Transition-metal dichalcogenide (TMD) semiconductors have been widely studied
due to their distinctive electronic and optical properties. The property of TMD
flakes is a function of its thickness, or layer number (N). How to determine N
of ultrathin TMDs materials is of primary importance for fundamental study and
practical applications. Raman mode intensity from substrates has been used to
identify N of intrinsic and defective multilayer graphenes up to N=100.
However, such analysis is not applicable for ultrathin TMD flakes due to the
lack of a unified complex refractive index (n~) from monolayer to bulk
TMDs. Here, we discuss the N identification of TMD flakes on the SiO2โ/Si
substrate by the intensity ratio between the Si peak from 100-nm (or 89-nm)
SiO2โ/Si substrates underneath TMD flakes and that from bare SiO2โ/Si
substrates. We assume the real part of n~ of TMD flakes as that of
monolayer TMD and treat the imaginary part of n~ as a fitting
parameter to fit the experimental intensity ratio. An empirical n~,
namely, n~effโ, of ultrathin MoS2โ, WS2โ and WSe2โ
flakes from monolayer to multilayer is obtained for typical laser excitations
(2.54 eV, 2.34 eV, or 2.09 eV). The fitted n~effโ of MoS2โ has
been used to identify N of MoS2โ flakes deposited on 302-nm SiO2โ/Si
substrate, which agrees well with that determined from their shear and
layer-breathing modes. This technique by measuring Raman intensity from the
substrate can be extended to identify N of ultrathin 2D flakes with N-dependent
n~ . For the application purpose, the intensity ratio excited by
specific laser excitations has been provided for MoS2โ, WS2โ and
WSe2โ flakes and multilayer graphene flakes deposited on Si substrates
covered by 80-110 nm or 280-310 nm SiO2โ layer.Comment: 10 pages, 4 figures. Accepted by Nanotechnolog