Magnetic nature of the 500 meV peak in LaSrCuO observed with resonant inelastic X-ray scattering at the Cu -edge

銅K吸収端での共鳴非弾性X線散乱で観測されるLaSrCuOの500meVピークの磁気的性質

Ellis, D. S.*; Kim, J.*; Hill, J. P.*; 脇本 秀一  ; Birgeneau, R. J.*; Shvyd'ko, Y.*; Casa, D.*; Gog, T.*; 石井 賢司; 池内 和彦*; Paramekanti, A.*; Kim, Y.-J.*

Ellis, D. S.*; Kim, J.*; Hill, J. P.*; Wakimoto, Shuichi; Birgeneau, R. J.*; Shvyd'ko, Y.*; Casa, D.*; Gog, T.*; Ishii, Kenji; Ikeuchi, Kazuhiko*; Paramekanti, A.*; Kim, Y.-J.*

We present a comprehensive study of the temperature and doping dependence of the 500 meV peak observed at in resonant inelastic X-ray scattering (RIXS) experiments on LaCuO. The intensity of this peak persists above the Nel temperature ( = 320 K), but decreases gradually with increasing temperature, reaching zero at around = 500 K. The peak energy decreases with temperature in close quantitative accord with the behavior of the two-magnon Raman peak in LaCuO and, with suitable rescaling, agrees with the Raman peak shifts in EuBaCuO and KNiF. The overall dispersion of this excitation in the Brillouin zone is found to be in agreement with theoretical calculations for a two-magnon excitation. Upon doping, the peak intensity decreases analogous to the Raman mode intensity and appears to track the doping dependence of the spin-correlation length. Taken together, these observations strongly suggest that the 500 meV mode is magnetic in character and is likely a two-magnon excitation.