. 2019 Jun 16;19(7):4702–4711. doi: 10.1021/acs.nanolett.9b01775

Table 2. Calculated and Experimental Frequencies of the Folding-Originated Modes for GaP TSL Expressed as Frequency Shifts from the TO Mode^a.

	TSL mode 1(cm^–1)	TSL mode2 (cm^–1)	TSL mode3 (cm^–1)	TSL mode 4 (cm^–1)	TSL mode 5 (cm^–1)	TSL mode 6 (cm^–1)	TSL mode 7(cm^–1)
theory	7.6	9.5	14.0	18.9	23.5	27.0	29.0
exp.	7.9	9.6	14.4	20.2	24.6		29.3

Experimental frequencies refer to the spectra displayed in Figure 3b. The TSL period in both theory and experiment is 9 nm. The scattering configuration used both for experiments and calculations is the x̅(yy)x. The error on the experimental values is ±1.5 cm^–1.

Table 2. Calculated and Experimental Frequencies of the Folding-Originated Modes for GaP TSL Expressed as Frequency Shifts from the TO Modea.

Table 2. Calculated and Experimental Frequencies of the Folding-Originated Modes for GaP TSL Expressed as Frequency Shifts from the TO Mode^a.