• Photonics Research
  • Vol. 7, Issue 2, 149 (2019)
Yu Yu1, Yating Zhang1、*, Lufan Jin1, Zhiliang Chen1, Yifan Li1, Qingyan Li1, Mingxuan Cao1, Yongli Che1, Haitao Dai2, Junbo Yang3, and Jianquan Yao1
Author Affiliations
  • 1Key Laboratory of Opto-Electronic Information Technology (Tianjin University), Ministry of Education, School of Precision Instruments and Opto-Electronics Engineering, Tianjin University, Tianjin 300072, China
  • 2Tianjin Key Laboratory of Low Dimensional Materials Physics and Preparing Technology, School of Science, Tianjin University, Tianjin 300072, China
  • 3Center of Material Science, National University of Defense Technology, Changsha 410073, China
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    DOI: 10.1364/PRJ.7.000149 Cite this Article Set citation alerts
    Yu Yu, Yating Zhang, Lufan Jin, Zhiliang Chen, Yifan Li, Qingyan Li, Mingxuan Cao, Yongli Che, Haitao Dai, Junbo Yang, Jianquan Yao. Self-powered lead-free quantum dot plasmonic phototransistor with multi-wavelength response[J]. Photonics Research, 2019, 7(2): 149 Copy Citation Text show less
    (a) Schematic diagram of plasmonic CuInSe2 QD FEpT architecture. (b) Cross-sectional SEM image of composite film between CuInSe2 and Au NPs (inset: TEM image of pristine CuInSe2 QDs). (c) AFM image of Au NPs on silicon substrate. (d) Optical absorption spectra of CuInSe2 QDs with (red line) and without (black line) deposited Au NPs on glass substrate.
    Fig. 1. (a) Schematic diagram of plasmonic CuInSe2 QD FEpT architecture. (b) Cross-sectional SEM image of composite film between CuInSe2 and Au NPs (inset: TEM image of pristine CuInSe2 QDs). (c) AFM image of Au NPs on silicon substrate. (d) Optical absorption spectra of CuInSe2 QDs with (red line) and without (black line) deposited Au NPs on glass substrate.
    Photoelectronic properties of the device. (a) Output characteristics (IDS−VDS curves) under different VGS (1 V increment) of plasmonic FEpT (dashed lines, in darkness; solid lines, under illumination of 700 mW·cm−2 of a 405 nm laser). (b) Transfer characteristics of typical CuInSe2 FEpTs, after Au NP deposition (black line, in darkness; red line, under illumination of an 845 mW·cm−2 of 808 nm laser) and before Au NPs deposition (blue line, in darkness; green line, under illumination of 845 mW·cm−2 of an 808 nm laser) with applied bias voltage VDS=1.2 V.
    Fig. 2. Photoelectronic properties of the device. (a) Output characteristics (IDSVDS curves) under different VGS (1 V increment) of plasmonic FEpT (dashed lines, in darkness; solid lines, under illumination of 700  mW·cm2 of a 405 nm laser). (b) Transfer characteristics of typical CuInSe2 FEpTs, after Au NP deposition (black line, in darkness; red line, under illumination of an 845  mW·cm2 of 808 nm laser) and before Au NPs deposition (blue line, in darkness; green line, under illumination of 845  mW·cm2 of an 808 nm laser) with applied bias voltage VDS=1.2  V.
    Time-dependent response of the device at zero bias with different wavelengths and irradiation intensities. (a), (d) 405 nm; (b), (e) 532 nm; (c), (f) 808 nm.
    Fig. 3. Time-dependent response of the device at zero bias with different wavelengths and irradiation intensities. (a), (d) 405 nm; (b), (e) 532 nm; (c), (f) 808 nm.
    Photoresponsivity (R) of the device with or without deposited Au NPs as a function of irradiance under different wavelengths with chopper frequency of 3944 Hz at a bias of 0 V: (a) 405 nm, (b) 532 nm, and (c) 808 nm.
    Fig. 4. Photoresponsivity (R) of the device with or without deposited Au NPs as a function of irradiance under different wavelengths with chopper frequency of 3944 Hz at a bias of 0 V: (a) 405 nm, (b) 532 nm, and (c) 808 nm.
    Time-dependent response of the device with or without deposited Au NPs as a function of irradiance under different wavelengths with chopper frequency of 3944 Hz at a bias of 0 V: (a) 405 nm, (b) 532 nm, and (c) 808 nm.
    Fig. 5. Time-dependent response of the device with or without deposited Au NPs as a function of irradiance under different wavelengths with chopper frequency of 3944 Hz at a bias of 0 V: (a) 405 nm, (b) 532 nm, and (c) 808 nm.
    (a) Structure diagram of FDTD simulation. The field distributions in the x–y plane under (b) 405 nm, (c) 532 nm, and (d) 808 nm light illumination.
    Fig. 6. (a) Structure diagram of FDTD simulation. The field distributions in the x–y plane under (b) 405 nm, (c) 532 nm, and (d) 808 nm light illumination.
    Electronic band structure and working principle of the CuInSe2 QD FEpTs with Au NPs.
    Fig. 7. Electronic band structure and working principle of the CuInSe2 QD FEpTs with Au NPs.
    DeviceIdark [nA]Iillu [nA]Idark/IilluResponsivity [μA·W1]D* [103 Jones]Rise/Decay Time [ms]
    Without Au NPs8.213.81.62.07.00.05/0.03
    With Au NPs5.728.95.04.414.40.1/0.06
    Table 1. Comparison in Device Performance of CuInSe2 FEpTs with or without Au NPs at the Strongest Enhancement with Wavelength of 405 nm
    Yu Yu, Yating Zhang, Lufan Jin, Zhiliang Chen, Yifan Li, Qingyan Li, Mingxuan Cao, Yongli Che, Haitao Dai, Junbo Yang, Jianquan Yao. Self-powered lead-free quantum dot plasmonic phototransistor with multi-wavelength response[J]. Photonics Research, 2019, 7(2): 149
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