V. D’Innocenzo, G. Grancini, M. Alcocer, A. Kandada, S. Stranks, M. Lee, G. Lanzani, H. Snaith, and A. Petrozza, Excitons versus free charges in organo-lead tri-halide perovskites, Nature Communications 5, 3586-1‑3586-6 (2014). doi: 10.1038/ncomms4586.
Methylammonium lead iodide: phase transition temperature Verified

See all entries for this property (20 total)

Origin: experimental
Phase transition
Initial crystal system tetragonal
Final crystal system orthorhombic
Initial space group Unknown
Final space group Unknown
Direction Cooling
Phase transition temperature 160.0 K

Hysteresis: 10

V. D’Innocenzo, G. Grancini, M. Alcocer, A. Kandada, S. Stranks, M. Lee, G. Lanzani, H. Snaith, and A. Petrozza, Excitons versus free charges in organo-lead tri-halide perovskites, Nature Communications 5, 3586-1‑3586-6 (2014). doi: 10.1038/ncomms4586.
System description
Dimensionality: D
Sample type: film

Starting materials: MAI, PbI2, DMF, Si glass

Product: MAPbI3 Thin-film on Si

Description: Dissolve methylammonium iodide and lead (II) iodide (Sigma-Aldrich) in anhydrous N,N-Dimethylformamide (DMF) at a 3:1 molar ratio of MAI to PbI2, with final concentrations of 2.64M methylammonium iodide. The perovskite layer was then formed by spin coating the precursor solutions directly on the glass substrate at 2,000 r.p.m. in air. The flat and thin meso samples were spin coated without dilution but mesoporous samples were spin coated from diluted (three parts in four) precursor solutions. After spin coating, anneal the CH3NH3PbI3 at 150°C for 15 min.

Method: UV-Vis absorption

Description: Absorption measurements were performed using a spectrophotometer (Perkin Elmer Lambda 1050) and a continuous flow static exchange gas cryostat (Oxford Instruments Optistat CF). The cryostat consist of three chambers, one inside the other. The sample is housed inside the internal chamber filled with gaseous He. The cryogenic liquid (He) is fluxed inside the second chamber allowing temperature control of the He atmosphere of the sample chamber. Eventually, a third chamber is evacuated (~10^-5–10^-6 mbar) in order to assure thermal isolation from the external ambient. Refer to Fig. 1.

Comment: Crystal sizes larger than 500nm

Extraction method: Manual entry
Entry added on: July 3, 2019, 12:04 p.m.
Entry added by: Xiaochen Du Duke University
Last updated on: Aug. 31, 2022, 2:54 p.m.
Last updated by: Rayan C Duke University
Data correctness verified by:
  • Rayan C Duke University

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