cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1749798
title: Materials Data on Li3Fe5(NiO6)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: 10.17188/1749802
title: Materials Data on La3Ir2 by Materials Project

description: La3Ir2 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. there are three inequivalent La sites. In the first La site, La is bonded in an octahedral geometry to six equivalent Ir atoms. All La–Ir bond lengths are 3.10 Å. In the second La site, La is bonded in a 6-coordinate geometry to six equivalent Ir atoms. There are three shorter (2.95 Å) and three longer (3.17 Å) La–Ir bond lengths. In the third La site, La is bonded in a 5-coordinate geometry to five equivalent Ir atoms. There are a spread of La–Ir bond distances ranging from 2.95–3.37 Å. Ir is bonded in a 8-coordinate geometry to eight La atoms.
DOI: 10.17188/1749803
title: Materials Data on YbCuPbS3 by Materials Project

description: YbCuPbS3 crystallizes in the orthorhombic Cmc2_1 space group. The structure is three-dimensional. Yb3+ is bonded to six S2- atoms to form YbS6 octahedra that share corners with two equivalent YbS6 octahedra, edges with two equivalent YbS6 octahedra, and edges with four equivalent CuS4 tetrahedra. The corner-sharing octahedral tilt angles are 40°. There are two shorter (2.78 Å) and four longer (2.79 Å) Yb–S bond lengths. Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with two equivalent CuS4 tetrahedra and edges with four equivalent YbS6 octahedra. There are three shorter (2.32 Å) and one longer (2.33 Å) Cu–S bond lengths. Pb2+ is bonded in a 6-coordinate geometry to six S2- atoms. There are a spread of Pb–S bond distances ranging from 2.94–3.11 Å. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a 6-coordinate geometry to two equivalent Yb3+, two equivalent Cu1+, and two equivalent Pb2+ atoms. In the second S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent Yb3+, one Cu1+, and two equivalent Pb2+ atoms. In the third S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent Yb3+, one Cu1+, and two equivalent Pb2+ atoms.
DOI: 10.17188/1749805
title: Materials Data on Hf4C3N by Materials Project

description: Hf4C3N is Caswellsilverite-like structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Hf sites. In the first Hf site, Hf is bonded to six C atoms to form a mixture of edge and corner-sharing HfC6 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are three shorter (2.30 Å) and three longer (2.35 Å) Hf–C bond lengths. In the second Hf site, Hf is bonded to three equivalent C and three equivalent N atoms to form a mixture of edge and corner-sharing HfC3N3 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. All Hf–C bond lengths are 2.26 Å. All Hf–N bond lengths are 2.34 Å. There are two inequivalent C sites. In the first C site, C is bonded to six Hf atoms to form CHf6 octahedra that share corners with three equivalent CHf6 octahedra, corners with three equivalent NHf6 octahedra, edges with three equivalent NHf6 octahedra, and edges with nine CHf6 octahedra. The corner-sharing octahedra tilt angles range from 2–3°. In the second C site, C is bonded to six equivalent Hf atoms to form a mixture of edge and corner-sharing CHf6 octahedra. The corner-sharing octahedral tilt angles are 2°. N is bonded to six equivalent Hf atoms to form NHf6 octahedra that share corners with six equivalent CHf6 octahedra, edges with six equivalent CHf6 octahedra, and edges with six equivalent NHf6 octahedra. The corner-sharing octahedral tilt angles are 3°.
DOI: 10.17188/1749806
title: Materials Data on Li3CoPCO7 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: 10.17188/1749807
title: Materials Data on LiMnPO4 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: 10.17188/1749808
title: Materials Data on Ho5Sb2Pd by Materials Project

description: Ho5PdSb2 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are four inequivalent Ho sites. In the first Ho site, Ho is bonded in a 5-coordinate geometry to one Pd and four equivalent Sb atoms. The Ho–Pd bond length is 2.87 Å. There are two shorter (3.15 Å) and two longer (3.16 Å) Ho–Sb bond lengths. In the second Ho site, Ho is bonded to one Pd and four equivalent Sb atoms to form a mixture of distorted edge and corner-sharing HoSb4Pd square pyramids. The Ho–Pd bond length is 2.99 Å. There are two shorter (3.12 Å) and two longer (3.13 Å) Ho–Sb bond lengths. In the third Ho site, Ho is bonded to one Pd and four equivalent Sb atoms to form a mixture of distorted edge and corner-sharing HoSb4Pd trigonal bipyramids. The Ho–Pd bond length is 2.86 Å. There are two shorter (3.19 Å) and two longer (3.21 Å) Ho–Sb bond lengths. In the fourth Ho site, Ho is bonded in a 2-coordinate geometry to two equivalent Pd and three equivalent Sb atoms. There are one shorter (2.84 Å) and one longer (2.96 Å) Ho–Pd bond lengths. There are a spread of Ho–Sb bond distances ranging from 3.30–3.56 Å. Pd is bonded in a 7-coordinate geometry to seven Ho atoms. Sb is bonded in a 9-coordinate geometry to nine Ho atoms.
DOI: 10.17188/1749809
title: Materials Data on Y(FeO2)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: 10.17188/1749810
title: Materials Data on YO3 by Materials Project

description: YO3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. Y is bonded in a 9-coordinate geometry to nine equivalent O atoms. There are three shorter (2.30 Å) and six longer (2.41 Å) Y–O bond lengths. O is bonded in a distorted trigonal planar geometry to three equivalent Y atoms.
DOI: 10.17188/1749811
title: Materials Data on Cu5Se4(ClO6)2 by Materials Project

description: Cu5Se4(O6Cl)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded to five O2- atoms to form distorted CuO5 trigonal bipyramids that share a cornercorner with one CuO6 octahedra, an edgeedge with one CuO6 octahedra, and an edgeedge with one CuCl2O3 trigonal bipyramid. The corner-sharing octahedral tilt angles are 51°. There are a spread of Cu–O bond distances ranging from 1.92–2.42 Å. In the second Cu2+ site, Cu2+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing CuO6 octahedra. There are a spread of Cu–O bond distances ranging from 1.98–2.41 Å. In the third Cu2+ site, Cu2+ is bonded to three O2- and two equivalent Cl1- atoms to form edge-sharing CuCl2O3 trigonal bipyramids. There are a spread of Cu–O bond distances ranging from 1.95–2.32 Å. There are one shorter (2.28 Å) and one longer (2.29 Å) Cu–Cl bond lengths. There are two inequivalent Se4+ sites. In the first Se4+ site, Se4+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There is one shorter (1.73 Å) and two longer (1.74 Å) Se–O bond length. In the second Se4+ site, Se4+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Se–O bond distances ranging from 1.72–1.80 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal non-coplanar geometry to two Cu2+ and one Se4+ atom. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cu2+ and one Se4+ atom. In the third O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two Cu2+ and one Se4+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Cu2+ and one Se4+ atom. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cu2+ and one Se4+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to two Cu2+ and one Se4+ atom. Cl1- is bonded in an L-shaped geometry to two equivalent Cu2+ atoms.
DOI: 10.17188/1749812
title: Materials Data on Na3MnBPO7 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: 10.17188/1749813
title: Materials Data on KCr2AgO7 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: 10.17188/1749814
title: Materials Data on MgSi2 by Materials Project

description: MgSi2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Mg sites. In the first Mg site, Mg is bonded in a 5-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.70–3.14 Å. In the second Mg site, Mg is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.77–2.96 Å. In the third Mg site, Mg is bonded in a 8-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.74–3.00 Å. In the fourth Mg site, Mg is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.73–2.99 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded in a 7-coordinate geometry to four Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.38–2.57 Å. In the second Si site, Si is bonded in a 7-coordinate geometry to three Mg and four Si atoms. There are a spread of Si–Si bond distances ranging from 2.38–2.58 Å. In the third Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.40–2.56 Å. In the fourth Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.38–2.55 Å. In the fifth Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms. In the sixth Si site, Si is bonded in a 6-coordinate geometry to two Mg and four Si atoms. In the seventh Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms. In the eighth Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms.
DOI: 10.17188/1749815
title: Materials Data on Y3Mg by Materials Project

description: MgY3 is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Mg is bonded to twelve equivalent Y atoms to form MgY12 cuboctahedra that share corners with six equivalent MgY12 cuboctahedra, corners with twelve equivalent YY8Mg4 cuboctahedra, edges with eighteen equivalent YY8Mg4 cuboctahedra, faces with eight equivalent MgY12 cuboctahedra, and faces with twelve equivalent YY8Mg4 cuboctahedra. There are six shorter (3.44 Å) and six longer (3.52 Å) Mg–Y bond lengths. Y is bonded to four equivalent Mg and eight equivalent Y atoms to form YY8Mg4 cuboctahedra that share corners with four equivalent MgY12 cuboctahedra, corners with fourteen equivalent YY8Mg4 cuboctahedra, edges with six equivalent MgY12 cuboctahedra, edges with twelve equivalent YY8Mg4 cuboctahedra, faces with four equivalent MgY12 cuboctahedra, and faces with sixteen equivalent YY8Mg4 cuboctahedra. There are a spread of Y–Y bond distances ranging from 3.45–3.59 Å.
DOI: 10.17188/1749816
title: Materials Data on Tm5(Co2Si7)2 by Materials Project

description: Tm5(Co2Si7)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Tm3+ sites. In the first Tm3+ site, Tm3+ is bonded to twelve Si+1.71- atoms to form TmSi12 cuboctahedra that share corners with four equivalent TmSi12 cuboctahedra, corners with four equivalent CoSi7 hexagonal pyramids, and faces with four equivalent CoSi7 hexagonal pyramids. There are a spread of Tm–Si bond distances ranging from 2.88–3.05 Å. In the second Tm3+ site, Tm3+ is bonded in a 10-coordinate geometry to ten Si+1.71- atoms. There are a spread of Tm–Si bond distances ranging from 2.88–3.08 Å. In the third Tm3+ site, Tm3+ is bonded in a 10-coordinate geometry to ten Si+1.71- atoms. There are a spread of Tm–Si bond distances ranging from 2.87–3.07 Å. There are two inequivalent Co+2.25+ sites. In the first Co+2.25+ site, Co+2.25+ is bonded to seven Si+1.71- atoms to form distorted CoSi7 hexagonal pyramids that share corners with two equivalent TmSi12 cuboctahedra, corners with four equivalent CoSi7 hexagonal pyramids, an edgeedge with one CoSi7 hexagonal pyramid, and faces with two equivalent TmSi12 cuboctahedra. There are a spread of Co–Si bond distances ranging from 2.27–2.49 Å. In the second Co+2.25+ site, Co+2.25+ is bonded in a 5-coordinate geometry to five Si+1.71- atoms. There are a spread of Co–Si bond distances ranging from 2.29–2.32 Å. There are seven inequivalent Si+1.71- sites. In the first Si+1.71- site, Si+1.71- is bonded in a 8-coordinate geometry to three Tm3+, two Co+2.25+, and three Si+1.71- atoms. There are a spread of Si–Si bond distances ranging from 2.41–2.59 Å. In the second Si+1.71- site, Si+1.71- is bonded in a 8-coordinate geometry to six Tm3+ and two Si+1.71- atoms. Both Si–Si bond lengths are 2.42 Å. In the third Si+1.71- site, Si+1.71- is bonded in a 9-coordinate geometry to six Tm3+, one Co+2.25+, and two Si+1.71- atoms. The Si–Si bond length is 2.40 Å. In the fourth Si+1.71- site, Si+1.71- is bonded in a 5-coordinate geometry to two equivalent Tm3+, three equivalent Co+2.25+, and four Si+1.71- atoms. There are one shorter (2.58 Å) and two longer (2.59 Å) Si–Si bond lengths. In the fifth Si+1.71- site, Si+1.71- is bonded in a 8-coordinate geometry to three Tm3+, two Co+2.25+, and three Si+1.71- atoms. The Si–Si bond length is 2.53 Å. In the sixth Si+1.71- site, Si+1.71- is bonded in a 8-coordinate geometry to three Tm3+, two Co+2.25+, and three Si+1.71- atoms. The Si–Si bond length is 2.41 Å. In the seventh Si+1.71- site, Si+1.71- is bonded in a 8-coordinate geometry to three Tm3+, two Co+2.25+, and three Si+1.71- atoms.
DOI: 10.3886/e119446v53-78440
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: 10.3886/e131361
title: Code for: Improving Financial Inclusion Through Digital Savings and Credit

description: The files here are the code and a description of where to get the data for the paper "Improving Financial Inclusion Through Digital Savings and Credit", by Prashant Bharadwaj, William Jack and Tavneet Suri, published in the AER Papers and Proceedings, May 2020. <br>
description: Credit data: random sample of 10,000 clients of the digital bank account who opened their accounts between January and March 2016, provided by Commercial Bank of Africa.<br><br>Savings data: random sample of 5,000 clients of the digital bank account who opened their accounts between January and March 2016, provided by Commercial Bank of Africa.<br>
DOI: 10.17188/1749818
title: Materials Data on La2S3O16 by Materials Project

description: La2S3O16 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent La sites. In the first La site, La is bonded in a 10-coordinate geometry to ten O atoms. There are a spread of La–O bond distances ranging from 2.41–3.18 Å. In the second La site, La is bonded in a 6-coordinate geometry to nine O atoms. There are a spread of La–O bond distances ranging from 2.39–3.10 Å. There are three inequivalent S sites. In the first S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.47–1.51 Å. In the second S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.43–1.58 Å. In the third S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.47–1.52 Å. There are sixteen inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to one La and one S atom. In the second O site, O is bonded in a distorted single-bond geometry to two La and one S atom. In the third O site, O is bonded in a 1-coordinate geometry to two La and one S atom. In the fourth O site, O is bonded in a distorted bent 150 degrees geometry to one La and one S atom. In the fifth O site, O is bonded in a distorted water-like geometry to one La and one S atom. In the sixth O site, O is bonded in a distorted bent 120 degrees geometry to one La and one S atom. In the seventh O site, O is bonded in a distorted bent 150 degrees geometry to two La and one S atom. In the eighth O site, O is bonded in a water-like geometry to one La and one S atom. In the ninth O site, O is bonded in a bent 150 degrees geometry to one La and one S atom. In the tenth O site, O is bonded in a 3-coordinate geometry to two La and one S atom. In the eleventh O site, O is bonded in a single-bond geometry to one S atom. In the twelfth O site, O is bonded in a water-like geometry to one La and one S atom. In the thirteenth O site, O is bonded in a distorted L-shaped geometry to one La and one O atom. The O–O bond length is 1.24 Å. In the fourteenth O site, O is bonded in a distorted single-bond geometry to one La and one O atom. The O–O bond length is 1.23 Å. In the fifteenth O site, O is bonded in a distorted single-bond geometry to one La and one O atom. In the sixteenth O site, O is bonded in a distorted bent 120 degrees geometry to one La and one O atom.
DOI: 10.3886/e131361v1
title: Code for: Improving Financial Inclusion Through Digital Savings and Credit

description: The files here are the code and a description of where to get the data for the paper "Improving Financial Inclusion Through Digital Savings and Credit", by Prashant Bharadwaj, William Jack and Tavneet Suri, published in the AER Papers and Proceedings, May 2020. <br>
description: Credit data: random sample of 10,000 clients of the digital bank account who opened their accounts between January and March 2016, provided by Commercial Bank of Africa.<br><br>Savings data: random sample of 5,000 clients of the digital bank account who opened their accounts between January and March 2016, provided by Commercial Bank of Africa.<br>
DOI: 10.3886/e122641
title: Data and code for: Adopting Mobile Money: Evidence from an Experiment in Rural Africa

description: Who uses mobile money, and what do people do with it? This paper describes mobile money adoption patterns following the experimental introduction of mobile money for the first time in rural areas of Southern Mozambique. We use administrative and household survey data to characterize adopters as well as their mobile money usage patterns over three years. Adopters of mobile money (and early adopters in particular) are more educated than nonadopters, and they are also more likely to already hold a bank account. Positive self-selection of adopters should be considered when introducing mobile money as a tool for rapid financial inclusion.<br>
DOI: 10.3886/e122641v1
title: Data and code for: Adopting Mobile Money: Evidence from an Experiment in Rural Africa

description: Who uses mobile money, and what do people do with it? This paper describes mobile money adoption patterns following the experimental introduction of mobile money for the first time in rural areas of Southern Mozambique. We use administrative and household survey data to characterize adopters as well as their mobile money usage patterns over three years. Adopters of mobile money (and early adopters in particular) are more educated than nonadopters, and they are also more likely to already hold a bank account. Positive self-selection of adopters should be considered when introducing mobile money as a tool for rapid financial inclusion.<br>
DOI: 10.17188/1749819
title: Materials Data on NaNiF3 by Materials Project

description: NaNiF3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Na1+ is bonded in a 8-coordinate geometry to eight F1- atoms. There are a spread of Na–F bond distances ranging from 2.30–2.58 Å. Ni2+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing NiF6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are two shorter (2.01 Å) and four longer (2.05 Å) Ni–F bond lengths. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded to two equivalent Na1+ and two equivalent Ni2+ atoms to form distorted corner-sharing FNa2Ni2 tetrahedra. In the second F1- site, F1- is bonded in a 5-coordinate geometry to three equivalent Na1+ and two equivalent Ni2+ atoms.