• Infrared and Laser Engineering
  • Vol. 52, Issue 6, 20230217 (2023)
Ping Liu1,2, Wei Xu1,2, Feng Xiong1,2, Jinbao Jiang1,2..., Xianyan Huang1,2 and Zhihong Zhu1,2,*|Show fewer author(s)
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies & Hunan Provincial Key Laboratory of Novel Nano-Optoelectronic Information Materials and Devices, National University of Defense Technology, Changsha 410073, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha 410073, China
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    DOI: 10.3788/IRLA20230217 Cite this Article
    Ping Liu, Wei Xu, Feng Xiong, Jinbao Jiang, Xianyan Huang, Zhihong Zhu. Photodetection properties of van der Waals vertical heterostructures based on photogenerated carrier-dominated FN tunneling[J]. Infrared and Laser Engineering, 2023, 52(6): 20230217 Copy Citation Text show less
    Structure and characterization of the graphene/MoS2/h-BN/graphene vertical heterostructure photodetector device; (a) Schematic of the device structure; (b) Corresponding optical microscopy image and AFM characterization of the real fabricated heterostructure device; (c1), (c2) Raman spectra of MoS2, graphene and h-BN
    Fig. 1. Structure and characterization of the graphene/MoS2/h-BN/graphene vertical heterostructure photodetector device; (a) Schematic of the device structure; (b) Corresponding optical microscopy image and AFM characterization of the real fabricated heterostructure device; (c1), (c2) Raman spectra of MoS2, graphene and h-BN
    Photocurrent characteristics of the graphene/MoS2/h-BN/graphene vertical heterostructure photodetector device. The I-V characteristics of the device under dark and 532 nm laser illumination with applied (a) negative bias and (b) positive bias; FN tunneling fitting curves of the device under dark and 532 nm laser illumination with applied (c) negative bias and (d) positive bias
    Fig. 2. Photocurrent characteristics of the graphene/MoS2/h-BN/graphene vertical heterostructure photodetector device. The I-V characteristics of the device under dark and 532 nm laser illumination with applied (a) negative bias and (b) positive bias; FN tunneling fitting curves of the device under dark and 532 nm laser illumination with applied (c) negative bias and (d) positive bias
    Energy band diagrams of the graphene/MoS2/h-BN/graphene heterostructure. (a) Energy band diagram of the device with zero bias. (b) Energy band diagrams of the device under dark and 532 nm laser illumination at Vds < VN-D-FN; (c) Energy band diagrams of the device under dark and 532 nm laser illumination at Vds > VP-D-FN
    Fig. 3. Energy band diagrams of the graphene/MoS2/h-BN/graphene heterostructure. (a) Energy band diagram of the device with zero bias. (b) Energy band diagrams of the device under dark and 532 nm laser illumination at Vds < VN-D-FN; (c) Energy band diagrams of the device under dark and 532 nm laser illumination at Vds > VP-D-FN
    Optoelectronic properties of the graphene/MoS2/h-BN/graphene vertical heterostructure device. (a) The I-V characteristics of the device under dark and 532 nm laser illumination with different power densities; (b) ln(Ids/V2)–1/Vds curves of the device under dark and 532 nm laser illumination with different power densities; (c) Power-dependent photocurrent of the device at Vds = 6.75 V; (d) Responsivity and Ilight/Idark ratio along with illumination intensities
    Fig. 4. Optoelectronic properties of the graphene/MoS2/h-BN/graphene vertical heterostructure device. (a) The I-V characteristics of the device under dark and 532 nm laser illumination with different power densities; (b) ln(Ids/V2)–1/Vds curves of the device under dark and 532 nm laser illumination with different power densities; (c) Power-dependent photocurrent of the device at Vds = 6.75 V; (d) Responsivity and Ilight/Idark ratio along with illumination intensities
    Comparison of the response time and cyclic stability between graphene/MoS2/h-BN/graphene vertical heterostructure and graphene/MoS2 heterostructure devices. (a) The dynamic temporal photoresponse of the graphene/MoS2/h-BN/graphene heterostructure device with the enlarged current profile between 11 s and 16 s; (b) The dynamic temporal photoresponse of the graphene/MoS2 heterostructure device with the enlarged current profile between 60 s and 100 s
    Fig. 5. Comparison of the response time and cyclic stability between graphene/MoS2/h-BN/graphene vertical heterostructure and graphene/MoS2 heterostructure devices. (a) The dynamic temporal photoresponse of the graphene/MoS2/h-BN/graphene heterostructure device with the enlarged current profile between 11 s and 16 s; (b) The dynamic temporal photoresponse of the graphene/MoS2 heterostructure device with the enlarged current profile between 60 s and 100 s
    VN-D-FN/V φh_Gra/eV VP-D-FN/V φh_MoS2/eV
    BNM-14−8.42.4 eV5.31.6
    Table 1. The transition bias and barrier height of the graphene/MoS2/h-BN/graphene vertical heterostructure photodetector device under 532 nm laser illumination
    Device structureDark current/AResponse time/sLaser wavelength/nmReference
    Gra/h-BN/MoS2/Gra ~10−12~0.3532This work
    Gra/MoS2~10−6~20532This work
    Gra/h-BN/MoS2~10−14~0.25405[17]
    Gra/h-BN/SnS2~10−12~2300[18]
    WSe2/Gra/h-BN/MoS2~10−14~0.4532[19]
    Gra/MoS2~10−51.2632.8[21]
    Gra/MoS2 island ~10−51.5632.8[22]
    Gra/MoS2/Gra ~10−40.59405-2 000[23]
    Table 2. Comparison between the performances of typical vertical heterostructure photodetector devices
    Ping Liu, Wei Xu, Feng Xiong, Jinbao Jiang, Xianyan Huang, Zhihong Zhu. Photodetection properties of van der Waals vertical heterostructures based on photogenerated carrier-dominated FN tunneling[J]. Infrared and Laser Engineering, 2023, 52(6): 20230217
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