Journal of Semiconductors, Volume. 46, Issue 5, 051804(2025)

Advances in multi-phase FAPbI3 perovskite: another perspective on photo-inactive δ-phase

Junyu Li1、†, Songwei Zhang1、†, Mohd Nazim Mohtar2, Nattha Jindapetch3, Istvan Csarnovics4, Mehmet Ertugrul5, Zhiwei Zhao1, Jing Chen1、*, Wei Lei1、**, and Xiaobao Xu1、***
Author Affiliations
  • 1Joint International Research Laboratory of Information Display and Visualization, School of Electronic Science and Engineering, Southeast University, Nanjing 211189, China
  • 2MyAgeingS1, University Putra Malaysia, Serdang, Selangor 43400, Malaysia
  • 3Department of Electrical and Biomedical Engineering, Faculty of Engineering, Prince of Songkla University, Hat Yai, Songkhla 90110, Thailand
  • 4Faculty of Science and Technology, University of Debrecen, Debrecen 4026, Hungary
  • 5Department of Metallurgy and Material Science Engineering Composite Materials, Engineering Faculty, Karadeniz Technical University, Trabzon 61080, Turkey
  • show less
    Figures & Tables(11)
    (Color online) Schematic diagram of FAPbI3 phases at different temperatures. Reprinted with permission from Ref. [21], Copyright 2018, American Chemical Society.
    (Color online) (a) XRD patterns with different periodic alignments for α- and δ-FAPbI3 single crystals and powder. (b) Different Raman shift for α- and δ-FAPbI3. (a) and (b) Reprinted with permission from Ref. [44], Copyright 2023, American Chemical Society. (c) Temperature-dependent steady-state PL spectrum of α-FAPbI3. (d) The extracted FWHM from steady-state PL spectrum of α-FAPbI3, and the well fitted red line indicates contributions from inhomogeneous broadening and Fröhlich coupling. (c) and (d) Reprinted with permission from Ref. [38], Copyright 2016, published under the terms of the Creative Commons CC BY license.
    (Color online) (a) Different structures of photoactive α-FAPbI3 and photo-inactive δ-FAPbI3. (b) Phonon density of states for the cubic, tetragonal, and hexagonal structures of FAPbI3, where the blue and red peaks represent the vibrations of the PbI3 octahedrons and FA+ cations, respectively. (a) and (b) Reprinted with permission from Ref. [33], Copyright 2022, American Chemical Society. (c) Schematic diagram of energy bands for STEs. Reprinted with permission from Ref. [24], Copyright 2020, Springer Nature. (d) PL spectra of α- and δ-FAPbI3. Reprinted with permission from Ref. [44], Copyright 2023, American Chemical Society.
    (Color online) (a)−(c) Real part of the permittivity of FAPbI3 measured at 100 kHz during temperature cycles at different conditions. Reprinted with permission from Ref. [46], Copyright 2019, American Chemical Society. (d) Thermal diffusivity test of α- and δ-FAPbI3. Reprinted with permission from Ref. [44], Copyright 2023, American Chemical Society.
    (Color online) (a) Schematic diagram of Gibbs free energy for α- and δ-FAPbI3. Reprinted with permission from Ref. [58], Copyright 2024, Elsevier. (b) The kinetic diagram with oriented and isotropic FA+ for cubic α-FAPbI3 and hexagonal δ-FAPbI3. Reprinted with permission from Ref. [59], Copyright 2016, published under the terms of the Creative Commons CC BY−NC license. (c) Phase stability comparison of α-FAPbI3 films with/without internal strain. Reprinted with permission from Ref. [60], Copyright 2020, Springer Nature. (d) Phase transition diagram of α-FAPbI3 during compression and decompression. Reprinted with permission from Ref. [22], Copyright 2018, American Chemical Society.
    (Color online) (a) Schematic diagram of phase transition between α- and δ-FAPbI3. Reprinted with permission from Ref. [58], Copyright 2024, published under the terms of the Creative Commons CC BY−NC−ND license. (b) Schematic diagram of the micro-area δ-to-α phase transition using direct-laser-writing. (c) Relationship between laser power and irradiation time of direct-laser-writing to realize δ-to-α phase transition. (d) Hybrid α-/δ-FAPbI3 under visible light and UV light constructed by direct-laser-writing, and the relationship between linewidth of the phase transition region and laser power. (b)−(d) Reprinted with permission from Ref. [44], Copyright 2023, American Chemical Society.
    (Color online) (a) Above-gap oscillations in the absorption spectra of FAPbI3 films at different temperatures. The inset illustrates two mechanisms that may result in the oscillations: quantum confinement in deep wells and periodicity of the superlattice confining potential. Reprinted with permission from Ref. [67], Copyright 2020, Springer Nature. (b) Schematic diagram of α-FAPbI3 single-crystal photothermal detector array, which denotes as device-α(SC) array, and the crosstalk of the nearest-neighbor and next-nearest-neighbor detection units in the device-α(SC) array. (c) Schematic diagram of hybrid α/δ-FAPbI3 single-crystal photothermal detector array by direct-laser-writing, which denotes as device-α array, and the crosstalk of the nearest-neighbor and next-nearest-neighbor detection units in the device-α array. (d) Terahertz photothermal proof-of-concept imaging of the device-α(SC) array. (e) Terahertz photothermal proof-of-concept imaging of the device-α array. (b)−(e) Reprinted with permission from Ref. [44], Copyright 2023, American Chemical Society.
    (Color online) (a) SEM images of micro-grating on α-FAPbI3 film constructed by direct-laser-writing. (b) Schematic diagram of polarization photodetector with micro-grating. (c) Polarization performance of the α-FAPbI3 photodetector with micro-grating, including angle-dependent photocurrent and linear sensitivity. (a)−(c) Reprinted with permission from Ref. [82], Copyright 2022, John Wiley and Sons.
    (Color online) (a) Schematic diagram of the fabrication process of the α/δ-FAPbI3 phase junction. (b) HRTEM of the α/δ-FAPbI3 phase junction. (c) Schematic diagrams of the energy levels of pure α-FAPbI3, pure δ-FAPbI3, and the α/δ-FAPbI3 phase junction. (d) Schematic diagram of the fabrication process of the bilayered δ-FAPbI3/perovskite films. (e) Current density−voltage curves for devices based on pristine perovskite films and bilayered δ-FAPbI3/perovskite films. (f) Statistics of PCEs and Jsc for devices based on pristine perovskite films and bilayered δ-FAPbI3/perovskite films. (g) Evolution of PCEs for devices based on pristine perovskite films and bilayered δ-FAPbI3/perovskite films under 40% ± 5% relative humidity (RH) at room temperature. (a)−(c) Reprinted with permission from Ref. [87], Copyright 2017, published under the terms of the Creative Commons CC BY−NC license. (d)−(g) Reprinted with permission from Ref. [88], Copyright 2022, John Wiley and Sons.
    (Color online) (a) Schematic diagram of the fabrication process of δ-FAPbI3 crystals, and the fabrication process of α-FAPbI3 thin films using δ-FAPbI3 crystals. (b) SEM image of the synthesized δ-FAPbI3 crystal. (c) Current density−voltage curves for devices based on intermediate δ-FAPbI3 single crystals (target) and powder sample (control). (d) Evolution of PCEs for target and control devices under continuous 1 sun illumination. (a)−(d) Reprinted with permission from Ref. [89], Copyright 2023, John Wiley and Sons.
    • Table 1. The comparison of α-FAPbI3 and δ-FAPbI3.

      View table
      View in Article

      Table 1. The comparison of α-FAPbI3 and δ-FAPbI3.

      Parametersα-FAPbI3δ-FAPbI3
      StructureCubic structure (Pm3¯m) with corner-sharing octahedronsHexagonal structure (P63mc) with face-sharing octahedrons
      StabilitySensitive to humidity and oxygenSensitive to humidity and oxygen
      Temperature dependenceThermodynamic instable at RT spontaneous transition to the δ-phaseThermodynamically stable at RT transition to the α-phase via heating (about 150 °C )
      Pressure influenceIn compression process, α-FAPbI3 undergoes Pm3¯m → P4/mbm → Im3¯ → partially amorphous from ambient pressure to 6.59 GPa, δ-FAPbI3 converts to the orthorhombic Cmc21 structure between 1.26 and 1.73 GPa (the phase transition can also be recovered during the decompression process)
      Mechanism of phase transitionThe lower Gibbs free energy in δ-FAPbI3 results in the inevitable α-to-δ phase transition at RT
      Kinetics of transitionThe driving force of the phase transition can be attributed to the temperature and internal/external pressure in the FAPbI3 unit cells
      Optoelectronic propertiesExcellentPoor
      ApplicationsActing as active layer materialsAssisting the photoactive α-FAPbI3 layer for functional applications
    Tools

    Get Citation

    Copy Citation Text

    Junyu Li, Songwei Zhang, Mohd Nazim Mohtar, Nattha Jindapetch, Istvan Csarnovics, Mehmet Ertugrul, Zhiwei Zhao, Jing Chen, Wei Lei, Xiaobao Xu. Advances in multi-phase FAPbI3 perovskite: another perspective on photo-inactive δ-phase[J]. Journal of Semiconductors, 2025, 46(5): 051804

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category: Research Articles

    Received: Nov. 25, 2024

    Accepted: --

    Published Online: Jun. 4, 2025

    The Author Email: Jing Chen (JChen), Wei Lei (WLei), Xiaobao Xu (XBXu)

    DOI:10.1088/1674-4926/24100024

    Topics