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  • Letter

Low-energy magneto-optics of Tb2Ti2O7 in a [111] magnetic field

Xinshu Zhang, Yi Luo, T. Halloran, J. Gaudet, Huiyuan Man, S. M. Koohpayeh, and N. P. Armitage
Phys. Rev. B 103, L140403 – Published 12 April 2021
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Abstract

The pyrochlore magnet Tb2Ti2O7 shows a lack of magnetic order to low temperatures and is considered to be a quantum spin liquid candidate. We perform time-domain THz spectroscopy on high-quality Tb2Ti2O7 crystals and study the low-energy excitations as a function of [111] magnetic field with high energy resolution. The low-energy crystal-field excitations change their energies anomalously under magnetic field. Despite several sharp field-dependent changes, we show that the material's spectrum can be described not by phase transitions but by field-dependent hybridization between the low-energy crystal-field levels. We highlight the strong coupling between spin and lattice degrees of freedom in Tb2Ti2O7 as evidenced by the magnetic-field tunable crystal-field environment. Calculations based on single ion physics with field-induced symmetry reduction of the crystal-field environment can reproduce our data.

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  • Received 25 September 2020
  • Accepted 22 March 2021

DOI:https://doi.org/10.1103/PhysRevB.103.L140403

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Xinshu Zhang1, Yi Luo1, T. Halloran1, J. Gaudet1, Huiyuan Man1, S. M. Koohpayeh1,2, and N. P. Armitage1

  • 1Institute for Quantum Matter, Department of Physics and Astronomy, The Johns Hopkins University, Baltimore, Maryland 21218, USA
  • 2Department of Materials Science and Engineering, The Johns Hopkins University, Baltimore, Maryland 21218, USA

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Issue

Vol. 103, Iss. 14 — 1 April 2021

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Images

  • Figure 1
    Figure 1

    Transmission amplitude for (a) left and (b) right circularly polarized THz light as a function of frequency and magnetic field up to 6.9 T at 1.6 K. Four excitations are observed in the left channel indicated by α1L, β1L,β2L, α2L, and two excitations in the right channel indicated by β1R and β2R. (c) schematic of CEF splitting in magnetic field labeled as G1, G2, E1, and E2. The red and blue arrows indicate transitions at two different sites α and β. (d) Tetrahedron with red and blue spheres represent the two different Tb ions under [111] magnetic field.

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  • Figure 2
    Figure 2

    (a) Calculated energy of four lowest crystal fields as a function of field for Tbα. The observed excitations α1L and α2L correspond to transitions G1G2 and G1E1 of Tbα. Color plot of calculated intensity as function of energy and field for Tbα in left (b) and right (c) channels. The weak intensity at low field in (c) is the transition from thermally populated G2E2. (d) Calculated energy of four lowest crystal fields as a function of field for Tbβ. The observed excitations β1L,β1R and β2L,β2R correspond to transitions G1E1 and G1E2 of Tbβ, respectively. (e), (f) Color plot of calculated intensity as function of energy and field for Tbβ in left and right.

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  • Figure 3
    Figure 3

    (a) Comparison between experiment and calculated energy with consideration of field-induced crystal-field environment change. Red and blue represent Tbα and Tbβ. Color plot of calculated intensity as function of energy and field for Tbα and Tbβ in left (b) and right (c) channels.

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