The long‐term success of photosynthetic organisms has resulted in their global superabundance, which is sustained by their widespread, continual mass‐production of the integral proteins that photocatalyze the chemical processes of natural photosynthesis. Here, a fast, general method to assemble multilayer films composed of one such photocatalytic protein complex, Photosystem I (PSI), onto a variety of substrates is reported. The resulting films, akin to the stacked thylakoid structures of leaves, consist of a protein matrix that is permeable to electrochemical mediators and contain a high concentration of photoelectrochemically active redox centers. These multilayer assemblies vastly outperform previously reported monolayer films of PSI in terms of photocurrent production when incorporated into an electrochemical system, and it is shown that these photocatalytic properties increase with the film thickness. These results demonstrate how the assembly of micron‐thick coatings of PSI on non‐biological substrates yields a biohybrid ensemble that manifests the photocatalytic activity of the film’s individual protein constituents, and represent significant progress toward affordable, biologically‐inspired renewable energy conversion platforms.

This work details the phase behavior of a pseudoternary polymer blend system containing poly(ethylene oxide) (PEO) and polystyrene (PS) homopolymers, a PS−PEO block copolymer, and lithium bis(trifluoromethane)sulfonamide (LiTFSI). The phase behavior of the system is described along the volumetrically symmetric isopleth at a fixed LiTFSI concentration relative to the PEO component. The addition of LiTFSI dramatically increases the segregation strength of the blend, causing the otherwise globally disordered blends to exhibit a variety of microstructured morphologies typically found in salt-free ternary polymer blends, such as lamellae, a hexagonal phase, and a bicontinuous microemulsion. The breadth of morphologies and segregation strengths that can be accessed in this system by simply tuning blend composition establishes a new framework for the design of future ternary blend systems and, more broadly, polymeric materials where microstructured, wellsegregated domains with tunable ion transport properties are desirable.

Polymer electrolytes are alternatives to liquid electrolytes traditionally used in electrochemical devices such as lithium-ion batteries and fuel cells. In particular, block polymer electrolytes are promising candidates because they self-assemble into well-defined microstructures, in which orthogonal properties can be integrated into a single material (e.g., high modulus in domain A, fast ion transport in domain B). However, the performance of block polymer electrolytes often falls short, due to the lack of long-range continuity of both domains and relatively low strength. We recently reported a simple, one-pot synthetic strategy to prepare polymer electrolytes with the highest reported combination of modulus and ionic conductivity, attributes enabled by a co-continuous, cross-linked network morphology. In this work we aim to understand the mechanism by which this nanoscale morphology is formed by performing a series of in situ, time-resolved experimentssmall-angle X-ray scattering, conductivity, rheology, and reaction kineticsto monitor the electrolyte as it transitions from a macroscopically homogeneous liquid to a microphase-separated solid. The results suggest that the chain connectivity of the diblock gives rise to isotropic concentration fluctuations that increase in amplitude and coherence such that the network morphology is ultimately produced. The kinetic trapping of this network morphology by chemical cross-linking prior to the ordering transition is shown to be critically important to the resulting advantageous bulk electrolyte properties.

We have established the existence of a line of congruent first-order lamellar-to-disorder (LAM–DIS) transitions when appropriate amounts of poly­(cyclohexyl­ethylene) (C) and poly­(ethylene) (E) homopolymers are mixed with a corresponding compositionally symmetric CE diblock copolymer. The line of congruent transitions, or the congruent isopleth, terminates at the bicontinuous microemulsion (BμE) channel, and its trajectory appears to be influenced by the critical composition of the C/E binary homopolymer blend. Blends satisfying congruency undergo a direct LAM–DIS transition without passing through a two-phase region. We present complementary optical transmission, small-angle X-ray scattering (SAXS), transmission electron microscopy (TEM), and dynamic mechanical spectroscopy (DMS) results that establish the phase behavior at constant copolymer volume fraction and varying C/E homopolymer volume ratios. Adjacent to the congruent composition at constant copolymer volume fraction, the lamellar and disordered phases are separated by two-phase coexistence windows, which converge, along with the line of congruent transitions, at an overall composition in the phase prism coincident with the BμE channel. Hexagonal and cubic (double gyroid) phases occur at higher diblock copolymer concentrations for asymmetric amounts of C and E homopolymers. These results establish a quantitative method for identifying the detailed phase behavior of ternary diblock copolymer–homopolymer blends, especially in the vicinity of the BμE.

We examine the relationship between structure and ionic conductivity in salt-containing ternary polymer blends that exhibit various microstructured morphologies, including lamellae, a hexagonal phase, and a bicontinuous microemulsion, as well as the disordered phase. These blends consist of polystyrene (PS, M n ≈ 600 g/mol) and poly(ethylene oxide) (PEO, M n ≈ 400 g/ mol) homopolymers, a nearly symmetric PS−PEO block copolymer (M n ≈ 4700 g/ mol), and lithium bis(trifluoromethane)sulfonamide (LiTFSI). These pseudoternary blends exhibit phase behavior that parallels that of well-studied ternary polymer blends consisting of A and B homopolymers compatibilized by an AB diblock copolymer. The utility of this framework is that all blends have nominally the same number of ethylene oxide, styrene, Li + , and TFSI − units, yet can exhibit a variety of microstructures depending on the relative ratio of the homopolymers to the block copolymer. For the systems studied, the ratio r = [Li + ]/[EO] is maintained at 0.06, and the volume fraction of PS homopolymer is kept equal to that of PEO homopolymer plus salt. The total volume fraction of homopolymer is varied from 0 to 0.70. When heated through the order−disorder transition, all blends exhibit an abrupt increase in conductivity. However, analysis of small-angle X-ray scattering data indicates significant structure even in the disordered state for several blend compositions. By comparing the nature and structure of the disordered states with their corresponding ordered states, we find that this increase in conductivity through the order−disorder transition is most likely due to the elimination of grain boundaries. In either disordered or ordered states, the conductivity decreases as the total amount of homopolymer is increased, an unanticipated observation. This trend with increasing homopolymer loading is hypothesized to result from an increased density of "dead ends" in the conducting channel due to poor continuity across grain boundaries in the ordered state and the formation of concave interfaces in the disordered state. The results demonstrate that disordered, microphase-separated morphologies provide better transport properties than compositionally equivalent polycrystalline systems with long-range order, an important criterion when optimizing the design of polymer electrolytes.