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At least 883 records · Page 49

Materials Data on RhN7ClO6 by Materials Project

RhNCl(N2)2(NO3)2 crystallizes in the tetragonal I4 space group. The structure is zero-dimensional and consists of eight ammonia molecules, four nitric acid molecules, and two RhNCl clusters. In each RhNCl cluster, Rh4+ is bonded in a distorted single-bond geometry to one N+1.29+ and one Cl1- atom. The Rh–N bond length is 1.70 Å. The Rh–Cl bond length is 2.57 Å. N+1.29+ is bonded in a single-bond geometry to one Rh4+ atom. Cl1- is bonded in a distorted single-bond geometry to one Rh4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Sn4As3 by Materials Project

Sn4As3 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of four 7440-31-5 molecules and two Sn2As3 clusters. In each Sn2As3 cluster, Sn+2.25+ is bonded in a single-bond geometry to one As3- atom. The Sn–As bond length is 2.64 Å. There are two inequivalent As3- sites. In the first As3- site, As3- is bonded in a linear geometry to two equivalent As3- atoms. Both As–As bond lengths are 2.30 Å. In the second As3- site, As3- is bonded in a linear geometry to one Sn+2.25+ and one As3- atom.

36 MATERIALS SCIENCE↗

Materials Data on RhN7ClO6 by Materials Project

RhNCl(N2)2(NO3)2 crystallizes in the tetragonal I4 space group. The structure is zero-dimensional and consists of eight ammonia molecules, four nitric acid molecules, and two RhNCl clusters. In each RhNCl cluster, Rh4+ is bonded in a distorted single-bond geometry to one N+1.29+ and one Cl1- atom. The Rh–N bond length is 1.72 Å. The Rh–Cl bond length is 2.62 Å. N+1.29+ is bonded in a single-bond geometry to one Rh4+ atom. Cl1- is bonded in a single-bond geometry to one Rh4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Fe2H3F2 by Materials Project

Fe2HF2H2 is Tenorite-like structured and crystallizes in the tetragonal P4/n space group. The structure is zero-dimensional and consists of eight hydrogen molecules and four Fe2HF2 clusters. In each Fe2HF2 cluster, Fe+2.50+ is bonded in a single-bond geometry to one F1- atom. The Fe–F bond length is 2.02 Å. H1- is bonded in a linear geometry to two equivalent F1- atoms. Both H–F bond lengths are 1.14 Å. F1- is bonded in a linear geometry to one Fe+2.50+ and one H1- atom.

36 MATERIALS SCIENCE↗

Materials Data on KOsBr4NO2 by Materials Project

KOsNO2(Br)4 is Cubane-like structured and crystallizes in the orthorhombic Cmc2_1 space group. The structure is zero-dimensional and consists of sixteen hydrobromic acid molecules and four KOsNO2 clusters. In each KOsNO2 cluster, K1+ is bonded in a distorted single-bond geometry to one O2- atom. The K–O bond length is 2.84 Å. Os4+ is bonded in a linear geometry to one N3- and one O2- atom. The Os–N bond length is 1.91 Å. The Os–O bond length is 1.75 Å. N3- is bonded in a linear geometry to one Os4+ and one O2- atom. The N–O bond length is 1.17 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one N3- atom. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one K1+ and one Os4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on IN5 by Materials Project

IN5 is lead oxide-like structured and crystallizes in the tetragonal P4/n space group. The structure is zero-dimensional and consists of two ammonia molecules and two IN4 clusters. In each IN4 cluster, N+0.20+ is bonded in a single-bond geometry to one I1- atom. The N–I bond length is 2.13 Å. I1- is bonded in a distorted square co-planar geometry to four equivalent N+0.20+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on CuC3N2O5 by Materials Project

NNCuCO(CO2)2 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of four carbon dioxide molecules and two NNCuCO clusters. In each NNCuCO cluster, Cu2+ is bonded in a distorted single-bond geometry to one O2- atom. The Cu–O bond length is 2.02 Å. C4+ is bonded in a 1-coordinate geometry to two N2- and one O2- atom. Both C–N bond lengths are 1.36 Å. The C–O bond length is 1.23 Å. There are two inequivalent N2- sites. In the first N2- site, N2- is bonded in a distorted single-bond geometry to one C4+ atom. In the second N2- site, N2- is bonded in a 1-coordinate geometry to one C4+ atom. O2- is bonded in a bent 120 degrees geometry to one Cu2+ and one C4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on OsN5Cl3 by Materials Project

(OsN)2N2(N2Cl)2(NCl2)2 crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four ammonia molecules, four azanylidyneosmium molecules, four dichloramine molecules, and four N2Cl clusters. In each N2Cl cluster, N+0.20+ is bonded in a single-bond geometry to one Cl1- atom. The N–Cl bond length is 1.70 Å. Cl1- is bonded in a linear geometry to two equivalent N+0.20+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on CoBr2N6O by Materials Project

CoN5NO(Br)2 crystallizes in the orthorhombic Cmcm space group. The structure is zero-dimensional and consists of eight hydrobromic acid molecules, four nitroxyl molecules, and four CoN5 clusters. In each CoN5 cluster, Co2+ is bonded in a distorted single-bond geometry to five N+1.67- atoms. There is one shorter (1.50 Å) and four longer (1.96 Å) Co–N bond length. There are three inequivalent N+1.67- sites. In the first N+1.67- site, N+1.67- is bonded in a distorted T-shaped geometry to one Co2+ and two equivalent N+1.67- atoms. Both N–N bond lengths are 1.42 Å. In the second N+1.67- site, N+1.67- is bonded in a distorted T-shaped geometry to one Co2+ and two equivalent N+1.67- atoms. In the third N+1.67- site, N+1.67- is bonded in a single-bond geometry to one Co2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Fe4AgP(XeF3)2 by Materials Project

(Xe)2Fe4AgF4PF2 crystallizes in the tetragonal I-4c2 space group. The structure is zero-dimensional and consists of four difluorophosphine molecules, eight xenon molecules, and four Fe4AgF4 clusters. In each Fe4AgF4 cluster, Fe is bonded in a distorted single-bond geometry to one F atom. The Fe–F bond length is 1.85 Å. Ag is bonded in a 4-coordinate geometry to four equivalent F atoms. All Ag–F bond lengths are 2.40 Å. F is bonded in an L-shaped geometry to one Fe and one Ag atom.

36 MATERIALS SCIENCE↗

Materials Data on CdCN2 by Materials Project

CdCN2 crystallizes in the trigonal R3m space group. The structure is zero-dimensional and consists of three hydrogen cyanide molecules and three CdN clusters. In each CdN cluster, Cd2+ is bonded in a distorted single-bond geometry to one N3- atom. The Cd–N bond length is 2.13 Å. N3- is bonded in a single-bond geometry to one Cd2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on LiB12PC by Materials Project

LiB6CP(B)6 crystallizes in the orthorhombic Ima2 space group. The structure is zero-dimensional and consists of twenty-four boron molecules and four LiB6CP clusters. In each LiB6CP cluster, Li1+ is bonded in a distorted single-bond geometry to one C4- and one P3- atom. The Li–C bond length is 2.74 Å. The Li–P bond length is 2.68 Å. There are four inequivalent B+0.50+ sites. In the first B+0.50+ site, B+0.50+ is bonded in a single-bond geometry to one C4- atom. The B–C bond length is 1.67 Å. In the second B+0.50+ site, B+0.50+ is bonded in a single-bond geometry to one P3- atom. The B–P bond length is 1.91 Å. In the third B+0.50+ site, B+0.50+ is bonded in a single-bond geometry to one C4- atom. The B–C bond length is 1.66 Å. In the fourth B+0.50+ site, B+0.50+ is bonded in a single-bond geometry to one P3- atom. The B–P bond length is 1.91 Å. C4- is bonded in a tetrahedral geometry to one Li1+, three B+0.50+, and one P3- atom. The C–P bond length is 1.87 Å. P3- is bonded in a 5-coordinate geometry to one Li1+, three B+0.50+, and one C4- atom.

36 MATERIALS SCIENCE↗

Phase Behavior and Ionic Conductivity of Blended, Ion-Condensed Electrolytes with Ordered Morphologies

In this study, the amphiphilic salt lithium trifluoromethanesulfonylimide octadecane (C18LiTFSI) was used as a basis to investigate the effects of anion density and cation coordination sites within blended electrolytes with strong ionic aggregation. C18LiTFSI was previously reported as a single-component, ion-condensed electrolyte with a wide layered liquid crystalline phase regime. Three additive molecules with varyingly sized polar sulfonyl groups attached to an octodecane-tail were synthesized and mixed with C18LiTFSI. The thermal properties, morphology, and ionic conductivity of the blended electrolytes were characterized. It was found that the blended electrolytes exhibited layered liquid crystalline morphology over a narrower temperature range than the pure salt, and the ionic conductivity of the blended liquid crystalline electrolytes were generally lower than that of the pure salt. Surprising, the additives were found to have the greatest effect on the bulk ionic conductivity of the semicrystalline phase of the electrolytes. Addition of minor fractions of methylsulfonyloctadecane to C18LiTFSI resulted in increases in conductivity of over two orders of magnitude at room temperature, while addition of ethylsulfonyloctadecane or isopropylsulfonyloctadecane with the larger head group resulted in decreased ionic conductivity over the entire composition space and temperature range investigated.

Collins, Hannah (ORCID:0000000338858136)↗

Dynamics of molecular associates in methanol/water mixtures

The dynamics of molecular associates in a methanol/water mixture was investigated using quasielastic neutron scattering. By measuring the signal from four methanol/water samples differing only by their isotopic composition, the relative motion of the water to methanol molecules, i.e. their mutual dynamics, was determined at the nanoscale. The thus obtained nanoscopic mutual diffusion coefficient signals a significantly slower process than the single particle diffusion of either methanol or water in the system as well as their macroscopic mutual diffusion. The data do not provide any indication of microsegregation in this preeminent alcohol/water mixture; however, they do indicate the existence of long lived but dynamic molecular associates of water and methanol molecules. Our analysis of the structural relaxation shows that the lifetime of molecular association through hydrogen bonding determines the fact that viscosity of the mixtures at intermediate concentrations is higher than that of both pure components.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Disorderly Conduct of Benzamide IV: Crystallographic and Computational Analysis of High Entropy Polymorphs of Small Molecules

Benzamide, a simple derivative of benzoic acid and a common intermediate of pharmaceutical compounds, was reported to form two polymorphs in 1832, but the single crystal structure of the more stable form was not solved until 1959. Nearly 50 years later, the second form was characterized by powder diffraction, followed shortly thereafter by characterization of a third form, a polytype of the most thermodynamically stable Form I. These two new forms, Forms II and III, are metastable. Herein, we describe a fourth polymorph, Form IV, discovered by melt crystallization concurrently with its crystallization under confinement at small length scales (<10 nm), where it is stable indefinitely. Form III exists under confinement in larger pores, and melting point data for different pore sizes corroborate the existence of Form IV below 10 nm. Form IV is highly disordered, precluding indexing of powder diffraction data other than hk0 reflections. Nonetheless, a combination of powder X-ray diffraction and computational crystal structure prediction reveals that Form IV contains a 2D motif resembling that of Form II, but with longrange order in the third dimension masked by ubiquitous stacking faults. This approach relies on distilling a large number of candidate structures to a few possible disorder models based on benzamide tetrads that organize in 2D parquet-like tiles, with organization along the third dimension, that can be modeled with various stacking fault configurations having distinct intermolecular interactions and translations in the dimension orthogonal to the tiling planes. These observations reveal a bewildering crystallographic complexity for such a simple molecule. Nonetheless, the approach described herein demonstrates that challenging structures that may be abandoned prematurely because of poor crystallinity, twinning, or disorder can be solved.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Systematic characterization of human gut microbiome-secreted molecules by integrated multi-omics

The human gut microbiome produces a complex mixture of biomolecules that interact with human physiology and play essential roles in health and disease. Crosstalk between micro-organisms and host cells is enabled by different direct contacts, but also by the export of molecules through secretion systems and extracellular vesicles. The resulting molecular network, comprised of various biomolecular moieties, has so far eluded systematic study. Here we present a methodological framework, optimized for the extraction of the microbiome-derived, extracellular biomolecular complement, including nucleic acids, (poly)peptides, and metabolites, from flash-frozen stool samples of healthy human individuals. Our method allows simultaneous isolation of individual biomolecular fractions from the same original stool sample, followed by specialized omic analyses. The resulting multi-omics data enable coherent data integration for the systematic characterization of this molecular complex. Our results demonstrate the distinctiveness of the different extracellular biomolecular fractions, both in terms of their taxonomic and functional composition. This highlights the challenge of inferring the extracellular biomolecular complement of the gut microbiome based on single-omic data. The developed methodological framework provides the foundation for systematically investigating mechanistic links between microbiome-secreted molecules, including those that are typically vesicle-associated, and their impact on host physiology in health and disease.

59 BASIC BIOLOGICAL SCIENCES↗

Beyond single crystals: Imaging rubrene polymorphism across crystalline batches through lattice phonon Raman microscopy

Polymorphism is an issue troubling numerous scientific fields. A phenomenon where molecules can arrange in different orientations in a crystal lattice, polymorphism in the field of organic photovoltaic materials can dramatically change electronic properties of these materials. Rubrene is a benchmark photovoltaic material showing high carrier mobility in only one of its three polymorphs. To use rubrene in devices, it is important to quantify the polymorph distribution arising from a particular crystal growth method. However, current methods for characterizing polymorphism are either destructive or inefficient for batch scale characterization. Lattice phonon Raman spectroscopy has the ability to distinguish between polymorphs based on low frequency intermolecular vibrations. Here, we present here the addition of microscopy to lattice phonon Raman spectroscopy, which allows us to not only characterize polymorphs efficiently and nondestructively through Raman spectroscopy but also concurrently gain information on the size and morphology of the polymorphs. We provide examples for how this technique can be used to perform large, batch scale polymorph characterization for crystals grown from solution and physical vapor transport.We end with a case study showing how Raman microscopy can be used to efficiently optimize a green crystal growth method, selecting for large orthorhombic crystals desired for rubrene electronic device applications.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

One Collision—Two Substituents: Gas–Phase Preparation of Xylenes under Single–Collision Conditions

The fundamental reaction pathways to the simplest dialkylsubstituted aromatics—xylenes (C 6 H 4 (CH 3 ) 2 )—in high-temperature combustion flames and in low-temperature extraterrestrial environments are still unknown, but critical to understand the chemistry and molecular mass growth processes in these extreme environments. Exploiting crossed molecular beam experiments augmented by state-of-the-art electronic structure and statistical calculations, this study uncovers a previously elusive, facile gas-phase synthesis of xylenes through an isomer-selective reaction of 1-propynyl (methylethynyl, CH 3 CC) with 2-methyl-1,3-butadiene (isoprene, C 5 H 8 ). The reaction dynamics are driven by a barrierless addition of the radical to the diene moiety of 2-methyl-1,3-butadiene followed by extensive isomerization (hydrogen shifts, cyclization) prior to unimolecular decomposition accompanied by aromatization via atomic hydrogen loss. This overall exoergic reaction affords a preparation of xylenes not only in high-temperature environments such as in combustion flames and around circumstellar envelopes of carbon-rich Asymptotic Giant Branch (AGB) stars, but also in low-temperature cold molecular clouds (10 K) and in hydrocarbon-rich atmospheres of planets and their moons such as Triton and Titan. Furthermore, our study established a hitherto unknown gas-phase route to xylenes and potentially more complex, disubstituted benzenes via a single collision event highlighting the significance of an alkyl-substituted ethynyl-mediated preparation of aromatic molecules in our Universe.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗