TY - JOUR
T1 - Symmetry breaking on the phonon Raman spectra only at the superconductor compositions in La2-xSrxCuO4
AU - Sugai, S.
AU - Shamoto, S.
AU - Sato, M.
AU - Ido, T.
AU - Takagi, H.
AU - Uchida, S.
N1 - Funding Information:
Acknowledgment - This work was supported by a Grant-in-Aid for Scientific Research on Priority Areas "Mechanism on Superconductivity" from the Ministry of Education, Science and Culture, Japan.
PY - 1990/10
Y1 - 1990/10
N2 - Phonons in La2-xSrxCuO4 were systematically investigated by Raman and infrared spectroscopy covering from the insulator, superconductor, to normal metal compositions. In the Raman spectra, modes which appear only at the superconductor compositions were found. Many of those modes were assigned to the infrared active transverse optical modes with the polarization vectors parallel to the CuO2 plane. The Raman and infrared activity is mutually exclusive in the crystal with inversion symmetry as in the present crystal structure. The appearance of the infrared active modes in the Raman spectra implies that the doped carriers take the states which break the inversion symmetry of phonons only at the superconductor compositions. The larger scattering intensity of those modes than of the natively active modes indicates that the deformation-potential-type electron-phonon interactions are very large. The experimental fact that the longitudinal optical modes do not appear in the Raman spectra indicates that the Fröhlich-type electron-phonon interactions induced by the macroscopic electric field of the longitudinal optical modes do not work.
AB - Phonons in La2-xSrxCuO4 were systematically investigated by Raman and infrared spectroscopy covering from the insulator, superconductor, to normal metal compositions. In the Raman spectra, modes which appear only at the superconductor compositions were found. Many of those modes were assigned to the infrared active transverse optical modes with the polarization vectors parallel to the CuO2 plane. The Raman and infrared activity is mutually exclusive in the crystal with inversion symmetry as in the present crystal structure. The appearance of the infrared active modes in the Raman spectra implies that the doped carriers take the states which break the inversion symmetry of phonons only at the superconductor compositions. The larger scattering intensity of those modes than of the natively active modes indicates that the deformation-potential-type electron-phonon interactions are very large. The experimental fact that the longitudinal optical modes do not appear in the Raman spectra indicates that the Fröhlich-type electron-phonon interactions induced by the macroscopic electric field of the longitudinal optical modes do not work.
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U2 - 10.1016/0038-1098(90)90857-8
DO - 10.1016/0038-1098(90)90857-8
M3 - Article
AN - SCOPUS:0025507318
VL - 76
SP - 371
EP - 376
JO - Solid State Communications
JF - Solid State Communications
SN - 0038-1098
IS - 3
ER -