Ferroelectric Polarization Effects on the Transport Properties of Graphene/PMN-PT Field Effect Transistors

Single-layer graphene was transferred onto (1 – x)[Pb(Mg1/3Nb2/3)O3]–x[PbTiO3]0.3 (PMN-PT) substrate to investigate the transport properties of graphene-based field effect transistors (FETs) by ferroelectric gating. The graphene/PMN-PT FET exhibited p-type characteristics with a large memory window...

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Veröffentlicht in:Journal of physical chemistry. C 2013-07, Vol.117 (26), p.13747-13752
Hauptverfasser: Jie, Wenjing, Hui, Yeung Yu, Chan, Ngai Yui, Zhang, Yang, Lau, Shu Ping, Hao, Jianhua
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container_end_page 13752
container_issue 26
container_start_page 13747
container_title Journal of physical chemistry. C
container_volume 117
creator Jie, Wenjing
Hui, Yeung Yu
Chan, Ngai Yui
Zhang, Yang
Lau, Shu Ping
Hao, Jianhua
description Single-layer graphene was transferred onto (1 – x)[Pb(Mg1/3Nb2/3)O3]–x[PbTiO3]0.3 (PMN-PT) substrate to investigate the transport properties of graphene-based field effect transistors (FETs) by ferroelectric gating. The graphene/PMN-PT FET exhibited p-type characteristics with a large memory window and an on/off current ratio of about 5.5 in air ambient conditions at room temperature. By prepoling the PMN-PT substrate, the FET showed a reduction in p-doping for the graphene/PMN-PT FET, implying the pre-polarization and the polarization reversal played an important part in the behaviors of graphene on PMN-PT. The observation of simultaneous rise in gate current with the dramatic transition in drain current suggested that the transport properties of graphene mainly stemmed from the coupling of the ferroelectric polarization to the charge carriers in graphene. The field effect mobility and the excess hole concentration were calculated to be about 4.52 × 103 cm2 V–1 s–1 and 6.74 × 1012 cm–2, respectively. Furthermore, the sheet resistance showed high dependence on temperature and gate voltage, indicating metallic behaviors of graphene on PMN-PT. Additionally, the sheet resistance of graphene on the PMN-PT was much smaller than that on SiO2.
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The graphene/PMN-PT FET exhibited p-type characteristics with a large memory window and an on/off current ratio of about 5.5 in air ambient conditions at room temperature. By prepoling the PMN-PT substrate, the FET showed a reduction in p-doping for the graphene/PMN-PT FET, implying the pre-polarization and the polarization reversal played an important part in the behaviors of graphene on PMN-PT. The observation of simultaneous rise in gate current with the dramatic transition in drain current suggested that the transport properties of graphene mainly stemmed from the coupling of the ferroelectric polarization to the charge carriers in graphene. The field effect mobility and the excess hole concentration were calculated to be about 4.52 × 103 cm2 V–1 s–1 and 6.74 × 1012 cm–2, respectively. Furthermore, the sheet resistance showed high dependence on temperature and gate voltage, indicating metallic behaviors of graphene on PMN-PT. 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subjects Applied sciences
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Cross-disciplinary physics: materials science
rheology
Dielectric, piezoelectric, ferroelectric and antiferroelectric materials
Dielectrics, piezoelectrics, and ferroelectrics and their properties
Electronics
Exact sciences and technology
Fullerenes and related materials
diamonds, graphite
Materials science
Physics
Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices
Specific materials
Transistors
title Ferroelectric Polarization Effects on the Transport Properties of Graphene/PMN-PT Field Effect Transistors
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