2021
DOI: 10.1103/physrevmaterials.5.024004
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Remote free-carrier screening to boost the mobility of Fröhlich-limited two-dimensional semiconductors

Abstract: Van der Waals heterostructures provide a versatile tool to not only protect or control, but also enhance the properties of a 2D material. We use ab initio calculations and semianalytical models to find strategies which boost the mobility of a current-carrying two-dimensional (2D) semiconductor within a heterostructure. Free-carrier screening from a metallic "screener" layer remotely suppresses electron-phonon interactions in the currentcarrying layer. This concept is most effective in 2D semiconductors whose s… Show more

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Cited by 20 publications
(9 citation statements)
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“…The second is a more peculiar multi-valley mechanism, that can actually enhance the coupling with LA and A1 modes at large doping, when K and Q (or Γ) are both occupied [33,62,63]. While some works have considered standard screening in the literature [64][65][66], the multivalley mechanism was only recently understood qualitatively for the A1 mode [33] and has not yet been accounted for in mobility simulations. Here, it is modeled quantitatively (see section 3) and discovered to govern the coupling to the LA mode as well.…”
Section: Transport As a Function Of Electrostatic Doping And Valley P...mentioning
confidence: 99%
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“…The second is a more peculiar multi-valley mechanism, that can actually enhance the coupling with LA and A1 modes at large doping, when K and Q (or Γ) are both occupied [33,62,63]. While some works have considered standard screening in the literature [64][65][66], the multivalley mechanism was only recently understood qualitatively for the A1 mode [33] and has not yet been accounted for in mobility simulations. Here, it is modeled quantitatively (see section 3) and discovered to govern the coupling to the LA mode as well.…”
Section: Transport As a Function Of Electrostatic Doping And Valley P...mentioning
confidence: 99%
“…For the LO and TA phonon, coupling to electrons via the Fröhlich and piezoelectric interactions, the matrix elements are corrected with the ratio of the dielectric functions computed as ε = 1 − v c (χ 0 + χ 0 d ), where v c = 2πe 2 q is the Coulomb kernel in 2D. χ 0 d is the dielectric susceptibility (of the neutral material) computed from DFPT as in [65]. The non-interacting susceptibility χ 0 from the added carriers is computed similarly to our previous work [65] but in the new shifted band structure:…”
Section: Mobilitymentioning
confidence: 99%
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“…For the LO and TA phonon, coupling to electrons via the Fröhlich and piezoelectric interactions, the matrix elements are corrected with the ratio of the dielectric functions computed as = 1 − v c χ 0 , where v c = 2π q is the Coulomb kernel in 2D. The non-interacting susceptibility χ 0 of the added carriers, is computed similarly to our previous work 71 but in the new shifted band structure:…”
Section: Mobilitymentioning
confidence: 99%
“…Work by Pizzi et al [30] on layer-dependent interactions in stacked materials composed of the same ML used symmetry arguments and a spring model to understand layer dependent vibrational properties in vdW structures. Sohier et al [31] examined the effect of dielectric heterostructuring on charge transport through explicit mutually induced electrostatics. In the hexagonal TMDs, Phillips et al [32] and Terrones et al [33] calculated the electronic structure of experimentally realized bilayer heterostructures in both AA and AA' stacking (known as "AB stacking" in their work) assuming a commensurate structure and found both direct and indirect electronic band gaps.…”
Section: Introductionmentioning
confidence: 99%