Center for Functional Nanomaterials

High-performance electrocatalytic CO₂ reduction to CO using Ni single-atom catalyst in an anion membrane electrode assembly.

Platinum group metal (PGM)-free catalysts for oxygen reduction reaction are essential for affordable fuel cells.

Abstract Metasurfaces offer a unique platform to precisely control optical wavefronts and enable the realization of flat lenses, or metalenses, which have the potential to substantially reduce the size and complexity of imaging systems and to realize new imaging modalities. However, it is a major challenge to create achromatic metalenses that produce a single focal length over a broad wavelength range because of the difficulty in simultaneously engineering phase profiles at distinct wavelengths on a single metasurface. For practical applications, there is a further challenge to create broadband achromatic metalenses that work in the transmission mode for incident light waves with any arbitrary polarization state. We developed a design methodology and created libraries of meta-units—building blocks of metasurfaces—with complex cross-sectional geometries to provide diverse phase dispersions (phase as a function of wavelength), which is crucial for creating broadband achromatic metalenses. We elucidated the fundamental limitations of achromatic metalens performance by deriving mathematical equations that govern the tradeoffs between phase dispersion and achievable lens parameters, including the lens diameter, numerical aperture (NA), and bandwidth of achromatic operation. We experimentally demonstrated several dielectric achromatic metalenses reaching the fundamental limitations. These metalenses work in the transmission mode with polarization-independent focusing efficiencies up to 50% and continuously provide a near-constant focal length over λ = 1200–1650 nm. These unprecedented properties represent a major advance compared to the state of the art and a major step toward practical implementations of metalenses.

Abstract A critical challenge in the commercialization of layer‐structured Ni‐rich materials is the fast capacity drop and voltage fading due to the interfacial instability and bulk structural degradation of the cathodes during battery operation. Herein, with the guidance of theoretical calculations of migration energy difference between La and Ti from the surface to the inside of LiNi 0.8 Co 0.1 Mn 0.1 O 2 , for the first time, Ti‐doped and La 4 NiLiO 8 ‐coated LiNi 0.8 Co 0.1 Mn 0.1 O 2 cathodes are rationally designed and prepared, via a simple and convenient dual‐modification strategy of synchronous synthesis and in situ modification. Impressively, the dual modified materials show remarkably improved electrochemical performance and largely suppressed voltage fading, even under exertive operational conditions at elevated temperature and under extended cutoff voltage. Further studies reveal that the nanoscale structural degradation on material surfaces and the appearance of intergranular cracks associated with the inconsistent evolution of structural degradation at the particle level can be effectively suppressed by the synergetic effect of the conductive La 4 NiLiO 8 coating layer and the strong TiO bond. The present work demonstrates that our strategy can simultaneously address the two issues with respect to interfacial instability and bulk structural degradation, and it represents a significant progress in the development of advanced cathode materials for high‐performance lithium‐ion batteries.

We have used the method of x-ray diffraction microscopy to image the complex-valued exit wave of an intact and unstained yeast cell. The images of the freeze-dried cell, obtained by using 750-eV x-rays from different angular orientations, portray several of the cell's major internal components to 30-nm resolution. The good agreement among the independently recovered structures demonstrates the accuracy of the imaging technique. To obtain the best possible reconstructions, we have implemented procedures for handling noisy and incomplete diffraction data, and we propose a method for determining the reconstructed resolution. This work represents a previously uncharacterized application of x-ray diffraction microscopy to a specimen of this complexity and provides confidence in the feasibility of the ultimate goal of imaging biological specimens at 10-nm resolution in three dimensions.

We prepared mono- and few-layer hexagonal boron nitride sheets by a chemical-solution-derived method starting from single-crystalline hexagonal boron nitride. Using high-resolution transmission electron microscopy and electron-energy-loss spectrometry, we characterized the microstructure, composition, and near-edge fine structure of the boron nitride sheets. We conclude that the fringe contrast in the edge and the moiré patterns are feasible criteria for determining the number of layers and their stacking orientation in the sheets. These criteria are also useful for other mono- and few-layer materials, such as graphene sheets.

precursors, respectively. This study shows how gas treatment synthesis such as ammoniation can transform carbide MXenes into 2D nitrides with higher electrical conductivities and metallic behavior, opening a new avenue in 2D materials synthesis.

We are inspired by the beauty and simplicity of self-organizing materials and the promise they hold for enabling continued improvements in semiconductor technology. Self assembly is the spontaneous arrangement of individual elements into regular patterns; under suitable conditions, certain materials self organize into useful nanometer-scale patterns of importance to high-performance microelectronics applications. Polymer self assembly is a nontraditional approach to patterning integrated circuit elements at dimensions and densities inaccessible to traditional lithography methods. We review here our efforts in IBM to develop and integrate self-assembly processes as high-resolution patterning alternatives and to demonstrate targeted applications in semiconductor device fabrication. We also provide a framework for understanding key requirements for the adoption of polymer self-assembly processes into semiconductor technology, as well as a discussion of the ultimate dimensional scalability of the technique.

We compare the low bias conductance of a series of alkanes terminated on their ends with dimethyl phosphines, methyl sulfides, and amines and find that junctions formed with dimethyl phosphine terminated alkanes have the highest conductance. We see unambiguous conductance signatures with these link groups, indicating that the binding is well-defined and electronically selective. This allows a detailed analysis of the single-molecule junction elongation properties which correlate well with calculations based on density functional theory.

A facile approach to the composition-controlled synthesis of monodisperse 2.2 nm AgPd alloy nanoparticles (NPs) is reported. The 2.2 nm AgPd NPs are highly active and durable catalysts for the dehydrogenation of formic acid. The study proves the unique approach in using alloying effects to enhance the catalytic activity of the NPs for hydrogen generation from formic acid (see picture). Formic acid (FA, HCOOH) is a common small organic acid with a melting point of 8.4 °C and boiling point of 100.8 °C. It can undergo a dehydrogenation reaction, HCOOH→H2+CO2, releasing H2 that will be important for hydrogen-based energy applications.1 Traditionally, the dehydrogenation of FA is catalyzed by metal complexes dissolved in an organic solvent and the catalysis is enhanced by adding an additive, such as sodium formate or amine adducts.2 To make more practical catalyst for the dehydrogenation reaction of FA, heterogeneous catalysts based on metal nanoparticles (NPs) have been developed. These catalysts are generally more stable but much less active than the homogeneous ones.3 Recently, bimetallic NP catalysts were found to be more active than their single component counterparts for the dehydrogenation of FA.4 For example, AgPd NPs supported on cerium oxide or AuPd NPs immobilized in a metal–organic framework showed an enhanced FA dehydrogenation catalysis with the initial turnover frequency (TOF) reaching 210 h−1 or 192 h−1 at 90 °C, respectively.5 However, the high rate of hydrogen generation observed from these heterogeneous catalysts could only be achieved when an additive was present and the reaction was maintained at temperatures close to 100 °C.6 Under these “harsh” conditions, HCOOH was also subject to an undesired dehydration reaction, HCOOH→H2O+CO.7 Interestingly, Ag/Pd core/shell NPs were found to be promising in catalyzing the dehydrogenation of FA in an aqueous FA solution at lower temperatures (up to 50 °C) without any additive.8 But their initial TOFs were in the range of 125–252 h−1 at temperatures between 25–50 °C. Considering the limitation seen from the previous syntheses in controlling the NP size and composition, we decided to re-evaluate the binary alloy NPs on their catalysis for the dehydrogenation of FA. Our very recent report showed that monodisperse 4 nm AuPd NPs were more active in catalyzing the dehydrogenation of FA in water at 50 °C without using any additive and their initial TOF reached 230 h−1.9 Encouraged by this result, we further improved our solution phase synthesis and produced monodisperse 2.2 nm AgPd NPs with the desired composition controls. We found that these monodisperse 2.2 nm AgPd alloy NPs were a highly active heterogeneous catalyst for the dehydrogenation of FA. In water without any additive, the Ag42Pd58 NPs showed the highest catalytic activity among all AgPd NPs tested with their initial TOF reaching 382 h−1 at 50 °C and apparent activation energy at 22±1 kJ mol−1. These are the best values ever reported by a heterogeneous catalyst for the dehydrogenation of FA in aqueous solution. It demonstrates the great potential of binary alloy NPs as a more practical catalyst for the dehydrogenation of FA and hydrogen generation. The 2.2 nm AgPd alloy NPs were synthesized by co-reduction of silver(I) acetate, Ag(Ac), and palladium(II) acetylacetonate, Pd(acac)2, in oleylamine (OAm), oleic acid (OA) and 1-octadecene (ODE) at 180 °C (Experimental Section). Here, OA served as a surfactant and OAm was added both as a co-surfactant and mild reducing agent. The composition of the AgPd NPs (Ag25Pd75, Ag42Pd58, Ag52Pd48, Ag60Pd40, and Ag80Pd20) were controlled by varying the molar ratio of Ag(Ac)/Pd(acac)2 and analyzed by inductively coupled plasma-atomic emission spectroscopy (ICP-AES; Table S1 in the Supporting Information). Transmission electron microscopy (TEM) images of the as-synthesized AgPd NPs show that they have a mean particle size of 2.2±0.1 nm (Figure 1 A and Figure S1A–D). Under similar reaction conditions, we also synthesized 2.2±0.1 nm Ag NPs (Figure S1E) and 4.5±0.2 nm Pd NPs (Figure S1F) by reducing only Ag(Ac) or Pd(acac)2. Different from the previous approaches to AgPd alloy NPs (larger than 7 nm) by a strong reducing agent,5a or a multi-step reaction scheme (diffusing Pd into Ag seeds at a high temperature),10 our one-step co-reduction of metal salts by OAm is highly efficient in producing monodisperse AgPd NPs at a particle size of only 2.2 nm. The use of an excess amount of OA was crucial for controlling the NP size. If OA was present in a small amount (e.g. 0.5 mL) or no OA was used, polydisperse AgPd NPs were obtained (Figure S2A&B). A) TEM image of the 2.2 nm Ag42Pd58 NPs. B) HRTEM image of the 2.2 nm Ag42Pd58 NPs. C) XRD patterns of the 2.2 nm Ag25Pd75, Ag42Pd58, Ag60Pd40 and Ag80Pd20 NPs (dashed line and solid line denote standard (111) peak positions of bulk Ag and Pd, respectively). D) TEM image of the carbon-supported 2.2 nm Ag42Pd58 NPs after treatment with acetic acid. A representative high-resolution (HR) TEM image of the 2.2 nm Ag42Pd58 NPs (Figure 1 B) shows the (111) lattice fringe distance of 0.23 nm, which is between the (111) lattice spacing of face-centered cubic (fcc) Ag (0.24 nm) and fcc Pd (0.22 nm) NPs. Figure 1 C is the X-ray diffraction (XRD) patterns of the 2.2 nm AgPd NPs. The AgPd NPs have a very weak peak intensity because of their small size. With the Ag amount increased in AgPd, the (111) peak shifts to a lower angle towards Ag(111) because of the increase of the lattice parameters, indicating that AgPd is formed as an alloy and not as a core/shell structure. Furthermore, AgPd NPs show almost no surface plasmon resonance (SPR) absorption in the UV/Vis spectra, whereas Ag NPs have a very strong SPR absorption at 425 nm (Figure S3). This SPR “quenching” caused by the alloying effect was also observed in other Ag- and Au-based alloy NPs.11 To study NP catalysis for the dehydrogenation of FA in water, we deposited Ag, Pd, or AgPd NPs on Ketjen carbon (C) and cleaned these C-NPs by acetic acid treatment and ethanol washing followed by drying under vacuum (Experimental Section). The representative TEM image (Figure 1 D) and the relevant ICP-AES analysis (Table S2) revealed that these C-AgPd NPs preserved their size, morphology, and composition after the cleaning process. The metal contents of the C-AgPd, C-Pd, and C-Ag catalysts were measured (by ICP-AES) to have 17 wt % AgPd, 19 wt % Pd, and 18 wt % Ag, respectively. The catalytic activity of the C NP catalysts in the dehydrogenation of FA was evaluated in a gas burette system. Figure 2 A shows the plots of volume of gas (CO2+H2) generated versus the reaction time during the dehydrogenation of the aqueous FA solution (10 mL, 1 M FA solution at 50 °C) catalyzed by different C-AgPd and C-Pd catalysts. We can see that most C-AgPd catalysts have a higher activity than the C-Pd NPs, except for C-Ag80Pd20. The C-Ag25Pd75, C-Ag42Pd58, and C-Ag52Pd48 catalysts have the initial TOF of 318, 382, and 228 h−1, respectively. They are even more active than the state-of-the-art AgPd alloy (TOF=210 h−1 at 92 °C) and Ag/Pd core/shell NPs (TOF=252 h−1 at 50 °C). Figure 2 B shows the plot of TOF versus the mole fraction of Ag for the C-AgPd catalyst at different compositions. The TOF increases with increasing Ag mole ratio up to 0.42 and then decreases. The observed “volcano”-type activity of the C-AgPd catalyst versus the Ag/Pd composition indicates that although neither Ag nor Pd is active for catalyzing the dehydrogenation reaction of FA, alloying Ag with Pd provides a necessary synergistic effect on the catalysis and Ag42Pd58 is the optimum catalyst for catalyzing the dehydrogenation of FA. This further supports that Ag and Pd form a uniform alloy structure in the synthesis. A) The plots of generated gas (CO2+H2) versus time during the dehydrogenation of an aqueous FA solution (10 mL of 1 M, 50 °C) in the presence of C-AgPd and C-Pd catalysts and B) TOF vs. mole fraction of Ag for the C-AgPd catalysts at different Ag and Pd compositions. Since dehydration route of FA (HCOOH→CO+H2O) is generally associated with the dehydrogenation at relatively high reaction temperatures (T>60 °C),3, 7 we also tested our reaction and characterized the evolving gas mixture with FT-IR and mass spectroscopy. We found no detectable amount of CO in the gas mixture generated from the C-Ag42Pd58 catalyzed the dehydrogenation of FA (Figure S4). After reacting the gas mixture with the aqueous NaOH solution, the volumes of CO2 and H2 were estimated and the gas mixture was found to consist of equal molar amounts of CO2 and H2 (Figure S5), proving that the AgPd catalyst promotes complete dehydrogenation of FA into CO2 and H2. The drastic dehydrogenation activity enhancement of these 2.2 nm AgPd NPs is likely caused by their small size and the synergistic effect between Ag and Pd in the alloy structure that inhibits the adsorption of CO on Pd. This is consistent with what was observed on the CeO2-supported MPd (M=Ag, Au) systems.5a However, our system is also different from the CeO2-supported MPd catalyst in which the enhanced activity was believed to originate from the NP-support interactions,5a and ours seem to show a more drastic alloy effect with their catalysis optimized when the AgPd catalysts has the composition Ag42Pd58. The concentration of the NP catalyst, FA concentration, and temperature effects were studied to obtain more kinetic information about the dehydrogenation of FA. In the first set of experiments, the dehydrogenation reaction was performed at different catalyst concentrations in the range of 10–40 mg (1.6–6.4 mM) Ag42Pd58 by keeping the FA concentration at 1.0 M and the temperature at 50 °C. The volume of generated gas (CO2+H2) was plotted versus the reaction time during the dehydrogenation of FA at different catalyst concentrations (Figure S6A). The hydrogen generation rates for each catalyst concentration were calculated from the linear portion of each plot comprising a reaction duration of 20 minutes. Figure S6B shows the logarithmic plot of the hydrogen generation rate versus the AgPd concentration. The line with a slope of 0.88 in Figure S6B indicates that the reaction is close to first-order with respect to the catalyst concentration. To study FA concentration effect on the gas generation rate, we kept the C-Ag42Pd58 concentration at 3.2 mM Ag42Pd58 and the temperature at 50 °C. Figure 3 A shows the volume of generated gas (CO2+H2) versus time at different FA concentrations. The initial TOFs (h−1) were calculated and presented in Figure 3 B. From Figure 3 A&B, we can see a volcano-shaped relationship between TOF and HCOOH concentration. The gas generation rate increases almost linearly with the FA concentration in the range of 0.125–1.0 M, but drops when the HCOOH concentration is higher than 1 M. This, plus the catalyst inactivity observed for the dehydrogenation of pure FA, reveals that a large amount of water plays an indispensable role in the catalytic dehydrogenation of FA. To measure the ease of the dehydrogenation reaction catalyzed by the AgPd alloy catalyst, we recorded the time-dependent H2 generation at different temperatures (25–50 °C) in the presence of C-Ag42Pd58 (3.2 mM AgPd) and FA (1 M), as shown in Figure 3 C. By converting the reactivity into TOF and by plotting the logarithmic TOF vs. 1/T, we obtained the Arrhenius plot (Figure 3 D). From the linear Arrhenius behavior, we calculated the apparent activation energy (Eaapp) to be 22±1 kJ mol−1 for the C-Ag42Pd58 catalyzed the dehydrogenation reaction of FA. This is the lowest value ever reported for the dehydrogenation reaction of FA catalyzed by a heterogeneous catalyst. A) The volume of the generated gas (CO2+H2) versus time for the dehydrogenation of FA catalyzed by the C-Ag42Pd58 at different FA concentrations (0.125–2 M). B) Plot of initial TOF (h−1) versus the FA concentration. C) Volume of the generated gas (CO2+H2) versus time for the dehydrogenation of FA catalyzed by C-Ag42Pd58 at different different temperatures (25–50 °C). D) Arrhenius plot (ln(TOF) vs. 1/T). We further tested briefly the stability of the C-Ag42Pd58 catalyst by performing the dehydrogenation of FA in water at 50 °C and recovering the catalyst from the solution after the reaction completion for the next round of reaction. Our tests showed that the C-Ag42Pd58 catalyst preserved 90 % of its initial activity after the fourth run (Figure S7A). We analyzed the recovered catalyst by ICP-AES and TEM (Figure S7B). We found no obvious change in the Ag/Pd composition, catalyst loading on carbon, and NP morphology. These findings indicate that the C-Ag42Pd58 catalyst was stable under the current FA dehydrogenation condition and could be re-used for multiple rounds of the dehydrogenation reaction. Herein, we have demonstrated a facile approach to a composition-controlled synthesis of monodisperse 2.2 nm AgPd NPs. These 2.2 nm AgPd NPs are highly active and durable as catalysts for the dehydrogenation of FA and for hydrogen generation without the need of any additive. Under our evaluation condition (in water at 50 °C), the AgPd NPs show the composition-dependent catalysis and the Ag42Pd58 NPs have the highest activity with an initial TOF of 382 h−1 and an apparent activation energy of 22±1 kJ mol−1—the best catalytic performance ever reported among all heterogeneous catalysts tested for the dehydrogenation of FA in aqueous solution. This, combining with the fact that Pd and Ag NPs are much less active in catalyzing the dehydrogenation of FA, proves the unique approach in using alloying effects to enhance NP catalysis. With the desired control on the NP sizes, compositions, and shapes, NP catalysis for the dehydrogenation of FA can be further optimized and a new type of heterogeneous catalyst may be developed for hydrogen generation and for hydrogen-based energy device applications. Synthesis of AgPd NPs: Under a gentle nitrogen flow, 0.084 g of silver(I) acetate (Ag(Ac), 0.5 mmol) and 0.15 g of palladium(II) acetylacetonate (Pd(acac)2, 0.5 mmol) were magnetically stirred in 4.5 mL of oleic acid (OAc), 0.5 mL of oleylamine (OAm), and 10 mL of 1-octadecene (ODE). The mixture was heated to 60 °C to generate a homogeneous solution. Then the solution was heated to 180 °C at a rate of 3–5 °C minutes−1 and kept at this temperature for 20 minutes during which the transparent solution gradually turned into brown and finally dark-brown color. Once the reaction solution was cooled down to room temperature, the NPs were separated by adding isopropanol (50 mL) and centrifugation (9500 rpm, 8 minutes). To remove the organic impurities and precursor residues, the product was redispersed in 10 mL of hexane and then recollected by adding 40 mL of ethanol and centrifugation (9500 rpm, 8 minutes). This synthesis yielded Ag42Pd58NPs (yield: 95 %), which were dispersed in hexane for future use. Under the same reaction condition, 0.134 g of Ag(Ac) (0.8 mmol) and 0.06 g of Pd(acac)2 (0. 2 mmol) led to the formation of Ag80Pd20 NPs; 0. 126 g of Ag(Ac) (0.75 mmol) and 0.075 g of Pd(acac)2 (0. 25 mmol) generated Ag60Pd40 NPs; 0. 1 g of Ag(Ac) (0.6 mmol) and 0.12 g of Pd(acac)2 (0. 4 mmol) produced Ag52Pd48 NPs; 0. 042 g of Ag(Ac) (0.25 mmol) and 0.225 g of Pd(acac)2 (0. 75 mmol) yielded Ag25Pd75 NPs. Under similar conditions, 0.168 g of Ag(Ac) (1 mmol) in the absence of Pd(acac)2 yielded 2.2 nm Ag NPs. The synthesis of 4.5 nm Pd NPs was conducted according to a protocol published elsewhere.12 Preparation of C-NP catalysts: In 10 mL of hexane 50 mg of Ketjen carbon were suspended and sonicated for 15 minutes. Next, about 25 mg of NPs in hexane was added dropwise into the carbon support mixture under sonication. The resulted mixture was sonicated for 1 h to ensure NP adsorption onto the carbon support. The C-NPs were separated by centrifugation and washed with ethanol. Next, the C-NPs were suspended in 30 mL of acetic acid and the suspension was heated for 10 h at 70 °C. 30 mL of ethanol was added and the mixture was centrifuged at 8500 rpm for 6 minutes. This ethanol washing procedure was repeated three times. The C-NPs were recovered and dried under vacuum. Formic acid dehydrogenation: In 9.6 mL of water 20 mg of C-NP catalysts were dispersed by sonication and then 0.4 mL of formic acid was injected into the catalyst solution at 50 °C. The volume of the gas (CO2+H2) generated during the catalytic reaction was monitored by a gas burette system. As a service to our authors and readers, this journal provides supporting information supplied by the authors. Such materials are peer reviewed and may be re-organized for online delivery, but are not copy-edited or typeset. Technical support issues arising from supporting information (other than missing files) should be addressed to the authors. Please note: The publisher is not responsible for the content or functionality of any supporting information supplied by the authors. Any queries (other than missing content) should be directed to the corresponding author for the article.

We apply our theoretical formalism for singlet exciton fission, introduced in the previous paper [T. C. Berkelbach, M. S. Hybertsen, and D. R. Reichman, J. Chem. Phys. 138, 114102 (2013)] to molecular dimers of pentacene, a widely studied material that exhibits singlet fission in the crystal phase. We address a longstanding theoretical issue, namely whether singlet fission proceeds via two sequential electron transfer steps mediated by charge-transfer states or via a direct two-electron transfer process. We find evidence for a superexchange mediated mechanism, whereby the fission process proceeds through virtual charge-transfer states which may be very high in energy. In particular, this mechanism predicts efficient singlet fission on the sub-picosecond timescale, in reasonable agreement with experiment. We investigate the role played by molecular vibrations in mediating relaxation and decoherence, finding that different physically reasonable forms for the bath relaxation function give similar results. We also examine the competing direct coupling mechanism and find it to yield fission rates slower in comparison with the superexchange mechanism for the dimer. We discuss implications for crystalline pentacene, including the limitations of the dimer model.

A carbon support with favorable balance between graphitization and hierarchical porosity is promising to address carbon corrosion issue in cathode catalysts for proton exchange membrane fuel cells (PEMFCs).

Silicon waveguide asymmetric Y junction mode multiplexers and demultiplexers are demonstrated for applications in on-chip mode-division multiplexing (MDM). We measure demultiplexed crosstalk as low as -30 dB, <-9 dB over the C band, and insertion loss <1.5 dB for multimode links up to 1.2 mm in length. The frequency response of these devices is shown to depend upon Y junction angle and multimode interconnect length. Interference effects are shown to be advantageous for low-crosstalk MDM, even while using compact Y junctions designed to be outside the mode-sorting regime.

Nanoscale zinc oxide (ZnO) rods of diameters close to the Bohr-exciton radius ( approximately 2 nm) can be prepared from a simple acetate precursor, resulting in ligand-capped rods of ZnO, highly dispersible in nonpolar solvents. Zinc oxide, ZnO, is a wide band-gap semiconductor with applications in blue/ultraviolet (UV) optoelectronic devices and piezoelectric devices. We observe self-assembly into uniform stacks of nanorods aligned parallel to each other with respect to the long axis, and photoluminescence measurements provide evidence for one-dimensional quantum confinement.

Singlet fission, a spin-allowed energy transfer process generating two triplet excitons from one singlet exciton, has the potential to dramatically increase the efficiency of organic solar cells. However, the dynamical mechanism of this phenomenon is not fully understood and a complete, microscopic theory of singlet fission is lacking. In this work, we assemble the components of a comprehensive microscopic theory of singlet fission that connects excited state quantum chemistry calculations with finite-temperature quantum relaxation theory. We elaborate on the distinction between localized diabatic and delocalized exciton bases for the interpretation of singlet fission experiments in both the time and frequency domains. We discuss various approximations to the exact density matrix dynamics and propose Redfield theory as an ideal compromise between speed and accuracy for the detailed investigation of singlet fission in dimers, clusters, and crystals. Investigations of small model systems based on parameters typical of singlet fission demonstrate the numerical accuracy and practical utility of this approach.

Low-temperature direct ammonia fuel cells (DAFCs) can use carbon-neutral ammonia as a fuel, which has attracted increasing attention recently due to ammonia's low source-to-tank energy cost, easy transport and storage, and wide availability.

This study details a new derivative of the contorted HBCs that self-organizes into one-dimensional, single-crystalline fibers. X-ray diffraction, transmission electron microscopy, and electron diffraction studies show that they have an orthorhombic unit cell with dimensions of 5.8 nm x 4.5 nm x 0.45 nm. Each fiber is composed of a few thousands columns. A method is put forth that utilizes elastomer stamps to manipulate and position isolated fibers in organic field effect transistors.

This study develops a tunable 3D nanostructured conductive gel framework as both binder and conductive framework for lithium ion batteries. A 3D nanostructured gel framework with continuous electron pathways can provide hierarchical pores for ion transport and form uniform coatings on each active particle against aggregation. The hybrid gel electrodes based on a polypyrrole gel framework and Fe 3 O 4 nanoparticles as a model system in this study demonstrate the best rate performance, the highest achieved mass ratio of active materials, and the highest achieved specific capacities when considering total electrode mass, compared to current literature. This 3D nanostructured gel‐based framework represents a powerful platform for various electrochemically active materials to enable the next‐generation high‐energy batteries.

Charge transport properties of metal-molecule interfaces depend strongly on the character of molecule-electrode interactions. Although through-bond coupled systems have attracted the most attention, through-space coupling is important in molecular systems when, for example, through-bond coupling is suppressed due to quantum interference effects. To date, a probe that clearly distinguishes these two types of coupling has not yet been demonstrated. Here, we investigate the origin of flicker noise in single molecule junctions and demonstrate how the character of the molecule-electrode coupling influences the flicker noise behavior of single molecule junctions. Importantly, we find that flicker noise shows a power law dependence on conductance in all junctions studied with an exponent that can distinguish through-space and through-bond coupling. Our results provide a new and powerful tool for probing and understanding coupling at the metal-molecule interface.

We extend our previous work on singlet exciton fission in isolated dimers to the case of crystalline materials, focusing on pentacene as a canonical and concrete example. We discuss the proper interpretation of the character of low-lying excited states of relevance to singlet fission. In particular, we consider a variety of metrics for measuring charge-transfer character, conclusively demonstrating significant charge-transfer character in the low-lying excited states. The impact of this electronic structure on the subsequent singlet fission dynamics is assessed by performing real-time master-equation calculations involving hundreds of quantum states. We make direct comparisons with experimental absorption spectra and singlet fission rates, finding good quantitative agreement in both cases, and we discuss the mechanistic distinctions that exist between small isolated aggregates and bulk systems.