147,084 Works

AmeriFlux US-BZS Bonanza Creek Black Spruce

Eugenie Euskirchen
This is the AmeriFlux version of the carbon flux data for the site US-BZS Bonanza Creek Black Spruce.

AmeriFlux US-BZF Bonanza Creek Rich Fen

Eugenie Euskirchen
This is the AmeriFlux version of the carbon flux data for the site US-BZF Bonanza Creek Rich Fen.

AmeriFlux MX-PMm Puerto Morelos mangrove

Ma. Alvarado-Barrientos
This is the AmeriFlux version of the carbon flux data for the site MX-PMm Puerto Morelos mangrove.

A Genomic Catalogue of Earth’s Microbiomes - Introductory KBase Narrative

Stephen Nayfach, Simon Roux, Rekha Seshadri, Daniel Udwary, Neha Varghese, Frederik Schulz, Dongying Wu, David Paez-Espino, I-Min Chen, Marcel Huntemann, Krishna Palaniappan, Joshua Ladau, Supratim Mukherjee, T.B.K. Reddy, Torben Nielsen, Edward Kirton, José P. Faria, Janaka N. Edirisinghe, Christopher S. Henry, Sean P. Jungbluth, Dylan Chivian, Paramvir Dehal, Elisha M. Wood-Charlson, Adam P. Arkin, Susannah Tringe … & Emiley Eloe-Fadrosh
The reconstruction of bacterial and archaeal genomes from shotgun metagenomes has enabled unprecedented insights into the ecology and evolution of environmental and host-associated microbiomes. Here we applied this powerful approach to over 10,000 metagenomes collected from diverse habitats covering all of Earth’s continents and oceans, human- and animal-host associated microbiomes, engineered environments, and natural and agricultural soils to capture extant microbial metabolic and functional potential. We present a comprehensive catalogue of 52,515 metagenome-assembled genomes representing...

Materials Data on Na2MoO6 by Materials Project

Kristin Persson
Na2MoO6 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. there are two inequivalent Na sites. In the first Na site, Na is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Na–O bond distances ranging from 2.38–2.63 Å. In the second Na site, Na is bonded in a 2-coordinate geometry to six O atoms. There are a spread of Na–O bond distances ranging from 2.27–2.84 Å. Mo...

Materials Data on AlFeIr2 by Materials Project

Kristin Persson
FeIr2Al is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Fe is bonded in a body-centered cubic geometry to eight equivalent Ir atoms. All Fe–Ir bond lengths are 2.62 Å. Ir is bonded in a body-centered cubic geometry to four equivalent Fe and four equivalent Al atoms. All Ir–Al bond lengths are 2.62 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ir atoms.

Materials Data on Nb2Ni3Ge by Materials Project

Kristin Persson
Nb2Ni3Ge is Hexagonal Laves-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Nb is bonded in a 12-coordinate geometry to four equivalent Nb, nine equivalent Ni, and three equivalent Ge atoms. There are one shorter (2.95 Å) and three longer (2.99 Å) Nb–Nb bond lengths. There are three shorter (2.79 Å) and six longer (2.87 Å) Nb–Ni bond lengths. All Nb–Ge bond lengths are 2.88 Å. Ni is bonded to...

Materials Data on CoP2O7 by Materials Project

Kristin Persson
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 Tb11(In3Si2)2 by Materials Project

Kristin Persson
Tb11Si4In6 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are four inequivalent Tb sites. In the first Tb site, Tb is bonded to four equivalent In and three Si atoms to form a mixture of distorted corner, edge, and face-sharing TbIn4Si3 pentagonal bipyramids. There are two shorter (3.37 Å) and two longer (3.45 Å) Tb–In bond lengths. There are a spread of Tb–Si bond distances ranging from 3.08–3.20 Å. In the...

Materials Data on U2Mo2C3 by Materials Project

Kristin Persson
U2Mo2C3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. U4+ is bonded in a pentagonal planar geometry to five C4- atoms. There are three shorter (2.43 Å) and two longer (2.46 Å) U–C bond lengths. Mo2+ is bonded to four C4- atoms to form a mixture of edge and corner-sharing MoC4 trigonal pyramids. There are a spread of Mo–C bond distances ranging from 2.11–2.18 Å. There are two inequivalent C4- sites. In...

Materials Data on Li3MnCoO5 by Materials Project

Kristin Persson
Li3MnCoO5 is Caswellsilverite-derived structured and crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are six inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with three equivalent LiO6 octahedra, corners with three equivalent MnO6 octahedra, edges with three equivalent MnO6 octahedra, and edges with nine LiO6 octahedra. The corner-sharing octahedra tilt angles range from 5–12°. There are...

Materials Data on LiNiO2 by Materials Project

Kristin Persson
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 Li3Ni2(PO4)3 by Materials Project

Kristin Persson
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 TlBiSe2 by Materials Project

Kristin Persson
TlBiSe2 is Caswellsilverite-like structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are four inequivalent Tl1+ sites. In the first Tl1+ site, Tl1+ is bonded to six Se2- atoms to form distorted TlSe6 octahedra that share a cornercorner with one BiSe6 octahedra, corners with five TlSe6 octahedra, edges with four equivalent BiSe6 octahedra, and edges with eight TlSe6 octahedra. The corner-sharing octahedra tilt angles range from 0–16°. There are a...

Materials Data on Mg3Zn by Materials Project

Kristin Persson
Mg3Zn1 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Mg is bonded to eight equivalent Mg and four equivalent Zn atoms to form MgMg8Zn4 cuboctahedra that share corners with twelve equivalent MgMg8Zn4 cuboctahedra, edges with eight equivalent ZnMg12 cuboctahedra, edges with sixteen equivalent MgMg8Zn4 cuboctahedra, faces with four equivalent ZnMg12 cuboctahedra, and faces with fourteen equivalent MgMg8Zn4 cuboctahedra. All Mg–Mg bond lengths are 3.08 Å. All Mg–Zn...

Materials Data on CdSO5 by Materials Project

Kristin Persson
CdSO5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Cd is bonded to six O atoms to form CdO6 octahedra that share corners with two equivalent CdO6 octahedra and corners with four equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 51°. There are a spread of Cd–O bond distances ranging from 2.28–2.32 Å. S is bonded to four O atoms to form SO4 tetrahedra that share corners with four equivalent CdO6...

Materials Data on Ca2CdP2 by Materials Project

Kristin Persson
Ca2CdP2 crystallizes in the orthorhombic Cmc2_1 space group. The structure is three-dimensional. there are two inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded to five P3- atoms to form CaP5 square pyramids that share corners with four equivalent CaP5 square pyramids, corners with four equivalent CdP4 tetrahedra, corners with seven equivalent CaP5 trigonal bipyramids, edges with two equivalent CaP5 square pyramids, edges with three equivalent CdP4 tetrahedra, and edges with two equivalent...

Materials Data on PrCo3Ni2 by Materials Project

Kristin Persson
PrCo3Ni2 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Pr is bonded in a 6-coordinate geometry to twelve equivalent Co and six equivalent Ni atoms. All Pr–Co bond lengths are 3.20 Å. All Pr–Ni bond lengths are 2.87 Å. Co is bonded to four equivalent Pr, four equivalent Co, and four equivalent Ni atoms to form a mixture of edge, face, and corner-sharing CoPr4Co4Ni4 cuboctahedra. All Co–Co bond lengths are 2.49 Å....

Materials Data on Cd(BrO2)2 by Materials Project

Kristin Persson
Cd(O2Br)2 crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. Cd is bonded in a distorted linear geometry to two equivalent O and four equivalent Br atoms. Both Cd–O bond lengths are 2.16 Å. All Cd–Br bond lengths are 2.97 Å. There are two inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to two equivalent O and one Br atom. Both O–O bond lengths are...

Materials Data on Li2Co(Si2O5)2 by Materials Project

Kristin Persson
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 YZrFe4 by Materials Project

Kristin Persson
YZrFe4 is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Y is bonded in a 12-coordinate geometry to four equivalent Zr and twelve equivalent Fe atoms. All Y–Zr bond lengths are 3.12 Å. All Y–Fe bond lengths are 2.99 Å. Zr is bonded in a 12-coordinate geometry to four equivalent Y and twelve equivalent Fe atoms. All Zr–Fe bond lengths are 2.98 Å. Fe is bonded to three...

Materials Data on TaCr3(CuS4)2 by Materials Project

Kristin Persson
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 Ta3Ru2 by Materials Project

Kristin Persson
Ta3Ru2 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are four inequivalent Ta sites. In the first Ta site, Ta is bonded in a 8-coordinate geometry to four equivalent Ta and four equivalent Ru atoms. All Ta–Ta bond lengths are 2.81 Å. All Ta–Ru bond lengths are 2.82 Å. In the second Ta site, Ta is bonded in a body-centered cubic geometry to eight Ru atoms. There are four shorter (2.74...

Materials Data on NaFeO3 by Materials Project

Kristin Persson
NaFeO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Na is bonded to twelve equivalent O atoms to form NaO12 cuboctahedra that share corners with twelve equivalent NaO12 cuboctahedra, faces with six equivalent NaO12 cuboctahedra, and faces with eight equivalent FeO6 octahedra. All Na–O bond lengths are 2.71 Å. Fe is bonded to six equivalent O atoms to form FeO6 octahedra that share corners with six equivalent...

Materials Data on Na6WN4 by Materials Project

Kristin Persson
Na6WN4 crystallizes in the tetragonal P4_2/nmc space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four equivalent N3- atoms. There are two shorter (2.40 Å) and two longer (2.81 Å) Na–N bond lengths. In the second Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four equivalent N3- atoms. There are two shorter (2.44 Å) and two longer...

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