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Lead–halide perovskites for next-generation self-powered photodetectors: a comprehensive review

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Abstract

Metal halide perovskites have aroused tremendous interest in optoelectronics due to their attractive properties, encouraging the development of high-performance devices for emerging application domains such as wearable electronics and the Internet of Things. Specifically, the development of high-performance perovskite-based photodetectors (PDs) as an ultimate substitute for conventional PDs made of inorganic semiconductors such as silicon, InGaAs, GaN, and germanium-based commercial PDs, attracts great attention by virtue of its solution processing, film deposition technique, and tunable optical properties. Importantly, perovskite PDs can also deliver high performance without an external power source; so-called self-powered perovskite photodetectors (SPPDs) have found eminent application in next-generation nanodevices operating independently, wirelessly, and remotely. Earlier research reports indicate that perovskite-based SPPDs have excellent photoresponsive behavior and wideband spectral response ranges. Despite the high-performance perovskite PDs, their commercialization is hindered by long-term material instability under ambient conditions. This review aims to provide a comprehensive compilation of the research results on self-powered, lead–halide perovskite PDs. In addition, a brief introduction is given to flexible SPPDs. Finally, we put forward some perspectives on the further development of perovskite-based self-powered PDs. We believe that this review can provide state-of-the-art current research on SPPDs and serve as a guide to improvising a path for enhancing the performance to meet the versatility of practical device applications.

© 2021 Chinese Laser Press

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Figures (14)

Fig. 1.
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.
Fig. 2.
Fig. 2. Schematic diagrams of working principle of SPPDs in PV mode: heterojunction type (left side) and Schottky type (right side).
Fig. 3.
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.
Fig. 4.
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.
Fig. 5.
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(200nm)/Au trilayer PDs; (g) I-V curve of trilayer PD device in dark and under 85μWcm2 405 nm illumination; (h) potential charges generation and transportation process under 85μWcm2 405 nm illumination illustrated by band diagram. Reproduced with permission from Ref. [67]. Copyright 2020, Institute of Physics.
Fig. 6.
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 6.4×104mWcm2; (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 100mWcm2 white light at 0 V. Reproduced with permission from Ref. [69]. Copyright 2019, Wiley-VCH.
Fig. 7.
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.
Fig. 8.
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 1000μW/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 1μmcm2 to 1mWcm2; (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.
Fig. 9.
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 100mWcm2. 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. 10.
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 6.2μWcm2 to 114mWcm2; (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. 11.
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=600nm and d=4mm. Reproduced with permission from Ref. [124]. Copyright 2019, American Chemical Society.
Fig. 12.
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.
Fig. 13.
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.
Fig. 14.
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.

Tables (3)

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Table 1. Basic Characteristic Physical Parameters of Perovskite Materials

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Table 2. Summary of Key Parameters of Perovskite-Based SPPDs

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Table 3. Summary of Flexible Self-Powered Perovskite-Based PDs

Equations (5)

Equations on this page are rendered with MathJax. Learn more.

R=IpPA,
D*=(AΔf)1/2inR=RA2qId,
EQE=Rhcqλ,
NEP=(AΔf)1/2D*=inR,
LDR=20logJmaxJdJminJd,
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