The full-potential linearized augmented plane wave method and the semi-classical Boltzmann theory are used to calculate the thermoelectric properties of monolayer BiSbTeSe2. For the monolayer BiSbTeSe2, the Tran-Blaha-modified Becke-Johnson (TB-mBJ) method calculates a larger band gap than that calculated by the generalized gradient approximation (GGA) method. Where the bandgap calculated by TB-mBJ is 0.94, while the bandgap calculated by GGA is 0.85. The absence of imaginary frequencies in the monolayer BiSbTeSe2 phonon band structure ensures its dynamic stability. The contribution of the optical branch to the lattice thermal conductivity is low due to the strong scattering of the optical branch. So the contribution to the lattice thermal conductivity mainly comes from the acoustic branch. The maximum frequency of the acoustic branch is 1.8. The monolayer BiSbTeSe2 has a low lattice thermal conductivity due to the low frequency of the acoustic branch. AIMD simulations confirm its thermal stability. Finally, the ZT value of monolayer BiSbTeSe2 is calculated using TB-mBJ to peak at about 0.98 at a carrier concentration of 2×1020 cm-3 and a temperature of 1125 K. The ZT value of monolayer BiSbTeSe2 is calculated using TB-mBJ.
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