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Percolation-Based Metal-Insulator Transition in Black Phosphorus Field Effect Transistors

Authors
Ali, N[Ali, Nasir]Lee, M[Lee, Myeongjin]Ali, F[Ali, Fida]Ngo, TD[Ngo, Tien Dat]Park, H[Park, Hyokwang]Shin, H[Shin, Hoseong]Yoo, WJ[Yoo, Won Jong]
Issue Date
15-Mar-2023
Publisher
AMER CHEMICAL SOC
Keywords
black phosphorus; metal-insulator transition; Mott VRH; density inhomogeneity; 2D percolation
Citation
ACS APPLIED MATERIALS & INTERFACES, v.15, no.10, pp.13299 - 13306
Indexed
SCIE
SCOPUS
Journal Title
ACS APPLIED MATERIALS & INTERFACES
Volume
15
Number
10
Start Page
13299
End Page
13306
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/102889
DOI
10.1021/acsami.2c22046
ISSN
1944-8244
Abstract
The existence of a novel phenomenon, such as the metal-insulator transition (MIT) in two-dimensional (2D) systems, affords emerging functional properties that provide new aspects for future electronics and optoelectronics. Here, we report the observation of the MIT in black phosphorus field effect transistors by tuning the carrier density (n) controlled by back-gate bias. We find that the conductivity follows an n dependence as sigma(n) proportional to n alpha with alpha 1, which indicates the presence of screened Coulomb impurity scattering at high carrier densities in the temperature range of 10-300 K. As n decreases, the screened Coulomb impurity scattering breaks down, developing strong charge density inhomogeneity leading to a percolation-based transition at the critical carrier density (nC). At low carrier densities (n < nC), the system is in the insulating regime, which is expressed by Mott variable range hopping that demonstrates the role of disorder in the system. In addition, the extracted average values of critical exponent delta are -1.29 +/- 0.01 and -1.14 +/- 0.01 for devices A and B, respectively, consistent with the 2D percolation exponent of 4/3, confirming the 2D percolation-based MIT in BP devices. Our findings strongly suggest that the 2D MIT observed in BP is a classical percolation-based transition caused by charge inhomogeneity induced by screened Coulomb charge impurity scattering around a transition point controlled by n through back gate bias.
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