scatters, just like graphene, the short-range conductivities of borophane have constant values (independent of the chemical potential), that are $\sigma_{xx}=250 \ e^2/h$ and $\sigma_{yy}=33 \ e^2/h$, at $T=20\, {\rm K}$, along the armchair and zigzag direction, respectively. As a measure of thermoelectric efficiency, the figure of merit, reaches to about $2.75$ and $1$, at $T\sim20 \, {\rm K}$ and room temperature ($T=300\, {\rm K}$), respectively. We also investigate the effect of the magnetic scatters on thermoelectric transport coefficients. The conductivities of the SREM scatterers have a linear dependence on the doping levels. These results propose that borophane could be a promising material for the thermoelectric applications.

The paper is organized as follows. In Sec. \[sec:model\], at first the model Hamiltonian and lattice structure of borophane is introduced and then the method which is used to calculate the conductivity and thermoelectric coefficients using the generalized Boltzmann method, is explained. In Sec. \[sec:results\], we present and describe our numerical results from the exact calculations for the conductivity and thermoelectric coefficients for borophane. Finally, we conclude and summarize our main results in Sec. \[sec:concl\].

Model Hamiltonian of borophene {#sec:model}
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In the following sections, we consider a monolayer of borophane at low temperature. 