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Temperature-dependent Raman and x-ray studies of the spin-ice pyrochlore Dy2Ti2O7 and nonmagnetic pyrochlore Lu2Ti2O7

Surajit Saha, Surjeet Singh, B. Dkhil, S. Dhar, R. Suryanarayanan, G. Dhalenne, A. Revcolevschi, and A. K. Sood
Phys. Rev. B 78, 214102 – Published 8 December 2008

Abstract

We present here temperature-dependent Raman, x-ray diffraction, and specific heat studies between room temperature and 12 K on single crystals of spin-ice pyrochlore compound Dy2Ti2O7 and its nonmagnetic analog Lu2Ti2O7. Raman data show a “new” band not predicted by factor group analysis of Raman-active modes for the pyrochlore structure in Dy2Ti2O7, appearing below a temperature of Tc=110K with a concomitant contraction of the cubic unit cell volume as determined from the powder x-ray diffraction analysis. Low-temperature Raman experiments on O18-isotope substituted Dy2Ti2O7 confirm the phonon origin of the new mode. These findings, absent in Lu2Ti2O7, suggest that the room-temperature cubic lattice of the pyrochlore Dy2Ti2O7 undergoes a “subtle” structural transformation near Tc. We find anomalous redshift of some of the phonon modes in both the Dy2Ti2O7 and the Lu2Ti2O7 as the temperature decreases, which is attributed to strong phonon-phonon anharmonic interactions.

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  • Received 9 July 2008

DOI:https://doi.org/10.1103/PhysRevB.78.214102

©2008 American Physical Society

Authors & Affiliations

Surajit Saha1, Surjeet Singh2, B. Dkhil3, S. Dhar4, R. Suryanarayanan2, G. Dhalenne2, A. Revcolevschi2, and A. K. Sood1,*

  • 1Department of Physics, Indian Institute of Science, Bangalore 560012, India
  • 2Laboratoire de Physico-Chimie de l’Etat Solide, ICMMO, CNRS, Universite Paris-Sud, UMR8648, Bâtiment 414, 91405 Orsay, France
  • 3Laboratoire Structures, Proprietes et Modelisation des Solides, Ecole Centrale Paris, CNRS-UMR8580, Grande voie des vignes, 92295 Chatenay-Malabry Cedex, France
  • 4Tata Institute of Fundamental Research, Mumbai 400 005, India

  • *asood@physics.iisc.ernet.in

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Vol. 78, Iss. 21 — 1 December 2008

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Images

  • Figure 1
    Figure 1
    Raman spectrum of Dy2Ti2O7 and Lu2Ti2O7 at 12 K. Open circles represent the experimental data. Raman intensity in the regions from 50–250, 425–475, 475–650, and 6501010cm1 are rescaled with respect to the region between 250425cm1 in order to view the weak modes clearly. The different modes labeled as M1(N1) to M14(N14) are assigned in the text (Table ).Reuse & Permissions
  • Figure 2
    Figure 2
    (Color online) Raman spectra of Dy2Ti2O7 at different temperatures. Solid lines are fit to the experimental data (open circles), as discussed in text. A new mode (M5) appears at 110 K which has been marked by arrows in panels corresponding to 100, 50, and 12 K. Raman intensity in the low frequency regions (50250cm1) has been rescaled.Reuse & Permissions
  • Figure 3
    Figure 3
    (Color online) Temperature dependence of the different modes of Dy2Ti2O7. Solid lines are guides for the eyes. New mode (M5) appears below 110 K.Reuse & Permissions
  • Figure 4
    Figure 4
    Temperature dependence of the different modes of Lu2Ti2O7.Reuse & Permissions
  • Figure 5
    Figure 5
    Raman spectra of O16 (open circle) and O18 (closed circle) isotopic Dy2Ti2O7 at 12 K in the range of 260–370cm1. A change in frequencies is seen with a change in O-ion isotopic mass.Reuse & Permissions
  • Figure 6
    Figure 6
    (Color online) Variation in the lattice parameter of Dy2Ti2O7 with temperature. An abrupt jump of the lattice parameter, indicative of a structural deformation, is seen near 100 K, a temperature where new mode appears in Raman spectrum. In comparison, the lattice parameter of nonmagnetic Lu2Ti2O7 varies smoothly over the entire range of temperature. Solid lines are fit to the data as discussed in text.Reuse & Permissions
  • Figure 7
    Figure 7
    (Color online) (a) Temperature dependence of specific heat (C) for the pyrochlores Dy2Ti2O7 (DTO) and Lu2Ti2O7 (LTO) in the temperature range 5–300 K. Inset: blown-up view of the low-temperature part of the main panel; (b) closed and open circles are data points corresponding to the difference CDTOCLTO. The closed circles represent approximate Schottky contribution (CSch) in the specific heat of DTO above 100 K. The solid line is the calculated Schottky anomaly due to the first five higher lying crystal field doublets at 385, 503, 547, 679, and 956 K taken from Ref. 32.Reuse & Permissions
  • Figure 8
    Figure 8
    Percentage change of frequencies (Δωω%) of (a) Dy2Ti2O7 and (b) Lu2Ti2O7 phonons with temperature which thus indicates a similar amount of phonon softening in both the pyrochlores.Reuse & Permissions
  • Figure 9
    Figure 9
    The intrinsic anharmonic contribution (Δωanh) to the change in frequency of Dy2Ti2O7 phonons estimated from experimental data.Reuse & Permissions
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