cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.13709919
title: Global FD Code ProcB copy from Tropical mammal functional diversity increases with productivity but decreases with anthropogenic disturbance

description: A variety of factors can affect the biodiversity of tropical mammal communities, but their relative importance and directionality remain uncertain. Previous global investigations of mammal functional diversity have relied on range maps instead of observational data to determine community composition. We test the effects of species pools, habitat heterogeneity, primary productivity and human disturbance on the functional diversity (dispersion and richness) of mammal communities using the largest standardized tropical forest camera trap monitoring system, the Tropical Ecology Assessment and Monitoring (TEAM) Network. We use occupancy values derived from the camera trap data to calculate occupancy-weighted functional diversity and use Bayesian generalized linear regression to determine the effects of multiple predictors. Mammal community functional dispersion increased with primary productivity, while functional richness decreased with human-induced local extinctions and was significantly lower in Madagascar than other tropical regions. The significant positive relationship between functional dispersion and productivity was evident only when functional dispersion was weighted by species' occupancies. Thus, observational data from standardized monitoring can reveal the drivers of mammal communities in ways that are not readily apparent from range map-based studies. The positive association between occupancy-weighted functional dispersion of tropical forest mammal communities and primary productivity suggests that unique functional traits may be more beneficial in more productive ecosystems and may allow species to persist at higher abundances.
DOI: 10.17188/1753833
title: Materials Data on LiMnPO5 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: 10.6084/m9.figshare.13709919.v1
title: Global FD Code ProcB copy from Tropical mammal functional diversity increases with productivity but decreases with anthropogenic disturbance

description: A variety of factors can affect the biodiversity of tropical mammal communities, but their relative importance and directionality remain uncertain. Previous global investigations of mammal functional diversity have relied on range maps instead of observational data to determine community composition. We test the effects of species pools, habitat heterogeneity, primary productivity and human disturbance on the functional diversity (dispersion and richness) of mammal communities using the largest standardized tropical forest camera trap monitoring system, the Tropical Ecology Assessment and Monitoring (TEAM) Network. We use occupancy values derived from the camera trap data to calculate occupancy-weighted functional diversity and use Bayesian generalized linear regression to determine the effects of multiple predictors. Mammal community functional dispersion increased with primary productivity, while functional richness decreased with human-induced local extinctions and was significantly lower in Madagascar than other tropical regions. The significant positive relationship between functional dispersion and productivity was evident only when functional dispersion was weighted by species' occupancies. Thus, observational data from standardized monitoring can reveal the drivers of mammal communities in ways that are not readily apparent from range map-based studies. The positive association between occupancy-weighted functional dispersion of tropical forest mammal communities and primary productivity suggests that unique functional traits may be more beneficial in more productive ecosystems and may allow species to persist at higher abundances.
DOI: 10.17188/1753834
title: Materials Data on Li3CoN2 by Materials Project

description: Li3CoN2 crystallizes in the cubic Ia-3 space group. The structure is three-dimensional. Li1+ is bonded to four N3- atoms to form distorted LiN4 tetrahedra that share corners with four equivalent CoN4 tetrahedra, corners with twelve equivalent LiN4 tetrahedra, edges with two equivalent CoN4 tetrahedra, and edges with four equivalent LiN4 tetrahedra. There are a spread of Li–N bond distances ranging from 2.03–2.22 Å. Co3+ is bonded to four N3- atoms to form CoN4 tetrahedra that share corners with four equivalent CoN4 tetrahedra, corners with twelve equivalent LiN4 tetrahedra, and edges with six equivalent LiN4 tetrahedra. There is one shorter (1.85 Å) and three longer (1.94 Å) Co–N bond length. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a body-centered cubic geometry to six equivalent Li1+ and two equivalent Co3+ atoms. In the second N3- site, N3- is bonded in a distorted body-centered cubic geometry to six equivalent Li1+ and two equivalent Co3+ atoms.
DOI: 10.6084/m9.figshare.13709920
title: Supplemental table 2

description: Quality of researches
DOI: 10.6084/m9.figshare.13709887
title: supplemental table 1.docx

description: Supplemental information of VSMC
DOI: 10.17188/1753835
title: Materials Data on HoRhO3 by Materials Project

description: HoRhO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Ho3+ is bonded to twelve equivalent O2- atoms to form HoO12 cuboctahedra that share corners with twelve equivalent HoO12 cuboctahedra, faces with six equivalent HoO12 cuboctahedra, and faces with eight equivalent RhO6 octahedra. All Ho–O bond lengths are 2.78 Å. Rh3+ is bonded to six equivalent O2- atoms to form RhO6 octahedra that share corners with six equivalent RhO6 octahedra and faces with eight equivalent HoO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Rh–O bond lengths are 1.97 Å. O2- is bonded to four equivalent Ho3+ and two equivalent Rh3+ atoms to form a mixture of distorted edge, corner, and face-sharing OHo4Rh2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°.
DOI: 10.17188/1753836
title: Materials Data on Nb3(Cl3O4)2 by Materials Project

description: (Nb3O7)2O2(Cl2)6 crystallizes in the cubic Fm-3m space group. The structure is zero-dimensional and consists of twenty-four chlorine molecules, eight water molecules, and four Nb3O7 clusters. In each Nb3O7 cluster, Nb is bonded in a 5-coordinate geometry to five O atoms. There is one shorter (1.73 Å) and four longer (2.10 Å) Nb–O bond length. There are two inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Nb atom. In the second O site, O is bonded in a distorted trigonal non-coplanar geometry to three equivalent Nb atoms.
DOI: 10.6084/m9.figshare.13709887.v1
title: supplemental table 1.docx

description: Supplemental information of VSMC
DOI: 10.6084/m9.figshare.13709907
title: TEAM Site Funct bi from Tropical mammal functional diversity increases with productivity but decreases with anthropogenic disturbance

description: A variety of factors can affect the biodiversity of tropical mammal communities, but their relative importance and directionality remain uncertain. Previous global investigations of mammal functional diversity have relied on range maps instead of observational data to determine community composition. We test the effects of species pools, habitat heterogeneity, primary productivity and human disturbance on the functional diversity (dispersion and richness) of mammal communities using the largest standardized tropical forest camera trap monitoring system, the Tropical Ecology Assessment and Monitoring (TEAM) Network. We use occupancy values derived from the camera trap data to calculate occupancy-weighted functional diversity and use Bayesian generalized linear regression to determine the effects of multiple predictors. Mammal community functional dispersion increased with primary productivity, while functional richness decreased with human-induced local extinctions and was significantly lower in Madagascar than other tropical regions. The significant positive relationship between functional dispersion and productivity was evident only when functional dispersion was weighted by species' occupancies. Thus, observational data from standardized monitoring can reveal the drivers of mammal communities in ways that are not readily apparent from range map-based studies. The positive association between occupancy-weighted functional dispersion of tropical forest mammal communities and primary productivity suggests that unique functional traits may be more beneficial in more productive ecosystems and may allow species to persist at higher abundances.
DOI: 10.6084/m9.figshare.13709934
title: Adaptation Data from Adaptation reduces competitive dominance and alters community assembly

description: Data used to test for adaptation to the high-temperature environment.
DOI: 10.6084/m9.figshare.13709937.v1
title: Analysis Code from Adaptation reduces competitive dominance and alters community assembly

description: The R code used to produce all the results presented in the paper.
DOI: 10.17188/1753837
title: Materials Data on Ca8TiMn7O23 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: 10.6084/m9.figshare.13709934.v1
title: Adaptation Data from Adaptation reduces competitive dominance and alters community assembly

description: Data used to test for adaptation to the high-temperature environment.
DOI: 10.6084/m9.figshare.13709937
title: Analysis Code from Adaptation reduces competitive dominance and alters community assembly

description: The R code used to produce all the results presented in the paper.
DOI: 10.17188/1753838
title: Materials Data on DySnO3 by Materials Project

description: DySnO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Dy3+ is bonded to twelve equivalent O2- atoms to form DyO12 cuboctahedra that share corners with twelve equivalent DyO12 cuboctahedra, faces with six equivalent DyO12 cuboctahedra, and faces with eight equivalent SnO6 octahedra. All Dy–O bond lengths are 2.93 Å. Sn3+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent SnO6 octahedra and faces with eight equivalent DyO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Sn–O bond lengths are 2.07 Å. O2- is bonded in a distorted linear geometry to four equivalent Dy3+ and two equivalent Sn3+ atoms.
DOI: 10.6084/m9.figshare.13709920.v1
title: Supplemental table 2

description: Quality of researches
DOI: 10.6084/m9.figshare.13709940.v1
title: Priority Effect Data from Adaptation reduces competitive dominance and alters community assembly

description: Data used to test for ecological and eco-evolutionary priority effects.
DOI: 10.17188/1753839
title: Materials Data on P3Pb5BrO12 by Materials Project

description: Pb5(PO4)3Br 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 5-coordinate geometry to six O2- and two equivalent Br1- atoms. There are a spread of Pb–O bond distances ranging from 2.39–3.18 Å. There are one shorter (3.18 Å) and one longer (3.26 Å) Pb–Br bond lengths. In the second Pb2+ site, Pb2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Pb–O bond distances ranging from 2.66–2.91 Å. In the third Pb2+ site, Pb2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Pb–O bond distances ranging from 2.66–2.91 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent BrPb6O6 cuboctahedra. There are a spread of P–O bond distances ranging from 1.55–1.58 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to three Pb2+ and one P5+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to three Pb2+, one P5+, and one Br1- atom. The O–Br bond length is 3.40 Å. In the third O2- site, O2- is bonded in a distorted single-bond geometry to three Pb2+, one P5+, and one Br1- atom. The O–Br bond length is 3.38 Å. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to three Pb2+ and one P5+ atom. Br1- is bonded to six equivalent Pb2+ and six O2- atoms to form distorted BrPb6O6 cuboctahedra that share corners with six equivalent PO4 tetrahedra and faces with two equivalent BrPb6O6 cuboctahedra.
DOI: 10.17188/1753840
title: Materials Data on ScCrO4 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: 10.6084/m9.figshare.13709940
title: Priority Effect Data from Adaptation reduces competitive dominance and alters community assembly

description: Data used to test for ecological and eco-evolutionary priority effects.
DOI: 10.17188/1753841
title: Materials Data on Y5Sc5Si6 by Materials Project

description: Y5Sc5Si6 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are three inequivalent Y sites. In the first Y site, Y is bonded in a 5-coordinate geometry to five Si atoms. There are a spread of Y–Si bond distances ranging from 2.87–3.26 Å. In the second Y site, Y is bonded in a 5-coordinate geometry to five Si atoms. There are a spread of Y–Si bond distances ranging from 2.87–3.27 Å. In the third Y site, Y is bonded in a 5-coordinate geometry to five Si atoms. There are a spread of Y–Si bond distances ranging from 2.86–3.25 Å. There are two inequivalent Sc sites. In the first Sc site, Sc is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Sc–Si bond distances ranging from 2.91–3.00 Å. In the second Sc site, Sc is bonded in a 3-coordinate geometry to five Si atoms. There are a spread of Sc–Si bond distances ranging from 2.80–3.25 Å. There are four inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to four Y and five Sc atoms. In the second Si site, Si is bonded in a 9-coordinate geometry to four Y and five Sc atoms. In the third Si site, Si is bonded in a 9-coordinate geometry to three Y and six Sc atoms. In the fourth Si site, Si is bonded in a 9-coordinate geometry to five Y and four equivalent Sc atoms.
DOI: 10.17188/1753842
title: Materials Data on ZnCo2 by Materials Project

description: Zn1Co2 is beta-derived structured and crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. Co is bonded to nine equivalent Co and three equivalent Zn atoms to form CoZn3Co9 cuboctahedra that share corners with three equivalent ZnZn6Co6 cuboctahedra, corners with nine equivalent CoZn3Co9 cuboctahedra, edges with nine equivalent ZnZn6Co6 cuboctahedra, edges with fifteen equivalent CoZn3Co9 cuboctahedra, faces with six equivalent ZnZn6Co6 cuboctahedra, and faces with twelve equivalent CoZn3Co9 cuboctahedra. There are three shorter (2.41 Å) and six longer (2.57 Å) Co–Co bond lengths. All Co–Zn bond lengths are 2.61 Å. Zn is bonded to six equivalent Co and six equivalent Zn atoms to form ZnZn6Co6 cuboctahedra that share corners with six equivalent CoZn3Co9 cuboctahedra, corners with six equivalent ZnZn6Co6 cuboctahedra, edges with six equivalent ZnZn6Co6 cuboctahedra, edges with eighteen equivalent CoZn3Co9 cuboctahedra, faces with six equivalent ZnZn6Co6 cuboctahedra, and faces with twelve equivalent CoZn3Co9 cuboctahedra. All Zn–Zn bond lengths are 2.57 Å.
DOI: 10.17188/1753843
title: Materials Data on Er5In3 by Materials Project

description: Er5In3 crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. there are two inequivalent Er sites. In the first Er site, Er is bonded in a 6-coordinate geometry to six equivalent In atoms. All Er–In bond lengths are 3.22 Å. In the second Er site, Er is bonded in a 5-coordinate geometry to five equivalent In atoms. There are a spread of Er–In bond distances ranging from 3.09–3.55 Å. In is bonded in a 9-coordinate geometry to nine Er atoms.
DOI: 10.17188/1753844
title: Materials Data on Cs(PIr)2 by Materials Project

description: Cs(IrP)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Cs is bonded in a body-centered cubic geometry to eight equivalent P atoms. All Cs–P bond lengths are 3.67 Å. Ir is bonded to four equivalent P atoms to form a mixture of distorted corner and edge-sharing IrP4 tetrahedra. All Ir–P bond lengths are 2.36 Å. P is bonded in a 8-coordinate geometry to four equivalent Cs and four equivalent Ir atoms.
DOI: 10.17188/1753846
title: Materials Data on CoPNO10 by Materials Project

description: CoPO9NO crystallizes in the orthorhombic Pmn2_1 space group. The structure is one-dimensional and consists of two nitroxyl molecules and two CoPO9 ribbons oriented in the (1, 0, 0) direction. In each CoPO9 ribbon, Co is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Co–O bond distances ranging from 1.62–2.03 Å. P is bonded in a tetrahedral geometry to four O atoms. There are a spread of P–O bond distances ranging from 1.47–1.68 Å. There are six inequivalent O sites. In the first O site, O is bonded in a 2-coordinate geometry to one Co and one O atom. The O–O bond length is 1.29 Å. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Co and one O atom. The O–O bond length is 1.43 Å. In the third O site, O is bonded in a single-bond geometry to one P atom. In the fourth O site, O is bonded in a distorted bent 120 degrees geometry to one P and one O atom. In the fifth O site, O is bonded in a bent 150 degrees geometry to one Co and one P atom. In the sixth O site, O is bonded in a single-bond geometry to one Co atom.
DOI: 10.17188/1753847
title: Materials Data on Li4Ti4Mn4CoO18 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: 10.17188/1753848
title: Materials Data on SrCuO2 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: 10.17188/1753849
title: Materials Data on Pr3(ReO5)2 by Materials Project

description: Pr3(ReO5)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Pr–O bond distances ranging from 2.42–2.57 Å. In the second Pr3+ site, Pr3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Pr–O bond distances ranging from 2.39–2.73 Å. Re+5.50+ is bonded to six O2- atoms to form edge-sharing ReO6 octahedra. There are a spread of Re–O bond distances ranging from 1.89–2.05 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to three Pr3+ and one Re+5.50+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Pr3+ and two equivalent Re+5.50+ atoms. In the third O2- site, O2- is bonded in a trigonal non-coplanar geometry to two equivalent Pr3+ and one Re+5.50+ atom. In the fourth O2- site, O2- is bonded to three Pr3+ and one Re+5.50+ atom to form a mixture of edge and corner-sharing OPr3Re tetrahedra.
DOI: 10.17188/1753850
title: Materials Data on InPO6 by Materials Project

description: (InPO5)2O2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional and consists of two hydrogen peroxide molecules and one InPO5 framework. In the InPO5 framework, In is bonded to five O atoms to form InO5 trigonal bipyramids that share corners with four equivalent PO4 tetrahedra. There are a spread of In–O bond distances ranging from 2.08–2.31 Å. P is bonded to four O atoms to form PO4 tetrahedra that share corners with four equivalent InO5 trigonal bipyramids. There are a spread of P–O bond distances ranging from 1.52–1.70 Å. There are five inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to one In and one P atom. In the second O site, O is bonded in a bent 120 degrees geometry to one In and one P atom. In the third O site, O is bonded in a 3-coordinate geometry to one In, one P, and one O atom. The O–O bond length is 1.49 Å. In the fourth O site, O is bonded in a bent 120 degrees geometry to one In and one P atom. In the fifth O site, O is bonded in a water-like geometry to one In and one O atom.
DOI: 10.17188/1753851
title: Materials Data on LiMgPb2 by Materials Project

description: LiMgPb2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Pb atoms. All Li–Pb bond lengths are 3.21 Å. Mg is bonded in a body-centered cubic geometry to eight equivalent Pb atoms. All Mg–Pb bond lengths are 3.21 Å. Pb is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Mg atoms.
DOI: 10.17188/1753854
title: Materials Data on Li2MnFe(BO3)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: 10.17188/1753855
title: Materials Data on AgSbS(OF3)2 by Materials Project

description: AgSbS(OF3)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ag1+ is bonded in a 8-coordinate geometry to two O2- and six F1- atoms. There are one shorter (2.64 Å) and one longer (2.67 Å) Ag–O bond lengths. There are a spread of Ag–F bond distances ranging from 2.55–2.85 Å. Sb3+ is bonded in an octahedral geometry to six F1- atoms. There is three shorter (1.92 Å) and three longer (1.93 Å) Sb–F bond length. S6+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both S–O bond lengths are 1.45 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Ag1+ and one S6+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Ag1+ and one S6+ atom. There are six inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted single-bond geometry to one Ag1+ and one Sb3+ atom. In the second F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ag1+ and one Sb3+ atom. In the third F1- site, F1- is bonded in a 2-coordinate geometry to one Ag1+ and one Sb3+ atom. In the fourth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ag1+ and one Sb3+ atom. In the fifth F1- site, F1- is bonded in a distorted single-bond geometry to one Ag1+ and one Sb3+ atom. In the sixth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ag1+ and one Sb3+ atom.