Using the maximum entropy principle, we present a general theory to describe ac and dc high-field transport in monolayer graphene within a dynamical context. Accordingly, we construct a closed set of hydrodynamic (HD) equations containing the same scattering mechanisms used in standard Monte Carlo (MC) approaches. The effects imputable to a linear band structure, the role of conductivity effective mass of carriers, and their connection with the coupling between the driving field and the dissipation phenomena are analyzed both qualitatively and quantitatively for different electron densities. The theoretical approach is validated by comparing HD results with existing MC simulations.

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37.
If m~ is expressed by means of a nonlinear function of ε, then (A4) can be considered only as a its first linear approximation m~(1). Therefore, using Eq. (A1), we will determine a more complicated expression for the energy with respect to a nonparabolic band structure (A3). However, by assuming that m~ is an increasing function of the energy with m~(ε)m(1)(ε), we obtain still a saturation velocity for the system, where |u|=|k|/m~|k|/m~(1)c.
38.
We remark that m is introduced only for dimensional reasons. Indeed, in Eq. (A2), m~ can be redefined only in terms of the new quantities α~0=mα0 and α~1=mα1 that are the only two experimental parameters that allow us to determine explicitly the conductivity effective mass.
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If α00, then uc and Γ+, but the quantity |α0|Γ tends always to finite value.
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Shishir and co-workers23,46 have employed an expression similar to Eq. (22) but with a factor of eight in the numerator and with an acoustic deformation potential DacMC=16.5eV. Therefore, in order to consider the same expression in the present HD model, we must assume in Eq. (22) Dac=16.58eV. Besides, they seem to ignore the inelastic intervalley (iv) transitions, by using the coupling constant DopMC=109eV/cm (as in the present paper) but with a smaller optical phonon energy of ωop=150meV.
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