Dec 3, 2024
4:30pm - 4:45pm
Hynes, Level 3, Room 308
David Cahen1,Gary Hodes1,Dan Oron1,Pallavi Singh1
Weizmann Institute of Science1
David Cahen1,Gary Hodes1,Dan Oron1,Pallavi Singh1
Weizmann Institute of Science1
Self-healing (SH) materials can become game changers in developing sustainable “stuff”, especially in (opto)electronics. In terms of sustainable use, APbX<sub>3 </sub>Halide (=X) Perovskite (HaP) semiconductors have a strong advantage over most others, as they can self-heal (SH) damage. We show SH, using "fluorescence recovery after photobleaching" (FRAP), also in (encapsulated) polycrystalline films, as used in most devices. There, SH from photodamage is faster for γ-CsPbI<sub>3</sub> and α-FAPbI<sub>3 </sub>than for MAPbI<sub>3</sub> and substituting ≧15 at.% MA<sup>+</sup> with guanidinium (Gua<sup>+</sup>) or acetamidinium (AA<sup>+</sup>) enhances SH. However, substituting dimethyl ammonium (DMA<sup>+</sup>), about the size of Gua<sup>+</sup> and AA<sup>+</sup>, for MA<sup>+</sup> does not change the SH rate. Thus, while the A cation is considered electronically relatively inactive, it affects both SH kinetics (and photodamage thresholds). Based on the time scale of SH, we infer that the rate-determining step of SH involves short-range diffusion of A<sup>+</sup> and/or Pb<sup>2+</sup> cations, complementing earlier findings, and implicating halides (X<sup>-</sup>) in SH. The SH rate correlates with the material’s strain, the A<sup>+</sup> dipole moment, and A<sup>+ …..</sup> I<sup>-</sup> hydrogen bonding, offering clues to the roles of ion, electron, and energy migration in the SH mechanism, which will help guide the design of SH materials.<br/><br/>* Work done with DR Ceratti (now at ENSCParis), Y Soffer, S Bera, Y Feldman & M Elbaum, all from the Weizmann Inst.