An
increasing number of studies have recently reported the rapid
degradation of hybrid and all-inorganic lead halide perovskite nanocrystals
under electron beam irradiation in the transmission electron microscope,
with the formation of nanometer size, high contrast particles. The
nature of these nanoparticles and the involved transformations in
the perovskite nanocrystals are still a matter of debate. Herein,
we have studied the effects of high energy (80/200 keV) electron irradiation
on colloidal cesium lead bromide (CsPbBr3) nanocrystals
with different shapes and sizes, especially 3 nm thick nanosheets,
a morphology that facilitated the analysis of the various ongoing
processes. Our results show that the CsPbBr3 nanocrystals
undergo a radiolysis process, with electron stimulated desorption
of a fraction of bromine atoms and the reduction of a fraction of
Pb2+ ions to Pb0. Subsequently Pb0 atoms diffuse and aggregate, giving rise to the high contrast particles,
as previously reported by various groups. The diffusion is facilitated
by both high temperature and electron beam irradiation. The early
stage Pb nanoparticles are epitaxially bound to the parent CsPbBr3 lattice, and evolve into nonepitaxially bound Pb crystals
upon further irradiation, leading to local amorphization and consequent
dismantling of the CsPbBr3 lattice. The comparison among
CsPbBr3 nanocrystals with various shapes and sizes evidences
that the damage is particularly pronounced at the corners and edges
of the surface, due to a lower diffusion barrier for Pb0 on the surface than inside the crystal and the presence of a larger
fraction of under-coordinated atoms.
Films
of colloidal CsPbX3 (X = I, Br or Cl) nanocrystals,
prepared by solution drop-casting or spin-coating on a silicon substrate,
were exposed to a low flux of X-rays from an X-ray photoelectron spectrometer
source, causing intermolecular C=C bonding of the organic ligands
that coat the surface of the nanocrystals. This transformation of
the ligand shell resulted in a greater stability of the film, which
translated into the following features: (i) Insolubility of the exposed
regions in organic solvents which caused instead complete dissolution
of the unexposed regions. This enabled the fabrication of stable and
strongly fluorescent patterns over millimeter scale areas. (ii) Inhibition
of the irradiated regions toward halide anion exchange reactions,
when the films were exposed either to halide anions in solution or
to hydrohalic vapors. This feature was exploited to create patterned
regions of different CsPbIxBryClz compositions, starting
from a film with homogeneous CsPbX3 composition. (iii)
Resistance of the films to degradation caused by exposure to air and
moisture, which represents one of the major drawbacks for the integration
of these materials in devices. (iv) Stability of the film in water
and biological buffer, which can open interesting perspectives for
applications of halide perovskite nanocrystals in aqueous environments.
Perovskite-related
Cs4PbBr6 nanocrystals
present a “zero-dimensional” crystalline structure where
adjacent [PbBr6]4– octahedra do not share
any corners. We show in this work that these nanocrystals can be converted
into “three-dimensional” CsPbBr3 perovskites
by extraction of CsBr. This conversion drastically changes the optoelectronic
properties of the nanocrystals that become highly photoluminescent.
The extraction of CsBr can be achieved either by thermal annealing
(physical approach) or by chemical reaction with Prussian Blue (chemical
approach). The former approach can be simply carried out on a dried
film without addition of any chemicals but does not yield a full transformation.
Instead, reaction with Prussian Blue in solution achieves a full transformation
into the perovskite phase. This transformation was also verified on
the iodide counterpart (Cs4PbI6).
CsPbBr3 nanocrystals passivated with short molecular
ligands and deposited on a substrate were annealed from room temperature
to 400 °C in inert atmosphere. Chemical, structural, and morphological
transformations were monitored in situ and ex situ by different techniques, while optoelectronic properties
of the film were also assessed. Annealing at 100 °C resulted
in a 1 order of magnitude increase in photocurrent and photoresponse
as a result of partial sintering of the NCs and residual solvent evaporation.
Beyond 150 °C the original orthorhombic NCs were partially transformed
into tetragonal CsPb2Br5 crystals, due to the
desorption of weakly bound propionic acid ligands. The photocurrent
increased moderately until 300 °C although the photoresponse
became slower as a result of the formation of surface trap states.
Eventually, annealing beyond 350 °C removed the strongly bound
butylamine ligands and reversed the transition to the original orthorhombic
phase, with a loss of photocurrent due to the numerous defects induced
by the stripping of the passivating butylamine.
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