2,891 Works

Data for \"Soil carbon dynamics during drying vs. rewetting: Importance of antecedent moisture conditions\"

Kaizad Patel
This dataset contains data used for the paper "Soil carbon dynamics during drying vs. rewetting: importance of antecedent moisture conditions". The Related References field will be updated with a full citation when available.Soil moisture influences soil carbon dynamics, including microbial growth and respiration. The response of such ‘soil respiration’ to moisture changes is generally assumed to be linear and reversible, i.e. to depend only on the current moisture state. Current models thus do not account...

Anion Data for the East River Watershed, Colorado

Kenneth Williams, Curtis Beutler, Wendy Brown, Amanda Henderson & Alex Newman
The anion data for the East River Watershed, Colorado, consists of fluoride, chloride, sulfate, nitrate, and phosphate concentrations collected at multiple, long-term monitoring sites that include stream, groundwater, and spring sampling locations. These locations represent important and/or unique end-member locations for which solute concentrations can be diagnostic of the connection between terrestrial and aquatic systems. Such locations include drainages underlined entirely or largely by shale bedrock, land covered dominated by conifers, aspens, or meadows, and...

Estimating Watershed Subsurface Permeability From Stream Discharge Data using Deep Neural Networks, Frontiers in Earth Science: Dataset

Erol Cromwell, Pin Shuai, Peishi Jiang, Ethan Coon, Scott Painter, David Moulton, Youzuo Lin & Xingyuan Chen
This data package contains watershed modeling inputs and outputs as well as deep neural networks training and testing results used in "Estimating Watershed Subsurface Permeability From Stream Discharge Data using Deep Neural Networks" (Cromwell et al., 2021). We train various deep neural network models with different architectures to predict subsurface permeability from stream discharge hydrograph at the watershed outlet. The training data are obtained from ensemble simulations of hydrographs corresponding to an permeability ensemble using...

Data from: \"Snowmelt Timing Regulates Community Composition, Phenology, and Physiological Performance of Alpine Plants\"

Daniel E. Winkler, Ramona J. Butz, Matthew J. Germino, Keith Reinhardt & Lara M. Kueppers
This archive contains data that were used to support conclusions drawn in “Snowmelt Timing Regulates Community Composition, Phenology, and Physiological Performance of Alpine Plants”, by Winkler et al., 2018. Data were collected throughout the 2009 growing season on Niwot Ridge, Colorado, before the site became part of the Alpine Treeline Warming Experiment (ATWE). Geospatial files are included in this archive to provide additional locational context. The files in this data package consist of five comma-separated-values...

Materials Data on NbAgN2 by Materials Project

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

Materials Data on La4Ti2Se5O4 by Materials Project

La4Ti2O4Se5 crystallizes in the orthorhombic Cmc2_1 space group. The structure is two-dimensional and consists of two La4Ti2O4Se5 sheets oriented in the (0, 1, 0) direction. there are eight inequivalent La3+ sites. In the first La3+ site, La3+ is bonded in a 3-coordinate geometry to four Se2- and three O2- atoms. There are two shorter (3.08 Å) and two longer (3.34 Å) La–Se bond lengths. There are two shorter (2.41 Å) and one longer (2.50 Å)...

Materials Data on V2Cu3NiO6 by Materials Project

V2NiCu3O6 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. V+3.50+ is bonded to six O2- atoms to form VO6 octahedra that share edges with three equivalent VO6 octahedra and edges with three equivalent NiO6 octahedra. There are four shorter (2.01 Å) and two longer (2.03 Å) V–O bond lengths. Ni2+ is bonded to six O2- atoms to form NiO6 octahedra that share edges with six equivalent VO6 octahedra. There are four shorter...

Materials Data on LiGaBH3O5 by Materials Project

LiGaBH3O5 crystallizes in the monoclinic Cc space group. The structure is two-dimensional and consists of two LiGaBH3O5 sheets oriented in the (0, 0, 1) direction. Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with three equivalent GaO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.94–2.03 Å. Ga3+ is bonded to four O2- atoms to form GaO4 tetrahedra that share corners with three equivalent LiO4 tetrahedra....

Materials Data on Ba2HgS5 by Materials Project

Ba2HgS5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ba2+ is bonded in a 9-coordinate geometry to nine S+1.20- atoms. There are a spread of Ba–S bond distances ranging from 3.20–3.52 Å. Hg2+ is bonded in a distorted linear geometry to four S+1.20- atoms. There are a spread of Hg–S bond distances ranging from 2.37–3.30 Å. There are four inequivalent S+1.20- sites. In the first S+1.20- site, S+1.20- is bonded in a...

Materials Data on ThCd(MoO4)3 by Materials Project

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

Materials Data on Li7Mn2(CoO4)3 by Materials Project

Li7Mn2(CoO4)3 is Caswellsilverite-derived structured and crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are seven inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with three equivalent LiO6 octahedra, corners with three equivalent MnO6 octahedra, edges with five MnO6 octahedra, and edges with seven LiO6 octahedra. The corner-sharing octahedra tilt angles range from 5–15°. There are a spread...

Materials Data on NaH4IO7 by Materials Project

NaH4O7I crystallizes in the triclinic P1 space group. The structure is three-dimensional. Na is bonded to seven O atoms to form distorted NaO7 pentagonal bipyramids that share edges with three equivalent IO6 octahedra. There are a spread of Na–O bond distances ranging from 2.37–2.59 Å. There are four inequivalent H sites. In the first H site, H is bonded in a single-bond geometry to one O atom. The H–O bond length is 1.01 Å. In...

Materials Data on Mg30CrCoO32 by Materials Project

Mg30CrCoO32 is alpha Po-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are eight inequivalent Mg2+ sites. In the first Mg2+ site, Mg2+ is bonded to six O2- atoms to form MgO6 octahedra that share corners with two equivalent MgO6 octahedra, corners with two equivalent CrO6 octahedra, corners with two equivalent CoO6 octahedra, and edges with twelve MgO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a...

Materials Data on Mn3(Co10B3)2 by Materials Project

Mn3(Co10B3)2 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Mn sites. In the first Mn site, Mn is bonded to twelve equivalent Co atoms to form MnCo12 cuboctahedra that share edges with twenty-four equivalent CoMnCo6B3 tetrahedra and faces with eight equivalent MnCo16 tetrahedra. All Mn–Co bond lengths are 2.46 Å. In the second Mn site, Mn is bonded to sixteen Co atoms to form MnCo16 tetrahedra that share...

Materials Data on Co(HO)2 by Materials Project

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

Materials Data on Cs2HgBr4 by Materials Project

Cs2HgBr4 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 8-coordinate geometry to eight Br1- atoms. There are a spread of Cs–Br bond distances ranging from 3.72–4.36 Å. In the second Cs1+ site, Cs1+ is bonded in a 8-coordinate geometry to eight Br1- atoms. There are a spread of Cs–Br bond distances ranging from 3.74–4.15 Å. Hg2+...

Materials Data on MgO by Materials Project

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

Materials Data on RbPdC4Br by Materials Project

RbPdC4Br crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Rb1+ is bonded in a rectangular see-saw-like geometry to four equivalent Br1- atoms. All Rb–Br bond lengths are 3.72 Å. There are two inequivalent Pd2+ sites. In the first Pd2+ site, Pd2+ is bonded to four equivalent C+0.50- and two equivalent Br1- atoms to form corner-sharing PdC4Br2 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pd–C bond lengths are 2.00 Å. Both...

Materials Data on NaLi5Fe2P2(CO7)2 by Materials Project

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

Materials Data on Mg30VSnO32 by Materials Project

Mg30VSnO32 is alpha Po-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are eight inequivalent Mg2+ sites. In the first Mg2+ site, Mg2+ is bonded to six O2- atoms to form MgO6 octahedra that share corners with two equivalent VO6 octahedra, corners with four MgO6 octahedra, and edges with twelve MgO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Mg–O bond distances ranging from...

Materials Data on Sr2Mn2O5 by Materials Project

Sr2Mn2O5 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Sr2+ is bonded in a distorted q6 geometry to ten O2- atoms. There are eight shorter (2.75 Å) and two longer (2.84 Å) Sr–O bond lengths. There are two inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded in a square co-planar geometry to four equivalent O2- atoms. All Mn–O bond lengths are 1.92 Å. In the second Mn3+ site, Mn3+...

Materials Data on MgSi by Materials Project

MgSi is Magnesium tetraboride-like structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Mg sites. In the first 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 2.73–2.89 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...

Materials Data on BaSrI4 by Materials Project

BaSrI4 is Fluorite-derived structured and crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. Ba2+ is bonded in a body-centered cubic geometry to eight equivalent I1- atoms. There are four shorter (3.58 Å) and four longer (3.62 Å) Ba–I bond lengths. Sr2+ is bonded in a body-centered cubic geometry to eight equivalent I1- atoms. All Sr–I bond lengths are 3.52 Å. I1- is bonded to two equivalent Ba2+ and two equivalent Sr2+ atoms...

Materials Data on CsTb(WO4)2 by Materials Project

CsTb(WO4)2 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Cs1+ is bonded in a 12-coordinate geometry to twelve O2- atoms. There are a spread of Cs–O bond distances ranging from 2.97–3.52 Å. Tb3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Tb–O bond distances ranging from 2.30–2.37 Å. W6+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing WO6 octahedra....

Materials Data on LiFe(PO3)4 by Materials Project

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

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  • 2021
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    2,891