Fig. 5: High photoexcitation limit.
From: Phonon transport manipulation in TiSe2 via reversible charge density wave melting
(Left) Comparison between the phonon dispersion of the CDW (black) and the 1 × 1 phase (red) along the Γ–M path for ne = 0.074640; the latter has been folded to allow a direct comparison. (Right) Cumulative thermal conductivity as a function of phonon frequency of the CDW phase.
