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At least 163 records · Page 9

Materials Data on Hf4N3 by Materials Project

Hf4N3 is MAX Phase-derived structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three Hf4N3 sheets oriented in the (0, 0, 1) direction. there are four inequivalent Hf sites. In the first Hf site, Hf is bonded to six N atoms to form a mixture of distorted corner and edge-sharing HfN6 pentagonal pyramids. The corner-sharing octahedral tilt angles are 2°. There are three shorter (2.29 Å) and three longer (2.32 Å) Hf–N bond lengths. In the second Hf site, Hf is bonded in a distorted T-shaped geometry to three equivalent N atoms. All Hf–N bond lengths are 2.23 Å. In the third Hf site, Hf is bonded in a distorted T-shaped geometry to three equivalent N atoms. All Hf–N bond lengths are 2.29 Å. In the fourth Hf site, Hf is bonded to six N atoms to form a mixture of corner and edge-sharing HfN6 octahedra. There are three shorter (2.22 Å) and three longer (2.27 Å) Hf–N bond lengths. There are three inequivalent N sites. In the first N site, N is bonded to six Hf atoms to form a mixture of corner and edge-sharing NHf6 octahedra. The corner-sharing octahedral tilt angles are 2°. In the second N site, N is bonded to six Hf atoms to form a mixture of corner, edge, and face-sharing NHf6 octahedra. The corner-sharing octahedral tilt angles are 47°. In the third N site, N is bonded to six Hf atoms to form a mixture of corner, edge, and face-sharing NHf6 octahedra. The corner-sharing octahedra tilt angles range from 2–47°.

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Materials Data on ReW2C by Materials Project

W2ReC is H-Phase-like structured and crystallizes in the trigonal P3m1 space group. The structure is two-dimensional and consists of one W2ReC sheet oriented in the (0, 0, 1) direction. there are four inequivalent W sites. In the first W site, W is bonded in a 6-coordinate geometry to three equivalent Re and three equivalent C atoms. All W–Re bond lengths are 2.80 Å. All W–C bond lengths are 2.12 Å. In the second W site, W is bonded in a 3-coordinate geometry to three equivalent C atoms. All W–C bond lengths are 2.14 Å. In the third W site, W is bonded to six Re atoms to form distorted WRe6 cuboctahedra that share corners with three equivalent CRe3W3 octahedra, edges with six equivalent WRe6 cuboctahedra, and edges with three equivalent CRe3W3 octahedra. The corner-sharing octahedral tilt angles are 18°. There are three shorter (2.78 Å) and three longer (2.85 Å) W–Re bond lengths. In the fourth W site, W is bonded in a 3-coordinate geometry to three equivalent C atoms. All W–C bond lengths are 2.11 Å. There are two inequivalent Re sites. In the first Re site, Re is bonded in a 3-coordinate geometry to three equivalent W and three equivalent C atoms. All Re–C bond lengths are 2.10 Å. In the second Re site, Re is bonded to six W atoms to form distorted ReW6 cuboctahedra that share corners with three equivalent CW6 octahedra, edges with six equivalent ReW6 cuboctahedra, and edges with three equivalent CW6 octahedra. The corner-sharing octahedral tilt angles are 16°. There are two inequivalent C sites. In the first C site, C is bonded to six W atoms to form CW6 octahedra that share corners with three equivalent ReW6 cuboctahedra, edges with three equivalent ReW6 cuboctahedra, and edges with six equivalent CW6 octahedra. In the second C site, C is bonded to three equivalent W and three equivalent Re atoms to form CRe3W3 octahedra that share corners with three equivalent WRe6 cuboctahedra, edges with three equivalent WRe6 cuboctahedra, and edges with six equivalent CRe3W3 octahedra.

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Materials Data on CsLuS2 by Materials Project

CsLuS2 is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cs1+ is bonded in a 6-coordinate geometry to six equivalent S2- atoms. All Cs–S bond lengths are 3.48 Å. Lu3+ is bonded to six equivalent S2- atoms to form edge-sharing LuS6 octahedra. All Lu–S bond lengths are 2.73 Å. S2- is bonded to three equivalent Cs1+ and three equivalent Lu3+ atoms to form a mixture of distorted corner, edge, and face-sharing SCs3Lu3 octahedra. The corner-sharing octahedra tilt angles range from 0–39°.

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Materials Data on CsYbS2 by Materials Project

CsYbS2 is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cs1+ is bonded in a 6-coordinate geometry to six equivalent S2- atoms. All Cs–S bond lengths are 3.51 Å. Yb3+ is bonded to six equivalent S2- atoms to form edge-sharing YbS6 octahedra. All Yb–S bond lengths are 2.83 Å. S2- is bonded to three equivalent Cs1+ and three equivalent Yb3+ atoms to form a mixture of distorted face, edge, and corner-sharing SCs3Yb3 octahedra. The corner-sharing octahedra tilt angles range from 0–41°.

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Materials Data on Zr2InN by Materials Project

Zr2InN is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Zr is bonded in a 3-coordinate geometry to three equivalent In and three equivalent N atoms. All Zr–In bond lengths are 3.12 Å. All Zr–N bond lengths are 2.29 Å. In is bonded to six equivalent Zr atoms to form distorted InZr6 cuboctahedra that share corners with six equivalent NZr6 octahedra, edges with six equivalent InZr6 cuboctahedra, and edges with six equivalent NZr6 octahedra. The corner-sharing octahedral tilt angles are 19°. N is bonded to six equivalent Zr atoms to form NZr6 octahedra that share corners with six equivalent InZr6 cuboctahedra, edges with six equivalent InZr6 cuboctahedra, and edges with six equivalent NZr6 octahedra.

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Materials Data on BiSbTe2 by Materials Project

SbBiSbTe3Bi2SbTe3 is MAX Phase-like structured and crystallizes in the trigonal P3m1 space group. The structure is two-dimensional and consists of one antimony molecule; one Bi2SbTe3 sheet oriented in the (0, 0, 1) direction; and one BiSbTe3 sheet oriented in the (0, 0, 1) direction. In the Bi2SbTe3 sheet, there are two inequivalent Bi1+ sites. In the first Bi1+ site, Bi1+ is bonded to six Te2- atoms to form BiTe6 octahedra that share corners with six equivalent SbTe6 octahedra, edges with six equivalent BiTe6 octahedra, and a faceface with one SbTe6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are three shorter (3.07 Å) and three longer (3.33 Å) Bi–Te bond lengths. In the second Bi1+ site, Bi1+ is bonded in a 3-coordinate geometry to three equivalent Te2- atoms. All Bi–Te bond lengths are 3.75 Å. Sb3+ is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with six equivalent BiTe6 octahedra, edges with six equivalent SbTe6 octahedra, and a faceface with one BiTe6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are three shorter (3.04 Å) and three longer (3.22 Å) Sb–Te bond lengths. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Bi1+ and three equivalent Sb3+ atoms to form distorted edge-sharing TeBi3Sb3 pentagonal pyramids. In the second Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Bi1+ atoms. In the third Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Bi1+ and three equivalent Sb3+ atoms. In the BiSbTe3 sheet, Bi1+ is bonded to six Te2- atoms to form BiTe6 octahedra that share corners with six equivalent SbTe6 octahedra, edges with six equivalent BiTe6 octahedra, and a faceface with one SbTe6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are three shorter (3.08 Å) and three longer (3.30 Å) Bi–Te bond lengths. Sb3+ is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with six equivalent BiTe6 octahedra, edges with six equivalent SbTe6 octahedra, and a faceface with one BiTe6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are three shorter (3.04 Å) and three longer (3.25 Å) Sb–Te bond lengths. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Bi1+ and three equivalent Sb3+ atoms to form distorted edge-sharing TeBi3Sb3 pentagonal pyramids. In the second Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Bi1+ atoms. In the third Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Sb3+ atoms.

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Materials Data on ScTaN2 by Materials Project

ScTaN2 is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Sc3+ is bonded to six equivalent N3- atoms to form ScN6 octahedra that share corners with six equivalent TaN6 pentagonal pyramids, edges with six equivalent ScN6 octahedra, and edges with six equivalent TaN6 pentagonal pyramids. All Sc–N bond lengths are 2.22 Å. Ta3+ is bonded to six equivalent N3- atoms to form distorted TaN6 pentagonal pyramids that share corners with six equivalent ScN6 octahedra, edges with six equivalent ScN6 octahedra, and edges with six equivalent TaN6 pentagonal pyramids. The corner-sharing octahedral tilt angles are 0°. All Ta–N bond lengths are 2.22 Å. N3- is bonded to three equivalent Sc3+ and three equivalent Ta3+ atoms to form a mixture of face, edge, and corner-sharing NSc3Ta3 octahedra. The corner-sharing octahedra tilt angles range from 0–47°.

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Materials Data on Ti2SiC by Materials Project

Ti2SiC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ti4+ is bonded in a 6-coordinate geometry to three equivalent Si4- and three equivalent C4- atoms. All Ti–Si bond lengths are 2.70 Å. All Ti–C bond lengths are 2.12 Å. Si4- is bonded in a 6-coordinate geometry to six equivalent Ti4+ atoms. C4- is bonded to six equivalent Ti4+ atoms to form edge-sharing CTi6 octahedra.

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Materials Data on Nb2GaC by Materials Project

Nb2GaC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Nb is bonded in a 3-coordinate geometry to three equivalent Ga and three equivalent C atoms. All Nb–Ga bond lengths are 2.85 Å. All Nb–C bond lengths are 2.19 Å. Ga is bonded in a 12-coordinate geometry to six equivalent Nb atoms. C is bonded to six equivalent Nb atoms to form edge-sharing CNb6 octahedra.

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Materials Data on V2GaC by Materials Project

V2GaC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. V is bonded in a 3-coordinate geometry to three equivalent Ga and three equivalent C atoms. All V–Ga bond lengths are 2.71 Å. All V–C bond lengths are 2.02 Å. Ga is bonded to six equivalent V atoms to form distorted GaV6 cuboctahedra that share corners with six equivalent CV6 octahedra, edges with six equivalent GaV6 cuboctahedra, and edges with six equivalent CV6 octahedra. The corner-sharing octahedral tilt angles are 18°. C is bonded to six equivalent V atoms to form CV6 octahedra that share corners with six equivalent GaV6 cuboctahedra, edges with six equivalent GaV6 cuboctahedra, and edges with six equivalent CV6 octahedra.

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Materials Data on TcW2C by Materials Project

W2TcC is H-Phase-like structured and crystallizes in the trigonal P3m1 space group. The structure is two-dimensional and consists of one W2TcC sheet oriented in the (0, 0, 1) direction. there are four inequivalent W+3.50+ sites. In the first W+3.50+ site, W+3.50+ is bonded in a distorted T-shaped geometry to three equivalent C4- atoms. All W–C bond lengths are 2.13 Å. In the second W+3.50+ site, W+3.50+ is bonded to three equivalent Tc3- and three equivalent C4- atoms to form distorted edge-sharing WTc3C3 octahedra. All W–Tc bond lengths are 2.80 Å. All W–C bond lengths are 2.12 Å. In the third W+3.50+ site, W+3.50+ is bonded in a 6-coordinate geometry to six Tc3- atoms. There are three shorter (2.73 Å) and three longer (2.88 Å) W–Tc bond lengths. In the fourth W+3.50+ site, W+3.50+ is bonded in a distorted T-shaped geometry to three equivalent C4- atoms. All W–C bond lengths are 2.12 Å. There are two inequivalent Tc3- sites. In the first Tc3- site, Tc3- is bonded in a 12-coordinate geometry to six W+3.50+ atoms. In the second Tc3- site, Tc3- is bonded in a 3-coordinate geometry to three equivalent W+3.50+ and three equivalent C4- atoms. All Tc–C bond lengths are 2.08 Å. There are two inequivalent C4- sites. In the first C4- site, C4- is bonded to three equivalent W+3.50+ and three equivalent Tc3- atoms to form edge-sharing CTc3W3 octahedra. In the second C4- site, C4- is bonded to six W+3.50+ atoms to form edge-sharing CW6 octahedra.

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Materials Data on TaTlO12 by Materials Project

TaO12Tl is Zintl Phase structured and crystallizes in the cubic Fd-3m space group. The structure is zero-dimensional and consists of eight thallium molecules and eight TaO12 clusters. In each TaO12 cluster, Ta is bonded in a cuboctahedral geometry to twelve equivalent O atoms. All Ta–O bond lengths are 2.24 Å. O is bonded in a distorted single-bond geometry to one Ta atom.

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Materials Data on NaSbO12 by Materials Project

NaO12Sb is Zintl Phase structured and crystallizes in the cubic Fd-3m space group. The structure is zero-dimensional and consists of eight stibium metallicum molecules and eight NaO12 clusters. In each NaO12 cluster, Na is bonded in a distorted cuboctahedral geometry to twelve equivalent O atoms. All Na–O bond lengths are 2.52 Å. O is bonded in a 3-coordinate geometry to one Na and two equivalent O atoms. Both O–O bond lengths are 1.52 Å.

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Materials Data on Nb4C3 by Materials Project

Nb4C3 is MAX Phase-derived structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three Nb4C3 sheets oriented in the (0, 0, 1) direction. there are four inequivalent Nb3+ sites. In the first Nb3+ site, Nb3+ is bonded to six C4- atoms to form a mixture of distorted edge and corner-sharing NbC6 pentagonal pyramids. The corner-sharing octahedral tilt angles are 0°. There are three shorter (2.27 Å) and three longer (2.28 Å) Nb–C bond lengths. In the second Nb3+ site, Nb3+ is bonded in a distorted T-shaped geometry to three equivalent C4- atoms. All Nb–C bond lengths are 2.16 Å. In the third Nb3+ site, Nb3+ is bonded in a distorted T-shaped geometry to three equivalent C4- atoms. All Nb–C bond lengths are 2.18 Å. In the fourth Nb3+ site, Nb3+ is bonded to six C4- atoms to form a mixture of edge and corner-sharing NbC6 octahedra. There are three shorter (2.24 Å) and three longer (2.26 Å) Nb–C bond lengths. There are three inequivalent C4- sites. In the first C4- site, C4- is bonded to six Nb3+ atoms to form a mixture of edge and corner-sharing CNb6 octahedra. The corner-sharing octahedral tilt angles are 1°. In the second C4- site, C4- is bonded to six Nb3+ atoms to form a mixture of edge, corner, and face-sharing CNb6 octahedra. The corner-sharing octahedral tilt angles are 47°. In the third C4- site, C4- is bonded to six Nb3+ atoms to form a mixture of edge, corner, and face-sharing CNb6 octahedra. The corner-sharing octahedra tilt angles range from 1–47°.

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Materials Data on Ge2Bi2Te5 by Materials Project

Ge2Bi2Te5 is MAX Phase-like structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three Ge2Bi2Te5 sheets oriented in the (0, 0, 1) direction. there are two inequivalent Ge2+ sites. In the first Ge2+ site, Ge2+ is bonded to six Te2- atoms to form a mixture of distorted edge and corner-sharing GeTe6 octahedra. The corner-sharing octahedral tilt angles are 14°. There are three shorter (2.86 Å) and three longer (3.44 Å) Ge–Te bond lengths. In the second Ge2+ site, Ge2+ is bonded to six Te2- atoms to form GeTe6 octahedra that share corners with three equivalent GeTe6 octahedra, corners with three equivalent BiTe6 octahedra, edges with three equivalent BiTe6 octahedra, and edges with nine GeTe6 octahedra. The corner-sharing octahedra tilt angles range from 5–14°. There are three shorter (2.87 Å) and three longer (3.30 Å) Ge–Te bond lengths. There are two inequivalent Bi3+ sites. In the first Bi3+ site, Bi3+ is bonded to six Te2- atoms to form BiTe6 octahedra that share corners with three equivalent GeTe6 octahedra, corners with three equivalent BiTe6 octahedra, edges with three equivalent GeTe6 octahedra, and edges with nine BiTe6 octahedra. The corner-sharing octahedra tilt angles range from 1–5°. There are three shorter (3.09 Å) and three longer (3.24 Å) Bi–Te bond lengths. In the second Bi3+ site, Bi3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing BiTe6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (3.06 Å) and three longer (3.29 Å) Bi–Te bond lengths. There are five inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to six Bi3+ atoms to form TeBi6 octahedra that share corners with three equivalent TeGe3Bi3 octahedra and edges with nine TeBi6 octahedra. The corner-sharing octahedral tilt angles are 3°. In the second Te2- site, Te2- is bonded to six Ge2+ atoms to form distorted TeGe6 octahedra that share corners with three equivalent TeGe3Bi3 octahedra and edges with nine TeGe6 octahedra. The corner-sharing octahedral tilt angles are 11°. In the third Te2- site, Te2- is bonded to three equivalent Ge2+ and three equivalent Bi3+ atoms to form a mixture of edge and corner-sharing TeGe3Bi3 octahedra. The corner-sharing octahedra tilt angles range from 3–11°. In the fourth Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the fifth Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Ge2+ atoms.

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Materials Data on BiSbTe3 by Materials Project

BiSbTe3 is MAX Phase-like structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three BiSbTe3 sheets oriented in the (0, 0, 1) direction. Bi3+ is bonded to six Te2- atoms to form BiTe6 octahedra that share corners with three equivalent SbTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with six equivalent BiTe6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (3.08 Å) and three longer (3.28 Å) Bi–Te bond lengths. Sb3+ is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with three equivalent BiTe6 octahedra, edges with three equivalent BiTe6 octahedra, and edges with six equivalent SbTe6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (3.03 Å) and three longer (3.21 Å) Sb–Te bond lengths. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Bi3+ and three equivalent Sb3+ atoms to form edge-sharing TeBi3Sb3 octahedra. In the second Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the third Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Sb3+ atoms.

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Materials Data on CsLaO2 by Materials Project

CsLaO2 is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cs1+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms. All Cs–O bond lengths are 3.17 Å. La3+ is bonded to six equivalent O2- atoms to form edge-sharing LaO6 octahedra. All La–O bond lengths are 2.49 Å. O2- is bonded to three equivalent Cs1+ and three equivalent La3+ atoms to form a mixture of distorted face, edge, and corner-sharing OCs3La3 octahedra. The corner-sharing octahedra tilt angles range from 0–40°.

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Materials Data on TiAl2Cr3C2 by Materials Project

TiCr3Al2C2 is H-Phase-derived structured and crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Ti is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ti–Al bond lengths are 2.84 Å. All Ti–C bond lengths are 2.08 Å. There are three inequivalent Cr sites. In the first Cr site, Cr is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Cr–Al bond lengths are 2.70 Å. All Cr–C bond lengths are 1.96 Å. In the second Cr site, Cr is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Cr–Al bond lengths are 2.67 Å. All Cr–C bond lengths are 1.98 Å. In the third Cr site, Cr is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Cr–Al bond lengths are 2.64 Å. All Cr–C bond lengths are 1.97 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded to six Cr and six equivalent Al atoms to form AlAl6Cr6 cuboctahedra that share corners with six equivalent AlAl6Cr6 cuboctahedra, corners with six CTi3Cr3 octahedra, edges with six equivalent AlAl6Cr6 cuboctahedra, edges with six CTi3Cr3 octahedra, and faces with six equivalent AlAl6Cr6 cuboctahedra. The corner-sharing octahedra tilt angles range from 19–20°. All Al–Al bond lengths are 2.90 Å. In the second Al site, Al is bonded to three equivalent Ti, three equivalent Cr, and six equivalent Al atoms to form AlTi3Al6Cr3 cuboctahedra that share corners with six equivalent AlTi3Al6Cr3 cuboctahedra, corners with six CTi3Cr3 octahedra, edges with six equivalent AlTi3Al6Cr3 cuboctahedra, edges with six CTi3Cr3 octahedra, and faces with six equivalent AlTi3Al6Cr3 cuboctahedra. The corner-sharing octahedra tilt angles range from 18–19°. All Al–Al bond lengths are 2.90 Å. There are two inequivalent C sites. In the first C site, C is bonded to three equivalent Ti and three equivalent Cr atoms to form CTi3Cr3 octahedra that share corners with six AlAl6Cr6 cuboctahedra, edges with six AlAl6Cr6 cuboctahedra, and edges with six equivalent CTi3Cr3 octahedra. In the second C site, C is bonded to six Cr atoms to form CCr6 octahedra that share corners with six AlAl6Cr6 cuboctahedra, edges with six AlAl6Cr6 cuboctahedra, and edges with six equivalent CCr6 octahedra.

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