• Laser & Optoelectronics Progress
  • Vol. 60, Issue 9, 0900002 (2023)
Wenzhen Zou1, Chu Zhang1, Hongmin Jiang1, Liguo Gao2, Meiqiang Fan1, and Tingli Ma1、*
Author Affiliations
  • 1College of Materials and Chemistry, China Jiliang University, Hangzhou 310018, Zhejiang, China
  • 2School of Chemical Engineering, Dalian University of Technology, Panjin 116086, Liaoning, China
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    DOI: 10.3788/LOP220620 Cite this Article Set citation alerts
    Wenzhen Zou, Chu Zhang, Hongmin Jiang, Liguo Gao, Meiqiang Fan, Tingli Ma. Application of Transition Metal Doping in Perovskite Photovoltaic Devices[J]. Laser & Optoelectronics Progress, 2023, 60(9): 0900002 Copy Citation Text show less
    Mn-doped CsPbI2Br[28]. (a) Schematic structure of device and description of Mn2+ doping modes: interstitial and substitution; scanning electron microscope (SEM) images of (b) original chlorinated paraffins and (c) 0.5%, (d) 1%, and (e) 2% MnCl2; (f) schematic diagram of grain growth driven by surface passivated MnCl2
    Fig. 1. Mn-doped CsPbI2Br[28]. (a) Schematic structure of device and description of Mn2+ doping modes: interstitial and substitution; scanning electron microscope (SEM) images of (b) original chlorinated paraffins and (c) 0.5%, (d) 1%, and (e) 2% MnCl2; (f) schematic diagram of grain growth driven by surface passivated MnCl2
    Mn-dopded CsPbI3[29]. (a) Structure and crystal junction diagram of Mn-doped CsPbI3 perovskite solar cells; (b) X-ray diffraction (XRD) patterns of Mn-doped PVK films; (c) partial XRD diffraction peak amplified at 14.36°; (d) energy dispersing X-ray spectroscopy (EDS) for 2% Mn-doped perovskite thin films; (e)~(g) X-ray photoelectron spectroscopy (XPS) for Cs, Pb and I in control film and 2% Mn-doped PVK film; (h) optimal current density and voltage (J-V) characteristic curves of PSC based on Mn-doped CsPbI3 in forward and reverse measurements
    Fig. 2. Mn-dopded CsPbI3[29]. (a) Structure and crystal junction diagram of Mn-doped CsPbI3 perovskite solar cells; (b) X-ray diffraction (XRD) patterns of Mn-doped PVK films; (c) partial XRD diffraction peak amplified at 14.36°; (d) energy dispersing X-ray spectroscopy (EDS) for 2% Mn-doped perovskite thin films; (e)~(g) X-ray photoelectron spectroscopy (XPS) for Cs, Pb and I in control film and 2% Mn-doped PVK film; (h) optimal current density and voltage (J-V) characteristic curves of PSC based on Mn-doped CsPbI3 in forward and reverse measurements
    Influence of Ag ion doping on PVK[33]. (a) Layout diagram of planar junction solar cell; (b) photovoltaic performance of MAB0.1Pb0.9I3 system with different B elements; (c) UV spectra curves of MAPb1-xHgxI3 films at different Hg2+ doping concentrations; (d) PCE box diagram of solar cells based on MAPb1-xHgxI3; (e) SEM images of perovskite films with different Hg2+ doping concentrations
    Fig. 3. Influence of Ag ion doping on PVK[33]. (a) Layout diagram of planar junction solar cell; (b) photovoltaic performance of MAB0.1Pb0.9I3 system with different B elements; (c) UV spectra curves of MAPb1-xHgxI3 films at different Hg2+ doping concentrations; (d) PCE box diagram of solar cells based on MAPb1-xHgxI3; (e) SEM images of perovskite films with different Hg2+ doping concentrations
    Influence of Co ion doping on PVK[34]. (a) Transmission electron microscope (TEM) cross-section image of MA(31Pb∶1Co)I3 thin film; (b)~(d) composite elemental maps performed with energy dispersive X-Ray spectroscopy (EDX) in scanning transmission electron microscopy (STEM) mode. Individual elemental maps of (b) Pb, (c) I, and (e) Co indicate that elements are distributed homogeneously throughout film thickness; (f) SEM images of MAPbI3 and MA(Pb∶Co)I3 thin films; (g) XPS images of MAPbI3 and MA(31Pb∶1Co)I3 thin films; (h) forward and reverse J-V diagrams of solar cell measurements, and average performance of optimized MA(Pb∶Co)I3 solar cells; (i) energy level diagram of MA (Pb∶Co)I3 relative to MAPbI3
    Fig. 4. Influence of Co ion doping on PVK[34]. (a) Transmission electron microscope (TEM) cross-section image of MA(31Pb∶1Co)I3 thin film; (b)~(d) composite elemental maps performed with energy dispersive X-Ray spectroscopy (EDX) in scanning transmission electron microscopy (STEM) mode. Individual elemental maps of (b) Pb, (c) I, and (e) Co indicate that elements are distributed homogeneously throughout film thickness; (f) SEM images of MAPbI3 and MA(Pb∶Co)I3 thin films; (g) XPS images of MAPbI3 and MA(31Pb∶1Co)I3 thin films; (h) forward and reverse J-V diagrams of solar cell measurements, and average performance of optimized MA(Pb∶Co)I3 solar cells; (i) energy level diagram of MA (Pb∶Co)I3 relative to MAPbI3
    Influence of Cd ion doping on PVK[31]. (a) Lattice relaxation mechanism. a-c are schematic diagram illustrating a local strain, which can be reduced by forming b point defects or c introducing small ions. d is schematic diagram shows strain in (002) plane, which is reduced by introduction of small B/X ions. e is B/X covalent candidate ions; (b) top view SEM images of perovskite thin films on TiO2/ITO substrates and cross-sectional SEM images of perovskite solar cells; (c) PCE statistics for 30 PSCs of each component; (d) evolution of PCE in solar cells as six devices age in ambient air (50 per cent relative humidity); (e) in air environment and (f) in nitrogen environment, unpackaged power factor correction circuit is operated under maximum power point conditions using an UV filter with cut-off wavelength of 420 nm
    Fig. 5. Influence of Cd ion doping on PVK[31]. (a) Lattice relaxation mechanism. a-c are schematic diagram illustrating a local strain, which can be reduced by forming b point defects or c introducing small ions. d is schematic diagram shows strain in (002) plane, which is reduced by introduction of small B/X ions. e is B/X covalent candidate ions; (b) top view SEM images of perovskite thin films on TiO2/ITO substrates and cross-sectional SEM images of perovskite solar cells; (c) PCE statistics for 30 PSCs of each component; (d) evolution of PCE in solar cells as six devices age in ambient air (50 per cent relative humidity); (e) in air environment and (f) in nitrogen environment, unpackaged power factor correction circuit is operated under maximum power point conditions using an UV filter with cut-off wavelength of 420 nm
    Nb ion and Ta ion doping in TiO2[54]. (a) Conduction band diagram of dopant regulated battery; (b) energy graph image of Nb-TiO2 thin film with respect to vacuum level calculated based on UV-VIS spectrum and uninterruptible power source measurement results; (c) top view a and cross section image b of TiO2 films prepared by SEM, and top view of Nb-TiO2 thin films containing 1%, 3%, 5%, 7%, 10%, and 20% mole fraction Nb atoms as shown by c-h; (d) XRD patterns of undoped and doped TiO2 nanowire arrays with different Ta doping levels; (e) a and c are undoped TiO2 nanowire arrays, b and d are TEM and high-resolution transmission electron microscopy (HRTEM) images of 0.1-Ta-TiO2 nanowire arrays; Illustrations in c and d are corresponding fast Fourier transform (FFT) diffraction patterns
    Fig. 6. Nb ion and Ta ion doping in TiO2[54]. (a) Conduction band diagram of dopant regulated battery; (b) energy graph image of Nb-TiO2 thin film with respect to vacuum level calculated based on UV-VIS spectrum and uninterruptible power source measurement results; (c) top view a and cross section image b of TiO2 films prepared by SEM, and top view of Nb-TiO2 thin films containing 1%, 3%, 5%, 7%, 10%, and 20% mole fraction Nb atoms as shown by c-h; (d) XRD patterns of undoped and doped TiO2 nanowire arrays with different Ta doping levels; (e) a and c are undoped TiO2 nanowire arrays, b and d are TEM and high-resolution transmission electron microscopy (HRTEM) images of 0.1-Ta-TiO2 nanowire arrays; Illustrations in c and d are corresponding fast Fourier transform (FFT) diffraction patterns
    Co ion doping in TiO2[61]. (a) MOF preparation process and perovskite solar cell structure; (b) J-V curves of solar cells with best performance using dye-sol TiO2 and co-doped TiO2 (mass fraction is 1%); (c) SEM images of dye-sol TiO2 and 1% mass fraction co-doped TiO2 on FTO coated glass; (d) EIS curves based on TiO2 and 1% mass fraction co-doped TiO2 thin films
    Fig. 7. Co ion doping in TiO2[61]. (a) MOF preparation process and perovskite solar cell structure; (b) J-V curves of solar cells with best performance using dye-sol TiO2 and co-doped TiO2 (mass fraction is 1%); (c) SEM images of dye-sol TiO2 and 1% mass fraction co-doped TiO2 on FTO coated glass; (d) EIS curves based on TiO2 and 1% mass fraction co-doped TiO2 thin films
    Ni ion doping in TiO2[66]. (a) Schematic diagram of solution treatment method for preparing Ni-TiO2 thin film; (b) schematic diagram of carbon base plane PSC structure and (c) high resolution cross-section SEM image; (d) energy level diagram; (e) steady-state luminescence spectra of ore on different substrates
    Fig. 8. Ni ion doping in TiO2[66]. (a) Schematic diagram of solution treatment method for preparing Ni-TiO2 thin film; (b) schematic diagram of carbon base plane PSC structure and (c) high resolution cross-section SEM image; (d) energy level diagram; (e) steady-state luminescence spectra of ore on different substrates
    Co ion doping in SiO2[73]. (a) Band diagrams of SnO2, SnO2-CoCl2, and PVK layers and J-V curves of prepared PSCs; (b) cross-sectional SEM images of PSC based on SnO2-CoCl2 at a scale of 500 nm; (c) PSCs PCE histogram based on SnO2 and SnO2-CoCl2; (d) XPS image of Co 2p; XPS image of O 1s for (e) pristine SnO2 and (f) SnO2-CoCl2
    Fig. 9. Co ion doping in SiO2[73]. (a) Band diagrams of SnO2, SnO2-CoCl2, and PVK layers and J-V curves of prepared PSCs; (b) cross-sectional SEM images of PSC based on SnO2-CoCl2 at a scale of 500 nm; (c) PSCs PCE histogram based on SnO2 and SnO2-CoCl2; (d) XPS image of Co 2p; XPS image of O 1s for (e) pristine SnO2 and (f) SnO2-CoCl2
    Pd ion doping in HTL[84]. (a) Schematic diagram of PSCs with HTL layer doped Pd nanosheets; (b) TEM image of Pd nanosheets; (c) energy level diagram of materials used in PSCs; (d) schematic of interface of PVK and HTM layers; (e) comparison of PCE distributions of 30 individual devices; (f) EIS plots of devices in dark at 0.8 mV forward bias voltage
    Fig. 10. Pd ion doping in HTL[84]. (a) Schematic diagram of PSCs with HTL layer doped Pd nanosheets; (b) TEM image of Pd nanosheets; (c) energy level diagram of materials used in PSCs; (d) schematic of interface of PVK and HTM layers; (e) comparison of PCE distributions of 30 individual devices; (f) EIS plots of devices in dark at 0.8 mV forward bias voltage
    Ag ion doping in NiOx[94]. (a) Device structure; (b) SEM image of cross section of complete solar cell device and (c) Ag-doped lattice structure diagram; (d) Ag 3d XPS image of pristine NiOx thin film and Ag∶NiOx thin film; (e) UV-VIS absorption spectra and (f) time-resolved PL spectra of MAPbI3 thin films grown on pristine NiOx and Ag∶NiOx thin films; (g) J-V curves with reverse direction and (h) IPCE spectra of best performed device based PEDOT∶PSS, NiOx, and Ag∶NiOx as HTLs; (i) normalized PCE of PSCs based on PEDOT∶PSS, pristine NiOx, and Ag∶NiOx HTL as a function of storage time in ambient environment (30±2% humidity, T = 25 °C)
    Fig. 11. Ag ion doping in NiOx[94]. (a) Device structure; (b) SEM image of cross section of complete solar cell device and (c) Ag-doped lattice structure diagram; (d) Ag 3d XPS image of pristine NiOx thin film and Ag∶NiOx thin film; (e) UV-VIS absorption spectra and (f) time-resolved PL spectra of MAPbI3 thin films grown on pristine NiOx and Ag∶NiOx thin films; (g) J-V curves with reverse direction and (h) IPCE spectra of best performed device based PEDOT∶PSS, NiOx, and Ag∶NiOx as HTLs; (i) normalized PCE of PSCs based on PEDOT∶PSS, pristine NiOx, and Ag∶NiOx HTL as a function of storage time in ambient environment (30±2% humidity, T = 25 °C)
    Cr ion doping in NiOx[97]. (a) Cr/CuGaO2-CC/NiOx HTL device structure and (b) its SEM image; (c) PSC device energy level diagram; (d) SEM images of perovskite on NiOx and Cr/CuGaO2-CC/NiOx HTL, respectively; (e) PL spectrograms of perovskites on NiOx and Cr/CuGaO2-CC/NiOx HTL
    Fig. 12. Cr ion doping in NiOx[97]. (a) Cr/CuGaO2-CC/NiOx HTL device structure and (b) its SEM image; (c) PSC device energy level diagram; (d) SEM images of perovskite on NiOx and Cr/CuGaO2-CC/NiOx HTL, respectively; (e) PL spectrograms of perovskites on NiOx and Cr/CuGaO2-CC/NiOx HTL
    ElementDoped materialPCE /%FunctionReference
    All inorganic perovskite layerMn2+CsPbI316.52Reduce crystal lattice,expand grain,reduce hysteresis phenomenon,reduce composite18
    CsPbI2Br13.47Enlarged grain size14
    CsPbIBr219.9017
    Mn2+、Ni2+、Cu2+、Zn2+CsPbBr36.37-9.18Enlarged grain size,charge composite decreases19
    Organic inorganic perovskite layerCu2+、Ag+、(Na+MAPbI3Successfully incorporated into lattice,regulating valence band,with good band gap arrangement24
    Mn2+MAPbI317.68-19.09Insert into octahedron,suppress vacancy defect,enlarge grain size,adjustable band gap27
    Cd2+、Zn2+、Fe2+、Ni2+、Co2+、Ti4+MAPbI3It causes lattice shrinkage and changes energy band. Fe3+ has a negative effect on battery performance28
    Mn2+、Fe2+、Co2+、Ni2+、Cu2+、Zn2+MAPbI3Co2+ can change energy level and band gap,while Fe2+ has a reaction29
    Cd2+CsMAFAIncrease grain size,reduce defects,and improve stability33
    Cd2+、Zn2+、Fe2+11.70-13.76(0.1% Zn)For Cd2+,Zn2+,grain size will be enlarged,crystallinity will be improved,composite sites will be reduced,and battery performance will be improved. Fe2+ will introduce flight radiation defects50
    TiO2 electron transport materialNb2+m-TiO212.20-13.40Similar band gap,improves electron transmission52
    compact -TiO2Improve electron transport,reduce hysteresis,make the potential positive shift53
    TiO220.40-21.40Can control conduction band,improve photocurrent density54
    Nb2+、Ta2+m-/c-TiO212.40-14.80(Nb)/15.00(Ta)Improve electronic transmission at interface55-56
    Ta2+TiO2 nanowire19.11Electronic structure of crystal can be adjusted to speed up charge transfer57
    Y2+c-TiO2 nanorods18.32Improved electronic transport and reduced recombination58
    TiO219.30Increase electron transfer,lower Schottky barrier59
    Co2+TiO2Band edges are enhanced,defects are reduced,and charge transport is improved60
    Co2+TiO2Improve charge transfer,reduce point defects,improve quality of perovskite film,overcome energy band25
    Co2+m-TiO215.73It can improve light absorption ability,promote charge transmission and reduce electron hole recombination61
    Zr2+TiO218.16Improved TiO2 electrical conductivity,enhanced charge collection,inhibited recombination and defects,adjusted band,good band alignment62
    Ru2+c-TiO214.83-18.35Provides suitable band gap,low resistivity,and improved carrier density63
    Ag+、Zn2+c-TiO211.00-14.10Improve performance64
    Fe3+c-TiO216.02-18.60Defect density is reduced,and conductivity and charge mobility are improved65
    Ni2+TiO217.46Charge transfer is promoted,recombination is inhibited,Fermi level is positively shifted,energy level is adjusted,and defect density is reduced66
    Pt2+TiO220.02Electron transport performance and membrane coverage are improved,and trap state is inhibited67
    Other electronic transport materialsNb2+SnO220.50Better surface coverage of perovskite films reduces series resistance and inhibits hysteresis68
    SnO218.64-20.07Improvement of electrical conductivity and improvement of electron transport motion mechanics66
    Y2+SnO2 GNPs16.25-17.29Speed up charge transfer,restrain electron hole recombination,adjust band arrangement,restrain hysteresis69
    Co2+SnO2Improve band arrangement,improve charge extraction,inhibit compound,improve voltage and efficiency70
    Zr2+SnO2 NPs17.30-19.54Adjust energy level,reduce defect density,reduce interface resistance,inhibit recombination71
    Ru2+SnO220.00-22.00Fermi level of SnO2 is adjusted and increased,charge transfer is improved,and defect density is reduced72
    Ni2+ZnO210.37-12.77It is beneficial to carrier extraction and reduce recombination75
    Ni2+、Ag2+ZnO26.57-7.25Doped with 5% Ag helps charge transfer and reduces recombination rate76
    NiOx hole transport layerCu2+NiOx15.40Increase conductivity,reduce loss of Jsc and FF,improve PCE84
    Cu2+NiOx15.52-17.74Low temperature treatment results in high temperature effect86
    NiOx
    NiOx18.02-20.41Higher carrier concentration,higher hole mobility and higher work function improve hole extraction and reduce compound losses88
    NiOx9.08-11.45Low conductivity,accelerated hole extraction89
    NiOx21.19-23.17Higher conductivity and faster charge transfer and extraction85
    NiOx15.40Improve perovskite hole transmission capacity and reduce series resistance of device91
    Fe3+NiOx15.41-17.57Improvement in conductivity and work function87
    Ag+NiOx13.46-16.86Improve optical transparency,work function,conductivity and hole mobility of nickel oxide thin films92
    Y2+NiOx12.32-16.31Improved hole mobility,effective charge extraction and lower probability of carrier recombination93
    Zn2+NiOx10.43-13.72Defect density at grain boundary is reduced,charge recombination is inhibited,and hysteresis is improved94
    Cr2+NiOx17.60-19.91It has enhanced electrical conductivity,more efficient charge transport,more favorable energy level arrangement and promotes perovskite crystal growth95
    V2+NiOx13.48-13.82Electrical conductivity and surface adhesion are improved,and PCE effect and stability are enhanced96
    Other hole transport materialsTi2+MoO215.10-15.80Better stability for humidity97
    Ni2+、Ti2+MoO217.50-18.10Better reduction stability98
    Pd2+P3HT17.80-18.90Improve electrical conductivity99
    Au+、Ag+PEDOT:PSS11.33-12.18(Au)/12.68(Ag)Improve power conversion efficiency100
    Cu2+CrOx11.48It can inhibit oxidation state of Cr6+,providing a new HTL system101-102
    Table 1. Doping situation of transition metal in each layer of PSCs
    Wenzhen Zou, Chu Zhang, Hongmin Jiang, Liguo Gao, Meiqiang Fan, Tingli Ma. Application of Transition Metal Doping in Perovskite Photovoltaic Devices[J]. Laser & Optoelectronics Progress, 2023, 60(9): 0900002
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