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The spectral shape around 85 meV in the present study, i.e., two-peak structure, is different from that reported in Ref.. In the previous investigation, the YVO3 crystal was not correctly oriented. Perhaps, the Raman spectra in Fig. 3 in Ref. were dominated by the polarization configuration of y(zz) ȳ. As for the Raman band around 85 meV in the y(zz) ȳ polarization, the broad shape and the temperature dependence imply that this mode may be electronic in origin, closely related with the spin- and orbital-ordered state. In the lightly hole-doped systems, La1-x Srx VO3, Nd1-x Srx VO3, and Pr1-x Cax VO3 (0
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The spectral shape around 85 meV in the present study, i.e., two-peak structure, is different from that reported in Ref.. In the previous investigation, the YVO3 crystal was not correctly oriented. Perhaps, the Raman spectra in Fig. 3 in Ref. were dominated by the polarization configuration of y(zz) ȳ. As for the Raman band around 85 meV in the y(zz) ȳ polarization, the broad shape and the temperature dependence imply that this mode may be electronic in origin, closely related with the spin- and orbital-ordered state. In the lightly hole-doped systems, La1-x Srx VO3, Nd1-x Srx VO3, and Pr1-x Cax VO3 (0
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