Rebecca L. Milot

Perovskite-perovskite tandem photovoltaics with optimized band gaps

Tandem perovskite cells The ready processability of organic-inorganic perovskite materials for solar cells should enable the fabrication of tandem solar cells, in which the top layer is tuned to absorb shorter wavelengths and the lower layer to absorb the remaining longer-wavelength light. The difficulty in making an all-perovskite cell is finding a material that absorbs the red end of the spectrum. Eperon et al. developed an infrared-absorbing mixed tin-lead material that can deliver 14.8% efficiency on its own and 20.3% efficiency in a four-terminal tandem cell. Science, this issue p. 861 A mixed tin-lead perovskite material with a narrow band gap enables efficient tandem solar cells. We demonstrate four- and two-terminal perovskite-perovskite tandem solar cells with ideally matched band gaps. We develop an infrared-absorbing 1.2–electron volt band-gap perovskite, FA0.75Cs0.25Sn0.5Pb0.5I3, that can deliver 14.8% efficiency. By combining this material with a wider–band gap FA0.83Cs0.17Pb(I0.5Br0.5)3 material, we achieve monolithic two-terminal tandem efficiencies of 17.0% with >1.65-volt open-circuit voltage. We also make mechanically stacked four-terminal tandem cells and obtain 20.3% efficiency. Notably, we find that our infrared-absorbing perovskite cells exhibit excellent thermal and atmospheric stability, not previously achieved for Sn-based perovskites. This device architecture and materials set will enable “all-perovskite” thin-film solar cells to reach the highest efficiencies in the long term at the lowest costs.

Electron-phonon coupling in hybrid lead halide perovskites.

Phonon scattering limits charge-carrier mobilities and governs emission line broadening in hybrid metal halide perovskites. Establishing how charge carriers interact with phonons in these materials is therefore essential for the development of high-efficiency perovskite photovoltaics and low-cost lasers. Here we investigate the temperature dependence of emission line broadening in the four commonly studied formamidinium and methylammonium perovskites, HC(NH2)2PbI3, HC(NH2)2PbBr3, CH3NH3PbI3 and CH3NH3PbBr3, and discover that scattering from longitudinal optical phonons via the Fröhlich interaction is the dominant source of electron–phonon coupling near room temperature, with scattering off acoustic phonons negligible. We determine energies for the interacting longitudinal optical phonon modes to be 11.5 and 15.3 meV, and Fröhlich coupling constants of ∼40 and 60 meV for the lead iodide and bromide perovskites, respectively. Our findings correlate well with first-principles calculations based on many-body perturbation theory, which underlines the suitability of an electronic band-structure picture for describing charge carriers in hybrid perovskites.

A visible light water-splitting cell with a photoanode formed by codeposition of a high-potential porphyrin and an iridium water-oxidation catalyst

A high-potential porphyrin is codeposited on TiO2 nanoparticles together with our Cp*–iridium water-oxidation catalyst to give a photoanode for a water-splitting cell. The photoanode optically resembles the porphyrin yet electrochemically responds like the Ir catalyst when it is immersed in aqueous solutions. Photoelectrochemical data show that illumination of the codeposited anode in water results in a marked enhancement and stability of the photocurrent, providing evidence for light-induced activation of the catalyst.

Charge‐Carrier Dynamics and Mobilities in Formamidinium Lead Mixed‐Halide Perovskites

The mixed-halide perovskite FAPb(Bry I1-y )3 is attractive for color-tunable and tandem solar cells. Bimolecular and Auger charge-carrier recombination rate constants strongly correlate with the Br content, y, suggesting a link with electronic structure. FAPbBr3 and FAPbI3 exhibit charge-carrier mobilities of 14 and 27 cm(2) V(-1) s(-1) and diffusion lengths exceeding 1 μm, while mobilities across the mixed Br/I system depend on crystalline phase disorder.

Photovoltaic mixed-cation lead mixed-halide perovskites: links between crystallinity, photo-stability and electronic properties

Lead mixed halide perovskites are highly promising semiconductors for both multi-junction photovoltaic and light emitting applications due to their tunable band gaps, with emission and absorption energies spanning the UV-visible to near IR regions. However, many such perovskites exhibit unwanted halide segregation under photo-illumination, the cause of which is still unclear. In our study, we establish crucial links between crystal phase stability, photostability and optoelectronic properties of the mixed-cation lead mixed-halide perovskite CsyFA(1−y)Pb(BrxI(1−x))3. We demonstrate a region for caesium content between 0.10 < y < 0.30 which features high crystalline quality, long charge-carrier lifetimes and high charge-carrier mobilities. Importantly, we show that for such high-quality perovskites, photo-induced halide segregation is strongly suppressed, suggesting that high crystalline quality is a prerequisite for good optoelectronic quality and band gap stability. We propose that regions of short-range crystalline order aid halide segregation, possibly by releasing lattice strain between iodide rich and bromide rich domains. For an optimized caesium content, we explore the orthogonal halide-variation parameter space for Cs0.17FA0.83Pb(BrxI(1−x))3 perovskites. We demonstrate excellent charge-carrier mobilities (11–40 cm2 V−1 s−1) and diffusion lengths (0.8–4.4 μm) under solar conditions across the full iodide–bromide tuning range. Therefore, the addition of caesium yields a more photo-stable perovskite system whose absorption onsets can be tuned for bandgap-optimized tandem solar cells.

Hydroxamate anchors for water-stable attachment to TiO2 nanoparticles

Surface functionalization of nanoparticles is of broad interest, such as for dye attachment in dye-sensitized solar cells (DSSCs) and photocatalysis. Visible-light photoexcitation of the dye gives interfacial electron transfer (IET) into the conduction band of a semiconductor host. In a Gr€atzel cell, TiO2 is functionalized with Ru polypyridyl complexes that attach via carboxylate substituents that permit ultrafast IET but are unstable in aqueous conditions. We now report on hydroxamate anchors for robust TiO2 functionalization even in aqueous conditions. Hydroxamate ligands bind tightly to transition metals, even in water. For example, bacterial siderophores that contain hydroxamates can dissolve Fe(III) from the oxide. Recent studies have reported binding of hydroxamic acids to TiO2. 8 Here, we investigate their potential as robust anchors for functionalization of TiO2 thinfilms commonly used in solar energy conversion and photocatalysis. We synthesize and deposit a hydroxamate-functionalized terpyridine and demonstrate visible-light sensitization of TiO2 and activation of Mn adsorbates by ultrafast IET by using spectroscopy and molecular modeling. The synthesis (Scheme 1) builds on prior methods and proceeds in two steps in good yield. The methyl ester (1) reacts with O-Bn hydroxylamine (BnONH2) in the presence of LiHMDS to give the corresponding ester. The ester is then deprotected with H2 and Pd/C to give the product 2. Degussa P25 TiO2 nanoparticles (NPs) were sensitized with a solution of 2 in dry EtOH using known techniques. The resulting sensitized nanoparticles were characterized using UV-visible and FTIR spectroscopy (see Fig. S1 and S2†). The spectroscopic data are consistent with 2 anchoring to TiO2 via the hydroxamate. Upon binding, the disappearance of a C]O stretch at 1635 cm 1 present in the IR of unbound 2 is consistent with a O–CR]N–O unit

Water-stable, hydroxamate anchors for functionalization of TiO2 surfaces with ultrafast interfacial electron transfer

A novel class of derivatized hydroxamic acid linkages for robust sensitization of TiO2 nanoparticles (NPs) under various aqueous conditions is described. The stability of linkages bound to metal oxides under various conditions is important in developing photocatalytic cells which incorporate transition metal complexes for solar energy conversion. In order to compare the standard carboxylate anchor to hydroxamates, two organic dyes differing only in anchoring groups were synthesized and attached to TiO2 NPs. At acidic, basic, and close to neutral pH, hydroxamic acid linkages resist detachment compared to the labile carboxylic acids. THz spectroscopy was used to compare ultrafast interfacial electron transfer (IET) into the conduction band of TiO2 for both linkages and found similar IET characteristics. Observable electron injection and stronger binding suggest that hydroxamates are a suitable class of anchors for designing water stable molecules for functionalizing TiO2.

Effect of Structural Phase Transition on Charge-Carrier Lifetimes and Defects in CH3NH3SnI3 Perovskite

Methylammonium tin triiodide (MASnI3) has been successfully employed in lead-free perovskite solar cells, but overall power-conversion efficiencies are still significantly lower than for lead-based perovskites. Here we present photoluminescence (PL) spectra and time-resolved PL from 8 to 295 K and find a marked improvement in carrier lifetime and a substantial reduction in PL line width below ∼110 K, indicating that the cause of the hindered performance is activated at the orthorhombic to tetragonal phase transition. Our measurements therefore suggest that targeted structural change may be capable of tailoring the relative energy level alignment of defects (e.g., tin vacancies) to reduce the background dopant density and improve charge extraction. In addition, we observe for the first time an above-gap emission feature that may arise from higher-lying interband transitions, raising the prospect of excess energy harvesting.

Formation Dynamics of CH3NH3PbI3 Perovskite Following Two-Step Layer Deposition

Hybrid metal-halide perovskites have emerged as a leading class of semiconductors for optoelectronic devices because of their desirable material properties and versatile fabrication methods. However, little is known about the chemical transformations that occur in the initial stages of perovskite crystal formation. Here we follow the real-time formation dynamics of MAPbI3 from a bilayer of lead iodide (PbI2) and methylammonium iodide (MAI) deposited through a two-step thermal evaporation process. By lowering the substrate temperature during deposition, we are able to initially inhibit intermixing of the two layers. We subsequently use infrared and visible light transmission, X-ray diffraction, and photoluminescence lifetime measurements to reveal the room-temperature transformations that occur in vacuum and ambient air, as MAI diffuses into the PbI2 lattice to form MAPbI3. In vacuum, the transformation to MAPbI3 is incomplete as unreacted MAI is retained in the film. However, exposure to moist air allows for conversion of the unreacted MAI to MAPbI3, demonstrating that moisture is essential in making MAI more mobile and thus aiding perovskite crystallization. These dynamic processes are reflected in the observed charge-carrier lifetimes, which strongly fluctuate during periods of large ion migration but steadily increase with improving crystallinity.

Interfacial electron transfer in photoanodes based on phosphorus(V) porphyrin sensitizers co-deposited on SnO2 with the Ir(III)Cp* water oxidation precatalyst

We introduce phosphorus(V) porphyrins (PPors) as sensitizers of high-potential photoanodes with potentials in the 1.62–1.65 V (vs. NHE) range when codeposited with Ir(III)Cp* on SnO2. The ability of PPors to advance the oxidation state of the Ir(III)Cp* to Ir(IV)Cp*, as required for catalytic water oxidation, is demonstrated by combining electron paramagnetic resonance (EPR), steady-state fluorescence and time-resolved terahertz spectroscopy (TRTS) measurements, in conjunction with quantum dynamics simulations based on DFT structural models. Contrary to most other types of porphyrins previously analyzed in solar cells, our PPors bind to metal-oxide surfaces through axial coordination, a binding mode that makes them less prone to aggregation. The comparison of covalent binding via anchoring groups, such as m-hydroxidebenzoate (−OPh–COO−) and 3-(3-phenoxy)-acetylacetonate (−OPh–AcAc) as well as by direct deposition upon exchange of a chloride (Cl−) ligand provides insight on the effect of the anchoring group on forward and reverse light-induced interfacial electron transfer (IET). TRTS and quantum dynamics simulations reveal efficient photoinduced electron injection, from the PPor to the conduction band of SnO2, with faster and more efficient IET from directly bound PPor than from anchor-bound PPors. The photocurrents of solar cells, however, are higher for PPor–OPh–COO− and PPor–OPh–AcAc than for the directly bound PPor–O− for which charge recombination is faster. The high-potentials and the ability to induce redox state transitions of Ir(III)Cp* suggest that PPor/SnO2 assemblies are promising photoanode components for direct solar water-oxidation devices.