on the electrical and thermal transport in borophane, by means of the Boltzmann transport equation. We first propose an accurate low-energy model Hamiltonian for borophane, then, the electronic contribution to the thermoelectric transport of the monolayer borophane is investigated. We consider a monolayer borophane in diffusive transport regime in the $x$–$y$ plane, driven by a lattice temperature gradient ${\vec{\nabla }}T$ and an electric field ${\vec{\mathcal{E}}}$. The generalized Boltzmann transport equation is applied to obtain the conductivity, Seebeck coefficient and the figure of merit, by considering the various types of resistive scattering potentials, (1) the short-range (SR) potential, (2) the long-range (LR) Coulomb potential, with a Thomas- Fermi screening as the source of scattering and (3) the impurities containing short-range electric and ferromagnetically ordered magnetic potentials, called electro-magnetic (SREM) scatterers. At low temperature elastic scattering becomes the dominant mechanism as inelastic scattering is strongly suppressed. In this work our focus is on elastic scattering and therefore, with good approximation, intervalley scattering (interband processes) is neglected  [@E.H.Hwang08].

Our calculations show that although the electrical conductivity of borophane is highly anisotropic, but the Seebeck coefficient and the corresponding figure of merit, irrespective of the underlying scattering mechanisms, are isotropic. Interestingly, for the short-range 