Abstract

We present a theory for single- and two-phonon charge carrier scattering in anisotropic two-dimensional semiconductors applied to single-layer black phosphorus (BP). We show that in contrast to graphene, where two-phonon processes due to the scattering by flexural phonons dominate at any practically relevant temperatures and are independent of the carrier concentration nn, two-phonon scattering in BP is less important and can be considered negligible at n≳1013n\gtrsim10^{13} cm−2^{-2}. At smaller nn, however, phonons enter in the essentially anharmonic regime. Compared to the hole mobility, which does not exhibit strong anisotropy between the principal directions of BP (μxx/μyy∼1.4μ_{xx}/μ_{yy}\sim1.4 at n=1013n=10^{13} cm−2^{-2} and T=300T=300 K), the electron mobility is found to be significantly more anisotropic (μxx/μyy∼6.2μ_{xx}/μ_{yy}\sim6.2). Absolute values of μxxμ_{xx} do not exceed 250 (700) cm2^2V−1^{-1}s−1^{-1} for holes (electrons), which can be considered as an upper limit for the mobility in BP at room temperature.

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