by h.[]{data-label="lattice"}](lattice){width="3.3in"}

![(Color online) The band structure of borophane in the first Brillouin zone along the $\Gamma-X$ direction. We have compared our used model Hamiltonian (Eq.\[boeqn\]) with the calculations, based on the density functional theory and non-equilibrium Green’s function approaches [@Anpccp2018].[]{data-label="fig-dis"}](fig-dis){width="3.3in"}

\[dispersion\]

![(Color online) (a) Isoenergy contour map of the electronic band structure of borophane in the $k-$space for $E(\vec{k}_{\rm F})=-0.5$ to $0.5$ eV. The contour lines are drawn at $0.05$ eV intervals in both the electron(solid-navy) and hole (dashed-green) doped cases. (b) Density of states (DOS) calculated for monolayer borophane (solid-navy) and graphene (dashed-green).[]{data-label="energyDispersion"}](fig1 "fig:"){width="3.5in"} ![(Color online) (a) Isoenergy contour map of the electronic band structure of borophane in the $k-$space for $E(\vec{k}_{\rm F})=-0.5$ to $0.5$ eV. The contour lines are drawn at $0.05$ eV intervals in both the electron(solid-navy) and hole (dashed-green) doped cases. (b) Density of states (DOS) calculated for monolayer borophane (solid-navy) and graphene (dashed-green).[]{data-label="energyDispersion"}](fig-dos "fig:"){width="3.5in"}

Anisotropic transport framework
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In this section, we present our main formalism for the numerical evaluation of the thermoelectric coefficients of borophane, in the diffusive regime, using the generalized semiclassical Boltzmann equation. In particular, we take into account three important cases of short-range impurities with Dirac delta potential (*e.g.*, defects 