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At least 721 records · Page 40

Materials Data on DyGaCo by Materials Project

DyCoGa crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Dy is bonded in a 10-coordinate geometry to four equivalent Co and six equivalent Ga atoms. There are a spread of Dy–Co bond distances ranging from 2.84–2.91 Å. There are a spread of Dy–Ga bond distances ranging from 2.99–3.08 Å. Co is bonded in a 8-coordinate geometry to four equivalent Dy and four equivalent Ga atoms. There are a spread of Co–Ga bond distances ranging from 2.48–2.51 Å. Ga is bonded in a 10-coordinate geometry to six equivalent Dy and four equivalent Co atoms.

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Materials Data on DyIn3Cu2 by Materials Project

DyCu2In3 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Dy is bonded in a 6-coordinate geometry to six equivalent Cu and twelve equivalent In atoms. All Dy–Cu bond lengths are 3.36 Å. All Dy–In bond lengths are 3.61 Å. Cu is bonded in a 9-coordinate geometry to three equivalent Dy and six equivalent In atoms. All Cu–In bond lengths are 2.71 Å. In is bonded to four equivalent Dy, four equivalent Cu, and four equivalent In atoms to form a mixture of distorted corner, edge, and face-sharing InDy4In4Cu4 cuboctahedra. All In–In bond lengths are 2.91 Å.

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Materials Data on Dy5(ReO6)2 by Materials Project

Dy5(ReO6)2 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are five inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded to seven O2- atoms to form distorted DyO7 pentagonal bipyramids that share corners with two equivalent DyO6 octahedra, an edgeedge with one DyO6 octahedra, edges with two equivalent ReO6 octahedra, and edges with two equivalent DyO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 56°. There are a spread of Dy–O bond distances ranging from 2.28–2.42 Å. In the second Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.28–2.50 Å. In the third Dy3+ site, Dy3+ is bonded to six O2- atoms to form DyO6 octahedra that share corners with four equivalent ReO6 octahedra, corners with four DyO7 pentagonal bipyramids, and edges with two DyO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 38°. There are two shorter (2.22 Å) and four longer (2.32 Å) Dy–O bond lengths. In the fourth Dy3+ site, Dy3+ is bonded to seven O2- atoms to form distorted DyO7 pentagonal bipyramids that share corners with two equivalent DyO6 octahedra, an edgeedge with one DyO6 octahedra, edges with two equivalent ReO6 octahedra, and edges with two equivalent DyO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 57°. There are a spread of Dy–O bond distances ranging from 2.28–2.43 Å. In the fifth Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.28–2.49 Å. Re+4.50+ is bonded to six O2- atoms to form ReO6 octahedra that share corners with two equivalent DyO6 octahedra, edges with two equivalent ReO6 octahedra, and edges with two DyO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 38°. There are a spread of Re–O bond distances ranging from 1.97–2.10 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded to three Dy3+ and one Re+4.50+ atom to form distorted ODy3Re tetrahedra that share corners with ten ODy3Re tetrahedra, a cornercorner with one ODy2Re2 trigonal pyramid, edges with four ODy3Re tetrahedra, and an edgeedge with one ODy2Re2 trigonal pyramid. In the second O2- site, O2- is bonded to four Dy3+ atoms to form ODy4 tetrahedra that share corners with twelve ODy3Re tetrahedra, a cornercorner with one ODy2Re2 trigonal pyramid, and edges with four ODy4 tetrahedra. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Dy3+ and two equivalent Re+4.50+ atoms. In the fourth O2- site, O2- is bonded to two Dy3+ and two equivalent Re+4.50+ atoms to form distorted ODy2Re2 tetrahedra that share corners with eight ODy4 tetrahedra, edges with four ODy3Re tetrahedra, and an edgeedge with one ODy2Re2 trigonal pyramid. In the fifth O2- site, O2- is bonded to two Dy3+ and two equivalent Re+4.50+ atoms to form distorted ODy2Re2 trigonal pyramids that share corners with eight ODy3Re tetrahedra and edges with five ODy2Re2 tetrahedra. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Dy3+ and two equivalent Re+4.50+ atoms. In the seventh O2- site, O2- is bonded to three Dy3+ and one Re+4.50+ atom to form distorted ODy3Re tetrahedra that share corners with eleven ODy3Re tetrahedra, edges with four ODy3Re tetrahedra, and an edgeedge with one ODy2Re2 trigonal pyramid. In the eighth O2- site, O2- is bonded to four Dy3+ atoms to form ODy4 tetrahedra that share corners with eleven ODy3Re tetrahedra, corners with two equivalent ODy2Re2 trigonal pyramids, and edges with four ODy4 tetrahedra.

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Materials Data on Dy5Ti5O17 by Materials Project

Dy5Ti5O17 crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. there are five inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.25–2.78 Å. In the second Dy3+ site, Dy3+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Dy–O bond distances ranging from 2.31–2.82 Å. In the third Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.29–2.50 Å. In the fourth Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.23–2.74 Å. In the fifth Dy3+ site, Dy3+ is bonded in a 9-coordinate geometry to eight O2- atoms. There are a spread of Dy–O bond distances ranging from 2.33–2.58 Å. There are five inequivalent Ti+3.80+ sites. In the first Ti+3.80+ site, Ti+3.80+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 15–38°. There are a spread of Ti–O bond distances ranging from 1.82–2.21 Å. In the second Ti+3.80+ site, Ti+3.80+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 14–39°. There are a spread of Ti–O bond distances ranging from 1.89–2.06 Å. In the third Ti+3.80+ site, Ti+3.80+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 13–39°. There are a spread of Ti–O bond distances ranging from 1.88–2.15 Å. In the fourth Ti+3.80+ site, Ti+3.80+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 13–32°. There are a spread of Ti–O bond distances ranging from 1.90–2.12 Å. In the fifth Ti+3.80+ site, Ti+3.80+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 15–38°. There are a spread of Ti–O bond distances ranging from 1.88–2.20 Å. There are seventeen inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to three Dy3+ and two equivalent Ti+3.80+ atoms. In the second O2- site, O2- is bonded in a distorted T-shaped geometry to one Dy3+ and two equivalent Ti+3.80+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two Dy3+ and two equivalent Ti+3.80+ atoms. In the fourth O2- site, O2- is bonded to three Dy3+ and one Ti+3.80+ atom to form corner-sharing ODy3Ti tetrahedra. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to three Dy3+ and one Ti+3.80+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to two Dy3+ and two equivalent Ti+3.80+ atoms. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Dy3+ and two Ti+3.80+ atoms. In the eighth O2- site, O2- is bonded to two equivalent Dy3+ and two Ti+3.80+ atoms to form distorted corner-sharing ODy2Ti2 tetrahedra. In the ninth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Dy3+ and two Ti+3.80+ atoms. In the tenth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Dy3+ and two Ti+3.80+ atoms. In the eleventh O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Dy3+ and two Ti+3.80+ atoms. In the twelfth O2- site, O2- is bonded to two equivalent Dy3+ and two Ti+3.80+ atoms to form distorted corner-sharing ODy2Ti2 tetrahedra. In the thirteenth O2- site, O2- is bonded in a 4-coordinate geometry to three Dy3+ and one Ti+3.80+ atom. In the fourteenth O2- site, O2- is bonded to three Dy3+ and one Ti+3.80+ atom to form corner-sharing ODy3Ti tetrahedra. In the fifteenth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Dy3+ and two Ti+3.80+ atoms. In the sixteenth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Dy3+ and two Ti+3.80+ atoms. In the seventeenth O2- site, O2- is bonded in a 3-coordinate geometry to two Dy3+ and two equivalent Ti+3.80+ atoms.

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Materials Data on LiDy2Al by Materials Project

LiDy2Al 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 Dy atoms. All Li–Dy bond lengths are 3.15 Å. Dy is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Al atoms. All Dy–Al bond lengths are 3.15 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on LiDy2Ir by Materials Project

LiDy2Ir 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 Dy atoms. All Li–Dy bond lengths are 3.01 Å. Dy is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ir atoms. All Dy–Ir bond lengths are 3.01 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on LiDy2Tc by Materials Project

LiDy2Tc 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 Dy atoms. All Li–Dy bond lengths are 3.02 Å. Dy is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Tc atoms. All Dy–Tc bond lengths are 3.02 Å. Tc is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2NiIr by Materials Project

Dy2IrNi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Ni atoms. All Dy–Ir bond lengths are 2.95 Å. All Dy–Ni bond lengths are 2.95 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Ni is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2NiRu by Materials Project

Dy2RuNi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Ni atoms. All Dy–Ru bond lengths are 2.94 Å. All Dy–Ni bond lengths are 2.94 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Ni is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2CuOs by Materials Project

Dy2OsCu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Os and four equivalent Cu atoms. All Dy–Os bond lengths are 2.97 Å. All Dy–Cu bond lengths are 2.97 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2CuRh by Materials Project

Dy2RhCu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Rh and four equivalent Cu atoms. All Dy–Rh bond lengths are 2.99 Å. All Dy–Cu bond lengths are 2.99 Å. Rh is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2CuIr by Materials Project

Dy2IrCu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Cu atoms. All Dy–Ir bond lengths are 2.98 Å. All Dy–Cu bond lengths are 2.98 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2CdIn by Materials Project

Dy2CdIn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Cd and four equivalent In atoms. All Dy–Cd bond lengths are 3.25 Å. All Dy–In bond lengths are 3.25 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. In is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2AgOs by Materials Project

Dy2OsAg is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Os and four equivalent Ag atoms. All Dy–Os bond lengths are 3.03 Å. All Dy–Ag bond lengths are 3.03 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Ag is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2AgIr by Materials Project

Dy2IrAg is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Ag atoms. All Dy–Ir bond lengths are 3.05 Å. All Dy–Ag bond lengths are 3.05 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Ag is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2IrRh by Materials Project

Dy2IrRh is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Rh atoms. All Dy–Ir bond lengths are 2.97 Å. All Dy–Rh bond lengths are 2.97 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Rh is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2ZnOs by Materials Project

Dy2OsZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to four equivalent Os and four equivalent Zn atoms. All Dy–Os bond lengths are 3.01 Å. All Dy–Zn bond lengths are 3.01 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. Zn is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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Materials Data on Dy2MgAl by Materials Project

MgDy2Al is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. All Mg–Dy bond lengths are 3.18 Å. Dy is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Al atoms. All Dy–Al bond lengths are 3.18 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

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