The ability to manipulate quantum dot (QD) surfaces is foundational to their technological deployment. Surface manipulation of metal halide perovskite (MHP) QDs has proven particularly challenging in comparison to that of more established inorganic materials due to dynamic surface species and low material formation energy; most conventional methods of chemical manipulation targeted at the MHP QD surface will result in transformation or dissolution of the MHP crystal. In previous work, we have demonstrated record-efficiency QD solar cells (QDSCs) based on ligand-exchange procedures that electronically couple MHP QDs yet maintain their nanocrystalline size, which stabilizes the corner-sharing structure of the constituent PbI octahedra with optoelectronic properties optimal for solar energy conversion. In this work, we employ a variety of spectroscopic techniques to develop a molecular-level understanding of the MHP QD surface chemistry in this system. We individually target both the anionic (oleate) and cationic (oleylammonium) ligands. We find that atmospheric moisture aids the process by hydrolysis of methyl acetate to generate acetic acid and methanol. Acetic acid then replaces native oleate ligands to yield QD surface-bound acetate and free oleic acid. The native oleylammonium ligands remain throughout this film deposition process and are exchanged during a final treatment step employing smaller cations-namely, formamidinium. This final treatment has a narrow processing window; initial treatment at this stage leads to a more strongly coupled QD regime followed by transformation into a bulk MHP film after longer treatment. These insights provide chemical understanding to the deposition of high-quality, electronically coupled MHP QD films that maintain both quantum confinement and their crystalline phase and attain high photovoltaic performance.
We
report a detailed study on APbX3 (A = formamidinium
(FA+), Cs+; X = I–, Br–) perovskite quantum dots (PQDs) with combined A- and
X-site alloying that exhibits both a wide bandgap and high open-circuit
voltage (V
oc) for the application of a
potential top cell in tandem junction photovoltaic (PV) devices. The
nanocrystal alloying affords control over the optical bandgap and
is readily achieved by solution-phase cation and anion exchange between
previously synthesized FAPbI3 and CsPbBr3 PQDs.
Increasing only the Br– content of the PQDs widens
the bandgap but results in shorter carrier lifetimes and associated V
oc losses in devices. These deleterious effects
can be mitigated by replacing Cs+ with FA+,
resulting in wide-bandgap PQD absorbers with improved charge-carrier
mobility and PVs with higher V
oc. Although
further device optimization is required, these results demonstrate
the potential of FA1–x
Cs
x
Pb(I1–x
Br
x
)3 PQDs for wide-bandgap perovskite
PVs with high V
oc.
Light-induced changes in photophysical and electronic
properties
in metal halide perovskites can affect their performance in photovoltaic
devices, light-emitting diodes, and other applications. Here we reveal
that light induces a slow, reversible enhancement in photoluminescence
(PL) lifetime and intensity in films of perovskite-phase CsPbI3 nanocrystals. When films of CsPbI3 nanocrystals
stored in air are photoexcited, their PL lifetime and intensity increase
by as much as a factor of 5 over the course of 20–30 min. Several
hours later, without additional light excitation, the initial PL lifetime
and intensity return. Placing the films under vacuum or nitrogen for
several minutes was also found to increase the PL lifetime and intensity.
We propose a model of slow, humidity- and light-sensitive surface
states in perovskite-phase CsPbI3 nanocrystals.
Color-changing materials have a variety
of applications, ranging
from smart windows to sensors. Here, we report deliquescent chromism
of thin, color neutral films of nickel(II) iodide (NiI2) that are less than 10 μm thick. This behavior does not occur
in the bulk material. Dark brown thin films of crystalline NiI2 turn clear when exposed to humidity and can be switched back
to the dark state when mildly heated (>35 °C). This optical
transition
between dark and clear states of an NiI2 thin film is reversible
with thermal cycling.
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