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Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

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At least 523 records · Page 29
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DOE OSTI2020

Materials Data on LiAl2Ir by Materials Project

LiIrAl2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a distorted body-centered cubic geometry to six equivalent Ir and eight equivalent Al atoms. All Li–Ir bond lengths are 3.02 Å. All Li–Al bond lengths are 2.62 Å. Ir is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Al atoms. All Ir–Al bond lengths are 2.62 Å. Al is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ir atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on NiSnRh2 by Materials Project

Rh2NiSn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Rh is bonded in a body-centered cubic geometry to four equivalent Ni and four equivalent Sn atoms. All Rh–Ni bond lengths are 2.69 Å. All Rh–Sn bond lengths are 2.69 Å. Ni is bonded in a body-centered cubic geometry to eight equivalent Rh atoms. Sn is bonded in a body-centered cubic geometry to eight equivalent Rh atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Ni3Sn by Materials Project

Ni3Sn is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Ni sites. In the first Ni site, Ni is bonded in a distorted body-centered cubic geometry to eight equivalent Ni and six equivalent Sn atoms. All Ni–Ni bond lengths are 2.56 Å. All Ni–Sn bond lengths are 2.96 Å. In the second Ni site, Ni is bonded in a distorted body-centered cubic geometry to four equivalent Ni and four equivalent Sn atoms. All Ni–Sn bond lengths are 2.56 Å. Sn is bonded in a distorted body-centered cubic geometry to fourteen Ni atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on NbAlRu2 by Materials Project

NbRu2Al is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Nb is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Nb–Ru bond lengths are 2.69 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Nb and four equivalent Al atoms. All Ru–Al bond lengths are 2.69 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ru atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on LiAlAg2 by Materials Project

LiAlAg2 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 Ag atoms. All Li–Ag bond lengths are 2.75 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Al atoms. All Ag–Al bond lengths are 2.75 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ag atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li2MgIn by Materials Project

Li2MgIn 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 four equivalent Mg and four equivalent In atoms. All Li–Mg bond lengths are 2.91 Å. All Li–In bond lengths are 2.91 Å. Mg is bonded in a distorted body-centered cubic geometry to eight equivalent Li atoms. In is bonded in a body-centered cubic geometry to eight equivalent Li atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on LuInPd2 by Materials Project

LuPd2In is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Lu is bonded in a body-centered cubic geometry to eight equivalent Pd atoms. All Lu–Pd bond lengths are 2.91 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Lu and four equivalent In atoms. All Pd–In bond lengths are 2.91 Å. In is bonded in a distorted body-centered cubic geometry to eight equivalent Pd atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li2CdSn by Materials Project

Li2CdSn 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 four equivalent Cd and four equivalent Sn atoms. All Li–Cd bond lengths are 2.91 Å. All Li–Sn bond lengths are 2.91 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Li atoms. Sn is bonded in a body-centered cubic geometry to eight equivalent Li atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on CoCu2Sn by Materials Project

CoCu2Sn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Co is bonded in a distorted body-centered cubic geometry to eight equivalent Cu atoms. All Co–Cu bond lengths are 2.62 Å. Cu is bonded in a body-centered cubic geometry to four equivalent Co and four equivalent Sn atoms. All Cu–Sn bond lengths are 2.62 Å. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Cu atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on CeMgZn2 by Materials Project

MgZn2Ce 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 Zn atoms. All Mg–Zn bond lengths are 3.01 Å. Ce is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All Ce–Zn bond lengths are 3.01 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Ce atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on LiGeRh2 by Materials Project

LiRh2Ge 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 Rh and six equivalent Ge atoms. All Li–Rh bond lengths are 2.57 Å. All Li–Ge bond lengths are 2.97 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ge atoms. All Rh–Ge bond lengths are 2.57 Å. Ge is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Rh atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on LiIn2Rh by Materials Project

LiRhIn2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a distorted body-centered cubic geometry to six equivalent Rh and eight equivalent In atoms. All Li–Rh bond lengths are 3.27 Å. All Li–In bond lengths are 2.83 Å. Rh is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent In atoms. All Rh–In bond lengths are 2.83 Å. In is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Rh atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li7PN4 by Materials Project

Li7PN4 crystallizes in the cubic P-43n space group. The structure is three-dimensional. there are five inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four N3- atoms. All Li–N bond lengths are 1.99 Å. In the second Li1+ site, Li1+ is bonded to four equivalent N3- atoms to form LiN4 tetrahedra that share corners with four equivalent PN4 tetrahedra, corners with twelve LiN4 tetrahedra, and edges with four equivalent LiN4 tetrahedra. All Li–N bond lengths are 2.12 Å. In the third Li1+ site, Li1+ is bonded to four N3- atoms to form distorted LiN4 tetrahedra that share corners with four PN4 tetrahedra, corners with nine LiN4 tetrahedra, and edges with six equivalent LiN4 tetrahedra. There are one shorter (1.99 Å) and three longer (2.26 Å) Li–N bond lengths. In the fourth Li1+ site, Li1+ is bonded to four N3- atoms to form distorted LiN4 tetrahedra that share corners with two equivalent PN4 tetrahedra, corners with fourteen LiN4 tetrahedra, an edgeedge with one PN4 tetrahedra, and edges with four equivalent LiN4 tetrahedra. There are two shorter (2.05 Å) and two longer (2.18 Å) Li–N bond lengths. In the fifth Li1+ site, Li1+ is bonded to four N3- atoms to form distorted LiN4 tetrahedra that share corners with two PN4 tetrahedra, corners with eleven LiN4 tetrahedra, an edgeedge with one PN4 tetrahedra, and edges with five LiN4 tetrahedra. There are a spread of Li–N bond distances ranging from 2.00–2.24 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four equivalent N3- atoms to form PN4 tetrahedra that share corners with sixteen LiN4 tetrahedra and edges with six equivalent LiN4 tetrahedra. All P–N bond lengths are 1.68 Å. In the second P5+ site, P5+ is bonded to four N3- atoms to form PN4 tetrahedra that share corners with sixteen LiN4 tetrahedra and edges with four equivalent LiN4 tetrahedra. All P–N bond lengths are 1.70 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted body-centered cubic geometry to seven Li1+ and one P5+ atom. In the second N3- site, N3- is bonded in a distorted body-centered cubic geometry to seven Li1+ and one P5+ atom. In the third N3- site, N3- is bonded in a distorted body-centered cubic geometry to seven Li1+ and one P5+ atom. There are a spread of N–Li bond distances ranging from 2.00–2.18 Å.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on CdGeP2 by Materials Project

CdGeP2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cd2+ is bonded in a body-centered cubic geometry to eight equivalent P3- atoms. All Cd–P bond lengths are 2.89 Å. Ge4+ is bonded in a body-centered cubic geometry to eight equivalent P3- atoms. All Ge–P bond lengths are 2.89 Å. P3- is bonded in a body-centered cubic geometry to four equivalent Cd2+ and four equivalent Ge4+ atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li2CdSb by Materials Project

Li2CdSb 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 four equivalent Cd and four equivalent Sb atoms. All Li–Cd bond lengths are 2.95 Å. All Li–Sb bond lengths are 2.95 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Li atoms. Sb is bonded in a body-centered cubic geometry to eight equivalent Li atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on MnCu2Sb by Materials Project

MnCu2Sb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mn is bonded in a distorted body-centered cubic geometry to eight equivalent Cu and six equivalent Sb atoms. All Mn–Cu bond lengths are 2.73 Å. All Mn–Sb bond lengths are 3.15 Å. Cu is bonded in a body-centered cubic geometry to four equivalent Mn and four equivalent Sb atoms. All Cu–Sb bond lengths are 2.73 Å. Sb is bonded in a distorted body-centered cubic geometry to six equivalent Mn and eight equivalent Cu atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li2HgGe by Materials Project

Li2HgGe 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 four equivalent Hg and four equivalent Ge atoms. All Li–Hg bond lengths are 2.80 Å. All Li–Ge bond lengths are 2.80 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Li atoms. Ge is bonded in a body-centered cubic geometry to eight equivalent Li atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on ZnNi2Ge by Materials Project

Ni2ZnGe is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ni is bonded in a body-centered cubic geometry to four equivalent Zn and four equivalent Ge atoms. All Ni–Zn bond lengths are 2.52 Å. All Ni–Ge bond lengths are 2.52 Å. Zn is bonded in a distorted body-centered cubic geometry to eight equivalent Ni and six equivalent Ge atoms. All Zn–Ge bond lengths are 2.91 Å. Ge is bonded in a distorted body-centered cubic geometry to eight equivalent Ni and six equivalent Zn atoms.

36 MATERIALS SCIENCE↗