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We report the results of Raman scattering experiments on single crystals of La 2x Sr x CuO 4  (La214) as a function of temperature and doping. In underdoped compounds low-energy B 1g  spectral weight is depleted in association with the opening of a pseudogap on regions of the Fermi surface located near (±π, 0) and (0, ±π).The magnitude of the depletion increases with decreasing doping, and in the most underdoped samples, with decreasing temperature.The spectral weight that is lost at low energies (ω [Formula: see text] 800 cm 1 ) is transferred to the higher energy region normally occupied by multimagnon scattering. From the normal-state B 2g  spectra we have determined the scattering rate Γ(ω,T) of qausiparticles located near the diagonal directions in k-space. In underdoped compounds, Γ(ω,T) is suppressed at low temperatures for energies less than E g(x)  [Formula: see text] 800 cm 1 . The doping dependence of both the two-magnon scattering and the scattering rate suppression suggest that the pseudogap is characterized by an energy scale E g  ~ J, where J is the antiferromagnetic super-exchange energy. Comparison with the results from other techniques provides a consistent picture of the pseudogap in La214.PACS Nos.: 74.25.Gz, 74.72.Dn, 78.30.Er

The pseudogap in La2xSrxCuO4: A Raman viewpoint

The pseudogap in La_2xSr_xCuO₄: A Raman viewpoint