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Phys. Rev. B 58, 9390–9401 (1998)

Midinfrared optical excitations in undoped lamellar copper oxides

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J. D. Perkins*
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
Center for Basic Sciences, National Renewable Energy Laboratory, Golden, Colorado 80401

R. J. Birgeneau
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

J. M. Graybeal
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
Department of Physics, University of Florida, Gainesville, Florida 32611

M. A. Kastner and D. S. Kleinberg
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

Received 2 April 1997; revised 31 March 1998; published in the issue dated 1 October 1998

The weakly electric-dipole-allowed midinfrared excitations are studied in insulating single crystals of La2CuO4, Sr2CuO2Cl2, and Nd2CuO4. These intrinsic excitations of the undoped CuO2 layers are lower in energy than the charge-transfer excitation. Temperature-dependent optical-absorption measurements are presented from 10 to 450 K. Photoinduced absorption measurements on single-crystal La2CuO4 are also presented. Recent theoretical work and optical-absorption experiments on La2NiO4, as well as the copper oxides, provide strong evidence that a sharp absorption peak seen in all the copper oxides at photon energy ∼0.4 eV and a related peak near 0.25 eV in La2NiO4 arise from phonon-assisted creation of a quasibound two-magnon state. A comparison between the intrinsic absorption in La2NiO4 and that in the copper oxides suggests that the broad midinfrared absorption bands observed between 0.4 and 1.2 eV in the undoped copper oxides have a different electronic origin. We discuss our measurements in regards to two proposed origins (phonon-multimagnon and exciton sidebands) for these broad higher-energy bands. We find that multimagnon and phonon sidebands associated with a Cu dx2-y2d3z2-r2 crystal-field exciton at ∼0.5 eV plausibly explain the structure, strength, and polarization dependence of these broadbands. Direct observation of this exciton would unambiguously confirm or refute this model.

© 1998 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.58.9390
DOI:
10.1103/PhysRevB.58.9390
PACS:
74.25.Gz, 74.72.-h, 75.30.Ds, 75.50.Ee

*Present address: National Renewable Energy Laboratory, Golden, CO 80401.

Present address: Department of Physics, University of Florida, Gainesville, FL 32611.