4.8 Article

Dynamic Stereochemical Activity of the Sn2+ Lone Pair in Perovskite CsSnBr3

Journal

JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
Volume 138, Issue 36, Pages 11820-11832

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/jacs.6b06287

Keywords

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Funding

  1. U.S. Department of Energy, Office of Science, Basic Energy Sciences [DE-SC-0012541]
  2. DOE Office of Science by Argonne National Laboratory [DE-AC02-06CH11357]
  3. MRSEC Program of the NSF [DMR 1121053]
  4. NSF
  5. Center for Scientific Computing from the CNSI, MRL: an NSF MRSEC [DMR-11210.53]
  6. NSF [CNS-0960316]
  7. National Science Foundation [DGE 1144085, DMR-1410242]
  8. Division Of Materials Research
  9. Direct For Mathematical & Physical Scien [1410242] Funding Source: National Science Foundation

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Stable s(2) lone pair electrons on heavy main-group elements in their lower oxidation states drive a range of important phenomena, such as the emergence of polar ground states in some ferroic materials. Here we study the perovskite halide CsSnBr3 as an embodiment of the broader materials class. We show that lone pair stereochemical activity due to the Sn2+ s(2) lone pair causes a crystallographically hidden; locally distorted state to appear upon warming, a phenomenon previously referred to as emphanisis. The synchrotron X-ray pair distribution function acquired between 300 and 420 K reveals emerging asymmetry in the nearest-neighbor Sn-Br correlations, consistent with dynamic Sn2+ off-centering, despite :there being no evidence of any deviation from the average cubic structure. Computation based on density functional theory supports the finding of a lattice instability associated: with dynamic off-centering of Sn2+ in its coordination environment. Photoluminescence measurements reveal an unusual blue shift with increasing temperature, closely linked to the structural evolution. At low temperatures, the structures reflect the influence of octahedral rotation. A continuous transition from an orthorhombic structure (Pnma, no. 62) to a tetragonal structure (P4/mbm, no. 127) is found around 250 K, with a final, first-order transformation at 286 K to the cubic structure (Pm (3) over barm, no. 221).

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