cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1728415
title: Materials Data on Ta3N by Materials Project

description: Ta3N is H-Phase-derived structured and crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. there are two inequivalent Ta sites. In the first Ta site, Ta is bonded to twelve Ta atoms to form TaTa12 cuboctahedra that share corners with six equivalent TaTa12 cuboctahedra, corners with twelve equivalent NTa6 octahedra, edges with six equivalent TaTa12 cuboctahedra, faces with six equivalent TaTa12 cuboctahedra, and faces with two equivalent NTa6 octahedra. The corner-sharing octahedral tilt angles are 44°. There are six shorter (3.01 Å) and six longer (3.03 Å) Ta–Ta bond lengths. In the second Ta site, Ta is bonded in a distorted T-shaped geometry to three equivalent Ta and three equivalent N atoms. All Ta–N bond lengths are 2.19 Å. N is bonded to six equivalent Ta atoms to form NTa6 octahedra that share corners with twelve equivalent TaTa12 cuboctahedra, edges with six equivalent NTa6 octahedra, and faces with two equivalent TaTa12 cuboctahedra.
DOI: 10.17188/1728416
title: Materials Data on Ti2GaW by Materials Project

description: Ti2WGa crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Ti2WGa ribbons oriented in the (1, 0, 0) direction. Ti is bonded in a linear geometry to one W and one Ga atom. The Ti–W bond length is 2.20 Å. The Ti–Ga bond length is 2.61 Å. W is bonded in a linear geometry to two equivalent Ti atoms. Ga is bonded in a linear geometry to two equivalent Ti atoms.
DOI: 10.17188/1728417
title: Materials Data on Ni2(SO4)3 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: 10.17188/1728418
title: Materials Data on Er2(GePt3)3 by Materials Project

description: Er2(Pt3Ge)3 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Er3+ is bonded in a 11-coordinate geometry to eleven Pt2- atoms. There are a spread of Er–Pt bond distances ranging from 2.96–3.21 Å. There are five inequivalent Pt2- sites. In the first Pt2- site, Pt2- is bonded in a 12-coordinate geometry to three equivalent Er3+ and three Ge4+ atoms. There are a spread of Pt–Ge bond distances ranging from 2.55–2.71 Å. In the second Pt2- site, Pt2- is bonded in a 2-coordinate geometry to two equivalent Er3+ and two Ge4+ atoms. There are one shorter (2.47 Å) and one longer (2.48 Å) Pt–Ge bond lengths. In the third Pt2- site, Pt2- is bonded in a 12-coordinate geometry to three equivalent Er3+ and three Ge4+ atoms. There are a spread of Pt–Ge bond distances ranging from 2.52–2.73 Å. In the fourth Pt2- site, Pt2- is bonded in a 2-coordinate geometry to two equivalent Er3+ and two equivalent Ge4+ atoms. Both Pt–Ge bond lengths are 2.48 Å. In the fifth Pt2- site, Pt2- is bonded in a 5-coordinate geometry to two equivalent Er3+ and three Ge4+ atoms. There are a spread of Pt–Ge bond distances ranging from 2.63–2.91 Å. There are two inequivalent Ge4+ sites. In the first Ge4+ site, Ge4+ is bonded in a distorted hexagonal bipyramidal geometry to eight Pt2- atoms. In the second Ge4+ site, Ge4+ is bonded in a 8-coordinate geometry to eight Pt2- atoms.
DOI: 10.17188/1728420
title: Materials Data on Rb2FeF5 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: 10.17188/1728421
title: Materials Data on Li4Cr3Ni(PO4)4 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: 10.17188/1728422
title: Materials Data on NpSc3 by Materials Project

description: NpSc3 is alpha La-derived structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Np is bonded to twelve Sc atoms to form NpSc12 cuboctahedra that share corners with four equivalent NpSc12 cuboctahedra, corners with eight equivalent ScNp4Sc8 cuboctahedra, edges with eight equivalent NpSc12 cuboctahedra, edges with sixteen equivalent ScNp4Sc8 cuboctahedra, faces with four equivalent NpSc12 cuboctahedra, and faces with fourteen ScNp4Sc8 cuboctahedra. There are four shorter (3.19 Å) and eight longer (3.28 Å) Np–Sc bond lengths. There are two inequivalent Sc sites. In the first Sc site, Sc is bonded to four equivalent Np and eight Sc atoms to form ScNp4Sc8 cuboctahedra that share corners with twelve equivalent ScNp4Sc8 cuboctahedra, edges with eight equivalent NpSc12 cuboctahedra, edges with sixteen ScNp4Sc8 cuboctahedra, faces with four equivalent NpSc12 cuboctahedra, and faces with fourteen ScNp4Sc8 cuboctahedra. There are four shorter (3.19 Å) and four longer (3.28 Å) Sc–Sc bond lengths. In the second Sc site, Sc is bonded to four equivalent Np and eight equivalent Sc atoms to form ScNp4Sc8 cuboctahedra that share corners with four equivalent ScNp4Sc8 cuboctahedra, corners with eight equivalent NpSc12 cuboctahedra, edges with twenty-four ScNp4Sc8 cuboctahedra, faces with six equivalent NpSc12 cuboctahedra, and faces with twelve ScNp4Sc8 cuboctahedra.
DOI: 10.17188/1728423
title: Materials Data on Li7H5N4 by Materials Project

description: Li7N4H5 crystallizes in the orthorhombic Pna2_1 space group. The structure is three-dimensional. there are seven inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 2-coordinate geometry to three N3- and one H1+ atom. There are a spread of Li–N bond distances ranging from 2.07–2.15 Å. The Li–H bond length is 2.12 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to three N3- and one H1+ atom. There are a spread of Li–N bond distances ranging from 2.07–2.13 Å. The Li–H bond length is 2.13 Å. In the third Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four N3- atoms. There are a spread of Li–N bond distances ranging from 1.95–2.29 Å. In the fourth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to four N3- and two H1+ atoms. There are a spread of Li–N bond distances ranging from 2.19–2.27 Å. There are one shorter (2.10 Å) and one longer (2.19 Å) Li–H bond lengths. In the fifth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to three N3- and one H1+ atom. There are one shorter (2.12 Å) and two longer (2.13 Å) Li–N bond lengths. The Li–H bond length is 2.13 Å. In the sixth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to three N3- and one H1+ atom. There are a spread of Li–N bond distances ranging from 1.98–2.10 Å. The Li–H bond length is 2.15 Å. In the seventh Li1+ site, Li1+ is bonded in a 4-coordinate geometry to three N3- and one H1+ atom. There are a spread of Li–N bond distances ranging from 2.00–2.14 Å. The Li–H bond length is 2.04 Å. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted single-bond geometry to six Li1+ and one H1+ atom. The N–H bond length is 1.03 Å. In the second N3- site, N3- is bonded in a distorted water-like geometry to four Li1+ and two H1+ atoms. There is one shorter (1.03 Å) and one longer (1.04 Å) N–H bond length. In the third N3- site, N3- is bonded in a distorted single-bond geometry to seven Li1+ and one H1+ atom. The N–H bond length is 1.03 Å. In the fourth N3- site, N3- is bonded in a distorted single-bond geometry to six Li1+ and one H1+ atom. The N–H bond length is 1.03 Å. There are five inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to three Li1+ and one N3- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one Li1+ and one N3- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to three Li1+ and one N3- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom.
DOI: 10.17188/1728424
title: Materials Data on In3NO3 by Materials Project

description: In3NO3 is Spinel-like structured and crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are four inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to two equivalent N3- and four O2- atoms to form InN2O4 octahedra that share corners with six equivalent InNO3 tetrahedra and edges with six InN2O4 octahedra. Both In–N bond lengths are 2.18 Å. There are two shorter (2.27 Å) and two longer (2.30 Å) In–O bond lengths. In the second In3+ site, In3+ is bonded to one N3- and three O2- atoms to form corner-sharing InNO3 tetrahedra. The corner-sharing octahedra tilt angles range from 55–61°. The In–N bond length is 2.10 Å. There are two shorter (2.16 Å) and one longer (2.18 Å) In–O bond lengths. In the third In3+ site, In3+ is bonded to two equivalent N3- and four O2- atoms to form InN2O4 octahedra that share corners with six equivalent InNO3 tetrahedra and edges with six InN2O4 octahedra. Both In–N bond lengths are 2.17 Å. There are two shorter (2.28 Å) and two longer (2.31 Å) In–O bond lengths. In the fourth In3+ site, In3+ is bonded to one N3- and five O2- atoms to form InNO5 octahedra that share corners with six equivalent InNO3 tetrahedra and edges with six InN2O4 octahedra. The In–N bond length is 2.16 Å. There are a spread of In–O bond distances ranging from 2.23–2.28 Å. N3- is bonded to four In3+ atoms to form distorted corner-sharing NIn4 trigonal pyramids. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to four In3+ atoms. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to four In3+ atoms. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to four In3+ atoms.
DOI: 10.17188/1728426
title: Materials Data on CdAs3 by Materials Project

description: CdAs3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cd2+ is bonded to twelve equivalent As+0.67- atoms to form a mixture of face and corner-sharing CdAs12 cuboctahedra. There are six shorter (3.07 Å) and six longer (3.08 Å) Cd–As bond lengths. As+0.67- is bonded in a distorted see-saw-like geometry to four equivalent Cd2+ atoms.
DOI: 10.17188/1728427
title: Materials Data on Ta2Mn(ReSe4)2 by Materials Project

description: TaReMnSe4TaSe2ReSe2 is Molybdenite-derived structured and crystallizes in the trigonal P3m1 space group. The structure is two-dimensional and consists of one ReSe2 sheet oriented in the (0, 0, 1) direction; one TaReMnSe4 sheet oriented in the (0, 0, 1) direction; and one TaSe2 sheet oriented in the (0, 0, 1) direction. In the ReSe2 sheet, Re3+ is bonded to six Se2- atoms to form distorted edge-sharing ReSe6 pentagonal pyramids. All Re–Se bond lengths are 2.54 Å. There are two inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a distorted T-shaped geometry to three equivalent Re3+ atoms. In the second Se2- site, Se2- is bonded in a distorted T-shaped geometry to three equivalent Re3+ atoms. In the TaReMnSe4 sheet, Ta4+ is bonded to six Se2- atoms to form distorted TaSe6 pentagonal pyramids that share corners with six equivalent MnSe6 octahedra, edges with six equivalent TaSe6 pentagonal pyramids, and a faceface with one MnSe6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are three shorter (2.61 Å) and three longer (2.64 Å) Ta–Se bond lengths. Re3+ is bonded to six Se2- atoms to form distorted ReSe6 pentagonal pyramids that share corners with six equivalent MnSe6 octahedra, edges with six equivalent ReSe6 pentagonal pyramids, and a faceface with one MnSe6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are three shorter (2.51 Å) and three longer (2.65 Å) Re–Se bond lengths. Mn2+ is bonded to six Se2- atoms to form MnSe6 octahedra that share corners with six equivalent TaSe6 pentagonal pyramids, corners with six equivalent ReSe6 pentagonal pyramids, edges with six equivalent MnSe6 octahedra, a faceface with one TaSe6 pentagonal pyramid, and a faceface with one ReSe6 pentagonal pyramid. There are three shorter (2.56 Å) and three longer (2.64 Å) Mn–Se bond lengths. There are four inequivalent Se2- sites. In the first Se2- site, Se2- is bonded to three equivalent Ta4+ and three equivalent Mn2+ atoms to form distorted edge-sharing SeTa3Mn3 pentagonal pyramids. In the second Se2- site, Se2- is bonded in a 6-coordinate geometry to three equivalent Re3+ and three equivalent Mn2+ atoms. In the third Se2- site, Se2- is bonded in a distorted T-shaped geometry to three equivalent Re3+ atoms. In the fourth Se2- site, Se2- is bonded in a 3-coordinate geometry to three equivalent Ta4+ atoms. In the TaSe2 sheet, Ta4+ is bonded to six equivalent Se2- atoms to form distorted edge-sharing TaSe6 pentagonal pyramids. All Ta–Se bond lengths are 2.61 Å. Se2- is bonded in a 3-coordinate geometry to three equivalent Ta4+ atoms.
DOI: 10.6073/pasta/f981443cdb9efa7b11b1a2b90f3e7aa4
title: Jornada Basin LTER: Wireless meteorological station at NPP M-NORT site: 30-minute soil volumetric water content data: 2013 - ongoing

description: 30-minute Soil Moisture data at NPP M-NORT met station. Collection of soil volumetric water content data at Jornada LTER NPP sites, New Mexico, supports the environmental monitoring objectives of the Jornada LTER monitoring program that look at plant-soil water dynamics. Volumetric water content, bulk electrical conductivity, soil temperature, and bulk dielectric permittivity are measured every 30 minutes at an automated meteorological station installed at Jornada LTER NPP M-NORT site. Measurements are made every 30 minutes at 10 cm, 20 cm, and 30 cm soil depths. This is an ONGOING dataset.
DOI: 10.17188/1728429
title: Materials Data on Pr2Ni7 by Materials Project

description: Pr2Ni7 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 12-coordinate geometry to twelve Ni atoms. There are a spread of Pr–Ni bond distances ranging from 2.91–3.25 Å. In the second Pr site, Pr is bonded in a 6-coordinate geometry to eighteen Ni atoms. There are a spread of Pr–Ni bond distances ranging from 2.93–3.32 Å. There are five inequivalent Ni sites. In the first Ni site, Ni is bonded in a 12-coordinate geometry to three equivalent Pr and six Ni atoms. There are three shorter (2.46 Å) and three longer (2.50 Å) Ni–Ni bond lengths. In the second Ni site, Ni is bonded to six equivalent Pr and six equivalent Ni atoms to form NiPr6Ni6 cuboctahedra that share corners with twelve equivalent NiPr5Ni7 cuboctahedra, edges with six equivalent NiPr6Ni6 cuboctahedra, and faces with eighteen equivalent NiPr5Ni7 cuboctahedra. All Ni–Ni bond lengths are 2.61 Å. In the third Ni site, Ni is bonded to four equivalent Pr and eight Ni atoms to form NiPr4Ni8 cuboctahedra that share corners with sixteen NiPr5Ni7 cuboctahedra, edges with ten NiPr5Ni7 cuboctahedra, and faces with ten NiPr4Ni8 cuboctahedra. There are a spread of Ni–Ni bond distances ranging from 2.48–2.54 Å. In the fourth Ni site, Ni is bonded to five Pr and seven Ni atoms to form distorted NiPr5Ni7 cuboctahedra that share corners with seventeen NiPr6Ni6 cuboctahedra, edges with eight NiPr4Ni8 cuboctahedra, and faces with fourteen NiPr6Ni6 cuboctahedra. There are a spread of Ni–Ni bond distances ranging from 2.48–2.54 Å. In the fifth Ni site, Ni is bonded in a 12-coordinate geometry to three equivalent Pr and six Ni atoms.
DOI: 10.17188/1728430
title: Materials Data on Mg4Si3 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: 10.17188/1728431
title: Materials Data on Pr2CuSn4 by Materials Project

description: Pr2CuSn4 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 10-coordinate geometry to ten Sn atoms. There are a spread of Pr–Sn bond distances ranging from 3.28–3.42 Å. In the second Pr site, Pr is bonded in a 4-coordinate geometry to four equivalent Cu and ten Sn atoms. All Pr–Cu bond lengths are 3.51 Å. There are a spread of Pr–Sn bond distances ranging from 3.41–3.79 Å. Cu is bonded in a 9-coordinate geometry to four equivalent Pr and five Sn atoms. There are a spread of Cu–Sn bond distances ranging from 2.53–2.69 Å. There are four inequivalent Sn sites. In the first Sn site, Sn is bonded in a 10-coordinate geometry to four Pr, two equivalent Cu, and four equivalent Sn atoms. All Sn–Sn bond lengths are 3.22 Å. In the second Sn site, Sn is bonded in a 10-coordinate geometry to four Pr, two equivalent Cu, and four equivalent Sn atoms. In the third Sn site, Sn is bonded in a 1-coordinate geometry to six Pr, one Cu, and two equivalent Sn atoms. Both Sn–Sn bond lengths are 2.95 Å. In the fourth Sn site, Sn is bonded in a 4-coordinate geometry to six Pr and two equivalent Sn atoms.
DOI: 10.17188/1728432
title: Materials Data on K2TlHgI6 by Materials Project

description: K2HgTlI6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. K1+ is bonded to twelve equivalent I1- atoms to form distorted KI12 cuboctahedra that share corners with twelve equivalent KI12 cuboctahedra, faces with six equivalent KI12 cuboctahedra, faces with four equivalent HgI6 octahedra, and faces with four equivalent TlI6 octahedra. All K–I bond lengths are 4.34 Å. Hg1+ is bonded to six equivalent I1- atoms to form HgI6 octahedra that share corners with six equivalent TlI6 octahedra and faces with eight equivalent KI12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Hg–I bond lengths are 3.01 Å. Tl3+ is bonded to six equivalent I1- atoms to form TlI6 octahedra that share corners with six equivalent HgI6 octahedra and faces with eight equivalent KI12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–I bond lengths are 3.12 Å. I1- is bonded in a linear geometry to four equivalent K1+, one Hg1+, and one Tl3+ atom.
DOI: 10.17188/1728433
title: Materials Data on Ta17Al12 by Materials Project

description: Ta17Al12 is alpha-derived structured and crystallizes in the cubic I-43m space group. The structure is three-dimensional. there are three inequivalent Ta sites. In the first Ta site, Ta is bonded in a 12-coordinate geometry to four equivalent Ta and twelve equivalent Al atoms. All Ta–Ta bond lengths are 3.07 Å. All Ta–Al bond lengths are 3.05 Å. In the second Ta site, Ta is bonded in a 9-coordinate geometry to four Ta and nine equivalent Al atoms. All Ta–Ta bond lengths are 2.86 Å. There are six shorter (2.98 Å) and three longer (3.30 Å) Ta–Al bond lengths. In the third Ta site, Ta is bonded in a 12-coordinate geometry to seven Ta and five equivalent Al atoms. There are two shorter (2.83 Å) and four longer (3.04 Å) Ta–Ta bond lengths. There are a spread of Ta–Al bond distances ranging from 2.72–2.92 Å. Al is bonded in a 12-coordinate geometry to nine Ta and three equivalent Al atoms. There are one shorter (2.56 Å) and two longer (2.63 Å) Al–Al bond lengths.
DOI: 10.17188/1728434
title: Materials Data on NdLu3 by Materials Project

description: Lu3Nd is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are three inequivalent Lu sites. In the first Lu site, Lu is bonded to eight Lu and four equivalent Nd atoms to form LuNd4Lu8 cuboctahedra that share corners with four equivalent NdLu12 cuboctahedra, corners with fourteen LuNd4Lu8 cuboctahedra, edges with six equivalent NdLu12 cuboctahedra, edges with twelve LuNd4Lu8 cuboctahedra, faces with four equivalent NdLu12 cuboctahedra, and faces with sixteen LuNd4Lu8 cuboctahedra. There are a spread of Lu–Lu bond distances ranging from 3.47–3.63 Å. There are two shorter (3.51 Å) and two longer (3.57 Å) Lu–Nd bond lengths. In the second Lu site, Lu is bonded to eight Lu and four equivalent Nd atoms to form LuNd4Lu8 cuboctahedra that share corners with four equivalent NdLu12 cuboctahedra, corners with fourteen LuNd4Lu8 cuboctahedra, edges with six equivalent NdLu12 cuboctahedra, edges with twelve LuNd4Lu8 cuboctahedra, faces with four equivalent NdLu12 cuboctahedra, and faces with sixteen LuNd4Lu8 cuboctahedra. Both Lu–Lu bond lengths are 3.47 Å. There are two shorter (3.51 Å) and two longer (3.57 Å) Lu–Nd bond lengths. In the third Lu site, Lu is bonded to eight Lu and four equivalent Nd atoms to form LuNd4Lu8 cuboctahedra that share corners with four equivalent NdLu12 cuboctahedra, corners with fourteen LuNd4Lu8 cuboctahedra, edges with six equivalent NdLu12 cuboctahedra, edges with twelve LuNd4Lu8 cuboctahedra, faces with four equivalent NdLu12 cuboctahedra, and faces with sixteen LuNd4Lu8 cuboctahedra. There are a spread of Lu–Lu bond distances ranging from 3.47–3.63 Å. There are two shorter (3.51 Å) and two longer (3.57 Å) Lu–Nd bond lengths. Nd is bonded to twelve Lu atoms to form NdLu12 cuboctahedra that share corners with six equivalent NdLu12 cuboctahedra, corners with twelve LuNd4Lu8 cuboctahedra, edges with eighteen LuNd4Lu8 cuboctahedra, faces with eight equivalent NdLu12 cuboctahedra, and faces with twelve LuNd4Lu8 cuboctahedra.
DOI: 10.17188/1728435
title: Materials Data on YInCu4 by Materials Project

description: YInCu4 crystallizes in the cubic F-43m space group. The structure is three-dimensional. Y is bonded in a 12-coordinate geometry to twelve equivalent Cu and four equivalent In atoms. All Y–Cu bond lengths are 3.00 Å. All Y–In bond lengths are 3.14 Å. Cu is bonded to three equivalent Y, six equivalent Cu, and three equivalent In atoms to form a mixture of edge, corner, and face-sharing CuY3In3Cu6 cuboctahedra. There are three shorter (2.55 Å) and three longer (2.57 Å) Cu–Cu bond lengths. All Cu–In bond lengths are 3.00 Å. In is bonded in a 4-coordinate geometry to four equivalent Y and twelve equivalent Cu atoms.
DOI: 10.17188/1728436
title: Materials Data on LiFe2(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: 10.6073/pasta/7fc995219ea8453af3eb3617c4388422
title: Jornada Basin LTER: Wireless meteorological station at NPP M-NORT site: Daily average soil volumetric water content data: 2013 - ongoing

description: Daily average of 30-minute Volumetric Water Content at NPP M-NORT met station. Collection of soil volumetric water content data at Jornada LTER NPP sites, New Mexico, supports the environmental monitoring objectives of the Jornada LTER monitoring program that look at plant-soil water dynamics. Volumetric water content, bulk electrical conductivity, soil temperature, and bulk dielectric permittivity are measured and calculated at an automated meteorological station installed at Jornada LTER NPP M-NORT site. The daily average at 3 soil depths is calculated from measurements made every 30 minutes at 10 cm, 20 cm, and 30 cm. This is an ONGOING dataset.