a canonical Van Vleck jeff=0j\rm{_{eff}}=0 singlet ground state whose excitations are coupled spin and crystalline electric field levels. Specifically, the anomalous Higgs mode [Jain et al. Nat. Phys. 13, 633 (2017)], spin-waves [S. Kunkem\"{o}ller et al. Phys. Rev. Lett. 115, 247201 (2015)], and orbital excitations [L. Das et al. Phys. Rev. X 8, 011048 (2018)] in the multiorbital Mott insulator Ca2_2RuO4_4 are captured and good agreement is found with previous neutron and inelastic x-ray spectroscopic measurements. Furthermore, our results illustrate how a crystalline electric field-induced singlet ground state can support coherent longitudinal, or amplitude excitations, and transverse wavelike dynamics. We use this description to discuss mechanisms for accessing a nearby critical point.Comment: 18 pages, 8 figure

    Fermi surface mapping and the nature of charge density wave order in the kagome superconductor CsV3_3Sb5_5

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    The recently discovered family of AV3_3Sb5_5 (A: K, Rb Cs) kagome metals possess a unique combination of nontrivial band topology, superconducting ground states, and signatures of electron correlations manifest via competing charge density wave order. Little is understood regarding the nature of the charge density wave (CDW) instability inherent to these compounds and the potential correlation with the accompanying onset of a large anomalous Hall response. To understand the impact of the CDW order on the electronic structure in these systems, we present quantum oscillation measurements on single crystals of CsV3_3Sb5_5. Our data provides direct evidence that the CDW invokes a substantial reconstruction of the Fermi surface pockets associated with the vanadium orbitals and the kagome lattice framework. In conjunction with density functional theory modeling, we are able to identify split oscillation frequencies originating from reconstructed pockets built from vanadium orbitals and Dirac-like bands. Complementary diffraction measurements are further able to demonstrate that the CDW instability has a correlated phasing between neighboring V3_3Sb5_5 planes. These results provide critical insights into the underlying CDW instability in AV3_3Sb5_5 kagome metals and support minimal models of CDW order arising from within the vanadium-based kagome lattice.Comment: 12 pages, 9 figure

    Spin-orbit excitons in CoO

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    CoO has an odd number of electrons in its unit cell, and therefore is expected to be metallic. Yet, CoO is strongly insulating owing to significant electronic correlations, thus classifying it as a Mott insulator. We investigate the magnetic fluctuations in CoO using neutron spectroscopy. The strong and spatially far-reaching exchange constants reported in [Sarte et al. Phys. Rev. B 98 024415 (2018)], combined with the single-ion spin-orbit coupling of similar magnitude [Cowley et al. Phys. Rev. B 88, 205117 (2013)] results in significant mixing between jeffj_{eff} spin-orbit levels in the low temperature magnetically ordered phase. The high degree of entanglement, combined with the structural domains originating from the Jahn-Teller structural distortion at ∼\sim 300 K, make the magnetic excitation spectrum highly structured in both energy and momentum. We extend previous theoretical work on PrTl3_{3} [Buyers et al. Phys. Rev. B 11, 266 (1975)] to construct a mean-field and multi-level spin exciton model employing the aforementioned spin exchange and spin-orbit coupling parameters for coupled Co2+^{2+} ions on a rocksalt lattice. This parameterization, based on a tetragonally distorted type-II antiferromagnetic unit cell, captures both the sharp low energy excitations at the magnetic zone center, and the energy broadened peaks at the zone boundary. However, the model fails to describe the momentum dependence of the excitations at high energy transfers, where the neutron response decays faster with momentum than the Co2+^{2+} form factor. We discuss such a failure in terms of a possible breakdown of localized spin-orbit excitons at high energy transfers.Comment: (main text - 21 pages, 12 figures; supplementary information - 15 pages, 3 figures, to be published in Phys. Rev. B

    Spin-orbital correlations from complex orbital order in MgV2_{2}O4_{4}

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    MgV2_{2}O4_{4} is a spinel based on magnetic V3+^{3+} ions which host both spin (S=1S=1) and orbital (leff=1l_{eff}=1) moments. Owing to the underlying pyrochlore coordination of the magnetic sites, the spins in MgV2_{2}O4_{4} only antiferromagnetically order once the frustrating interactions imposed by the Fd3‾mFd\overline{3}m lattice are broken through an orbitally-driven structural distortion at TS_{S} ≃\simeq 60 K. Consequently, a N\'eel transition occurs at TN_{N} ≃\simeq 40 K. Low temperature spatial ordering of the electronic orbitals is fundamental to both the structural and magnetic properties, however considerable discussion on whether it can be described by complex or real orbital ordering is ambiguous. We apply neutron spectroscopy to resolve the nature of the orbital ground state and characterize hysteretic spin-orbital correlations using x-ray and neutron diffraction. Neutron spectroscopy finds multiple excitation bands and we parameterize these in terms of a multi-level (or excitonic) theory based on the orbitally degenerate ground state. Meaningful for the orbital ground state, we report an "optical-like" mode at high energies that we attribute to a crystal-field-like excitation from the spin-orbital jeffj_{eff}=2 ground state manifold to an excited jeffj_{eff}=1 energy level. We parameterize the magnetic excitations in terms of a Hamiltonian with spin-orbit coupling and local crystalline electric field distortions resulting from deviations from perfect octahedra surrounding the V3+^{3+} ions. We suggest that this provides compelling evidence for complex orbital order in MgV2_{2}O4_{4}. We then apply the consequences of this model to understand hysteretic effects in the magnetic diffuse scattering where we propose that MgV2_{2}O4_{4} displays a high temperature orbital memory of the low temperature spin order.Comment: 21 pages and 13 figure

    Absence of moment fragmentation in the mixed B-site pyrochlore Nd<sub>2</sub>GaSbO<sub>7</sub>

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    Nd-based pyrochlore oxides of the form Nd2B2_{2}B_{2}O7_{7} have garnered a significant amount of interest owing to the moment fragmentation physics observed in Nd2_{2}Zr2_{2}O7_{7} and speculated in Nd2_{2}Hf2_{2}O7_{7}. Notably this phenomenon is not ubiquitous in this family, as it is absent in Nd2_{2}Sn2_{2}O7_{7}, which features a smaller ionic radius on the BB-site. Here, we explore the necessary conditions for moment fragmentation in the Nd pyrochlore family through a detailed study of the mixed BB-site pyrochlore Nd2_{2}GaSbO7_{7}. The BB-site of this system is characterized by significant disorder and an extremely small average ionic radius. Similarly to Nd2_{2}Sn2_{2}O7_{7}, we find no evidence for moment fragmentation through our bulk characterization and neutron scattering experiments, indicating that chemical pressure (and not necessarily the BB-site disorder) plays a key role in the presence or absence of this phenomenon in this material family. Surprisingly, the presence of significant BB-site disorder in Nd2_{2}GaSbO7_{7} does not generate a spin glass ground state and instead the same all-in-all-out magnetic order identified in other Nd pyrochlores is found here.Comment: 11 pages, 8 figure
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