1 research outputs found
Cs<sub>1β<i>x</i></sub>Rb<sub><i>x</i></sub>PbCl<sub>3</sub> and Cs<sub>1β<i>x</i></sub>Rb<sub><i>x</i></sub>PbBr<sub>3</sub> Solid Solutions: Understanding Octahedral Tilting in Lead Halide Perovskites
The structures of
the lead halide perovskites CsPbCl<sub>3</sub> and CsPbBr<sub>3</sub> have been determined from X-ray powder diffraction
data to be orthorhombic with <i>Pnma</i> space group symmetry.
Their structures are distorted from the cubic structure of their hybrid
analogs, CH<sub>3</sub>NH<sub>3</sub>PbX<sub>3</sub> (X = Cl, Br),
by tilts of the octahedra (Glazer tilt system <i>a</i><sup>β</sup><i>b</i><sup>+</sup><i>a</i><sup>β</sup>). Substitution of the smaller Rb<sup>+</sup> for Cs<sup>+</sup> increases the octahedral tilting distortion and eventually
destabilizes the perovskite structure altogether. To understand this
behavior, bond valence parameters appropriate for use in chloride
and bromide perovskites have been determined for Cs<sup>+</sup>, Rb<sup>+</sup>, and Pb<sup>2+</sup>. As the tolerance factor decreases,
the band gap increases, by 0.15 eV in Cs<sub>1β<i>x</i></sub>Rb<sub><i>x</i></sub>PbCl<sub>3</sub> and 0.20 eV
in Cs<sub>1β<i>x</i></sub>Rb<sub><i>x</i></sub>PbBr<sub>3</sub>, upon going from <i>x</i> = 0 to <i>x</i> = 0.6. The band gap shows a linear dependence on tolerance
factor, particularly for the Cs<sub>1β<i>x</i></sub>Rb<sub><i>x</i></sub>PbBr<sub>3</sub> system. Comparison
with the cubic perovskites CH<sub>3</sub>NH<sub>3</sub>PbCl<sub>3</sub> and CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> shows that the
band gaps of the methylammonium perovskites are anomalously large
for APbX<sub>3</sub> perovskites with a cubic structure. This comparison
suggests that the local symmetry of CH<sub>3</sub>NH<sub>3</sub>PbCl<sub>3</sub> and CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> deviate
significantly from the cubic symmetry of the average structure