Infrared spectroscopic study of CuO: Signatures of strong spin-phonon interaction and structural distortion

A. B. Kuz’menko, D. van der Marel, P. J. M. van Bentum, E. A. Tishchenko, C. Presura, and A. A. Bush
Phys. Rev. B 63, 094303 – Published 2 February 2001
PDFExport Citation

Abstract

Optical properties of single-crystal monoclinic CuO in the range 706000cm1 were studied at temperatures from 7 to 300 K. Normal reflection spectra were obtained from the (001) and (010) crystal faces thus giving separate data for the Au and Bu phonon modes excited in the purely transverse way (TO modes). Mode parameters, including polarizations of the Bu modes not determined by the crystal symmetry, were extracted by the dispersion analysis of reflectivity curves as a function of temperature. Spectra of all the components of the optical conductivity tensor were obtained using the Kramers-Kronig method recently extended to the case of the low-symmetry crystals. The number of strong phonon modes is in agreement with the factor-group analysis for the crystal structure currently accepted for the CuO. However, several “extra” modes of minor intensity are detected; some of them are observed in the whole studied temperature range, while existence of others becomes evident at low temperatures. Comparison of frequencies of “extra” modes with the available phonon dispersion curves points to possible “diagonal” doubling of the unit cell {a,b,c}{a+c,b,ac} and formation of the superlattice. The previously reported softening of the Au3 mode (400cm1) with cooling at TN is found to be 10% for the TO mode. The mode is very broad at high temperatures and strongly narrows in the antiferromagnetic phase. We attribute this effect to strong resonance coupling of this mode to optical or acoustic bimagnons and reconstruction of the magnetic excitations spectrum at the Néel point. A significant anisotropy of ε is observed: it was found to be 5.9 along the b axis, 6.2 along the [101] chains, and 7.8 along the [101¯] chains. The transverse effective charge eT* is more or less isotropic; its value is about two electrons.

  • Received 24 January 2000

DOI:https://doi.org/10.1103/PhysRevB.63.094303

©2001 American Physical Society

Authors & Affiliations

A. B. Kuz’menko1, D. van der Marel2, P. J. M. van Bentum3, E. A. Tishchenko1, C. Presura2, and A. A. Bush4

  • 1P. L. Kapitza Institute for Physical Problems RAS, Kosygina street, 2, Moscow, 117334, Russia
  • 2Solid State Physics Laboratory, University of Groningen, Nijenborgh 4, 9747 AG Groningen, The Netherlands
  • 3High Field Magnet Laboratory, University of Nijmegen, 6525 ED, Nijmegen, The Netherlands
  • 4Moscow State Institute of Radiotechnics, Electronics and Automation, Vernadskogo pr., 78, Moscow, 117464, Russia

References (Subscription Required)

Click to Expand
Issue

Vol. 63, Iss. 9 — 1 March 2001

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×
×

Images

×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×