Fig. 1. Mn-doped CsPbI
2Br
[28]. (a) Schematic structure of device and description of Mn
2+ doping modes: interstitial and substitution; scanning electron microscope (SEM) images of (b) original chlorinated paraffins and (c) 0.5%, (d) 1%, and (e) 2% MnCl
2; (f) schematic diagram of grain growth driven by surface passivated MnCl
2 Fig. 2. Mn-dopded CsPbI
3[29]. (a) Structure and crystal junction diagram of Mn-doped CsPbI
3 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 CsPbI
3 in forward and reverse measurements
Fig. 3. Influence of Ag ion doping on PVK
[33]. (a) Layout diagram of planar junction solar cell; (b) photovoltaic performance of MAB
0.1Pb
0.9I
3 system with different B elements; (c) UV spectra curves of MAPb
1-xHg
xI
3 films at different Hg
2+ doping concentrations; (d) PCE box diagram of solar cells based on MAPb
1-xHg
xI
3; (e) SEM images of perovskite films with different Hg
2+ doping concentrations
Fig. 4. Influence of Co ion doping on PVK
[34]. (a) Transmission electron microscope (TEM) cross-section image of MA(31Pb∶1Co)I
3 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 MAPbI
3 and MA(Pb∶Co)I
3 thin films; (g) XPS images of MAPbI
3 and MA(31Pb∶1Co)I
3 thin films; (h) forward and reverse
J-
V diagrams of solar cell measurements, and average performance of optimized MA(Pb∶Co)I
3 solar cells; (i) energy level diagram of MA (Pb∶Co)I
3 relative to MAPbI
3 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 TiO
2/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. 6. Nb ion and Ta ion doping in TiO
2[54]. (a) Conduction band diagram of dopant regulated battery; (b) energy graph image of Nb-TiO
2 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 TiO
2 films prepared by SEM, and top view of Nb-TiO
2 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 TiO
2 nanowire arrays with different Ta doping levels; (e) a and c are undoped TiO
2 nanowire arrays, b and d are TEM and high-resolution transmission electron microscopy (HRTEM) images of 0.1-Ta-TiO
2 nanowire arrays; Illustrations in c and d are corresponding fast Fourier transform (FFT) diffraction patterns
Fig. 7. Co ion doping in TiO
2[61]. (a) MOF preparation process and perovskite solar cell structure; (b)
J-
V curves of solar cells with best performance using dye-sol TiO
2 and co-doped TiO
2 (mass fraction is 1%); (c) SEM images of dye-sol TiO
2 and 1% mass fraction co-doped TiO
2 on FTO coated glass; (d) EIS curves based on TiO
2 and 1% mass fraction co-doped TiO
2 thin films
Fig. 8. Ni ion doping in TiO
2[66]. (a) Schematic diagram of solution treatment method for preparing Ni-TiO
2 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. 9. Co ion doping in SiO
2[73]. (a) Band diagrams of SnO
2, SnO
2-CoCl
2, and PVK layers and
J-
V curves of prepared PSCs; (b) cross-sectional SEM images of PSC based on SnO
2-CoCl
2 at a scale of 500 nm; (c) PSCs PCE histogram based on SnO
2 and SnO
2-CoCl
2; (d) XPS image of Co 2p; XPS image of O 1s for (e) pristine SnO
2 and (f) SnO
2-CoCl
2 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
Fig. 11. Ag ion doping in NiO
x[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 NiO
x thin film and Ag∶NiO
x thin film; (e) UV-VIS absorption spectra and (f) time-resolved PL spectra of MAPbI
3 thin films grown on pristine NiO
x and Ag∶NiO
x thin films; (g)
J-
V curves with reverse direction and (h) IPCE spectra of best performed device based PEDOT∶PSS, NiO
x, and Ag∶NiO
x as HTLs; (i) normalized PCE of PSCs based on PEDOT∶PSS, pristine NiO
x, and Ag∶NiO
x HTL as a function of storage time in ambient environment (30±2% humidity,
T = 25 °C)
Fig. 12. Cr ion doping in NiO
x[97]. (a) Cr/CuGaO
2-CC/NiO
x HTL device structure and (b) its SEM image; (c) PSC device energy level diagram; (d) SEM images of perovskite on NiO
x and Cr/CuGaO
2-CC/NiO
x HTL, respectively; (e) PL spectrograms of perovskites on NiO
x and Cr/CuGaO
2-CC/NiO
x HTL
| Element | Doped material | PCE /% | Function | Reference |
---|
All inorganic perovskite layer | Mn2+ | CsPbI3 | 16.52 | Reduce crystal lattice,expand grain,reduce hysteresis phenomenon,reduce composite | [18] | CsPbI2Br | 13.47 | Enlarged grain size | [14] | CsPbIBr2 | 19.90 | | [17] | Mn2+、Ni2+、Cu2+、Zn2+ | CsPbBr3 | 6.37-9.18 | Enlarged grain size,charge composite decreases | [19] | Organic inorganic perovskite layer | Cu2+、Ag+、(Na+) | MAPbI3 | | Successfully incorporated into lattice,regulating valence band,with good band gap arrangement | [24] | Mn2+ | MAPbI3 | 17.68-19.09 | Insert into octahedron,suppress vacancy defect,enlarge grain size,adjustable band gap | [27] | Cd2+、Zn2+、Fe2+、Ni2+、Co2+、Ti4+ | MAPbI3 | | It causes lattice shrinkage and changes energy band. Fe3+ has a negative effect on battery performance | [28] | Mn2+、Fe2+、Co2+、Ni2+、Cu2+、Zn2+ | MAPbI3 | | Co2+ can change energy level and band gap,while Fe2+ has a reaction | [29] | Cd2+ | CsMAFA | | Increase grain size,reduce defects,and improve stability | [33] | 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 defects | [50] | TiO2 electron transport material | Nb2+ | m-TiO2 | 12.20-13.40 | Similar band gap,improves electron transmission | [52] | compact -TiO2 | | Improve electron transport,reduce hysteresis,make the potential positive shift | [53] | TiO2 | 20.40-21.40 | Can control conduction band,improve photocurrent density | [54] | Nb2+、Ta2+ | m-/c-TiO2 | 12.40-14.80(Nb)/15.00(Ta) | Improve electronic transmission at interface | [55-56] | Ta2+ | TiO2 nanowire | 19.11 | Electronic structure of crystal can be adjusted to speed up charge transfer | [57] | Y2+ | c-TiO2 nanorods | 18.32 | Improved electronic transport and reduced recombination | [58] | TiO2 | 19.30 | Increase electron transfer,lower Schottky barrier | [59] | Co2+ | TiO2 | | Band edges are enhanced,defects are reduced,and charge transport is improved | [60] | Co2+ | TiO2 | | Improve charge transfer,reduce point defects,improve quality of perovskite film,overcome energy band | [25] | Co2+ | m-TiO2 | 15.73 | It can improve light absorption ability,promote charge transmission and reduce electron hole recombination | [61] | Zr2+ | TiO2 | 18.16 | Improved TiO2 electrical conductivity,enhanced charge collection,inhibited recombination and defects,adjusted band,good band alignment | [62] | Ru2+ | c-TiO2 | 14.83-18.35 | Provides suitable band gap,low resistivity,and improved carrier density | [63] | Ag+、Zn2+ | c-TiO2 | 11.00-14.10 | Improve performance | [64] | Fe3+ | c-TiO2 | 16.02-18.60 | Defect density is reduced,and conductivity and charge mobility are improved | [65] | Ni2+ | TiO2 | 17.46 | Charge transfer is promoted,recombination is inhibited,Fermi level is positively shifted,energy level is adjusted,and defect density is reduced | [66] | Pt2+ | TiO2 | 20.02 | Electron transport performance and membrane coverage are improved,and trap state is inhibited | [67] | Other electronic transport materials | Nb2+ | SnO2 | 20.50 | Better surface coverage of perovskite films reduces series resistance and inhibits hysteresis | [68] | | SnO2 | 18.64-20.07 | Improvement of electrical conductivity and improvement of electron transport motion mechanics | [66] | Y2+ | SnO2 GNPs | 16.25-17.29 | Speed up charge transfer,restrain electron hole recombination,adjust band arrangement,restrain hysteresis | [69] | Co2+ | SnO2 | | Improve band arrangement,improve charge extraction,inhibit compound,improve voltage and efficiency | [70] | Zr2+ | SnO2 NPs | 17.30-19.54 | Adjust energy level,reduce defect density,reduce interface resistance,inhibit recombination | [71] | Ru2+ | SnO2 | 20.00-22.00 | Fermi level of SnO2 is adjusted and increased,charge transfer is improved,and defect density is reduced | [72] | Ni2+ | ZnO2 | 10.37-12.77 | It is beneficial to carrier extraction and reduce recombination | [75] | Ni2+、Ag2+ | ZnO2 | 6.57-7.25 | Doped with 5% Ag helps charge transfer and reduces recombination rate | [76] | NiOx hole transport layer | Cu2+ | NiOx | 15.40 | Increase conductivity,reduce loss of Jsc and FF,improve PCE | [84] | Cu2+ | NiOx | 15.52-17.74 | Low temperature treatment results in high temperature effect | [86] | | NiOx | | | | | NiOx | 18.02-20.41 | Higher carrier concentration,higher hole mobility and higher work function improve hole extraction and reduce compound losses | [88] | | NiOx | 9.08-11.45 | Low conductivity,accelerated hole extraction | [89] | | NiOx | 21.19-23.17 | Higher conductivity and faster charge transfer and extraction | [85] | | NiOx | 15.40 | Improve perovskite hole transmission capacity and reduce series resistance of device | [91] | Fe3+ | NiOx | 15.41-17.57 | Improvement in conductivity and work function | [87] | Ag+ | NiOx | 13.46-16.86 | Improve optical transparency,work function,conductivity and hole mobility of nickel oxide thin films | [92] | Y2+ | NiOx | 12.32-16.31 | Improved hole mobility,effective charge extraction and lower probability of carrier recombination | [93] | Zn2+ | NiOx | 10.43-13.72 | Defect density at grain boundary is reduced,charge recombination is inhibited,and hysteresis is improved | [94] | Cr2+ | NiOx | 17.60-19.91 | It has enhanced electrical conductivity,more efficient charge transport,more favorable energy level arrangement and promotes perovskite crystal growth | [95] | V2+ | NiOx | 13.48-13.82 | Electrical conductivity and surface adhesion are improved,and PCE effect and stability are enhanced | [96] | Other hole transport materials | Ti2+ | MoO2 | 15.10-15.80 | Better stability for humidity | [97] | Ni2+、Ti2+ | MoO2 | 17.50-18.10 | Better reduction stability | [98] | Pd2+ | P3HT | 17.80-18.90 | Improve electrical conductivity | [99] | Au+、Ag+ | PEDOT:PSS | 11.33-12.18(Au)/12.68(Ag) | Improve power conversion efficiency | [100] | Cu2+ | CrOx | 11.48 | It can inhibit oxidation state of Cr6+,providing a new HTL system | [101-102] |
|
Table 1. Doping situation of transition metal in each layer of PSCs