Affiliation:
1. Department of Chemistry Indian Institute of Science Education and Research (IISER) Pune 411008 India
2. Department of Physics Indian Institute of Science Education and Research (IISER) Pune 411008 India
3. Polymer Science and Engineering Division CSIR‐National Chemical Laboratory (CSIR‐NCL) Pune 411008 India
4. Academy of Scientific and Innovative Research (AcSIR) Ghaziabad 201002 India
5. Department of Physics Indian Institute of Science Education and Research (IISER) Bhopal 462066 India
Abstract
AbstractTypical layered 2D A2PbX4 (A: organic ammonium cation, X: Br, I) perovskites undergo irreversible decomposition at high temperatures. Can they be designed to melt at lower temperatures without decomposition? Which thermodynamic parameter drive the melting of layered perovskites? These questions are addressed by considering the melt of A2PbX4 as a mixture of ions (like ionic liquids), and hypothesized that the increase in the structural entropy of fusion (ΔSfus) will be the driving force to decrease their melting temperature. Then to increase structural ΔSfus, A‐site cations are designed that are rigid in the solid crystal, and become flexible in the molten state. Different tail groups in the A‐site cations form hydrogen‐, halogen‐ and even covalent bonding‐interactions, making the cation‐layer rigid in the solid form. Additionally, the rotation of ─NH3+ head group is suppressed by replacing ─H with ─CH3, further enhancing the rigidity. Six A2PbX4 crystals with high ΔSfus and low melting temperatures are prepared using this approach. For example, [I−(CH2)3−NH2(CH3)]2PbI4 reversibly melts at 388 K (decomposition temperature 500 K), and then recrystallizes back upon cooling. Consequently, melt‐pressed films are grown demonstrating the solvent‐ and vacuum‐free perovskite films for future optoelectronic devices.
Funder
Council of Scientific and Industrial Research, India
University Grants Commission
Science and Engineering Research Board