or neutral adatoms), the long-range Coulomb impurities and finally the electro-magnetic scatterers, containing short-range electric and ferromagnetically ordered magnetic potentials. Electrical conductance, thermal conductance, Seebeck coefficient, and thermoelectric figure of merit ([*ZT*]{}) of borophane in the presence of both the electric field and the temperature gradient will be studied.

In order to calculate the transport coefficients, we use the following expression for the charge current ${\bf j}$ and energy flux density ${\bf j}^{q}$ $$\begin{aligned}
\left[\begin{array}{c}
{\bf j}  \\
{\bf j}^{q}
\end{array}
\right]=\int\frac{d^2k}{(2\pi)^2}
\left[\begin{array}{c}
-e  \\ \varepsilon({\vec{k}})-\mu
\end{array}
\right]{ v(\vec{k})} f({\vec{k}})
\label{currents}\end{aligned}$$ where ${ v(\vec{k})} =v(\phi)(\cos\xi, \sin\xi)$ is the semiclassical velocity of the carriers, which is related to the energy dispersion $\varepsilon_{\vec{k}}$ through ${\bf v}=(1/\hbar)\nabla_{\vec{k}}\varepsilon_{{\vec{k}}}$ . $f({\vec{k}})$, is the nonequilibrium quantum distribution function, describes the evolution of the charge distribution in the presence of thermoelectric forces, must be computed from the Boltzmann equation. $\xi$ is the angle of the velocity vector with respect to $x$ axis. For this purpose, we take the Boltzmann equation up to a linear order in the presence of thermoelectric forces

$$\begin{aligned}
&&\hspace*{-10pt}\left(-e{\vec{\mathcal{E}}}+\frac{\varepsilon-\mu}{T}{\vec \nabla} T\right)\cdot{\vec{v}}({\vec{k}})\left[-\partial_{\varepsilon}f^{0}(\varepsilon_{{\vec{k}}})\right]=\left(\frac{df}{dt}\right)_{{\rm coll.}}
\label{2dani}\end{aligned}$$

where $w({\vec{k}},{\vec{k}'})$ is the scattering rate from state ${\vec{k}}$ to state ${\vec{k}'}$ which needs to be specified according to the 