TY - JOUR
T1 - Wafer-scale synthesis of 2D dirac heterostructures for self-driven, fast, broadband photodetectors
AU - Yu, Wenzhi
AU - Dong, Zhuo
AU - Mu, Haoran
AU - Ren, Guanghui
AU - He, Xiaoyue
AU - Li, Xiu
AU - Lin, Shenghuang
AU - Zhang, Kai
AU - Bao, Qiaoliang
AU - Mokkapati, Sudha
N1 - Funding Information:
This work was financially supported by the Starting Research Fund from Songshan Lake Materials Laboratory. S.M. acknowledges the support from the Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET). The authors also acknowledge the support from the National Natural Science Foundation of China (Grant No. 61922082, 61875223), and the Shenzhen Nanshan District Pilotage Team Program (LHTD20170006). This work was also supported by the National Key R&D Program of China (No. 2021YFA1202902), Guangdong Basic and Applied Basic Research Foundation (No. 2021B1515120034).
Publisher Copyright:
© 2022 American Chemical Society.
PY - 2022/8/23
Y1 - 2022/8/23
N2 - Type-II Dirac semimetal platinum ditelluride (PtTe2) is a promising functional material for photodetectors because of its specially tilted Dirac cones, strong light absorption, and high carrier mobilities. The stack of two-dimensional (2D) Dirac heterostructures consisting of PtTe2 and graphene could overcome the limit of detection range and response time occurring in the heterostructures of graphene and other low-mobility and large-gap transition metal dichalcogenides (TMDs). Here, we report an approach for achieving highly controllable, wafer-scale production of 2D Dirac heterostructures of PtTe2/graphene with tunable thickness, variable size, and CMOS compatibility. More importantly, the optimized recipes achieve the exact stoichiometric ratio of 1:2 for Pt and Te elements without contaminating the underlayer graphene film. Because of the built-in electric field at the junction area, the photodetectors based on the PtTe2/graphene heterostructure are self-driven with a broadband photodetection from 405 to 1850 nm. In particular, the photodetectors have a high responsivity of up to 0.52 AW-1 (without bias) and a fast response time of 8.4 μs. Our work demonstrated an approach to synthesizing hybrid 2D Dirac heterostructures, which can be applied in the integration of on-chip, CMOS-compatible photodetectors with near-infrared detection, high sensitivity, and low energy consumption.
AB - Type-II Dirac semimetal platinum ditelluride (PtTe2) is a promising functional material for photodetectors because of its specially tilted Dirac cones, strong light absorption, and high carrier mobilities. The stack of two-dimensional (2D) Dirac heterostructures consisting of PtTe2 and graphene could overcome the limit of detection range and response time occurring in the heterostructures of graphene and other low-mobility and large-gap transition metal dichalcogenides (TMDs). Here, we report an approach for achieving highly controllable, wafer-scale production of 2D Dirac heterostructures of PtTe2/graphene with tunable thickness, variable size, and CMOS compatibility. More importantly, the optimized recipes achieve the exact stoichiometric ratio of 1:2 for Pt and Te elements without contaminating the underlayer graphene film. Because of the built-in electric field at the junction area, the photodetectors based on the PtTe2/graphene heterostructure are self-driven with a broadband photodetection from 405 to 1850 nm. In particular, the photodetectors have a high responsivity of up to 0.52 AW-1 (without bias) and a fast response time of 8.4 μs. Our work demonstrated an approach to synthesizing hybrid 2D Dirac heterostructures, which can be applied in the integration of on-chip, CMOS-compatible photodetectors with near-infrared detection, high sensitivity, and low energy consumption.
KW - near-infrared
KW - photodetector
KW - platinum ditelluride
KW - self-driven device
KW - two-dimensional heterostructures
UR - http://www.scopus.com/inward/record.url?scp=85136106243&partnerID=8YFLogxK
U2 - 10.1021/acsnano.2c05278
DO - 10.1021/acsnano.2c05278
M3 - Article
C2 - 35904281
AN - SCOPUS:85136106243
SN - 1936-0851
VL - 16
SP - 12922
EP - 12929
JO - ACS Nano
JF - ACS Nano
IS - 8
ER -