cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1726526
title: Materials Data on K3YCl6 by Materials Project

description: K3YCl6 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are three inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of K–Cl bond distances ranging from 3.32–3.88 Å. In the second K1+ site, K1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of K–Cl bond distances ranging from 3.09–3.71 Å. In the third K1+ site, K1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of K–Cl bond distances ranging from 3.15–3.75 Å. There are two inequivalent Y3+ sites. In the first Y3+ site, Y3+ is bonded in an octahedral geometry to six Cl1- atoms. There are a spread of Y–Cl bond distances ranging from 2.62–2.67 Å. In the second Y3+ site, Y3+ is bonded in an octahedral geometry to six Cl1- atoms. There are a spread of Y–Cl bond distances ranging from 2.63–2.68 Å. There are six inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom. In the second Cl1- site, Cl1- is bonded in a 4-coordinate geometry to four K1+ and one Y3+ atom. In the third Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom. In the fourth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom. In the fifth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom. In the sixth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom.
DOI: 10.17188/1726528
title: Materials Data on KAs2HO6 by Materials Project

description: KAs2HO6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. K1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of K–O bond distances ranging from 2.73–2.96 Å. There are two inequivalent As5+ sites. In the first As5+ site, As5+ is bonded to four O2- atoms to form corner-sharing AsO4 tetrahedra. The corner-sharing octahedra tilt angles range from 54–60°. There are a spread of As–O bond distances ranging from 1.68–1.76 Å. In the second As5+ site, As5+ is bonded to six O2- atoms to form AsO6 octahedra that share corners with three equivalent AsO4 tetrahedra and an edgeedge with one AsO6 octahedra. There are a spread of As–O bond distances ranging from 1.79–1.92 Å. H1+ is bonded in a single-bond geometry to two O2- atoms. There is one shorter (1.00 Å) and one longer (1.74 Å) H–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one K1+, one As5+, and one H1+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one K1+ and two equivalent As5+ atoms. In the third O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent K1+, one As5+, and one H1+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to one K1+ and two As5+ atoms. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to two As5+ atoms. In the sixth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one K1+ and two As5+ atoms.
DOI: 10.17188/1726529
title: Materials Data on Li4Fe5NiO12 by Materials Project

description: Li4Fe5NiO12 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Li is bonded in a distorted rectangular see-saw-like geometry to four O atoms. There are a spread of Li–O bond distances ranging from 2.04–2.09 Å. There are three inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are four shorter (1.96 Å) and two longer (2.12 Å) Fe–O bond lengths. In the second Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share edges with three equivalent FeO6 octahedra and edges with three equivalent NiO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.91–2.13 Å. In the third Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are two shorter (2.03 Å) and four longer (2.07 Å) Fe–O bond lengths. Ni is bonded to six O atoms to form NiO6 octahedra that share edges with six equivalent FeO6 octahedra. There are two shorter (2.08 Å) and four longer (2.12 Å) Ni–O bond lengths. There are four inequivalent O sites. In the first O site, O is bonded to two equivalent Li, two equivalent Fe, and one Ni atom to form a mixture of distorted corner and edge-sharing OLi2Fe2Ni trigonal bipyramids. In the second O site, O is bonded to two equivalent Li and three Fe atoms to form a mixture of distorted corner and edge-sharing OLi2Fe3 trigonal bipyramids. In the third O site, O is bonded in a distorted T-shaped geometry to three Fe atoms. In the fourth O site, O is bonded in a distorted trigonal non-coplanar geometry to two equivalent Fe and one Ni atom.
DOI: 10.17188/1726530
title: Materials Data on Dy2(MoO4)3 by Materials Project

description: Dy2(MoO4)3 crystallizes in the tetragonal P-42_1m space group. The structure is three-dimensional. Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.26–2.44 Å. There are two inequivalent Mo6+ sites. In the first Mo6+ site, Mo6+ is bonded in a tetrahedral geometry to four O2- atoms. There is three shorter (1.78 Å) and one longer (1.83 Å) Mo–O bond length. In the second Mo6+ site, Mo6+ is bonded in a tetrahedral geometry to four equivalent O2- atoms. All Mo–O bond lengths are 1.79 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to one Dy3+ and one Mo6+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Dy3+ and one Mo6+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Dy3+ and one Mo6+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to one Dy3+ and one Mo6+ atom.
DOI: 10.17188/1726531
title: Materials Data on Gd2CdHg by Materials Project

description: Gd2HgCd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Gd is bonded in a body-centered cubic geometry to four equivalent Hg and four equivalent Cd atoms. All Gd–Hg bond lengths are 3.25 Å. All Gd–Cd bond lengths are 3.25 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Gd atoms. Cd is bonded in a body-centered cubic geometry to eight equivalent Gd atoms.
DOI: 10.17188/1726532
title: Materials Data on ZrMo by Materials Project

description: Zr(Mo) crystallizes in the orthorhombic Cmmm space group. The structure is two-dimensional and consists of two Zr(Mo) sheets oriented in the (0, 1, 0) direction. Zr is bonded in a 4-coordinate geometry to four equivalent Mo atoms. All Zr–Mo bond lengths are 2.80 Å. Mo is bonded in a 4-coordinate geometry to four equivalent Zr atoms.
DOI: 10.5281/zenodo.4483235
title: VIODE

description: Dynamic environments such as urban areas are still challenging for popular visual-inertial odometry (VIO) algo- rithms. Existing datasets typically fail to capture the dynamic nature of these environments, therefore making it difficult to quantitatively evaluate the robustness of existing VIO methods. To address this issue, we propose three contributions: firstly, we provide the VIODE benchmark, a novel dataset recorded from a simulated UAV that navigates in challenging dynamic environments. The unique feature of the VIODE dataset is the systematic introduction of moving objects into the scenes. It includes three environments, each of which is available in four dynamic levels that progressively add moving objects. The dataset contains synchronized stereo images and IMU data, as well as ground-truth trajectories and instance segmentation masks. Secondly, we compare state-of-the-art VIO algorithms on the VIODE dataset and show that they display substantial performance degradation in highly dynamic scenes. Thirdly, we propose a simple extension for visual localization algorithms that relies on semantic information. Our results show that scene semantics are an effective way to mitigate the adverse effects of dynamic objects on VIO algorithms. Finally, we make the VIODE dataset publicly available at https://github.com/kminoda/VIODE.
DOI: 10.17188/1726533
title: Materials Data on Co2C2O7 by Materials Project

description: Co2C2O7 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are three inequivalent Co3+ sites. In the first Co3+ site, Co3+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.78–1.90 Å. In the second Co3+ site, Co3+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.77–1.92 Å. In the third Co3+ site, Co3+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.80–1.91 Å. There are three inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.28–1.31 Å. In the second C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.29 Å) and one longer (1.30 Å) C–O bond length. In the third C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.29 Å) and one longer (1.30 Å) C–O bond length. There are eleven inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the second O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent Co3+ atoms. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the sixth O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the seventh O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the eighth O2- site, O2- is bonded in a linear geometry to two Co3+ atoms. In the ninth O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the tenth O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom. In the eleventh O2- site, O2- is bonded in a bent 120 degrees geometry to one Co3+ and one C4+ atom.
DOI: 10.17188/1726535
title: Materials Data on Mg2MnAl3S8 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1726536
title: Materials Data on TlCu2(AsO4)2 by Materials Project

description: Cu2Tl(AsO4)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Cu+1.50+ sites. In the first Cu+1.50+ site, Cu+1.50+ is bonded in a distorted rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.88–1.99 Å. In the second Cu+1.50+ site, Cu+1.50+ is bonded to five O2- atoms to form distorted CuO5 trigonal bipyramids that share corners with five AsO4 tetrahedra. There are a spread of Cu–O bond distances ranging from 1.92–2.49 Å. Tl3+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Tl–O bond distances ranging from 2.58–2.77 Å. There are two inequivalent As5+ sites. In the first As5+ site, As5+ is bonded to four O2- atoms to form AsO4 tetrahedra that share corners with three equivalent CuO5 trigonal bipyramids. There are a spread of As–O bond distances ranging from 1.71–1.78 Å. In the second As5+ site, As5+ is bonded to four O2- atoms to form AsO4 tetrahedra that share corners with two equivalent CuO5 trigonal bipyramids. There are a spread of As–O bond distances ranging from 1.69–1.76 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to two Cu+1.50+ and one As5+ atom. In the second O2- site, O2- is bonded in a water-like geometry to one Cu+1.50+ and one As5+ atom. In the third O2- site, O2- is bonded in a water-like geometry to one Cu+1.50+ and one As5+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to two Cu+1.50+ and one As5+ atom. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to one Tl3+ and one As5+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Cu+1.50+, one Tl3+, and one As5+ atom. In the seventh O2- site, O2- is bonded in a 2-coordinate geometry to one Cu+1.50+, one Tl3+, and one As5+ atom. In the eighth O2- site, O2- is bonded in a bent 120 degrees geometry to one Cu+1.50+ and one As5+ atom.
DOI: 10.17188/1726537
title: Materials Data on Na2H(CO2)2 by Materials Project

description: (NaCO2)4H2 crystallizes in the orthorhombic P2_12_12 space group. The structure is three-dimensional and consists of two hydrogen molecules and one NaCO2 framework. In the NaCO2 framework, Na1+ is bonded in a 3-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.41–2.88 Å. C+2.50+ is bonded in a bent 120 degrees geometry to two O2- atoms. There is one shorter (1.26 Å) and one longer (1.28 Å) C–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Na1+ and one C+2.50+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to four equivalent Na1+ and one C+2.50+ atom.
DOI: 10.17188/1726539
title: Materials Data on KCr3BiO12 by Materials Project

description: KCr3BiO12 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. K1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of K–O bond distances ranging from 2.80–3.29 Å. There are three inequivalent Cr6+ sites. In the first Cr6+ site, Cr6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Cr–O bond distances ranging from 1.61–1.71 Å. In the second Cr6+ site, Cr6+ is bonded to four O2- atoms to form corner-sharing CrO4 tetrahedra. There are a spread of Cr–O bond distances ranging from 1.60–1.79 Å. In the third Cr6+ site, Cr6+ is bonded to four O2- atoms to form corner-sharing CrO4 tetrahedra. There are a spread of Cr–O bond distances ranging from 1.61–1.78 Å. Bi5+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Bi–O bond distances ranging from 2.30–2.60 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one K1+ and one Bi5+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one K1+ and one Cr6+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one Cr6+ and two equivalent Bi5+ atoms. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to one K1+, one Cr6+, and one Bi5+ atom. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to one Cr6+ and one Bi5+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to one K1+, one Cr6+, and one Bi5+ atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to one Cr6+ atom. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to one Cr6+ and one Bi5+ atom. In the ninth O2- site, O2- is bonded in a bent 120 degrees geometry to two Cr6+ atoms. In the tenth O2- site, O2- is bonded in a distorted single-bond geometry to one K1+, one Cr6+, and one Bi5+ atom. In the eleventh O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent K1+ and one Cr6+ atom. In the twelfth O2- site, O2- is bonded in a single-bond geometry to one K1+ and one Cr6+ atom.
DOI: 10.17188/1726540
title: Materials Data on CeSe2 by Materials Project

description: CeSe2 is Low Tridymite-like structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Ce4+ sites. In the first Ce4+ site, Ce4+ is bonded to four Se2- atoms to form corner-sharing CeSe4 tetrahedra. There are one shorter (2.71 Å) and three longer (2.72 Å) Ce–Se bond lengths. In the second Ce4+ site, Ce4+ is bonded to four Se2- atoms to form corner-sharing CeSe4 tetrahedra. There are two shorter (2.72 Å) and two longer (2.73 Å) Ce–Se bond lengths. In the third Ce4+ site, Ce4+ is bonded to four Se2- atoms to form corner-sharing CeSe4 tetrahedra. There are a spread of Ce–Se bond distances ranging from 2.71–2.73 Å. There are eight inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a bent 150 degrees geometry to two Ce4+ atoms. In the second Se2- site, Se2- is bonded in a bent 150 degrees geometry to two Ce4+ atoms. In the third Se2- site, Se2- is bonded in a bent 150 degrees geometry to two Ce4+ atoms. In the fourth Se2- site, Se2- is bonded in a linear geometry to two equivalent Ce4+ atoms. In the fifth Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms. In the sixth Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms. In the seventh Se2- site, Se2- is bonded in a bent 150 degrees geometry to two Ce4+ atoms. In the eighth Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms.
DOI: 10.17188/1726541
title: Materials Data on Cr3(P2O7)2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1726542
title: Materials Data on ErSiPt by Materials Project

description: ErPtSi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Er is bonded in a 12-coordinate geometry to six equivalent Pt and six equivalent Si atoms. There are a spread of Er–Pt bond distances ranging from 2.99–3.16 Å. There are a spread of Er–Si bond distances ranging from 2.96–3.15 Å. Pt is bonded in a 10-coordinate geometry to six equivalent Er and four equivalent Si atoms. There are a spread of Pt–Si bond distances ranging from 2.50–2.70 Å. Si is bonded in a 10-coordinate geometry to six equivalent Er and four equivalent Pt atoms.
DOI: 10.17188/1726543
title: Materials Data on B2Pb4O7 by Materials Project

description: Pb4O(BO3)2 crystallizes in the orthorhombic Aea2 space group. The structure is three-dimensional. there are two inequivalent B3+ sites. In the first B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.39 Å) and one longer (1.40 Å) B–O bond length. In the second B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.37 Å) and one longer (1.42 Å) B–O bond length. There are four inequivalent Pb2+ sites. In the first Pb2+ site, Pb2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Pb–O bond distances ranging from 2.31–3.11 Å. In the second Pb2+ site, Pb2+ is bonded in a distorted square pyramidal geometry to five O2- atoms. There are a spread of Pb–O bond distances ranging from 2.32–2.63 Å. In the third Pb2+ site, Pb2+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Pb–O bond distances ranging from 2.30–2.36 Å. In the fourth Pb2+ site, Pb2+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Pb–O bond distances ranging from 2.24–2.31 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one B3+ and two Pb2+ atoms. In the second O2- site, O2- is bonded to four Pb2+ atoms to form distorted edge-sharing OPb4 trigonal pyramids. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one B3+ and two Pb2+ atoms. In the fourth O2- site, O2- is bonded in a bent 120 degrees geometry to two equivalent B3+ atoms. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to one B3+ and two Pb2+ atoms. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to one B3+ and two Pb2+ atoms. In the seventh O2- site, O2- is bonded to four Pb2+ atoms to form edge-sharing OPb4 tetrahedra. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to one B3+ and three Pb2+ atoms.
DOI: 10.17188/1726544
title: Materials Data on LiMnOF2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1726545
title: Materials Data on LiMn(SiO3)2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1726546
title: Materials Data on TmTc2 by Materials Project

description: TmTc2 is Hexagonal Laves structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Tm is bonded in a 12-coordinate geometry to twelve Tc atoms. There are a spread of Tm–Tc bond distances ranging from 3.13–3.15 Å. There are two inequivalent Tc sites. In the first Tc site, Tc is bonded to six equivalent Tm and six equivalent Tc atoms to form a mixture of corner, edge, and face-sharing TcTm6Tc6 cuboctahedra. All Tc–Tc bond lengths are 2.72 Å. In the second Tc site, Tc is bonded to six equivalent Tm and six Tc atoms to form a mixture of corner, edge, and face-sharing TcTm6Tc6 cuboctahedra. There are two shorter (2.58 Å) and two longer (2.76 Å) Tc–Tc bond lengths.
DOI: 10.17188/1726547
title: Materials Data on InAgGeSe4 by Materials Project

description: AgInGeSe4 crystallizes in the tetragonal I-4 space group. The structure is three-dimensional. Ag1+ is bonded to four equivalent Se2- atoms to form AgSe4 tetrahedra that share corners with four equivalent InSe4 tetrahedra and corners with four equivalent GeSe4 tetrahedra. All Ag–Se bond lengths are 2.69 Å. In3+ is bonded to four equivalent Se2- atoms to form InSe4 tetrahedra that share corners with four equivalent AgSe4 tetrahedra and corners with four equivalent GeSe4 tetrahedra. All In–Se bond lengths are 2.65 Å. Ge4+ is bonded to four equivalent Se2- atoms to form GeSe4 tetrahedra that share corners with four equivalent AgSe4 tetrahedra and corners with four equivalent InSe4 tetrahedra. All Ge–Se bond lengths are 2.42 Å. Se2- is bonded in a trigonal non-coplanar geometry to one Ag1+, one In3+, and one Ge4+ atom.