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CMP
Credit: Jack Hobhouse

Dr Dharmalingam Prabhakaran

Researcher

Research theme

  • Quantum materials

Sub department

  • Condensed Matter Physics

Research groups

  • Synthesis and crystal growth
dharmalingam.prabhakaran@physics.ox.ac.uk
Telephone: 01865 (2)72270,01865 (2)72351,01865 (2)72341
Clarendon Laboratory, room 175,375,374B,374A,371A,371,177,115,373 (office)
  • About
  • Publications

Tracking a hysteretic and disorder-broadened phase transition via the electromagnon response in improper ferroelectrics

JOURNAL OF PHYSICS D-APPLIED PHYSICS 51:8 (2018) ARTN 084002

Authors:

CDW Mosley, D Prabhakaran, J Lloyd-Hughes
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Coupling between Spin and Charge Order Driven by Magnetic Field in Triangular Ising System LuFe2O4+delta

CRYSTALS 8:2 (2018) ARTN 88

Authors:

L Ding, F Orlandi, DD Khalyavin, AT Boothroyd, D Prabhakaran, G Balakrishnan, P Manuel
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Stability of charge-stripe ordered La2−xSrxNiO4+δ at one third doping

Physica B: Condensed Matter Elsevier 536 (2017) 720-725

Authors:

PG Freeman, RA Mole, NB Christensen, A Stunault, Dharmalingam Prabhakaran

Abstract:

The stability of charge ordered phases is doping dependent, with different materials having particularly stable ordered phases. In the half filled charge ordered phases of the cuprates this occurs at one eighth doping, whereas in charge-stripe ordered La2−xSrxNiO4+δ there is enhanced stability at one third doping. In this paper we discuss the known details of the charge-stripe order in La2−x SrxNiO4+δ, and how these properties lead to the one third doping stability.
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The full magnon spectrum of yttrium iron garnet

npj Quantum Materials 2:1 (2017)

Authors:

AJ Princep, RA Ewings, S Ward, S Tóth, C Dubs, D Prabhakaran, AT Boothroyd
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Terahertz spectroscopy of anisotropic materials using beams with rotatable polarization.

Scientific Reports 7:1 (2017) 12337-12337

Authors:

CDW Mosley, M Failla, D Prabhakaran, J Lloyd-Hughes

Abstract:

We introduce a polarization-resolved terahertz time-domain spectrometer with a broadband (0.3-2.5 THz), rotatable THz polarization state, and which exhibits minimal change in the electric field amplitude and polarization state upon rotation. This was achieved by rotating an interdigitated photoconductive emitter, and by detecting the orthogonal components of the generated THz pulse via electro-optic sampling. The high precision (<0.1°) and accuracy (<1.0°) of this approach is beneficial for the study of anisotropic materials without rotating the sample, which can be impractical, for instance for samples held in a cryostat. The versatility of this method was demonstrated by studying the anisotropic THz optical properties of uniaxial and biaxial oxide crystals. For uniaxial ZnO and LaAlO3, which have minimal THz absorption across the measurement bandwidth, the orientations of the eigenmodes of propagation were conveniently identified as the orientation angles that produced a transmitted THz pulse with zero ellipticity, and the birefringence was quantified. In CuO, a multiferroic with improper ferroelectricity, the anisotropic THz absorption created by an electromagnon was investigated, mapping its selection rule precisely. For this biaxial crystal, which has phonon and electromagnon absorption, the polarization eigenvectors exhibited chromatic dispersion, as a result of the monoclinic crystal structure and the frequency-dependent complex refractive index.
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