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. 2019 Nov 11;10:5119. doi: 10.1038/s41467-019-12963-3

Fig. 4.

Fig. 4

Time-resolved photoluminescence and Raman scattering spectra. a PL decay traces for a WSe2 monolayer placed on a planar GaP substrate (purple) and coupled to a nano-antenna with r=200 nm (yellow). Grey shows the instrument response function (IRF). The PL signal is measured with a 90-ps pulsed laser, under low excitation power of 0.2 W/cm2, to avoid exciton–exciton annihilation processes. Resolution-limited dynamics are measured for WSe2 coupled to a dimer. Dotted black lines show results of the fitting with exponential decay. b Raman scattering spectra for 1L-WSe2 placed on GaP nano-antennas with r = 50 nm (red) and 200 nm (yellow) and on the planar GaP (black). c Raman scattering spectra for 2L-WSe2 on a r = 200 nm GaP nano-antenna (orange) and on the planar GaP (black). d Experimental Raman enhancement factor, EFRaman (see Eq. (3) in ‘Methods’), obtained (after background subtraction) for the 250 cm1 peak in 1L- and 2L-WSe2 coupled to nano-antennas with various r