cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.3886/e130824v1
title: Political Shock 2018-2020

description: Some political events are so tumultuous that, similar to earthquakes, they alter the political landscape in their wake. Grounded in sociological and consumer theories of tribes, this research examines the downstream consequences of shocking political events on consumer behavior. Our theory proposes and our analysis confirms that political shocks affect tribal homophily, issue self-relevance, and work through fear and flight to impact political engagement and actual 2018 voting behaviors. Study 1 explores the classification of historical and recent events to determine if political shock perceptions exist. Using a multi-wave study, study 2 follows the events surrounding Justice Brett Kavanaugh’s confirmation to the US Supreme Court and the 2018 midterm elections to understand political shocks influence on political activism and voting behaviors. Finally, in study 3, tweets from different political affiliations during the time period of President Trump’s presidential campaign announcement to the 2018 midterm election are analyzed and support the proposed model. The findings suggest that in periods of chaos, consumers react to political shocks by joining the most relevant political tribe, are motivated to engage in political activism behavior and more likely to vote.
DOI: 10.17188/1280904
title: Materials Data on Pd(XeF8)2 by Materials Project

description: Pd(XeF8)2 crystallizes in the orthorhombic Pca2_1 space group. The structure is zero-dimensional and consists of four Pd(XeF8)2 clusters. there are two inequivalent Xe sites. In the first Xe site, Xe is bonded in a 5-coordinate geometry to six F atoms. There are a spread of Xe–F bond distances ranging from 1.99–2.45 Å. In the second Xe site, Xe is bonded in a 5-coordinate geometry to six F atoms. There are a spread of Xe–F bond distances ranging from 1.99–2.47 Å. Pd is bonded in an octahedral geometry to six F atoms. There are a spread of Pd–F bond distances ranging from 1.94–1.97 Å. There are sixteen inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Pd atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom. In the fourth F site, F is bonded in a single-bond geometry to one Xe atom. In the fifth F site, F is bonded in a single-bond geometry to one Xe atom. In the sixth F site, F is bonded in a single-bond geometry to one Xe atom. In the seventh F site, F is bonded in a single-bond geometry to one Xe atom. In the eighth F site, F is bonded in a distorted single-bond geometry to one Pd atom. In the ninth F site, F is bonded in a single-bond geometry to one Xe atom. In the tenth F site, F is bonded in a single-bond geometry to one Pd atom. In the eleventh F site, F is bonded in a single-bond geometry to one Pd atom. In the twelfth F site, F is bonded in a single-bond geometry to one Xe atom. In the thirteenth F site, F is bonded in a distorted bent 150 degrees geometry to one Xe and one Pd atom. In the fourteenth F site, F is bonded in a single-bond geometry to one Xe atom. In the fifteenth F site, F is bonded in a distorted bent 150 degrees geometry to one Xe and one Pd atom. In the sixteenth F site, F is bonded in a single-bond geometry to one Xe atom.
DOI: 10.17188/1280905
title: Materials Data on As3Pb5ClO9 by Materials Project

description: Pb5As3O9Cl crystallizes in the hexagonal P6_3 space group. The structure is three-dimensional. there are three inequivalent Pb2+ sites. In the first Pb2+ site, Pb2+ is bonded in a 4-coordinate geometry to three O2- and one Cl1- atom. There are two shorter (2.30 Å) and one longer (2.64 Å) Pb–O bond lengths. The Pb–Cl bond length is 3.04 Å. In the second Pb2+ site, Pb2+ is bonded in a 7-coordinate geometry to six O2- and one Cl1- atom. There are three shorter (2.67 Å) and three longer (2.76 Å) Pb–O bond lengths. The Pb–Cl bond length is 2.92 Å. In the third Pb2+ site, Pb2+ is bonded to six equivalent O2- atoms to form distorted face-sharing PbO6 octahedra. There are three shorter (2.43 Å) and three longer (2.91 Å) Pb–O bond lengths. As3+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There are a spread of As–O bond distances ranging from 1.79–1.83 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to three Pb2+ and one As3+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to two Pb2+ and one As3+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two Pb2+ and one As3+ atom. Cl1- is bonded in a trigonal pyramidal geometry to four Pb2+ atoms.
DOI: 10.17188/1280906
title: Materials Data on Cu3SbS4 by Materials Project

description: Cu3SbS4 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Cu1+ sites. In the first Cu1+ site, Cu1+ is bonded in a square co-planar geometry to four equivalent S2- atoms. All Cu–S bond lengths are 2.57 Å. In the second Cu1+ site, Cu1+ is bonded in a square co-planar geometry to four equivalent S2- atoms. All Cu–S bond lengths are 2.57 Å. Sb5+ is bonded in a tetrahedral geometry to four equivalent S2- atoms. All Sb–S bond lengths are 2.37 Å. S2- is bonded in a 4-coordinate geometry to three equivalent Cu1+ and one Sb5+ atom.
DOI: 10.3886/e131161
title: Construct Confounding

description: Identifying which early mathematics skills have the largest effects on later mathematics achievement has important implica- tions. However, regression-based estimates often rely on untested assumptions: (a) Scores on different mathematics skills reflect unique constructs, and (b) other factors affecting early and later mathematics achievement are fully controlled. We illustrate a process to test these assumptions with a sample of third and fourth graders who completed measures of mathemat- ics skills, working memory and motivation, and standardized mathematics and English language arts tests. Factor analyses indicated that mathematics skills largely reflect the same underlying construct. The skills that loaded highest on the general factor most predicted both later mathematics and English language arts, even after adjusting for working memory and moti- vation. Findings suggest that relations between earlier mathematics and later achievement largely reflected more general factors that contribute to children’s learning. We discuss the importance of establishing construct validity in correlational studies.
DOI: 10.3886/e131161v1
title: Construct Confounding

description: Identifying which early mathematics skills have the largest effects on later mathematics achievement has important implica- tions. However, regression-based estimates often rely on untested assumptions: (a) Scores on different mathematics skills reflect unique constructs, and (b) other factors affecting early and later mathematics achievement are fully controlled. We illustrate a process to test these assumptions with a sample of third and fourth graders who completed measures of mathemat- ics skills, working memory and motivation, and standardized mathematics and English language arts tests. Factor analyses indicated that mathematics skills largely reflect the same underlying construct. The skills that loaded highest on the general factor most predicted both later mathematics and English language arts, even after adjusting for working memory and moti- vation. Findings suggest that relations between earlier mathematics and later achievement largely reflected more general factors that contribute to children’s learning. We discuss the importance of establishing construct validity in correlational studies.
DOI: 10.3886/e131081
title: The Effect of Graphics on Reading Comprehension

description: Coding sheet
DOI: 10.3886/e131081v1
title: The Effect of Graphics on Reading Comprehension

description: Coding sheet
DOI: 10.17188/1280908
title: Materials Data on KVS2O9 (SG:19) 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: 10.17188/1280909
title: Materials Data on CaSiO3 by Materials Project

description: CaSiO3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Ca–O bond distances ranging from 2.27–2.69 Å. In the second Ca2+ site, Ca2+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Ca–O bond distances ranging from 2.16–2.40 Å. In the third Ca2+ site, Ca2+ is bonded in a 2-coordinate geometry to five O2- atoms. There are a spread of Ca–O bond distances ranging from 2.17–2.70 Å. There are three inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. In the third Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.63–1.72 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to two Ca2+ and one Si4+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Ca2+ and two Si4+ atoms. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Si4+ atoms. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to two Ca2+ and one Si4+ atom. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to one Ca2+ and two Si4+ atoms. In the sixth O2- site, O2- is bonded in a 1-coordinate geometry to two Ca2+ and one Si4+ atom. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to two Ca2+ and one Si4+ atom. In the eighth O2- site, O2- is bonded in a 1-coordinate geometry to two Ca2+ and one Si4+ atom. In the ninth O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Ca2+ and one Si4+ atom.
DOI: 10.17188/1280911
title: Materials Data on Ce9(Ni13P6)2 by Materials Project

description: Ce9(Ni13P6)2 crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. there are three inequivalent Ce sites. In the first Ce site, Ce is bonded in a 8-coordinate geometry to ten Ni and six P atoms. There are a spread of Ce–Ni bond distances ranging from 2.98–3.14 Å. There are two shorter (2.95 Å) and four longer (2.99 Å) Ce–P bond lengths. In the second Ce site, Ce is bonded in a 12-coordinate geometry to ten Ni and four equivalent P atoms. There are a spread of Ce–Ni bond distances ranging from 3.00–3.13 Å. All Ce–P bond lengths are 2.97 Å. In the third Ce site, Ce is bonded in a 12-coordinate geometry to twelve Ni and four equivalent P atoms. There are a spread of Ce–Ni bond distances ranging from 2.87–3.17 Å. All Ce–P bond lengths are 3.09 Å. There are eight inequivalent Ni sites. In the first Ni site, Ni is bonded in a 9-coordinate geometry to six equivalent Ce and three equivalent Ni atoms. All Ni–Ni bond lengths are 2.40 Å. In the second Ni site, Ni is bonded to four Ce and four P atoms to form a mixture of distorted edge, corner, and face-sharing NiCe4P4 tetrahedra. There are a spread of Ni–P bond distances ranging from 2.31–2.36 Å. In the third Ni site, Ni is bonded in a 3-coordinate geometry to three Ce, one Ni, and three P atoms. The Ni–Ni bond length is 2.49 Å. There are one shorter (2.24 Å) and two longer (2.35 Å) Ni–P bond lengths. In the fourth Ni site, Ni is bonded in a 10-coordinate geometry to two equivalent Ce and eight Ni atoms. There are two shorter (2.44 Å) and four longer (2.45 Å) Ni–Ni bond lengths. In the fifth Ni site, Ni is bonded in a distorted single-bond geometry to two equivalent Ce, four equivalent Ni, and one P atom. The Ni–P bond length is 2.17 Å. In the sixth Ni site, Ni is bonded to four Ce and four P atoms to form a mixture of distorted edge, corner, and face-sharing NiCe4P4 tetrahedra. There are two shorter (2.31 Å) and two longer (2.33 Å) Ni–P bond lengths. In the seventh Ni site, Ni is bonded in a 2-coordinate geometry to six Ce, one Ni, and two equivalent P atoms. Both Ni–P bond lengths are 2.25 Å. In the eighth Ni site, Ni is bonded in a 3-coordinate geometry to six equivalent Ce and three equivalent P atoms. All Ni–P bond lengths are 2.31 Å. There are three inequivalent P sites. In the first P site, P is bonded in a 9-coordinate geometry to four equivalent Ce and five Ni atoms. In the second P site, P is bonded in a 9-coordinate geometry to two equivalent Ce and seven Ni atoms. In the third P site, P is bonded in a 9-coordinate geometry to four Ce and five Ni atoms.
DOI: 10.17188/1280912
title: Materials Data on NaAlSiO4 by Materials Project

description: NaAlSiO4 crystallizes in the hexagonal P6_3 space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in an octahedral geometry to six O2- atoms. There are three shorter (2.46 Å) and three longer (2.58 Å) Na–O bond lengths. In the second Na1+ site, Na1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Na–O bond distances ranging from 2.33–2.73 Å. There are two inequivalent Al3+ sites. In the first Al3+ site, Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share a cornercorner with one SiO4 tetrahedra. All Al–O bond lengths are 1.75 Å. In the second Al3+ site, Al3+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There are a spread of Al–O bond distances ranging from 1.75–1.82 Å. There are two inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one AlO4 tetrahedra. There is one shorter (1.63 Å) and three longer (1.64 Å) Si–O bond length. In the second Si4+ site, Si4+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There are a spread of Si–O bond distances ranging from 1.64–1.74 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Al3+, and one Si4+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Al3+, and one Si4+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Si4+, and one O2- atom. The O–O bond length is 1.50 Å. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two Na1+, one Al3+, and one Si4+ atom. In the fifth O2- site, O2- is bonded in a distorted linear geometry to three equivalent Na1+, one Al3+, and one Si4+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Al3+, and one O2- atom.
DOI: 10.17188/1280913
title: Materials Data on NbO2 by Materials Project

description: NbO2 crystallizes in the tetragonal I4_1/a space group. The structure is three-dimensional. there are two inequivalent Nb4+ sites. In the first Nb4+ site, Nb4+ is bonded to four O2- atoms to form distorted corner-sharing NbO4 trigonal pyramids. There are a spread of Nb–O bond distances ranging from 1.74–2.23 Å. In the second Nb4+ site, Nb4+ is bonded to five O2- atoms to form distorted NbO5 trigonal bipyramids that share corners with five equivalent NbO4 trigonal pyramids and edges with two equivalent NbO5 trigonal bipyramids. There are a spread of Nb–O bond distances ranging from 1.85–2.09 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one Nb4+ atom. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Nb4+ atoms. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to two Nb4+ atoms. In the fourth O2- site, O2- is bonded in a distorted T-shaped geometry to three Nb4+ atoms.
DOI: 10.17188/1280916
title: Materials Data on AgAsS6N4(OF3)2 by Materials Project

description: AgAsN4S6(OF3)2 crystallizes in the orthorhombic Pcca space group. The structure is two-dimensional and consists of one AgAsN4S6(OF3)2 sheet oriented in the (0, 1, 0) direction. Ag1+ is bonded in a 6-coordinate geometry to two equivalent N4+, two equivalent O2-, and two equivalent F1- atoms. Both Ag–N bond lengths are 2.32 Å. Both Ag–O bond lengths are 2.57 Å. Both Ag–F bond lengths are 2.86 Å. As5+ is bonded in an octahedral geometry to six F1- atoms. All As–F bond lengths are 1.78 Å. There are two inequivalent N4+ sites. In the first N4+ site, N4+ is bonded in a bent 120 degrees geometry to two S2- atoms. There is one shorter (1.56 Å) and one longer (1.61 Å) N–S bond length. In the second N4+ site, N4+ is bonded in a distorted bent 120 degrees geometry to one Ag1+ and two S2- atoms. There is one shorter (1.62 Å) and one longer (1.67 Å) N–S bond length. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted water-like geometry to one N4+ and one O2- atom. The S–O bond length is 1.48 Å. In the second S2- site, S2- is bonded in a water-like geometry to two N4+ atoms. In the third S2- site, S2- is bonded in a 1-coordinate geometry to one N4+ atom. O2- is bonded in a 1-coordinate geometry to one Ag1+ and one S2- atom. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a single-bond geometry to one As5+ atom. In the second F1- site, F1- is bonded in a single-bond geometry to one As5+ atom. In the third F1- site, F1- is bonded in a distorted single-bond geometry to one Ag1+ and one As5+ atom.
DOI: 10.17188/1280917
title: Materials Data on CuSbPbS3 by Materials Project

description: PbCuSbS3 crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. Cu1+ is bonded to four S2- atoms to form corner-sharing CuS4 tetrahedra. There are a spread of Cu–S bond distances ranging from 2.30–2.39 Å. There are two inequivalent Pb2+ sites. In the first Pb2+ site, Pb2+ is bonded in a 6-coordinate geometry to six S2- atoms. There are a spread of Pb–S bond distances ranging from 2.84–3.56 Å. In the second Pb2+ site, Pb2+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Pb–S bond distances ranging from 2.85–3.39 Å. There are two inequivalent Sb3+ sites. In the first Sb3+ site, Sb3+ is bonded in a distorted T-shaped geometry to three S2- atoms. There are two shorter (2.49 Å) and one longer (2.50 Å) Sb–S bond lengths. In the second Sb3+ site, Sb3+ is bonded in a distorted T-shaped geometry to three S2- atoms. There are one shorter (2.47 Å) and two longer (2.49 Å) Sb–S bond lengths. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted trigonal pyramidal geometry to two equivalent Cu1+, one Pb2+, and one Sb3+ atom. In the second S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent Cu1+, two Pb2+, and one Sb3+ atom. In the third S2- site, S2- is bonded in a 2-coordinate geometry to one Cu1+, two Pb2+, and one Sb3+ atom. In the fourth S2- site, S2- is bonded in a 2-coordinate geometry to one Cu1+, three Pb2+, and one Sb3+ atom.
DOI: 10.17188/1280918
title: Materials Data on CoCu2GeS4 by Materials Project

description: Cu2CoGeS4 is Stannite structured and crystallizes in the tetragonal I-42m space group. The structure is three-dimensional. Co2+ is bonded to four equivalent S2- atoms to form CoS4 tetrahedra that share corners with four equivalent GeS4 tetrahedra and corners with eight equivalent CuS4 tetrahedra. All Co–S bond lengths are 2.26 Å. Cu1+ is bonded to four equivalent S2- atoms to form CuS4 tetrahedra that share corners with four equivalent CoS4 tetrahedra, corners with four equivalent CuS4 tetrahedra, and corners with four equivalent GeS4 tetrahedra. All Cu–S bond lengths are 2.28 Å. Ge4+ is bonded to four equivalent S2- atoms to form GeS4 tetrahedra that share corners with four equivalent CoS4 tetrahedra and corners with eight equivalent CuS4 tetrahedra. All Ge–S bond lengths are 2.31 Å. S2- is bonded to one Co2+, two equivalent Cu1+, and one Ge4+ atom to form corner-sharing SCoCu2Ge tetrahedra.
DOI: 10.17188/1280928
title: Materials Data on Sn(S4I)4 by Materials Project

description: Sn(S)16(I)4 crystallizes in the orthorhombic Fdd2 space group. The structure is zero-dimensional and consists of eight 7440-31-5 molecules, thirty-two hydriodic acid molecules, and sixteen octasulfur molecules.
DOI: 10.17188/1280929
title: Materials Data on BaLiBO3 by Materials Project

description: LiBaBO3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded to five O2- atoms to form a mixture of distorted edge and corner-sharing LiO5 trigonal bipyramids. There are a spread of Li–O bond distances ranging from 2.00–2.23 Å. Ba2+ is bonded in a 6-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.73–3.29 Å. 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. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to one Li1+, three equivalent Ba2+, and one B3+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Li1+, three equivalent Ba2+, and one B3+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Li1+, three equivalent Ba2+, and one B3+ atom.
DOI: 10.17188/1280930
title: Materials Data on V2Te2O9 (SG:43) 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: 10.17188/1280931
title: Materials Data on CsPr(MoO4)2 (SG:49) 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: 10.17188/1280932
title: Materials Data on BaCeC2O6F (SG:166) 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