  We theoretically study the influence of impurity scattering on the electric
and thermal transport of borophane layer, a two-dimensional anisotropic Dirac
semi-metal with two tilted and anisotropic Dirac cones. In a systematic
framework, we have calculated exactly the electrical conductivity and
thermoelectric coefficients of borophane in the presence of the short-range,
long-range charged impurity and the short-range electro-magnetic (SREM)
scatterers, by using the exact solution of the Boltzmann transport equation
within the linear-response theory. Contrary to the large electron-hole
asymmetry in borophane, its electron-hole conductivity is nearly symmetric.
Interestingly, for the short-range scatters, just like graphene, the
short-range conductivities of borophane have the constant values, independent
of the chemical potential, while the conductivities of the SREM scatterers are
linearly dependent on the chemical potential. Regardless of the impurity type,
the electric conductivity of borophane is highly anisotropic, while the Seebeck
coefficient and figure of merit (${\it ZT}$) are isotropic. Along with the
ambipolar nature of the borophane thermopower, a very high value of ${\it ZT}$
around unity is obtained at room temperature, due to the large asymmetry
between electrons and holes in borophane. More importantly, borophane attains
its maximum value of ${\it ZT}$ at very low chemical potentials, in the
vicinity of the charge neutrality point. In comparison to phosphorene, a highly
unique anisotropic 2D material, borophane with a higher anisotropy ratio
($\sigma_{xx}/\sigma_{yy}\sim10$), is an unprecedented anisotropic material.
This high anisotropy ratio together with the large figure of merit, suggest
that borophane is promising for the thermoelectric applications and transport
switching in the Dirac transport channels.
