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. 2016 Aug 1;113(33):9177–9181. doi: 10.1073/pnas.1606562113

Fig. 2.

Fig. 2.

(A) Symmetry-dependent Raman spectra of FeSe (SP208 crystal) above TS = 87 K using 2.33 eV photons. The sharp peaks superimposed on the electronic continuum are due to Raman active optical phonons. Also shown in Inset are the schematics k-space structures of the Raman form factors in different symmetries (blue and red colors indicate positive and negative amplitudes, respectively), and the polarization configurations used to select them. (B) Temperature dependence of the low energy B1g spectra above TS. (C) Evolution of the B1g spectra across TS. The Inset shows the spectra across the superconducting transition at Tc = 8.5 K (SP208). The arrows indicate 2Δ superconducting peaks.