• Photonics Research
  • Vol. 9, Issue 6, 968 (2021)
Chandrasekar Perumal Veeramalai1, Shuai Feng1, Xiaoming Zhang1、5、*, S. V. N. Pammi2, Vincenzo Pecunia3, and Chuanbo Li1、4、6、*
Author Affiliations
  • 1School of Science, Minzu University of China, Beijing 100081, China
  • 2Department of Materials Science and Engineering, Chungnam National University, 34134 Daejeon, Republic of Korea
  • 3Jiangsu Key Laboratory for Carbon-Based Functional Materials & Devices, Institute of Functional Nano & Soft Materials (FUNSOM), Joint International Research Laboratory of Carbon-Based Functional Materials and Devices, Soochow University, Suzhou 215123, China
  • 4Optoelectronics Research Center, Minzu University of China, Beijing 100081, China
  • 5e-mail: xmzhang@muc.edu.cn
  • 6e-mail: cbli@muc.edu.cn
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    DOI: 10.1364/PRJ.418450 Cite this Article Set citation alerts
    Chandrasekar Perumal Veeramalai, Shuai Feng, Xiaoming Zhang, S. V. N. Pammi, Vincenzo Pecunia, Chuanbo Li. Lead–halide perovskites for next-generation self-powered photodetectors: a comprehensive review[J]. Photonics Research, 2021, 9(6): 968 Copy Citation Text show less
    (a), (b) Schematic crystal structure of representative perovskite materials CH3NH3PbI3 and CsPbBr3, simulated from Vesta.3 Software; (c) comparative optical absorption behavior of semiconducting materials. Reproduced from Ref. [6] with permission. Copyright 2014, Springer Nature.
    Fig. 1. (a), (b) Schematic crystal structure of representative perovskite materials CH3NH3PbI3 and CsPbBr3, simulated from Vesta.3 Software; (c) comparative optical absorption behavior of semiconducting materials. Reproduced from Ref. [6] with permission. Copyright 2014, Springer Nature.
    Schematic diagrams of working principle of SPPDs in PV mode: heterojunction type (left side) and Schottky type (right side).
    Fig. 2. Schematic diagrams of working principle of SPPDs in PV mode: heterojunction type (left side) and Schottky type (right side).
    (a) Preparation process of the MAPbBr3/MAPbIxBr3−x heterojunction; (b) responsivity of APbBr3/MAPbIxBr3−x and single crystal MAPbBr3 PDs at zero bias under the incident light with wavelengths of 350–800 nm and 400–800 nm, respectively; (c) schematic energy level diagram at the MAPbBr3/MAPbIxBr3−x junction under irradiation. Reproduced with permission from Ref. [56]. Copyright 2016, American Institute of Physics. (d) Photographic image of the as-grown heterostructure single crystal (top); SEM image of the heterostructure interface (bottom). (e) Band diagram of the (4-AMP)(MA)2Pb3Br10/MAPbBr3 heterostructure detector; (f) plots of the R and D* as a function of light intensity; (g) response speed of (4-AMP)(MA)2Pb3Br10/MAPbBr3 heterostructure device at rise edges and fall edges. Reproduced with permission from Ref. [57]. Copyright 2020, Wiley-VCH. (h) Schematic illustration of the Au–Al electrodes separated by 30 μm on MAPbI3 single crystal; (i) schematic illustration of the working mechanism for Schottky junction based on asymmetric electrodes; (j) photocurrent response of Au/MAPbI3/Al device at different wavelengths; (k) spectral photoresponsivity of MAPbI3 single crystal PD. Reproduced with permission from Ref. [58]. Copyright 2016, Royal Society of Chemistry.
    Fig. 3. (a) Preparation process of the MAPbBr3/MAPbIxBr3x heterojunction; (b) responsivity of APbBr3/MAPbIxBr3x and single crystal MAPbBr3 PDs at zero bias under the incident light with wavelengths of 350–800 nm and 400–800 nm, respectively; (c) schematic energy level diagram at the MAPbBr3/MAPbIxBr3x junction under irradiation. Reproduced with permission from Ref. [56]. Copyright 2016, American Institute of Physics. (d) Photographic image of the as-grown heterostructure single crystal (top); SEM image of the heterostructure interface (bottom). (e) Band diagram of the (4-AMP)(MA)2Pb3Br10/MAPbBr3 heterostructure detector; (f) plots of the R and D* as a function of light intensity; (g) response speed of (4-AMP)(MA)2Pb3Br10/MAPbBr3 heterostructure device at rise edges and fall edges. Reproduced with permission from Ref. [57]. Copyright 2020, Wiley-VCH. (h) Schematic illustration of the Au–Al electrodes separated by 30 μm on MAPbI3 single crystal; (i) schematic illustration of the working mechanism for Schottky junction based on asymmetric electrodes; (j) photocurrent response of Au/MAPbI3/Al device at different wavelengths; (k) spectral photoresponsivity of MAPbI3 single crystal PD. Reproduced with permission from Ref. [58]. Copyright 2016, Royal Society of Chemistry.
    (a) Photographic image of CsPbBr3 single crystal; (b) I-V curve of device Au/CsPbBr3/Pt in dark and under illumination; (c) photoresponse of device Au/CsPbBr3/Pt under light pulses measured under zero bias. Reproduced with permission from Ref. [28]. Copyright 2017, Wiley-VCH. (d) Carrier separation transmission diagram of the device based on CH3NH3PbI3 single crystal PD; (e) variation of light responsivity of devices with different channel widths; (f) dependence of responsivity and on–off ratio on the light intensity. Reproduced with permission from Ref. [60]. Copyright 2021, Elsevier.
    Fig. 4. (a) Photographic image of CsPbBr3 single crystal; (b) I-V curve of device Au/CsPbBr3/Pt in dark and under illumination; (c) photoresponse of device Au/CsPbBr3/Pt under light pulses measured under zero bias. Reproduced with permission from Ref. [28]. Copyright 2017, Wiley-VCH. (d) Carrier separation transmission diagram of the device based on CH3NH3PbI3 single crystal PD; (e) variation of light responsivity of devices with different channel widths; (f) dependence of responsivity and on–off ratio on the light intensity. Reproduced with permission from Ref. [60]. Copyright 2021, Elsevier.
    (a) Schematic illustration of MAPbI3 NC synthesis; (b) TEM image of MAPbI3 NCs (the inset shows MAPbI3 nanocrystal size distribution plot); (c) schematic diagram of the MAPbI3 NC based self-powered PD; (d) J-V curves of the MAPbI3 NC-based self-powered PD under 808 nm illumination; (e) photocurrent versus time for the PD under light on/off cycles at 0 V under 808 nm illumination. Reproduced with permission from Ref. [50]. Copyright 2020, Wiley-VCH. (f) Cross-sectional SEM image of ITO/ZnO(70 nm)/CdS(150 nm) /CsPbBr3(200 nm)/Au trilayer PDs; (g) I-V curve of trilayer PD device in dark and under 85 μW cm−2 405 nm illumination; (h) potential charges generation and transportation process under 85 μW cm−2 405 nm illumination illustrated by band diagram. Reproduced with permission from Ref. [67]. Copyright 2020, Institute of Physics.
    Fig. 5. (a) Schematic illustration of MAPbI3 NC synthesis; (b) TEM image of MAPbI3 NCs (the inset shows MAPbI3 nanocrystal size distribution plot); (c) schematic diagram of the MAPbI3 NC based self-powered PD; (d) J-V curves of the MAPbI3 NC-based self-powered PD under 808 nm illumination; (e) photocurrent versus time for the PD under light on/off cycles at 0 V under 808 nm illumination. Reproduced with permission from Ref. [50]. Copyright 2020, Wiley-VCH. (f) Cross-sectional SEM image of ITO/ZnO(70 nm)/CdS(150 nm) /CsPbBr3(200  nm)/Au trilayer PDs; (g) I-V curve of trilayer PD device in dark and under 85  μWcm2 405 nm illumination; (h) potential charges generation and transportation process under 85  μWcm2 405 nm illumination illustrated by band diagram. Reproduced with permission from Ref. [67]. Copyright 2020, Institute of Physics.
    (a) Schematic illustration of the synthesis process of the CsPbBr3 NWs and CsPbBr3 micro- and nanostructures; (b) schematic illustration of the perovskite NW PD; (c) energy band diagram of the perovskite NW PD. (d) J-t curve at the light intensity of 6.4×10−4 mW cm−2; (e) responsivity and detectivity of the device under various optical power. Reproduced with permission from Ref. [68]. Copyright 2018, Elsevier. (f) Schematic illustration of the fabrication process of the P3PCS PD; (g) CsPbBr3 nanowire array; (h) schematic of device structure; (i) responsivity and detectivity curves of P3PCS device; (j) long-term photoresponse curves of P3PCS device under 100 mW cm−2 white light at 0 V. Reproduced with permission from Ref. [69]. Copyright 2019, Wiley-VCH.
    Fig. 6. (a) Schematic illustration of the synthesis process of the CsPbBr3 NWs and CsPbBr3 micro- and nanostructures; (b) schematic illustration of the perovskite NW PD; (c) energy band diagram of the perovskite NW PD. (d) J-t curve at the light intensity of 6.4×104  mWcm2; (e) responsivity and detectivity of the device under various optical power. Reproduced with permission from Ref. [68]. Copyright 2018, Elsevier. (f) Schematic illustration of the fabrication process of the P3PCS PD; (g) CsPbBr3 nanowire array; (h) schematic of device structure; (i) responsivity and detectivity curves of P3PCS device; (j) long-term photoresponse curves of P3PCS device under 100  mWcm2 white light at 0 V. Reproduced with permission from Ref. [69]. Copyright 2019, Wiley-VCH.
    (a) SEM image of CsPbBr3 microplatelets shows sharp edge and smooth surface morphology. (b) Schematic layout of the perovskite CsPbBr3 microplatelets PD based on vertical Schottky junction structure; (c) I-V characteristics of the CsPbBr3 microplatelets PD under 405 nm light illumination with different density; (d) normalized I-t curves of CsPbBr3 microplatelets PD with long-term storage without encapsulation. Reproduced with permission from Ref. [75]. Copyright 2020, Royal Society of Chemistry. (e) Schematic of fabricating process of the CsPbBr3 microcrystal-based PD; (f) room temperature spectral responsivity curves of the CsPbBr3 microcrystal-based PD at 0 V bias. Reproduced with permission from Ref. [76]. Copyright 2019, American Chemical Society. (g) SEM image of CsPbBr3 microcrystal perovskite film. The inset is a digital photograph of the perovskite film under 365 nm purple flashlight. (h) Schematic illustration of the CsPbBr3 microcrystal perovskite PD; (i) power-dependent R and D*CsPbBr3 microcrystal perovskite PD under 0 V bias. Reproduced with permission from Ref. [77]. Copyright 2019, American Chemical Society.
    Fig. 7. (a) SEM image of CsPbBr3 microplatelets shows sharp edge and smooth surface morphology. (b) Schematic layout of the perovskite CsPbBr3 microplatelets PD based on vertical Schottky junction structure; (c) I-V characteristics of the CsPbBr3 microplatelets PD under 405 nm light illumination with different density; (d) normalized I-t curves of CsPbBr3 microplatelets PD with long-term storage without encapsulation. Reproduced with permission from Ref. [75]. Copyright 2020, Royal Society of Chemistry. (e) Schematic of fabricating process of the CsPbBr3 microcrystal-based PD; (f) room temperature spectral responsivity curves of the CsPbBr3 microcrystal-based PD at 0 V bias. Reproduced with permission from Ref. [76]. Copyright 2019, American Chemical Society. (g) SEM image of CsPbBr3 microcrystal perovskite film. The inset is a digital photograph of the perovskite film under 365 nm purple flashlight. (h) Schematic illustration of the CsPbBr3 microcrystal perovskite PD; (i) power-dependent R and D*CsPbBr3 microcrystal perovskite PD under 0 V bias. Reproduced with permission from Ref. [77]. Copyright 2019, American Chemical Society.
    (a) Device structure of the hybrid perovskite PD; (b) LDR of the PD with the device structure ITO/PEDOT:PSS/CH3NH3PbI3−xClx/PCBM/PFN/Al. The PD has a large LDR of 4100 dB. Reproduced with permission from Ref. [85]. Copyright 2014, Springer Nature. (c) SEM image of MAPbI3−xClx thin films on glass substrate; (d) schematic representation of a photodetector device configuration; (e) transient photocurrent properties of device under illumination at 632 nm; (f) long-term photo stability illuminated under 1000 μW/cm2 with different intervals up to 500 h. Reproduced with permission from Ref. [86]. Copyright 2020, Elsevier. (g) SEM image of PMMA-modified CsPbBr3 film; (h) schematic and cross-sectional SEM image of the as-fabricated PD with a structure of ITO/CsPbBr3/PMMA/Ag. Reproduced with permission from Ref. [87]. Copyright 2020, Royal Society of Chemistry. (i) Schematic structure of PD based on all-inorganic perovskite CsPbIxBr3−x; (j) current density-voltage (J-V) curves of CsPbIBr2-based PDs under dark and illumination of 450 nm monochrome light with intensity of 1 μm cm−2 to 1 mW cm−2; (k) photoresponsivity evolution of PDs based on inorganic perovskite CsPbIxBr3−x and hybrid perovskite MAPbI3 in air ambient condition without encapsulation. Reproduced with permission from Ref. [88]. Copyright 2018, Wiley-VCH. (l) Schematic illustration of as-fabricated self-powered PD based on CsxDMA1−xPbI3 perovskite films; (m) responsivity spectrum of the self-powered PD based on the film with CsI/DMAPbI3 molar ratio of 1:2 in the precursor at 0 V; (n) variation of spectral responsivity with time of the self-powered PD in air (10%–20% RH) at a bias voltage of 0 V under 532 nm illumination. Reproduced with permission from Ref. [89]. Copyright 2020, Elsevier. (o) Disordered state of ions under dark (upper) and mobile ions accumulated at the opposite interfaces under illumination due to the light-induced self-poling effect (lower), resulting in the built-in electric field; (p) energy band schematics of the MOS structure under dark before contact. Reproduced with permission from Ref. [90]. Copyright 2019, Royal Society of Chemistry.
    Fig. 8. (a) Device structure of the hybrid perovskite PD; (b) LDR of the PD with the device structure ITO/PEDOT:PSS/CH3NH3PbI3xClx/PCBM/PFN/Al. The PD has a large LDR of 4100 dB. Reproduced with permission from Ref. [85]. Copyright 2014, Springer Nature. (c) SEM image of MAPbI3xClx thin films on glass substrate; (d) schematic representation of a photodetector device configuration; (e) transient photocurrent properties of device under illumination at 632 nm; (f) long-term photo stability illuminated under 1000  μW/cm2 with different intervals up to 500 h. Reproduced with permission from Ref. [86]. Copyright 2020, Elsevier. (g) SEM image of PMMA-modified CsPbBr3 film; (h) schematic and cross-sectional SEM image of the as-fabricated PD with a structure of ITO/CsPbBr3/PMMA/Ag. Reproduced with permission from Ref. [87]. Copyright 2020, Royal Society of Chemistry. (i) Schematic structure of PD based on all-inorganic perovskite CsPbIxBr3x; (j) current density-voltage (J-V) curves of CsPbIBr2-based PDs under dark and illumination of 450 nm monochrome light with intensity of 1  μmcm2 to 1  mWcm2; (k) photoresponsivity evolution of PDs based on inorganic perovskite CsPbIxBr3x and hybrid perovskite MAPbI3 in air ambient condition without encapsulation. Reproduced with permission from Ref. [88]. Copyright 2018, Wiley-VCH. (l) Schematic illustration of as-fabricated self-powered PD based on CsxDMA1xPbI3 perovskite films; (m) responsivity spectrum of the self-powered PD based on the film with CsI/DMAPbI3 molar ratio of 1:2 in the precursor at 0 V; (n) variation of spectral responsivity with time of the self-powered PD in air (10%–20% RH) at a bias voltage of 0 V under 532 nm illumination. Reproduced with permission from Ref. [89]. Copyright 2020, Elsevier. (o) Disordered state of ions under dark (upper) and mobile ions accumulated at the opposite interfaces under illumination due to the light-induced self-poling effect (lower), resulting in the built-in electric field; (p) energy band schematics of the MOS structure under dark before contact. Reproduced with permission from Ref. [90]. Copyright 2019, Royal Society of Chemistry.
    (a) Device structure of self-powered PD with MAPbI3 as the photosensitive and triboelectric layer; (b) change of Voc upon repeated illumination that varies in intensity at 100 mW cm−2. Reproduced with permission from Ref. [93]. Copyright 2015, American Chemical Society. (c) Schematic of a triboelectric-assisted perovskite PD showing charge carrier separation assisted by the triboelectric charges created by the TENG; (d) schematic diagram and the working principle of the (+) triboelectric-assisted perovskite PD; (e) transient photoresponse of the triboelectric-actuated perovskite PD (blue) and perovskite PD without assistance of triboelectricity (red) under alternating on–off laser light (50 mW) illumination with a 3 Hz chopping frequency. Reproduced with permission from Ref. [94]. Copyright 2019, Elsevier.
    Fig. 9. (a) Device structure of self-powered PD with MAPbI3 as the photosensitive and triboelectric layer; (b) change of Voc upon repeated illumination that varies in intensity at 100  mWcm2. Reproduced with permission from Ref. [93]. Copyright 2015, American Chemical Society. (c) Schematic of a triboelectric-assisted perovskite PD showing charge carrier separation assisted by the triboelectric charges created by the TENG; (d) schematic diagram and the working principle of the (+) triboelectric-assisted perovskite PD; (e) transient photoresponse of the triboelectric-actuated perovskite PD (blue) and perovskite PD without assistance of triboelectricity (red) under alternating on–off laser light (50 mW) illumination with a 3 Hz chopping frequency. Reproduced with permission from Ref. [94]. Copyright 2019, Elsevier.
    (a) Plane-view SEM image of CsPbBr3 perovskite thin films Al2O3-modified FTO substrates; (b) photoresponse curves of CsPbBr3 perovskite PDs, Al2O3/CsPbBr3 perovskite PDs, and Al2O3/CsPbBr3/TiO2 perovskite PDs, respectively; (c) energy band diagram of heterojunctions; (d) current–voltage (I-V) curves of PDs under dark and illumination of 405 nm laser with intensity of 6.2 μW cm−2 to 114 mW cm−2; (e) photoresponse curves of ACT PDs under modulated 405 nm laser with various light intensity (0 V); (f) light current and dark current stability at different days for hard substrate device; (g) light current and dark current of flexible device after different bending cycles. Reproduced with permission from Ref. [123]. Copyright 2019, Wiley-VCH.
    Fig. 10. (a) Plane-view SEM image of CsPbBr3 perovskite thin films Al2O3-modified FTO substrates; (b) photoresponse curves of CsPbBr3 perovskite PDs, Al2O3/CsPbBr3 perovskite PDs, and Al2O3/CsPbBr3/TiO2 perovskite PDs, respectively; (c) energy band diagram of heterojunctions; (d) current–voltage (I-V) curves of PDs under dark and illumination of 405 nm laser with intensity of 6.2  μWcm2 to 114  mWcm2; (e) photoresponse curves of ACT PDs under modulated 405 nm laser with various light intensity (0 V); (f) light current and dark current stability at different days for hard substrate device; (g) light current and dark current of flexible device after different bending cycles. Reproduced with permission from Ref. [123]. Copyright 2019, Wiley-VCH.
    (a) FESEM image of a typical PD with Au/Ag electrode pair; (b) I-V curves of the CH3NH3PbI3 MWs array-based PDs with asymmetric contact electrodes (Au/Ag, Au/Al); (c) histogram of Voc and Isc for devices with different asymmetric electrode pairs; (d) dark current and photocurrent of the flexible PD being bent to various radii. Reproduced with permission from Ref. [71]. Copyright 2019, Wiley-VCH. (e) Device structure and (f) cross-sectional SEM image of MAPbI3:graphene QD based PD. (g) NEP/spectral detectivity of PD. The inset shows excellent flexibility of the PD. (h) Evolution of responsivity during repeated 1000 bending cycles at λ=600 nm and d=4 mm. Reproduced with permission from Ref. [124]. Copyright 2019, American Chemical Society.
    Fig. 11. (a) FESEM image of a typical PD with Au/Ag electrode pair; (b) I-V curves of the CH3NH3PbI3 MWs array-based PDs with asymmetric contact electrodes (Au/Ag, Au/Al); (c) histogram of Voc and Isc for devices with different asymmetric electrode pairs; (d) dark current and photocurrent of the flexible PD being bent to various radii. Reproduced with permission from Ref. [71]. Copyright 2019, Wiley-VCH. (e) Device structure and (f) cross-sectional SEM image of MAPbI3:graphene QD based PD. (g) NEP/spectral detectivity of PD. The inset shows excellent flexibility of the PD. (h) Evolution of responsivity during repeated 1000 bending cycles at λ=600  nm and d=4  mm. Reproduced with permission from Ref. [124]. Copyright 2019, American Chemical Society.
    (a) Schematic illustration of ferroelectric polarization-induced formation of internal electric field in the nanowire array device; (b) schematic illustration of the fabrication process of flexible P(VDF-TrFE)/perovskite hybrid nanowire arrays-based PD; (c) 650 nm wavelength light illumination of flexible P(VDF-TrFE)/perovskite PDs with various power intensities at 0 V; (d) I-t curves of the poled perovskite-0.6 device under 650 nm light illumination at bending angles with the intersection angle between bending direction and nanowire direction of 0°. Reproduced with permission from Ref. [125]. Copyright 2019, Wiley-VCH. (e) I-t curve of flexible P(VDF-TrFE)/perovskite PDs at different bending cycles. Reproduced with permission from Ref. [126]. Copyright 2019, Wiley-VCH.
    Fig. 12. (a) Schematic illustration of ferroelectric polarization-induced formation of internal electric field in the nanowire array device; (b) schematic illustration of the fabrication process of flexible P(VDF-TrFE)/perovskite hybrid nanowire arrays-based PD; (c) 650 nm wavelength light illumination of flexible P(VDF-TrFE)/perovskite PDs with various power intensities at 0 V; (d) I-t curves of the poled perovskite-0.6 device under 650 nm light illumination at bending angles with the intersection angle between bending direction and nanowire direction of 0°. Reproduced with permission from Ref. [125]. Copyright 2019, Wiley-VCH. (e) I-t curve of flexible P(VDF-TrFE)/perovskite PDs at different bending cycles. Reproduced with permission from Ref. [126]. Copyright 2019, Wiley-VCH.
    (a) Schematic diagram of the SFPDs with integrated TENG; (b) change in the measured voltage (ΔV) and voltage responsivity of the device at different light intensities; (c) ΔV at various angles of incident light. Reproduced with permission from Ref. [129]. Copyright 2018, Wiley-VCH. (d) Schematic illustration of the integrated nanosystem, consisting of an energy conversion unit, a light sensing unit, and a current measurement system. (e) J-V curves of the as-fabricated integrated perovskite solar cell; (f) photoresponse curves after 100 and 200 bending cycles. Reproduced with permission from Ref. [130]. Copyright 2016, Wiley-VCH.
    Fig. 13. (a) Schematic diagram of the SFPDs with integrated TENG; (b) change in the measured voltage (ΔV) and voltage responsivity of the device at different light intensities; (c) ΔV at various angles of incident light. Reproduced with permission from Ref. [129]. Copyright 2018, Wiley-VCH. (d) Schematic illustration of the integrated nanosystem, consisting of an energy conversion unit, a light sensing unit, and a current measurement system. (e) J-V curves of the as-fabricated integrated perovskite solar cell; (f) photoresponse curves after 100 and 200 bending cycles. Reproduced with permission from Ref. [130]. Copyright 2016, Wiley-VCH.
    (a) Photoresponsivity evolution of PDs based on inorganic perovskite CsPbIxBr3−x and hybrid perovskite MAPbI3 at 100°C in N2 ambient condition. XRD spectra and digital photographs of (b) CsPbIBr2 and (c) MAPbI3 devices before and after heated at 100°C in N2-filled glove box for 244 h. The obvious PbI2 peak in XRD spectrum of MAPbI3 devices after being heated indicates the decomposition of MAPbI3. Reproduced with permission from Ref. [88]. Copyright 2018, Wiley-VCH. (d) Thermal stability of MAPbI3 NCs; photographic image of samples under 365 nm illumination. The samples are annealed at 40°C, 50°C, 60°C, 70°C, and 80°C for 10 min in open air. Reproduced with permission from Ref. [50]. Copyright 2020, Wiley-VCH.
    Fig. 14. (a) Photoresponsivity evolution of PDs based on inorganic perovskite CsPbIxBr3x and hybrid perovskite MAPbI3 at 100°C in N2 ambient condition. XRD spectra and digital photographs of (b) CsPbIBr2 and (c) MAPbI3 devices before and after heated at 100°C in N2-filled glove box for 244 h. The obvious PbI2 peak in XRD spectrum of MAPbI3 devices after being heated indicates the decomposition of MAPbI3. Reproduced with permission from Ref. [88]. Copyright 2018, Wiley-VCH. (d) Thermal stability of MAPbI3 NCs; photographic image of samples under 365 nm illumination. The samples are annealed at 40°C, 50°C, 60°C, 70°C, and 80°C for 10 min in open air. Reproduced with permission from Ref. [50]. Copyright 2020, Wiley-VCH.
    MaterialDiffusion Length (μm)Lifetime (μs)Mobility (cm2V1s1)Trap Density (cm3)Reference
    MAPbI3 thin film0.1–10.01–11–1010151016[25]
    MAPbI3 single crystal2–80.5–124–1051010[26]
    CsPbBr3 thin film9.241.3[27]
    CsPbBr3 single crystal5.525521.1×1010[28,29]
    Table 1. Basic Characteristic Physical Parameters of Perovskite Materials
    Device StructurePhysical Mechanism for Self-Mode (Junction)Response Wavelength (nm)R (mA W–1)D*(Jones)τr/τfReference
    ZnO NRs-Spiro-MeOTADPV (heterojunction)470 nm6.5Not mentioned4/10 ms[95]
    CH3NH3PbBr3/CH3NH3PbIxBr3xPV (heterojunction)450 nm11.5Not mentioned2.3/2.76 s[57]
    Au/CH3NH3PbI3/AlPV (Schottky)240Not mentioned71/112 μs[59]
    ITO/ZnO:CsPbBr3/AgPV (Schottky)405 nm11.5Not mentioned0.409/0.017 s[96]
    Au/CsPbBr3/PtPV (Schottky)550 nm281.7×1011230/60 ms[28]
    MoS2/CH3NH3PbI3PV (heterojunction)60not mentioned2149/899 ms[97]
    ITO/PTAA/PEIE/CsPbIxBr3x/PCPM/AgPV (p-i-n structure)525 nm2809.7×101220 ns[90]
    PSCH3NH3PbI3Electric field polingVisible light6101.5×101313 ms/14 ms[98]
    ZnONRs/CsPbBr3PV (heterojunction)Visible light3001.15×1013[99]
    PtSe2/Cs:FAPbI3PV (heterojunction)808 nm117.72.91×101270/60 ns[100]
    ITO/SnO2/CsPbBr3/PTAA/AuPV (heterojunction)473 nm2067.23×101230/39 μs[80]
    CsPbBr3PV (p-i-n structure)473 nm3001×10130.4/0.43 ms[70]
    ITO/SnO2/CsPbBr3/SpiroMeOTAD/AuPV (heterojunction)473 nm1724.8×10120.14/0.12 ms[79]
    PVP-CsPbI3PV (heterojunction)400–700 nm1001×10125.7/6.2 μs[101]
    P3HT-PDPP3T/CsPbBr3/SnO2Photovoltaic (heterojunction)300–950 nm2501.2×1013111/306 μs[71]
    CH3NH3PbI3PV (heterojunction)400 nm2501.53×1011110/72 ms[102]
    Carbon-CH3NH3PbI3PV (heterojunction)White light1.38.2×1011200/500 ms[103]
    Al/Si/SiO2/CH3NH3PbI3/PtLight-induced self-poling effectWhite lightNot mentioned8.8×101025.8/0.62 ms[94]
    GaN/CsPbBr3MCs/ZnOPV (heterojunction)540 nm89.51014100/140 μs[78]
    CsBi3I10/siliconPV (heterojunction)820 nm178.74.99×101073/36 μs[104]
    PdSe2/FA1xCsxPbI3PV (heterojunction)800 nm31310133.5/4 μs[105]
    FTO/TiO2/CsPbBr3/carbonPV (heterojunction)520 nm3501.94×10130.58 μs/–[106]
    FTO/c-TiO2/Cs0.05MA0.16FA0.79Pb(I0.9Br0.1)3/Spiro/AuPV (heterojunction)625 nm5208.8×101219/21 μs[107]
    ITO/PTAA/PMMA/CsxDMA1xPbI3/PCPM/Bphen/CuPV (heterojunction)532 nm3801×1013558 ns/–[91]
    ITO/CH3NH3PbI3/AgPV (Schottky)808 nm1.42×1031.77×1013279/341 ms[51]
    ITO/CsPbBr3/PMMA/AgPV (Schottky)450 nm1104.4×10113.8/4.6 μs[89]
    ITO/MAPbI3:CuSCN/PCBM/BCP/AgPV (heterojunction)640 nm3701.06×10125.02/5.50 μs[108]
    FTO/NiOx/MAPbI3x/PCPM/AuPV (heterojunction)632 nm112×1033.5×10140.23/0.38 s[88]
    ITO/ZnO/CdS/CsPbBr3/AuPV (heterojunction)405 nm866.2×10110.3/0.25 s[109]
    ITO/SnO2/CH3NH3PbI3/SpiroOMeTAD/AgPV (heterojunction)720 nm4731.35×10130.35/0.18 ms[110]
    Au/CH3NH3PbI3/AuPV (Schottky)400 nm1605.89×1011150/50 ms[62]
    FTO/PEI/CsPbIBr3/carbonPV (Schottky)520 nm3203.74×1012−/1.21 μs[111]
    FTO/TiO2/CsPbBr3/carbonPV (heterojunction)405 nm3503.83×1013−/1.46 μs[112]
    (4-AMP)(MA)2Pb3Br10/MAPbBr3PV (heterojunction)405 nm1.191.26×1012600/600 μs[58]
    ITO/CsPbBr3/AuPV (Schottky)500 nm208101275/70 μs[77]
    Au/CH3NH3PbI3/AuTENGWhite light196 V/(mW cm2)[113]
    CH3NH3PbI3TENGUV-visible7.5 V/W<80  ms/[95]
    Table 2. Summary of Key Parameters of Perovskite-Based SPPDs
    Primary Component of the PD Device StructurePhysical Mechanism for Self-Mode (Junction)R (mA W−1) (Response Wavelength)D* (Jones)τr/τfBending CycleReference
    ITO/CH3NH3PbI3/AuIntegrated TENG418 (sunlight)1.22×101380/80 ms1000[132]
    Au/CH3NH3PbI3NRs/AuPV (Schottky junction)2.2 (300 nm)1.76×101127.2/26.2 ms[132]
    Gr/PEDOT:PSS:GQDs/CH3NH3PbI3:GQDs/PCPM/BCP/AlPV (heterojunction)420 (600 nm)8.42×10120.96 μs/–1000[127]
    Au/CH3NH3PbI3 MWs/AgPV (Schottky junction)161.1 (520 nm)1.3×101213.8/16.1 μs[73]
    Ag/Spiro/CH3NH3PbI3/In2O3/ITOPV (heterojunction)451 (720 nm)1.1×1011<200/<200  ms500[133]
    FTO/Al2O3/CsPbBr3/TiO2/AuPV (heterojunction)440 (405 nm)1.88×101328/270 μs3000[126]
    Al/BCP/PCBM/CH3NH3PbI3/PEDOT:PSS/AuCl3-graphenePV (heterojunction)400 (600 nm)5.3×10131000[134]
    Au/PTAA/MAPbI3/ZnO/n-type GRPV (heterojunction)343 (700 nm)5.82×1091/1 μs1000[135]
    C/TiO2/perovskite/CuO/Cu2O/CuPV (heterojunction)563 (800 nm)2.15×1013<200/<200  ms60[136]
    ITO/CH3NH3PbI3/ITOSolar cell110 (730 nm)2200/300 ms200[133]
    Au/P(VDF-rFE)/CH3NH3PbI3/AuPV (heterojunction)20 (650 nm)1.4×101392/193 μs200[129]
    Au/P(VDF-TrFE)/CH3NH3PbI3 nanowires/AuPV (heterojunction)12 (650 nm)7.3×101288/184 μs200[128]
    Au NWs/PEDOT:PSS/CH3NH3PbI3/PCPM/AlPV (heterojunction)321 (670 nm)4/3.3 μs[123]
    C/TiO2/perovskite/SpiroOMeTAD/AuPV (heterojunction)182 (750 nm)1.24×1011<200/<200  ms80[130]
    Ni/CH3NH3PbI3/AlPV (Schottky junction)227 (532 nm)1.36×101161/42 ms1500[72]
    ITO/TiO2/CsPbBr3/SpiroOMeTAD/AuPV (heterojunction)10.1×103 (405 nm)9.35×10138.0/2.3 s1600[136]
    Table 3. Summary of Flexible Self-Powered Perovskite-Based PDs
    Chandrasekar Perumal Veeramalai, Shuai Feng, Xiaoming Zhang, S. V. N. Pammi, Vincenzo Pecunia, Chuanbo Li. Lead–halide perovskites for next-generation self-powered photodetectors: a comprehensive review[J]. Photonics Research, 2021, 9(6): 968
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