Figure 2
From: Dynamic control of heat flow using a spin-chain ladder cuprate film and an ionic liquid

In situ Raman spectroscopy under voltage application. (a) Schematic cross section of the sample, which is drawn neglecting the light refraction. (b) Raman spectra when V = 0 V and when the laser spot is focused on the half-depth area of the ionic liquid (IL spectrum) and the interface between the ionic liquid and the LCCO film (IL/LCCO spectrum). The IL/LCCO–IL spectrum shows an increase in intensity compared with the IL and IL/LCCO spectra, where IL/LCCO has been normalized so that the peak at ~ 3,000 cm−1 in DEME+30 disappears in the IL/LCCO–IL spectrum. (c) Change in the IL/LCCO–IL spectrum by repetitive voltage application and short-circuiting, as shown in (d). (e) V dependence of the change in intensity at ~ 2,000 cm−1.