cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.3886/e131363v1
title: Establishing a comprehensive census of undergraduate economics curricula: Foundational and special requirements for major programs in the U.S.

description: This study is the first of a series of studies, collectively embodying a multiphase mixed methods design. The overall objective of these studies is to explore and address a variety of issues and features of the discipline of economics, particularly as they relate to and represent past present and future factors of globalization, education, citizenship, and society. This is done by collecting and analyzing data on numerous aspects of the undergraduate economics curriculum, economics as a discipline, and economics as applied in the real world.<br><br> The overall purpose of these studies is to inform ongoing debates concerning the future of the discipline of economics and how it is taught, by examining and creating paradigms and methods that may be of aide. Additionally these studies collectively aim to outline, and in small ways develop, potential technological and organizational solutions for detailed longitudinal curriculum tracking. The frameworks employed and developed in these studies may eventually be scaled and adapted for all sorts of curricula. Ideally, the completion of this study’s overall objective yields practical insights and tools that empower faculty and departments, in economics and eventually in general, to better understand and design their own curriculum.<br><br> This immediate study fills gaps in and updates data on the curriculum of undergraduate economics majors in U.S. institutions, while also establishing a baseline data set for future studies to build on. A qualitative census methodology is adapted and employed to explore how various institutional and program factors relate to certain types of major program requirements. Descriptive statistics are used for analysis, primarily to allow for comparisons to previous studies. In sum, the purpose of the data collected and analyzed in this census is to give a glimpse into the current state of the undergraduate economics curriculum in the U.S., and to inform the qualitative, quantitative, and transformative studies that are to follow in this multiphase series.
description: web scraping;
description: All economic core requirements (i.e. intros, intermediates, quant) and special requirements (i.e. capstone) for all four year undergraduate economics major programs in US higher education institutions for the 2017-2018 school year.
DOI: 10.17188/1714582
title: Materials Data on In2AgTe3Br by Materials Project

description: AgIn2Te3Br crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Ag1+ is bonded to six Te2- atoms to form AgTe6 octahedra that share corners with four equivalent AgTe6 octahedra, edges with four equivalent AgTe6 octahedra, and edges with eight equivalent InTe5Br octahedra. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.80 Å) and four longer (3.04 Å) Ag–Te bond lengths. In3+ is bonded to five Te2- and one Br1- atom to form distorted InTe5Br octahedra that share corners with six equivalent InTe5Br octahedra, edges with four equivalent AgTe6 octahedra, and edges with four equivalent InTe5Br octahedra. The corner-sharing octahedra tilt angles range from 0–11°. There are four shorter (3.05 Å) and one longer (3.09 Å) In–Te bond lengths. The In–Br bond length is 2.76 Å. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to one Ag1+ and four equivalent In3+ atoms to form TeIn4Ag square pyramids that share corners with five equivalent TeIn4Ag square pyramids, edges with four equivalent TeIn2Ag4 octahedra, and edges with four equivalent TeIn4Ag square pyramids. In the second Te2- site, Te2- is bonded to four equivalent Ag1+ and two equivalent In3+ atoms to form TeIn2Ag4 octahedra that share corners with four equivalent TeIn2Ag4 octahedra, edges with four equivalent TeIn2Ag4 octahedra, and edges with eight equivalent TeIn4Ag square pyramids. The corner-sharing octahedral tilt angles are 0°. Br1- is bonded in a linear geometry to two equivalent In3+ atoms.
DOI: 10.17188/1714584
title: Materials Data on RbPrO2 by Materials Project

description: RbPrO2 is Caswellsilverite structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Rb1+ is bonded to six equivalent O2- atoms to form distorted RbO6 octahedra that share corners with six equivalent PrO6 octahedra, edges with six equivalent RbO6 octahedra, and edges with six equivalent PrO6 octahedra. The corner-sharing octahedral tilt angles are 15°. All Rb–O bond lengths are 3.00 Å. Pr3+ is bonded to six equivalent O2- atoms to form PrO6 octahedra that share corners with six equivalent RbO6 octahedra, edges with six equivalent RbO6 octahedra, and edges with six equivalent PrO6 octahedra. The corner-sharing octahedral tilt angles are 15°. All Pr–O bond lengths are 2.45 Å. O2- is bonded to three equivalent Rb1+ and three equivalent Pr3+ atoms to form a mixture of distorted corner and edge-sharing ORb3Pr3 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1714585
title: Materials Data on Li3Mn(PO4)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: 10.17188/1714586
title: Materials Data on Mg3(FeN2)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: 10.17188/1714587
title: Materials Data on Rb2HgRuF6 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: 10.17188/1714588
title: Materials Data on Y2Fe17C2 by Materials Project

description: Y2Fe17C2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Y is bonded in a distorted bent 120 degrees geometry to nine Fe and two equivalent C atoms. There are a spread of Y–Fe bond distances ranging from 3.06–3.35 Å. Both Y–C bond lengths are 2.51 Å. There are seven inequivalent Fe sites. In the first Fe site, Fe is bonded in a 2-coordinate geometry to one Y and thirteen Fe atoms. There are a spread of Fe–Fe bond distances ranging from 2.39–2.75 Å. In the second Fe site, Fe is bonded to three equivalent Y and nine Fe atoms to form FeY3Fe9 cuboctahedra that share corners with eleven FeY3Fe9 cuboctahedra, corners with four equivalent CY2Fe4 octahedra, edges with four FeY3Fe9 cuboctahedra, faces with eight FeY3Fe9 cuboctahedra, and faces with two equivalent CY2Fe4 octahedra. The corner-sharing octahedra tilt angles range from 64–69°. There are a spread of Fe–Fe bond distances ranging from 2.47–2.63 Å. In the third Fe site, Fe is bonded in a single-bond geometry to five Fe and one C atom. There are two shorter (2.48 Å) and one longer (2.56 Å) Fe–Fe bond lengths. The Fe–C bond length is 1.92 Å. In the fourth Fe site, Fe is bonded to two equivalent Y and ten Fe atoms to form distorted FeY2Fe10 cuboctahedra that share corners with eight FeY3Fe9 cuboctahedra, corners with four equivalent CY2Fe4 octahedra, edges with three FeY2Fe10 cuboctahedra, edges with two equivalent CY2Fe4 octahedra, and faces with nine FeY3Fe9 cuboctahedra. The corner-sharing octahedra tilt angles range from 23–29°. There are two shorter (2.44 Å) and two longer (2.48 Å) Fe–Fe bond lengths. In the fifth Fe site, Fe is bonded in a single-bond geometry to six Fe and one C atom. Both Fe–Fe bond lengths are 2.43 Å. The Fe–C bond length is 1.86 Å. In the sixth Fe site, Fe is bonded to two equivalent Y and ten Fe atoms to form distorted FeY2Fe10 cuboctahedra that share corners with fourteen FeY3Fe9 cuboctahedra, edges with two equivalent FeY3Fe9 cuboctahedra, faces with ten FeY3Fe9 cuboctahedra, and faces with four equivalent CY2Fe4 octahedra. In the seventh Fe site, Fe is bonded to two equivalent Y and ten Fe atoms to form FeY2Fe10 cuboctahedra that share corners with eight FeY3Fe9 cuboctahedra, corners with two equivalent CY2Fe4 octahedra, edges with four FeY2Fe10 cuboctahedra, faces with eight FeY3Fe9 cuboctahedra, and faces with two equivalent CY2Fe4 octahedra. The corner-sharing octahedral tilt angles are 44°. C is bonded to two equivalent Y and four Fe atoms to form CY2Fe4 octahedra that share corners with ten FeY3Fe9 cuboctahedra, corners with two equivalent CY2Fe4 octahedra, edges with two equivalent FeY2Fe10 cuboctahedra, and faces with six FeY2Fe10 cuboctahedra. The corner-sharing octahedral tilt angles are 62°.
DOI: 10.17188/1714589
title: Materials Data on K3In(IO3)6 by Materials Project

description: K3In(O3I)6 crystallizes in the orthorhombic Fdd2 space group. The structure is three-dimensional. there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are four shorter (2.74 Å) and four longer (3.18 Å) K–O bond lengths. In the second K1+ site, K1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of K–O bond distances ranging from 2.71–3.24 Å. In3+ is bonded in an octahedral geometry to six O2- atoms. There are a spread of In–O bond distances ranging from 2.15–2.21 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two K1+ and two I5+ atoms. There are one shorter (1.84 Å) and one longer (2.75 Å) O–I bond lengths. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one K1+, one In3+, and one I5+ atom. The O–I bond length is 1.89 Å. In the third O2- site, O2- is bonded in a 1-coordinate geometry to one K1+ and one I5+ atom. The O–I bond length is 1.83 Å. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to one K1+ and one I5+ atom. The O–I bond length is 1.84 Å. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one In3+ and one I5+ atom. The O–I bond length is 1.86 Å. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent K1+ and two I5+ atoms. There are one shorter (1.83 Å) and one longer (2.71 Å) O–I bond lengths. In the seventh O2- site, O2- is bonded in a 2-coordinate geometry to one K1+, one In3+, and one I5+ atom. The O–I bond length is 1.88 Å. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to two K1+ and two I5+ atoms. There are one shorter (1.83 Å) and one longer (2.76 Å) O–I bond lengths. In the ninth O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent K1+ and two I5+ atoms. There are one shorter (1.84 Å) and one longer (2.73 Å) O–I bond lengths. There are three inequivalent I5+ sites. In the first I5+ site, I5+ is bonded in a 3-coordinate geometry to four O2- atoms. In the second I5+ site, I5+ is bonded in a 3-coordinate geometry to five O2- atoms. In the third I5+ site, I5+ is bonded in a 3-coordinate geometry to four O2- atoms.
DOI: 10.17188/1714590
title: Materials Data on Mn10NiN8 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: 10.17188/1714591
title: Materials Data on Fe2Pb3N4 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: 10.17188/1714592
title: Materials Data on SmRe2SiC by Materials Project

description: SmRe2SiC crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Sm2+ is bonded in a 7-coordinate geometry to three equivalent Si4- and four equivalent C4- atoms. There are one shorter (3.04 Å) and two longer (3.14 Å) Sm–Si bond lengths. All Sm–C bond lengths are 2.76 Å. Re3+ is bonded in a single-bond geometry to three equivalent Si4- and one C4- atom. There are one shorter (2.49 Å) and two longer (2.52 Å) Re–Si bond lengths. The Re–C bond length is 1.96 Å. Si4- is bonded in a 9-coordinate geometry to three equivalent Sm2+ and six equivalent Re3+ atoms. C4- is bonded to four equivalent Sm2+ and two equivalent Re3+ atoms to form a mixture of corner and edge-sharing CSm4Re2 octahedra. The corner-sharing octahedral tilt angles are 20°.
DOI: 10.17188/1714593
title: Materials Data on Nd2Ta6O19 by Materials Project

description: Nd2Ta6O19 crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. Nd is bonded to six equivalent O atoms to form distorted edge-sharing NdO6 octahedra. All Nd–O bond lengths are 2.37 Å. Ta is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Ta–O bond distances ranging from 1.94–2.12 Å. There are four inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to two equivalent Nd and one Ta atom. In the second O site, O is bonded in a bent 150 degrees geometry to two equivalent Ta atoms. In the third O site, O is bonded in a trigonal planar geometry to three equivalent Ta atoms. In the fourth O site, O is bonded in a bent 150 degrees geometry to two equivalent Ta atoms.
DOI: 10.17188/1714594
title: Materials Data on LiHoSn2 by Materials Project

description: LiHoSn2 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Li is bonded in a 5-coordinate geometry to four equivalent Ho and five Sn atoms. All Li–Ho bond lengths are 3.38 Å. There are a spread of Li–Sn bond distances ranging from 2.46–2.67 Å. Ho is bonded in a 4-coordinate geometry to four equivalent Li and ten Sn atoms. There are a spread of Ho–Sn bond distances ranging from 3.34–3.63 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a distorted single-bond geometry to one Li and six equivalent Ho atoms. In the second Sn site, Sn is bonded to four equivalent Li and four equivalent Ho atoms to form a mixture of face and edge-sharing SnLi4Ho4 tetrahedra.
DOI: 10.17188/1714596
title: Materials Data on CaLaMnFeO6 by Materials Project

description: CaLaMnFeO6 is Orthorhombic Perovskite-derived structured and crystallizes in the monoclinic Pc space group. The structure is three-dimensional. Ca2+ is bonded in a 9-coordinate geometry to five O2- atoms. There are a spread of Ca–O bond distances ranging from 2.37–2.49 Å. La3+ is bonded in a 12-coordinate geometry to five O2- atoms. There are a spread of La–O bond distances ranging from 2.38–2.54 Å. Mn4+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 20–27°. There is four shorter (1.94 Å) and two longer (1.95 Å) Mn–O bond length. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 20–27°. There are two shorter (2.00 Å) and four longer (2.01 Å) Fe–O bond lengths. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to one La3+, one Mn4+, and one Fe3+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to one Ca2+, one La3+, one Mn4+, and one Fe3+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one Ca2+, one La3+, one Mn4+, and one Fe3+ atom. In the fourth O2- site, O2- is bonded in a 5-coordinate geometry to one Ca2+, one Mn4+, and one Fe3+ atom. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to one Ca2+, one La3+, one Mn4+, and one Fe3+ atom. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to one Ca2+, one La3+, one Mn4+, and one Fe3+ atom.
DOI: 10.17188/1714597
title: Materials Data on MgOsN2 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: 10.17188/1714598
title: Materials Data on Mn3V(PO4)4 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: 10.17188/1714600
title: Materials Data on SmV2Fe10N by Materials Project

description: SmV2Fe10N crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Sm is bonded in a linear geometry to two equivalent V, ten Fe, and two equivalent N atoms. Both Sm–V bond lengths are 3.05 Å. There are two shorter (3.17 Å) and eight longer (3.23 Å) Sm–Fe bond lengths. Both Sm–N bond lengths are 2.39 Å. V is bonded in a 10-coordinate geometry to one Sm, one V, and twelve Fe atoms. The V–V bond length is 2.37 Å. There are a spread of V–Fe bond distances ranging from 2.61–2.88 Å. There are four inequivalent Fe sites. In the first Fe site, Fe is bonded in a single-bond geometry to two equivalent V, six Fe, and one N atom. There are four shorter (2.44 Å) and two longer (2.68 Å) Fe–Fe bond lengths. The Fe–N bond length is 1.95 Å. In the second Fe site, Fe is bonded in a single-bond geometry to two equivalent V, six Fe, and one N atom. There are four shorter (2.46 Å) and two longer (2.59 Å) Fe–Fe bond lengths. The Fe–N bond length is 1.89 Å. In the third Fe site, Fe is bonded to two equivalent Sm, two equivalent V, and eight Fe atoms to form distorted FeSm2V2Fe8 cuboctahedra that share corners with ten equivalent FeSm2V2Fe8 cuboctahedra, corners with two equivalent NSm2Fe4 octahedra, edges with four equivalent FeSm2V2Fe8 cuboctahedra, faces with six equivalent FeSm2V2Fe8 cuboctahedra, and faces with two equivalent NSm2Fe4 octahedra. The corner-sharing octahedral tilt angles are 68°. There are two shorter (2.39 Å) and two longer (2.64 Å) Fe–Fe bond lengths. In the fourth Fe site, Fe is bonded in a 1-coordinate geometry to one Sm, four equivalent V, and nine Fe atoms. The Fe–Fe bond length is 2.20 Å. N is bonded to two equivalent Sm and four Fe atoms to form NSm2Fe4 octahedra that share corners with eight equivalent FeSm2V2Fe8 cuboctahedra, corners with two equivalent NSm2Fe4 octahedra, and faces with eight equivalent FeSm2V2Fe8 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1714601
title: Materials Data on GdTa4O12 by Materials Project

description: GdTa4O12 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. Gd is bonded in a 12-coordinate geometry to twelve O atoms. There are a spread of Gd–O bond distances ranging from 2.40–3.12 Å. Ta is bonded to six O atoms to form corner-sharing TaO6 octahedra. The corner-sharing octahedra tilt angles range from 7–16°. There are a spread of Ta–O bond distances ranging from 1.93–2.05 Å. There are five inequivalent O sites. In the first O site, O is bonded in a distorted linear geometry to one Gd and two equivalent Ta atoms. In the second O site, O is bonded in a distorted T-shaped geometry to one Gd and two equivalent Ta atoms. In the third O site, O is bonded in a 3-coordinate geometry to two equivalent Gd and two equivalent Ta atoms. In the fourth O site, O is bonded in a linear geometry to two equivalent Ta atoms. In the fifth O site, O is bonded in a distorted T-shaped geometry to one Gd and two equivalent Ta atoms.
DOI: 10.17188/1714602
title: Materials Data on Mn3Al2(GeO4)3 by Materials Project

description: Mn3Al2Ge3O12 crystallizes in the cubic Ia-3d space group. The structure is three-dimensional. Mn2+ is bonded in a distorted body-centered cubic geometry to eight equivalent O2- atoms. There are four shorter (2.29 Å) and four longer (2.47 Å) Mn–O bond lengths. Al3+ is bonded to six equivalent O2- atoms to form AlO6 octahedra that share corners with six equivalent GeO4 tetrahedra. All Al–O bond lengths are 1.92 Å. Ge4+ is bonded to four equivalent O2- atoms to form GeO4 tetrahedra that share corners with four equivalent AlO6 octahedra. The corner-sharing octahedral tilt angles are 49°. All Ge–O bond lengths are 1.78 Å. O2- is bonded in a 4-coordinate geometry to two equivalent Mn2+, one Al3+, and one Ge4+ atom.
DOI: 10.17188/1714603
title: Materials Data on Er2ZnGa by Materials Project

description: Er2ZnGa is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded in a body-centered cubic geometry to four equivalent Zn and four equivalent Ga atoms. All Er–Zn bond lengths are 3.06 Å. All Er–Ga bond lengths are 3.06 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Er atoms. Ga is bonded in a body-centered cubic geometry to eight equivalent Er atoms.
DOI: 10.17188/1714604
title: Materials Data on Na2PrO3 by Materials Project

description: Na2PrO3 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Na1+ is bonded in a square co-planar geometry to four O2- atoms. There are two shorter (2.39 Å) and two longer (2.40 Å) Na–O bond lengths. Pr4+ is bonded to six O2- atoms to form corner-sharing PrO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.39 Å) and two longer (2.40 Å) Pr–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Na1+ and two equivalent Pr4+ atoms to form corner-sharing ONa4Pr2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second O2- site, O2- is bonded in a square co-planar geometry to two equivalent Na1+ and two equivalent Pr4+ atoms.
DOI: 10.17188/1714605
title: Materials Data on Al2O3 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: 10.17188/1714606
title: Materials Data on Er2Mo2C3 by Materials Project

description: Er2Mo2C3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Er3+ is bonded to five C4- atoms to form distorted ErC5 square pyramids that share corners with two equivalent ErC5 square pyramids, corners with seven equivalent MoC4 trigonal pyramids, edges with five equivalent ErC5 square pyramids, and edges with three equivalent MoC4 trigonal pyramids. There are a spread of Er–C bond distances ranging from 2.41–2.59 Å. Mo3+ is bonded to four C4- atoms to form MoC4 trigonal pyramids that share corners with seven equivalent ErC5 square pyramids, corners with three equivalent MoC4 trigonal pyramids, edges with three equivalent ErC5 square pyramids, and edges with two equivalent MoC4 trigonal pyramids. There are a spread of Mo–C bond distances ranging from 2.03–2.13 Å. There are two inequivalent C4- sites. In the first C4- site, C4- is bonded to four equivalent Er3+ and two equivalent Mo3+ atoms to form CEr4Mo2 octahedra that share corners with twelve equivalent CEr3Mo3 octahedra, edges with two equivalent CEr4Mo2 octahedra, and faces with two equivalent CEr3Mo3 octahedra. The corner-sharing octahedra tilt angles range from 43–57°. In the second C4- site, C4- is bonded to three equivalent Er3+ and three equivalent Mo3+ atoms to form CEr3Mo3 octahedra that share corners with six equivalent CEr4Mo2 octahedra, edges with six equivalent CEr3Mo3 octahedra, and a faceface with one CEr4Mo2 octahedra. The corner-sharing octahedra tilt angles range from 43–57°.