cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.3886/e131481
title: Who’s Taking What? “Applied STEM” Coursetaking for High School Students with Learning Disabilities

description: Increasing and improving the science, technology, engineering, and mathematics (STEM) educational pipeline has been a point of emphasis for decades, and federal policy in the United States has urged high schools to embed new types of STEM courses into the curriculum. As one example, applied STEM courses – one growing branch within career and technical education (CTE) – are designed to reinforce traditional academic STEM content and to motivate students’ interests and long-term pursuits in STEM areas. That said, little is known about who takes these courses, and applied-STEM-CTE enrollment in these courses has not been explored in the research for students with learning disabilities. Using the High School Longitudinal Study (a nationally representative data set of high school students), we asked whether CTE coursetaking differed for students with learning disabilities compared to those without disabilities, and whether there were specific coursetaking differences in applied-STEM-CTE. We found that students with learning disabilities were more likely to earn more units in CTE courses compared to students without disabilities. Yet, when looking at applied-STEM-CTE courses, we see that although students with learning disabilities earn more CTE units than students without disabilities, students with learning disabilities do not take different amounts of applied-STEM-CTE courses. <br>
description: high school students<br>.
DOI: 10.3886/e131481v1
title: Who’s Taking What? “Applied STEM” Coursetaking for High School Students with Learning Disabilities

description: Increasing and improving the science, technology, engineering, and mathematics (STEM) educational pipeline has been a point of emphasis for decades, and federal policy in the United States has urged high schools to embed new types of STEM courses into the curriculum. As one example, applied STEM courses – one growing branch within career and technical education (CTE) – are designed to reinforce traditional academic STEM content and to motivate students’ interests and long-term pursuits in STEM areas. That said, little is known about who takes these courses, and applied-STEM-CTE enrollment in these courses has not been explored in the research for students with learning disabilities. Using the High School Longitudinal Study (a nationally representative data set of high school students), we asked whether CTE coursetaking differed for students with learning disabilities compared to those without disabilities, and whether there were specific coursetaking differences in applied-STEM-CTE. We found that students with learning disabilities were more likely to earn more units in CTE courses compared to students without disabilities. Yet, when looking at applied-STEM-CTE courses, we see that although students with learning disabilities earn more CTE units than students without disabilities, students with learning disabilities do not take different amounts of applied-STEM-CTE courses. <br>
description: high school students<br>.
DOI: 10.17188/1749821
title: Materials Data on KLiMnPCO7 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: 10.17188/1749822
title: Materials Data on ZnCoO3 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: 10.3886/e131561v1
title: Community Response to Solar

description: In order to learn what the most common community reactions were to utility-scale solar energy projects in Michigan, Wisconsin, Minnesota, and Indiana, this study conducts a content analysis of locally-based newspaper articles. The data collection of articles was generated through a keyword search of all local newspaper articles in each targeted state from 1 January 2019 [M1] to 12 May 2020, a time period intended to capture the most recent experiences with solar at the genesis of this research project in Summer of 2020. In order to ensure that this study captured all of the newspaper mentions of utility-scale solar developments within these dates, a variety of terms for solar projects were tested. Ultimately, the terms “solar farm,” “solar development” and “solar project”—each in both the singular and plural form—provided the most full and focused sample. The data sample, as of 1/1/2019 to 5/12/2020, resulted in 153 articles for Michigan, 246 articles for Wisconsin, 149 articles for Minnesota, and 244 articles for Indiana.
DOI: 10.17188/1749823
title: Materials Data on Ge(SeO3)2 by Materials Project

description: Ge(SeO3)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ge4+ is bonded in an octahedral geometry to six O2- atoms. There is four shorter (1.92 Å) and two longer (1.94 Å) Ge–O bond length. Se4+ is bonded in a distorted T-shaped geometry to three O2- atoms. There are a spread of Se–O bond distances ranging from 1.74–1.76 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to one Ge4+ and one Se4+ atom. In the second O2- site, O2- is bonded in a bent 120 degrees geometry to one Ge4+ and one Se4+ atom. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to one Ge4+ and one Se4+ atom.
DOI: 10.3886/e126681v1
title: Data and Code for: "City Limits: What Do Local-Area Minimum Wages Do?"

description: Cities are increasingly setting their own minimum wages, and this trend has accelerated sharply in recent years. While in 2010 there were only three cities with their own minimum wages exceeding the state or federal standard, by 2020 there were 42. This new phenomenon raises the question: is it desirable to have city-level variation in minimum wage polices? We discuss the main trade-offs emerging from local variation in minimum wage polices and evaluate their empirical relevance. First, we document what type of cities raise minimum wages and we discuss how these characteristics can potentially impact the effectiveness of city-level minimum wage policies. Second, we summarize the evolving evidence on city-level minimum wage changes and provide some new evidence of our own. Early evidence suggests that the impact of the policy on wages and employment to date has been broadly similar to the evidence on state and federal-level minimum wage changes. Overall, city-level minimum wages seem to be able to tailor the policy to local economic environment without imposing substantial distortions in allocation of labor and businesses across locations.
description: Working age US population. Smallest Geographic Unit: City
DOI: 10.17188/1749824
title: Materials Data on K2YAgBr6 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: 10.17188/1749826
title: Materials Data on CsGe2N3 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: 10.3886/e119446v54
title: COVID-19 US State Policy Database

description: For questions or comments about the database please contact:<br>Alexandra Skinner <br>skinnera@bu.edu <br>Research Fellow & Database Manager<br>Department of Health Law, Policy & Management <br>Boston University School of Public Health<br><br>Database of state policies on closures, shelter-in-place orders, housing protections, changes to Medicaid and SNAP, physical distancing closures, reopening, and more created by researchers at the Boston University School of Public Health. Policies included are state-wide directives or mandates, not guidance or recommendations. In order for a policy to be included, it must apply to the entire state. We are working quickly to go through state government websites to make the policy database as complete and accurate as possible in a rapidly changing policy context. If you use data on a given policy, we encourage you to triangulate based on additional sources of policy data and to review the source documentation to consider the coding decisions that are right for your work. Of course, please email us if you note a discrepancy so we can improve the database for everyone. State policy source documentation can be found at: tinyurl.com/statepolicysources.
description: other; Contributors: Megan Cole Brahim, Noa Krawczyk, Carolyn Hoffman, Claire Corkish, Elizabeth Ferrara, Elizabeth Long, Emily Baroni, Faith Contador, Hannah Simon, Morgan Simko, Rachel Scheckman, Sarah Brewer, Sue Kulkarni, Felicia Heykoop, Manish Patel, Aishwarya Vidyasagaran, Andrew Chiao, Cara Safon, Samantha Burkhart, Harry Jung, Victor Lee, Marina MacKinnon, Aarohi Rede, Marie Vearling, Sophie Li, Christina Wang, Tim Levengood, María Jordán P. Emma Chistolini
description: State policies. Smallest Geographic Unit: State
DOI: 10.17188/1749828
title: Materials Data on Pr3InFeS7 by Materials Project

description: Pr3FeInS7 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are three inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Pr–S bond distances ranging from 2.85–3.12 Å. In the second Pr3+ site, Pr3+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Pr–S bond distances ranging from 2.85–3.12 Å. In the third Pr3+ site, Pr3+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Pr–S bond distances ranging from 2.85–3.12 Å. Fe2+ is bonded to six S2- atoms to form face-sharing FeS6 octahedra. There are a spread of Fe–S bond distances ranging from 2.50–2.57 Å. In3+ is bonded in a tetrahedral geometry to four S2- atoms. There are a spread of In–S bond distances ranging from 2.43–2.48 Å. There are seven inequivalent S2- sites. In the first S2- site, S2- is bonded to three Pr3+ and two equivalent Fe2+ atoms to form distorted SPr3Fe2 square pyramids that share corners with two equivalent SPr3Fe2 square pyramids, corners with three equivalent SPr3In tetrahedra, edges with four SPr3Fe2 square pyramids, and faces with two SPr3Fe2 square pyramids. In the second S2- site, S2- is bonded to three Pr3+ and two equivalent Fe2+ atoms to form distorted SPr3Fe2 square pyramids that share corners with two equivalent SPr3Fe2 square pyramids, corners with three equivalent SPr3In tetrahedra, edges with four SPr3Fe2 square pyramids, and faces with two SPr3Fe2 square pyramids. In the third S2- site, S2- is bonded to three Pr3+ and two equivalent Fe2+ atoms to form distorted SPr3Fe2 square pyramids that share corners with two equivalent SPr3Fe2 square pyramids, corners with three equivalent SPr3In tetrahedra, edges with four SPr3Fe2 square pyramids, and faces with two SPr3Fe2 square pyramids. In the fourth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Pr3+ and one In3+ atom. In the fifth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Pr3+ and one In3+ atom. In the sixth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Pr3+ and one In3+ atom. In the seventh S2- site, S2- is bonded to three Pr3+ and one In3+ atom to form corner-sharing SPr3In tetrahedra.
DOI: 10.17188/1749830
title: Materials Data on Na3CoPCO7 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: 10.17188/1749831
title: Materials Data on Rb3HoCl6 by Materials Project

description: Rb3HoCl6 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are three inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.53–3.84 Å. In the second Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.25–3.68 Å. In the third Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.29–3.71 Å. There are two inequivalent Ho3+ sites. In the first Ho3+ site, Ho3+ is bonded in an octahedral geometry to six Cl1- atoms. There are two shorter (2.61 Å) and four longer (2.65 Å) Ho–Cl bond lengths. In the second Ho3+ site, Ho3+ is bonded in an octahedral geometry to six Cl1- atoms. There are two shorter (2.64 Å) and four longer (2.66 Å) Ho–Cl bond lengths. There are six inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Ho3+ atom. In the second Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Ho3+ atom. In the third Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Ho3+ atom. In the fourth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Ho3+ atom. In the fifth Cl1- site, Cl1- is bonded in a 1-coordinate geometry to four Rb1+ and one Ho3+ atom. In the sixth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Ho3+ atom.
DOI: 10.17188/1749833
title: Materials Data on Al2HgS4 by Materials Project

description: HgAl2S4 is Spinel structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Hg2+ is bonded to four equivalent S2- atoms to form HgS4 tetrahedra that share corners with twelve equivalent AlS6 octahedra. The corner-sharing octahedral tilt angles are 60°. All Hg–S bond lengths are 2.53 Å. Al3+ is bonded to six equivalent S2- atoms to form AlS6 octahedra that share corners with six equivalent HgS4 tetrahedra and edges with six equivalent AlS6 octahedra. All Al–S bond lengths are 2.45 Å. S2- is bonded to one Hg2+ and three equivalent Al3+ atoms to form a mixture of distorted corner and edge-sharing SAl3Hg tetrahedra.
DOI: 10.17188/1749834
title: Materials Data on Ce3In4Ge by Materials Project

description: Ce3In4Ge crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. there are two inequivalent Ce sites. In the first Ce site, Ce is bonded in a 8-coordinate geometry to six equivalent In and two equivalent Ge atoms. There are two shorter (3.09 Å) and four longer (3.32 Å) Ce–In bond lengths. Both Ce–Ge bond lengths are 3.12 Å. In the second Ce site, Ce is bonded in a 2-coordinate geometry to eight equivalent In and two equivalent Ge atoms. All Ce–In bond lengths are 3.29 Å. Both Ce–Ge bond lengths are 2.89 Å. In is bonded in a 1-coordinate geometry to five Ce and three equivalent In atoms. There are two shorter (2.88 Å) and one longer (2.95 Å) In–In bond lengths. Ge is bonded to six Ce atoms to form corner-sharing GeCe6 octahedra. The corner-sharing octahedra tilt angles range from 0–38°.
DOI: 10.17188/1749835
title: Materials Data on CsLi2Cl3 by Materials Project

description: CsLi2Cl3 crystallizes in the orthorhombic Pbcn space group. The structure is three-dimensional. Cs1+ is bonded in a 10-coordinate geometry to ten Cl1- atoms. There are a spread of Cs–Cl bond distances ranging from 3.56–4.03 Å. Li1+ is bonded to four Cl1- atoms to form corner-sharing LiCl4 tetrahedra. There are a spread of Li–Cl bond distances ranging from 2.36–2.40 Å. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted linear geometry to four equivalent Cs1+ and two equivalent Li1+ atoms. In the second Cl1- site, Cl1- is bonded in a distorted trigonal planar geometry to three equivalent Cs1+ and three equivalent Li1+ atoms.
DOI: 10.17188/1749836
title: Materials Data on Mg2AgPd by Materials Project

description: Mg2PdAg crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Mg2PdAg ribbons oriented in the (1, 0, 0) direction. Mg is bonded in a linear geometry to one Pd and one Ag atom. The Mg–Pd bond length is 2.46 Å. The Mg–Ag bond length is 2.66 Å. Pd is bonded in a linear geometry to two equivalent Mg atoms. Ag is bonded in a linear geometry to two equivalent Mg atoms.
DOI: 10.17188/1749837
title: Materials Data on Th2SiGe by Materials Project

description: Th2GeSi crystallizes in the orthorhombic Pmc2_1 space group. The structure is three-dimensional. there are two inequivalent Th sites. In the first Th site, Th is bonded in a 7-coordinate geometry to three equivalent Ge and four equivalent Si atoms. There are a spread of Th–Ge bond distances ranging from 3.12–3.28 Å. There are two shorter (3.05 Å) and two longer (3.09 Å) Th–Si bond lengths. In the second Th site, Th is bonded in a 7-coordinate geometry to four equivalent Ge and three equivalent Si atoms. There are two shorter (3.07 Å) and two longer (3.09 Å) Th–Ge bond lengths. There are a spread of Th–Si bond distances ranging from 3.07–3.30 Å. Ge is bonded in a 9-coordinate geometry to seven Th and two equivalent Si atoms. Both Ge–Si bond lengths are 2.80 Å. Si is bonded in a 9-coordinate geometry to seven Th and two equivalent Ge atoms.
DOI: 10.17188/1749838
title: Materials Data on RbSmI3 by Materials Project

description: RbSmI3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Rb1+ is bonded in a 8-coordinate geometry to eight I1- atoms. There are a spread of Rb–I bond distances ranging from 3.73–4.08 Å. Sm2+ is bonded to six I1- atoms to form a mixture of corner and edge-sharing SmI6 octahedra. The corner-sharing octahedral tilt angles are 39°. There are two shorter (3.17 Å) and four longer (3.19 Å) Sm–I bond lengths. There are two inequivalent I1- sites. In the first I1- site, I1- is bonded in a 5-coordinate geometry to three equivalent Rb1+ and two equivalent Sm2+ atoms. In the second I1- site, I1- is bonded in a 4-coordinate geometry to two equivalent Rb1+ and two equivalent Sm2+ atoms.
DOI: 10.17188/1749840
title: Materials Data on NbV3Fe2(PO4)6 by Materials Project

description: NbV3Fe2(PO4)6 crystallizes in the trigonal R3 space group. The structure is three-dimensional. Nb5+ is bonded to six O2- atoms to form NbO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.95 Å) and three longer (2.06 Å) Nb–O bond lengths. There are three inequivalent V+2.33+ sites. In the first V+2.33+ site, V+2.33+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.98 Å) and three longer (2.09 Å) V–O bond lengths. In the second V+2.33+ site, V+2.33+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.96 Å) and three longer (2.08 Å) V–O bond lengths. In the third V+2.33+ site, V+2.33+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.99 Å) and three longer (2.06 Å) V–O bond lengths. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are three shorter (2.17 Å) and three longer (2.34 Å) Fe–O bond lengths. In the second Fe3+ site, Fe3+ is bonded in a 6-coordinate geometry to six O2- atoms. All Fe–O bond lengths are 2.23 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one NbO6 octahedra and corners with three VO6 octahedra. The corner-sharing octahedra tilt angles range from 22–50°. There are a spread of P–O bond distances ranging from 1.51–1.58 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one NbO6 octahedra and corners with three VO6 octahedra. The corner-sharing octahedra tilt angles range from 27–47°. There are a spread of P–O bond distances ranging from 1.52–1.60 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one V+2.33+ and one P5+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one V+2.33+, one Fe3+, and one P5+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Nb5+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one V+2.33+, one Fe3+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one V+2.33+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Nb5+, one Fe3+, and one P5+ atom. In the seventh O2- site, O2- is bonded in a 3-coordinate geometry to one V+2.33+, one Fe3+, and one P5+ atom. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one V+2.33+ and one P5+ atom.
DOI: 10.17188/1749841
title: Materials Data on YbGa2Cu3 by Materials Project

description: YbCu3Ga2 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Yb is bonded in a 6-coordinate geometry to twelve equivalent Cu and six equivalent Ga atoms. All Yb–Cu bond lengths are 3.30 Å. All Yb–Ga bond lengths are 3.02 Å. Cu is bonded to four equivalent Yb, four equivalent Cu, and four equivalent Ga atoms to form a mixture of corner, edge, and face-sharing CuYb4Ga4Cu4 cuboctahedra. All Cu–Cu bond lengths are 2.62 Å. All Cu–Ga bond lengths are 2.52 Å. Ga is bonded in a 9-coordinate geometry to three equivalent Yb and six equivalent Cu atoms.
DOI: 10.17188/1749842
title: Materials Data on RbP by Materials Project

description: PRb is Halite, Rock Salt structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Rb1+ is bonded to six equivalent P1- atoms to form a mixture of edge and corner-sharing RbP6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–P bond lengths are 3.53 Å. P1- is bonded to six equivalent Rb1+ atoms to form a mixture of edge and corner-sharing PRb6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1749982
title: Materials Data on CsEuSiS4 by Materials Project

description: CsEuSiS4 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Cs1+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Cs–S bond distances ranging from 3.56–3.89 Å. Eu3+ is bonded to seven S2- atoms to form distorted EuS7 pentagonal bipyramids that share corners with two equivalent EuS7 pentagonal bipyramids, a cornercorner with one SiS4 tetrahedra, edges with two equivalent EuS7 pentagonal bipyramids, and edges with three equivalent SiS4 tetrahedra. There are a spread of Eu–S bond distances ranging from 2.88–3.03 Å. Si4+ is bonded to four S2- atoms to form SiS4 tetrahedra that share a cornercorner with one EuS7 pentagonal bipyramid and edges with three equivalent EuS7 pentagonal bipyramids. There are a spread of Si–S bond distances ranging from 2.12–2.15 Å. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a 5-coordinate geometry to three equivalent Cs1+, one Eu3+, and one Si4+ atom. In the second S2- site, S2- is bonded in a 4-coordinate geometry to one Cs1+, two equivalent Eu3+, and one Si4+ atom. In the third S2- site, S2- is bonded in a 1-coordinate geometry to two equivalent Cs1+, two equivalent Eu3+, and one Si4+ atom. In the fourth S2- site, S2- is bonded in a 1-coordinate geometry to two equivalent Cs1+, two equivalent Eu3+, and one Si4+ atom.