Metal halide perovskites (MHPs) have inherent properties that show strong potential for light emission-based optoelectronic applications. MHPs typically employ an ABX3 crystal structure where A is an organic, inorganic, or hybrid cation, B is typically lead or tin, and X is a halide anion. 

By introducing dopants into the B-site, one can improve the MHPs' optoelectronic properties, which can result into higher performance devices. 

I have investigated the introduction of transition metal dopants (e.g., Mn2+, Ni2+, Zn2+, etc.) into the MHPs' B-site and their effects on perovskite LED performance. For instance, in our JACS paper we looked at the effects of transition metal dopants on MHP nanocrystals at device relevant conditions. We showed both theoretically and experimentally how the  lattice periodicity breaking effect primarily enhances the radiative rates in doped MHP nanocrystals.

Zooming in on the effects of Mn2+ on perovskite LEDs, I engineered Mn2+ doped perovskite LEDs and studied their performance with respect to external quantum efficiency and operational stability. In our Device paper, by introducing a molecular additive known as tris(4-fluorophenyl)phosphine oxide (TFPPO), we were able to simultaneously achieve incredibly bright and efficient transition metal doped LEDs. However, we also found that the operational stability of these LEDs is degraded with higher concentrations of TFPPO. We studied this efficiency-stability trade-off with optoelectronic and photophysical characterization on the Mn2+ doped perovskite LEDs and found that while TFPPO treatment does initially improve LED performance, this enhancement is not resilient under identical device operating conditions. This implies that before phosphine oxide additives are universally adopted in perovskite LEDs, their stability degradation mechanisms must be further investigated.

Today, most perovskite LEDs are fabricated using spin-coating techniques for the solution-based deposition of the perovskite active layer. While these techniques have led to rapid progress in achieving high external quantum efficiencies(EQEs) in perovskite LEDs (within the last decade, >20% EQEs have been achieved for red and green perovskite LEDs), spin-coating based fabrication of perovskite LEDs limits their commercial viability. This is largely due to the large sample-sample variability and substrate area limitations incurred by spin-coating. In contrast, other LEDs such as organic LEDs (OLEDs) are fabricated using vacuum thermal evaporation techniques.

Vacuum thermal evaporation (VTE) holds the potential to reduce perovskite LED variability, increase pixel resolution by using precise metal masks, and enable cleaner production since no harmful solvents are needed. VTE involves heating perovskite precursor materials to form gaseous molecules that then interact with each other on the LED substrate surface to form a perovskite active layer. This process involves careful optimization of the nucleus formation, stoichiometric ratio of precursors, and regulation of evaporation rates to result in efficient vacuum-evaporated perovskite LEDs.

I am interested in optimizing the performance of vacuum-evaporated perovskite LEDs both within the visible and ultraviolet spectrums to the levels achieved in solution-processed perovskite LEDs by studying the formation of the vacuum-evaporated perovskite layer, incorporating various additives and precursors to yield highly emissive active layers, and engineering new device architectures that promote efficient charge carrier transport within vacuum-evaporated perovskite LEDs.

While most metal halide perovskites (MHPs) will employ a 3D ABX3  structure, we can employ a ligand (or ligand-like) species, L, to limit the growth of the MHP in one dimension and result in a colloidally stable perovskite nanoplatelet structure. Thus, the formula of perovskite nanoplatelets is denoted by L2[ABX3]n-1BX4 where L is the ligand species and n-1 represents the thickness of the nanoplatelet in terms of the bulk perovskite. 

Previously, the use of lead within colloidal perovskite nanoplatelets has been well studied and has demonstrated tunable emission across the visible spectrum. Additionally, the use of tin instead of lead has also been studied within perovskite nanoplatelets but generally lacks the stability and tunability offered by lead-based perovskite nanoplatelets.

In order to enable lead-free perovskite-based light emission, we must consider other candidates besides tin. In particular, there is substantial interest to enable lead-free light emission in the deep blue and violet ranges given the limited demonstrations.

By employing rare earth elements, I have synthesized bright, lead-free, colloidal perovskite nanoplatelets that emit in the deep blue and violet ranges (between 400 and 460 nm) - demonstrating a new route towards non-toxic high energy visible light emission. These lead-free nanoplatelets show excellent tunability in this high energy range across halide, thickness, and ligand-like species (i.e., organic spacer cation). 

While the vast majority of perovskite LEDs have focused on light emission within the visible spectrum, there is significant interest in engineering perovskite LEDs that can emit at higher energies (i.e., the ultraviolet (UV) spectrum). UV LEDs have direct applications in human health applications (e.g., sterilization and water purification), 3D printing, sensing, and nanofabrication.

In order to design perovskites with wider bandgaps which can then emit higher energy light, we must consider additional tunability techniques in addition to halide engineering. One potential pathway is the integration of quantum confined 2D lead halide perovskites. 

In our Matter paper, we introduced a trace amount of water into the perovskite precursor solution to control the crystallization of the 2D PEA2PbBr4 thin film. As a result, we were able to demonstrate a 408 nm violet-emitting perovskite LED with a maximum external quantum efficiency of 0.41%, a five-fold increase over control devices.

In our recent work (in press at Device), we showed that by replacing 25% of the bromide within the 2D PEA2PbBr4 perovskite with chloride as well as employing a dual electron transport layer device architecture, we can achieve a 399 nm UV-emitting perovskite LED based on a PEA2PbCl1Br3 perovskite. This perovskite LED demonstrated a maximum external quantum efficiency of 0.16% and is, to our best knowledge, the first demonstration of UV light emission from a lead halide perovskite.