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Wide-Field High-Performance Geosynchronous Imaging

The NASA Mission to Planet Earth (MTPE) Program and the National Oceanographic and Atmospheric Administration (NOAA) are sponsoring the Advanced Geosynchronous Studies (AGS) to develop technologies and system concepts for Earth observation from geosynchronous orbit. This series of studies is intended to benefit both MTPE science and the NOAA GOES Program. Within the AGS program, advanced imager trade studies have investigated two candidate concepts for near-term advanced geosynchronous imagers. One concept uses a scan mirror to direct the line of sight from a 3-axis stabilized platform. Another eliminates the need for a scan mirror by using an agile spacecraft bus to scan the entire instrument. The purpose of this paper is to discuss the optical design trades and system issues encountered in evaluating the two scanning approaches.

Wood, H. John↗

Materials Data on CrAg(PS3)2 by Materials Project

CrAg(PS3)2 crystallizes in the monoclinic P2/c space group. The structure is two-dimensional and consists of one CrAg(PS3)2 sheet oriented in the (0, 0, 1) direction. Cr3+ is bonded to six S2- atoms to form CrS6 octahedra that share an edgeedge with one AgS6 octahedra and edges with two equivalent CrS6 octahedra. There are a spread of Cr–S bond distances ranging from 2.43–2.45 Å. Ag1+ is bonded to six S2- atoms to form distorted AgS6 octahedra that share an edgeedge with one CrS6 octahedra and edges with two equivalent AgS6 octahedra. There are a spread of Ag–S bond distances ranging from 2.74–2.88 Å. P4+ is bonded in a trigonal non-coplanar geometry to three S2- atoms. There are a spread of P–S bond distances ranging from 1.98–2.13 Å. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a trigonal non-coplanar geometry to two equivalent Cr3+ and one P4+ atom. In the second S2- site, S2- is bonded in a 3-coordinate geometry to one Cr3+, one Ag1+, and one P4+ atom. In the third S2- site, S2- is bonded in a 1-coordinate geometry to two equivalent Ag1+ and one P4+ atom.

36 MATERIALS SCIENCE↗

Polydopamine Surface Coating Synergizes the Antimicrobial Activity of Silver Nanoparticles

Metal nanoparticles, especially silver nanoparticles (AgNPs), have drawn increasing attention for antimicrobial applications. Most studies have emphasized on the correlations between the antibacterial potency of AgNPs and the kinetics of metallic to ionic Ag conversion, while other antimicrobial mechanisms have been underestimated. In this work, we focused on the surface effects of polydopamine (PDA) coating on the antimicrobial activity of AgNPs. A method of fast deposition of PDA was used to synthesize the PDA-AgNPs with controllable coating thickness ranging from 3 to 25 nm. The antimicrobial activities of the PDA-AgNPs were analyzed by fluorescence-based growth curve assays on Escherichia coli. The results indicated that the PDA-AgNPs exhibited significantly higher antibacterial activities than poly(vinylpyrrolidone)-passivated AgNPs (PVP-AgNPs) and PDA themselves. It was found that the PDA coating synergized with the AgNPs to prominently enhance the potency of the PDA-AgNPs against bacteria. Additionally, the analysis of X-ray photoelectron spectroscopy and Fourier transform infrared spectroscopy elucidated that the synergistic effects could be originated from the interaction/coordination between Ag and catechol group on the PDA coating. The synergistic effects led to increased generation of reactive oxygen species and the consequent bacterial damage. Overall, these findings demonstrated the importance of the surface effects on the antimicrobial properties of AgNPs. The underlying molecular mechanisms have shined light on the future development of more potent metal nanoparticle-based antimicrobial agents.

36 MATERIALS SCIENCE↗

Materials Data on Ag10Te4Br3 by Materials Project

Ag10Te4Br3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are seven inequivalent Ag1+ sites. In the first Ag1+ site, Ag1+ is bonded in a 1-coordinate geometry to three Te+1.75- and one Br1- atom. There are a spread of Ag–Te bond distances ranging from 2.83–3.17 Å. The Ag–Br bond length is 2.79 Å. In the second Ag1+ site, Ag1+ is bonded in a 2-coordinate geometry to eight Ag1+ and two equivalent Te+1.75- atoms. All Ag–Ag bond lengths are 2.97 Å. Both Ag–Te bond lengths are 2.80 Å. In the third Ag1+ site, Ag1+ is bonded in a 1-coordinate geometry to two Ag1+, two Te+1.75-, and one Br1- atom. The Ag–Ag bond length is 3.04 Å. There are one shorter (2.82 Å) and one longer (2.85 Å) Ag–Te bond lengths. The Ag–Br bond length is 2.89 Å. In the fourth Ag1+ site, Ag1+ is bonded in a 2-coordinate geometry to one Ag1+, two Te+1.75-, and two Br1- atoms. There are one shorter (2.87 Å) and one longer (2.94 Å) Ag–Te bond lengths. There are one shorter (2.74 Å) and one longer (2.85 Å) Ag–Br bond lengths. In the fifth Ag1+ site, Ag1+ is bonded in a distorted single-bond geometry to one Ag1+, three Te+1.75-, and one Br1- atom. The Ag–Ag bond length is 3.09 Å. There are one shorter (2.90 Å) and two longer (2.98 Å) Ag–Te bond lengths. The Ag–Br bond length is 2.74 Å. In the sixth Ag1+ site, Ag1+ is bonded in a distorted linear geometry to ten Ag1+ and two equivalent Te+1.75- atoms. All Ag–Ag bond lengths are 3.06 Å. Both Ag–Te bond lengths are 2.80 Å. In the seventh Ag1+ site, Ag1+ is bonded in a 1-coordinate geometry to one Ag1+, two Te+1.75-, and one Br1- atom. There are one shorter (2.81 Å) and one longer (2.87 Å) Ag–Te bond lengths. The Ag–Br bond length is 2.88 Å. There are four inequivalent Te+1.75- sites. In the first Te+1.75- site, Te+1.75- is bonded in a 6-coordinate geometry to six Ag1+ and one Te+1.75- atom. The Te–Te bond length is 3.59 Å. In the second Te+1.75- site, Te+1.75- is bonded in a 6-coordinate geometry to four Ag1+ and two Te+1.75- atoms. The Te–Te bond length is 2.87 Å. In the third Te+1.75- site, Te+1.75- is bonded in a 7-coordinate geometry to seven Ag1+ atoms. In the fourth Te+1.75- site, Te+1.75- is bonded in a 8-coordinate geometry to six Ag1+ atoms. There are three inequivalent Br1- sites. In the first Br1- site, Br1- is bonded in a 4-coordinate geometry to four Ag1+ atoms. In the second Br1- site, Br1- is bonded in a 3-coordinate geometry to three Ag1+ atoms. In the third Br1- site, Br1- is bonded in a 4-coordinate geometry to four Ag1+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ag2SeO3 by Materials Project

Ag2SeO3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Ag1+ sites. In the first Ag1+ site, Ag1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ag–O bond distances ranging from 2.39–3.06 Å. In the second Ag1+ site, Ag1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Ag–O bond distances ranging from 2.33–2.80 Å. Se4+ is bonded in a distorted trigonal non-coplanar geometry to three O2- atoms. There is two shorter (1.74 Å) and one longer (1.75 Å) Se–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to four Ag1+ and one Se4+ atom. In the second O2- site, O2- is bonded in a 5-coordinate geometry to four Ag1+ and one Se4+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to three Ag1+ and one Se4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Mn3V3(AgO6)2 by Materials Project

V3Mn3(AgO6)2 is Esseneite-like structured and crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are two inequivalent V5+ sites. In the first V5+ site, V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with six MnO6 octahedra. The corner-sharing octahedra tilt angles range from 55–59°. There is two shorter (1.74 Å) and two longer (1.78 Å) V–O bond length. In the second V5+ site, V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with six MnO6 octahedra. The corner-sharing octahedra tilt angles range from 40–62°. There are a spread of V–O bond distances ranging from 1.72–1.77 Å. There are two inequivalent Mn+2.33+ sites. In the first Mn+2.33+ site, Mn+2.33+ is bonded to six O2- atoms to form distorted MnO6 octahedra that share corners with six VO4 tetrahedra and edges with two equivalent MnO6 octahedra. There are a spread of Mn–O bond distances ranging from 2.17–2.23 Å. In the second Mn+2.33+ site, Mn+2.33+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six VO4 tetrahedra and edges with two MnO6 octahedra. There are a spread of Mn–O bond distances ranging from 2.04–2.29 Å. There are two inequivalent Ag1+ sites. In the first Ag1+ site, Ag1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ag–O bond distances ranging from 2.49–3.05 Å. In the second Ag1+ site, Ag1+ is bonded in a distorted rectangular see-saw-like geometry to four equivalent O2- atoms. There are two shorter (2.46 Å) and two longer (2.49 Å) Ag–O bond lengths. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one V5+, one Mn+2.33+, and two equivalent Ag1+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one V5+ and two Mn+2.33+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one V5+ and two equivalent Mn+2.33+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one V5+, one Mn+2.33+, and two equivalent Ag1+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to one V5+ and two Mn+2.33+ atoms. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to one V5+, one Mn+2.33+, and two equivalent Ag1+ atoms.

36 MATERIALS SCIENCE↗

Stable abnormal N-heterocyclic carbenes and their applications

Although N-heterocyclic carbenes (NHCs) have been known as ligands for organometallic complexes since the 1960s, these carbenes did not attract considerable attention until Arduengo et al. reported the isolation of a metal-free imidazol-2-ylidene in 1991. In 2001 Crabtree et al. reported a few complexes featuring an NHC isomer, namely an imidazol-5-ylidene, also termed abnormal NHC (aNHCs). In 2009, it was shown that providing to protect the C-2 position of an imidazolium salt, the deprotonation occurred at the C-5 position, affording imidazol-5-ylidenes that could be isolated. Over the last ten years, stable aNHCs have been used for designing a range of catalysts employing Pd(II), Cu(I), Ni(II), Fe(0), Zn(II), Ag(I), and Au(I/III) metal based precursors. These catalysts were utilized for different organic transformations such as the Suzuki–Miyaura cross-coupling reaction, C–H bond activation, dehydrogenative coupling, Huisgen 1,3-dipolar cycloaddition (click reaction), hydroheteroarylation, hydrosilylation reaction and migratory insertion of carbenes. Main-group metal complexes were also synthesized, including K(I), Al(III), Zn(II), Sn(II), Ge(II), and Si(II/IV). Among them, K(I), Al(III), and Zn(II) complexes were used for the polymerization of caprolactone and rac-lactide at room temperature. In addition, based on the superior nucleophilicity of aNHCs, relative to that of their nNHCs isomers, they were used for small molecules activation, such as carbon dioxide (CO 2 ), nitrous oxide (N 2 O), tetrahydrofuran (THF), tetrahydrothiophene and 9-borabicyclo[3.3.1]nonane (9BBN). aNHCs have also been shown to be efficient metal-free catalysts for ring opening polymerization of different cyclic esters at room temperature; they are among the most active metal-free catalysts for ε-caprolactone polymerization. Recently, aNHCs successfully accomplished the metal-free catalytic formylation of amides using CO 2 and the catalytic reduction of carbon dioxide, including atmospheric CO 2 , into methanol, under ambient conditions. Although other transition metal complexes featuring aNHCs as ligand have been prepared and used in catalysis, this review article summarize the results obtained with the isolated aNHCs.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Plasmonics in argentene

Merging concepts from the fields of ab initio materials science and nanophotonics, there is now an opportunity to engineer new photonic materials whose optical, transport, and scattering properties are tailored to attain thermodynamic and quantum limits. Here we present first-principles calculations predicting that Argentene, a single-crystalline hexagonal close-packed monolayer of Ag, can dramatically surpass the optical properties and electrical conductivity of conventional plasmonic materials. In the low-frequency limit, we show that the scattering rate and resistivity reduce by a factor of 3 compared to the bulk three-dimensional metal. Most importantly, the low scattering rate extends to optical frequencies in sharp contrast to, e.g., graphene, whose scattering rate increase drastically in the near-infrared range due to optical-phonon scattering. Combined with an intrinsically high carrier density, this facilitates highly confined surface plasmons extending to visible frequencies. We evaluate Argentene across three distinct figures of merit, in each outperforming the state-of-the-art, making it a valuable addition to the two-dimensional heterostructure toolkit for quantum optoelectronics.

36 MATERIALS SCIENCE↗

Materials Data on SiAg2S3 by Materials Project

Ag2SiS3 is Chalcostibite-like structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Ag1+ sites. In the first Ag1+ site, Ag1+ is bonded in a 4-coordinate geometry to four S2- atoms. There are a spread of Ag–S bond distances ranging from 2.59–2.80 Å. In the second Ag1+ site, Ag1+ is bonded to four S2- atoms to form distorted AgS4 trigonal pyramids that share corners with five equivalent SiS4 tetrahedra and corners with two equivalent AgS4 trigonal pyramids. There are a spread of Ag–S bond distances ranging from 2.54–3.03 Å. Si4+ is bonded to four S2- atoms to form SiS4 tetrahedra that share corners with five equivalent AgS4 trigonal pyramids and an edgeedge with one SiS4 tetrahedra. There are two shorter (2.12 Å) and two longer (2.19 Å) Si–S bond lengths. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded to three Ag1+ and one Si4+ atom to form distorted corner-sharing SSiAg3 tetrahedra. In the second S2- site, S2- is bonded in a 3-coordinate geometry to one Ag1+ and two equivalent Si4+ atoms. In the third S2- site, S2- is bonded in a 5-coordinate geometry to four Ag1+ and one Si4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on MgAg(PO3)3 by Materials Project

MgAg(PO3)3 crystallizes in the orthorhombic Pcca space group. The structure is three-dimensional. there are two inequivalent Mg2+ sites. In the first Mg2+ site, Mg2+ is bonded to six O2- atoms to form MgO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Mg–O bond distances ranging from 2.04–2.15 Å. In the second Mg2+ site, Mg2+ is bonded to six O2- atoms to form MgO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Mg–O bond distances ranging from 2.07–2.12 Å. Ag1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ag–O bond distances ranging from 2.39–2.83 Å. There are three inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two MgO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedral tilt angles are 44°. There is two shorter (1.50 Å) and two longer (1.62 Å) P–O bond length. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent MgO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 38–53°. There are a spread of P–O bond distances ranging from 1.50–1.62 Å. In the third P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent MgO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 37–53°. There are a spread of P–O bond distances ranging from 1.49–1.63 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one Mg2+, one Ag1+, and one P5+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Mg2+, one Ag1+, and one P5+ atom. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to two equivalent P5+ atoms. In the fourth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Mg2+, one Ag1+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to one Mg2+, one Ag1+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the seventh O2- site, O2- is bonded in a 3-coordinate geometry to one Mg2+, one Ag1+, and one P5+ atom. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent P5+ atoms. In the ninth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the tenth O2- site, O2- is bonded in a 2-coordinate geometry to one Mg2+, one Ag1+, and one P5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on MgAgF5 by Materials Project

MgAgF5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Mg2+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Mg–F bond distances ranging from 1.96–2.41 Å. Ag3+ is bonded to six F1- atoms to form corner-sharing AgF6 octahedra. The corner-sharing octahedral tilt angles are 52°. There are a spread of Ag–F bond distances ranging from 2.01–2.25 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Mg2+ and one Ag3+ atom. In the second F1- site, F1- is bonded in a 3-coordinate geometry to two equivalent Mg2+ and one Ag3+ atom. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to one Mg2+ and one Ag3+ atom. In the fourth F1- site, F1- is bonded in a linear geometry to one Mg2+ and one Ag3+ atom. In the fifth F1- site, F1- is bonded in a distorted trigonal planar geometry to one Mg2+ and two equivalent Ag3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on AgSbS2 by Materials Project

AgSbS2 crystallizes in the monoclinic Cc space group. The structure is two-dimensional and consists of two AgSbS2 sheets oriented in the (-1, 0, 1) direction. there are two inequivalent Ag1+ sites. In the first Ag1+ site, Ag1+ is bonded in a linear geometry to two S2- atoms. Both Ag–S bond lengths are 2.40 Å. In the second Ag1+ site, Ag1+ is bonded in a linear geometry to two S2- atoms. There are one shorter (2.40 Å) and one longer (2.41 Å) Ag–S bond lengths. There are two inequivalent Sb3+ sites. In the first Sb3+ site, Sb3+ is bonded in a trigonal non-coplanar geometry to three S2- atoms. There are two shorter (2.48 Å) and one longer (2.49 Å) Sb–S bond lengths. In the second Sb3+ site, Sb3+ is bonded in a trigonal non-coplanar geometry to three S2- atoms. There are two shorter (2.48 Å) and one longer (2.49 Å) Sb–S bond lengths. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a water-like geometry to two Sb3+ atoms. In the second S2- site, S2- is bonded in a 3-coordinate geometry to two Ag1+ and one Sb3+ atom. In the third S2- site, S2- is bonded in a 3-coordinate geometry to two Ag1+ and one Sb3+ atom. In the fourth S2- site, S2- is bonded in a water-like geometry to two Sb3+ atoms.

36 MATERIALS SCIENCE↗

KGML-ag: a modeling framework of knowledge-guided machine learning to simulate agroecosystems: a case study of estimating N<sub>2</sub>O emission using data from mesocosm experiments

Abstract. Agricultural nitrous oxide (N2O) emission accounts for a non-trivial fraction of global greenhouse gas (GHG) budget. To date, estimating N2O fluxes from cropland remains a challenging task because the related microbial processes (e.g., nitrification and denitrification) are controlled by complex interactions among climate, soil, plant and human activities. Existing approaches such as process-based (PB) models have well-known limitations due to insufficient representations of the processes or uncertainties of model parameters, and due to leverage recent advances in machine learning (ML) a new method is needed to unlock the “black box” to overcome its limitations such as low interpretability, out-of-sample failure and massive data demand. In this study, we developed a first-of-its-kind knowledge-guided machine learning model for agroecosystems (KGML-ag) by incorporating biogeophysical and chemical domain knowledge from an advanced PB model, ecosys, and tested it by comparing simulating daily N2O fluxes with real observed data from mesocosm experiments. The gated recurrent unit (GRU) was used as the basis to build the model structure. To optimize the model performance, we have investigated a range of ideas, including (1) using initial values of intermediate variables (IMVs) instead of time series as model input to reduce data demand; (2) building hierarchical structures to explicitly estimate IMVs for further N2O prediction; (3) using multi-task learning to balance the simultaneous training on multiple variables; and (4) pre-training with millions of synthetic data generated from ecosys and fine-tuning with mesocosm observations. Six other pure ML models were developed using the same mesocosm data to serve as the benchmark for the KGML-ag model. Results show that KGML-ag did an excellent job in reproducing the mesocosm N2O fluxes (overall r2=0.81, and RMSE=3.6 mgNm-2d-1 from cross validation). Importantly, KGML-ag always outperforms the PB model and ML models in predicting N2O fluxes, especially for complex temporal dynamics and emission peaks. Besides, KGML-ag goes beyond the pure ML models by providing more interpretable predictions as well as pinpointing desired new knowledge and data to further empower the current KGML-ag. We believe the KGML-ag development in this study will stimulate a new body of research on interpretable ML for biogeochemistry and other related geoscience processes.

54 ENVIRONMENTAL SCIENCES↗

Materials Data on DyAgTe2 by Materials Project

DyAgTe2 crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Dy3+ is bonded to six Te2- atoms to form DyTe6 octahedra that share corners with six equivalent AgTe4 tetrahedra, edges with six equivalent DyTe6 octahedra, and edges with three equivalent AgTe4 tetrahedra. There are three shorter (3.06 Å) and three longer (3.16 Å) Dy–Te bond lengths. Ag1+ is bonded to four Te2- atoms to form AgTe4 tetrahedra that share corners with six equivalent DyTe6 octahedra, corners with six equivalent AgTe4 tetrahedra, and edges with three equivalent DyTe6 octahedra. The corner-sharing octahedra tilt angles range from 11–58°. There are one shorter (2.78 Å) and three longer (2.84 Å) Ag–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Dy3+ and one Ag1+ atom to form distorted TeDy3Ag trigonal pyramids that share corners with six equivalent TeDy3Ag3 octahedra, corners with six equivalent TeDy3Ag trigonal pyramids, and edges with three equivalent TeDy3Ag3 octahedra. The corner-sharing octahedra tilt angles range from 3–66°. In the second Te2- site, Te2- is bonded to three equivalent Dy3+ and three equivalent Ag1+ atoms to form TeDy3Ag3 octahedra that share corners with six equivalent TeDy3Ag trigonal pyramids, edges with six equivalent TeDy3Ag3 octahedra, and edges with three equivalent TeDy3Ag trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on HoAgTe2 by Materials Project

HoAgTe2 crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Ho3+ is bonded to six Te2- atoms to form HoTe6 octahedra that share corners with six equivalent AgTe4 tetrahedra, edges with six equivalent HoTe6 octahedra, and edges with three equivalent AgTe4 tetrahedra. There are three shorter (3.06 Å) and three longer (3.16 Å) Ho–Te bond lengths. Ag1+ is bonded to four Te2- atoms to form AgTe4 tetrahedra that share corners with six equivalent HoTe6 octahedra, corners with six equivalent AgTe4 tetrahedra, and edges with three equivalent HoTe6 octahedra. The corner-sharing octahedra tilt angles range from 11–58°. There are one shorter (2.79 Å) and three longer (2.83 Å) Ag–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Ho3+ and one Ag1+ atom to form distorted TeHo3Ag trigonal pyramids that share corners with six equivalent TeHo3Ag3 octahedra, corners with six equivalent TeHo3Ag trigonal pyramids, and edges with three equivalent TeHo3Ag3 octahedra. The corner-sharing octahedra tilt angles range from 3–67°. In the second Te2- site, Te2- is bonded to three equivalent Ho3+ and three equivalent Ag1+ atoms to form TeHo3Ag3 octahedra that share corners with six equivalent TeHo3Ag trigonal pyramids, edges with six equivalent TeHo3Ag3 octahedra, and edges with three equivalent TeHo3Ag trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on TmAgTe2 by Materials Project

TmAgTe2 crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Tm3+ is bonded to six Te2- atoms to form TmTe6 octahedra that share corners with six equivalent AgTe4 tetrahedra, edges with six equivalent TmTe6 octahedra, and edges with three equivalent AgTe4 tetrahedra. There are three shorter (3.03 Å) and three longer (3.13 Å) Tm–Te bond lengths. Ag1+ is bonded to four Te2- atoms to form AgTe4 tetrahedra that share corners with six equivalent TmTe6 octahedra, corners with six equivalent AgTe4 tetrahedra, and edges with three equivalent TmTe6 octahedra. The corner-sharing octahedra tilt angles range from 9–58°. There are one shorter (2.77 Å) and three longer (2.85 Å) Ag–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Tm3+ and one Ag1+ atom to form distorted TeTm3Ag trigonal pyramids that share corners with six equivalent TeTm3Ag3 octahedra, corners with six equivalent TeTm3Ag trigonal pyramids, and edges with three equivalent TeTm3Ag3 octahedra. The corner-sharing octahedra tilt angles range from 3–64°. In the second Te2- site, Te2- is bonded to three equivalent Tm3+ and three equivalent Ag1+ atoms to form TeTm3Ag3 octahedra that share corners with six equivalent TeTm3Ag trigonal pyramids, edges with six equivalent TeTm3Ag3 octahedra, and edges with three equivalent TeTm3Ag trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on YAgTe2 by Materials Project

YAgTe2 crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Y3+ is bonded to six Te2- atoms to form YTe6 octahedra that share corners with six equivalent AgTe4 tetrahedra, edges with six equivalent YTe6 octahedra, and edges with three equivalent AgTe4 tetrahedra. There are three shorter (3.08 Å) and three longer (3.17 Å) Y–Te bond lengths. Ag1+ is bonded to four Te2- atoms to form AgTe4 tetrahedra that share corners with six equivalent YTe6 octahedra, corners with six equivalent AgTe4 tetrahedra, and edges with three equivalent YTe6 octahedra. The corner-sharing octahedra tilt angles range from 12–58°. There are one shorter (2.80 Å) and three longer (2.83 Å) Ag–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Y3+ and one Ag1+ atom to form distorted TeY3Ag trigonal pyramids that share corners with six equivalent TeY3Ag3 octahedra, corners with six equivalent TeY3Ag trigonal pyramids, and edges with three equivalent TeY3Ag3 octahedra. The corner-sharing octahedra tilt angles range from 3–67°. In the second Te2- site, Te2- is bonded to three equivalent Y3+ and three equivalent Ag1+ atoms to form TeY3Ag3 octahedra that share corners with six equivalent TeY3Ag trigonal pyramids, edges with six equivalent TeY3Ag3 octahedra, and edges with three equivalent TeY3Ag trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on ErAgTe2 by Materials Project

ErAgTe2 crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Er3+ is bonded to six Te2- atoms to form ErTe6 octahedra that share corners with six equivalent AgTe4 tetrahedra, edges with six equivalent ErTe6 octahedra, and edges with three equivalent AgTe4 tetrahedra. There are three shorter (3.04 Å) and three longer (3.15 Å) Er–Te bond lengths. Ag1+ is bonded to four Te2- atoms to form AgTe4 tetrahedra that share corners with six equivalent ErTe6 octahedra, corners with six equivalent AgTe4 tetrahedra, and edges with three equivalent ErTe6 octahedra. The corner-sharing octahedra tilt angles range from 11–58°. There are one shorter (2.79 Å) and three longer (2.83 Å) Ag–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Er3+ and one Ag1+ atom to form distorted TeEr3Ag trigonal pyramids that share corners with six equivalent TeEr3Ag3 octahedra, corners with six equivalent TeEr3Ag trigonal pyramids, and edges with three equivalent TeEr3Ag3 octahedra. The corner-sharing octahedra tilt angles range from 3–67°. In the second Te2- site, Te2- is bonded to three equivalent Er3+ and three equivalent Ag1+ atoms to form TeEr3Ag3 octahedra that share corners with six equivalent TeEr3Ag trigonal pyramids, edges with six equivalent TeEr3Ag3 octahedra, and edges with three equivalent TeEr3Ag trigonal pyramids.

36 MATERIALS SCIENCE↗