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At least 1,621 records · Page 90

Materials Data on BaZnSn2 by Materials Project

BaZnSn2 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Ba is bonded in a 4-coordinate geometry to six equivalent Zn and eight Sn atoms. There are two shorter (3.63 Å) and four longer (4.02 Å) Ba–Zn bond lengths. There are a spread of Ba–Sn bond distances ranging from 3.62–4.03 Å. Zn is bonded in a 1-coordinate geometry to six equivalent Ba, two equivalent Zn, and one Sn atom. Both Zn–Zn bond lengths are 2.51 Å. The Zn–Sn bond length is 2.78 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 8-coordinate geometry to four equivalent Ba and four equivalent Sn atoms. There are two shorter (3.01 Å) and two longer (3.18 Å) Sn–Sn bond lengths. In the second Sn site, Sn is bonded in a distorted single-bond geometry to four equivalent Ba, one Zn, and four equivalent Sn atoms.

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Materials Data on ZrSn by Materials Project

ZrSn crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are three inequivalent Zr sites. In the first Zr site, Zr is bonded in a 5-coordinate geometry to five Sn atoms. There are a spread of Zr–Sn bond distances ranging from 3.05–3.19 Å. In the second Zr site, Zr is bonded in a 12-coordinate geometry to five Sn atoms. There are a spread of Zr–Sn bond distances ranging from 2.94–3.32 Å. In the third Zr site, Zr is bonded in a 6-coordinate geometry to six Sn atoms. There are a spread of Zr–Sn bond distances ranging from 2.99–3.18 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 8-coordinate geometry to eight Zr atoms. In the second Sn site, Sn is bonded in a 2-coordinate geometry to three Zr atoms. In the third Sn site, Sn is bonded in a 12-coordinate geometry to five Zr atoms.

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Materials Data on Th3Sn13Ru4 by Materials Project

Th3Ru4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Th is bonded in a 12-coordinate geometry to four equivalent Ru and twelve equivalent Sn atoms. All Th–Ru bond lengths are 3.58 Å. There are four shorter (3.54 Å) and eight longer (3.57 Å) Th–Sn bond lengths. Ru is bonded in a 6-coordinate geometry to three equivalent Th and six equivalent Sn atoms. All Ru–Sn bond lengths are 2.77 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent Th, two equivalent Ru, and one Sn atom. The Sn–Sn bond length is 3.46 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on Ce3Sn13Ir4 by Materials Project

Ce3Ir4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Ce is bonded in a 12-coordinate geometry to four equivalent Ir and twelve equivalent Sn atoms. All Ce–Ir bond lengths are 3.47 Å. There are eight shorter (3.44 Å) and four longer (3.45 Å) Ce–Sn bond lengths. Ir is bonded in a 6-coordinate geometry to three equivalent Ce and six equivalent Sn atoms. All Ir–Sn bond lengths are 2.69 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent Ce, two equivalent Ir, and one Sn atom. The Sn–Sn bond length is 3.37 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on Sr3Sn13Ir4 by Materials Project

Sr3Ir4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Sr is bonded in a 12-coordinate geometry to four equivalent Ir and twelve equivalent Sn atoms. All Sr–Ir bond lengths are 3.52 Å. There are four shorter (3.50 Å) and eight longer (3.52 Å) Sr–Sn bond lengths. Ir is bonded in a 6-coordinate geometry to three equivalent Sr and six equivalent Sn atoms. All Ir–Sn bond lengths are 2.72 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent Sr, two equivalent Ir, and one Sn atom. The Sn–Sn bond length is 3.36 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on Sm3Sn13Ru4 by Materials Project

Sm3Ru4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Sm is bonded in a 12-coordinate geometry to four equivalent Ru and twelve equivalent Sn atoms. All Sm–Ru bond lengths are 3.47 Å. There are four shorter (3.43 Å) and eight longer (3.47 Å) Sm–Sn bond lengths. Ru is bonded in a 6-coordinate geometry to three equivalent Sm and six equivalent Sn atoms. All Ru–Sn bond lengths are 2.68 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent Sm, two equivalent Ru, and one Sn atom. The Sn–Sn bond length is 3.36 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on LiDySn by Materials Project

LiDySn crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded in a 3-coordinate geometry to six Dy and four Sn atoms. There are a spread of Li–Dy bond distances ranging from 3.12–3.42 Å. There are a spread of Li–Sn bond distances ranging from 2.72–3.24 Å. In the second Li site, Li is bonded in a 4-coordinate geometry to six equivalent Dy and four Sn atoms. There are three shorter (3.17 Å) and three longer (3.49 Å) Li–Dy bond lengths. There are three shorter (2.74 Å) and one longer (2.91 Å) Li–Sn bond lengths. There are two inequivalent Dy sites. In the first Dy site, Dy is bonded in a 12-coordinate geometry to six Li and six Sn atoms. There are a spread of Dy–Sn bond distances ranging from 3.18–3.38 Å. In the second Dy site, Dy is bonded in a 12-coordinate geometry to six equivalent Li and six equivalent Sn atoms. There are three shorter (3.19 Å) and three longer (3.37 Å) Dy–Sn bond lengths. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 3-coordinate geometry to four Li and six Dy atoms. In the second Sn site, Sn is bonded in a 4-coordinate geometry to four Li and six equivalent Dy atoms.

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Materials Data on ScTi(NiSn)2 by Materials Project

ScTi(NiSn)2 is half-Heusler-derived structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Sc is bonded in a 4-coordinate geometry to four Ni and six Sn atoms. There are three shorter (2.64 Å) and one longer (2.67 Å) Sc–Ni bond lengths. There are three shorter (3.04 Å) and three longer (3.06 Å) Sc–Sn bond lengths. Ti is bonded in a 4-coordinate geometry to four Ni and six Sn atoms. All Ti–Ni bond lengths are 2.59 Å. There are three shorter (2.98 Å) and three longer (3.01 Å) Ti–Sn bond lengths. There are two inequivalent Ni sites. In the first Ni site, Ni is bonded in a body-centered cubic geometry to one Sc, three equivalent Ti, and four Sn atoms. There are one shorter (2.53 Å) and three longer (2.61 Å) Ni–Sn bond lengths. In the second Ni site, Ni is bonded in a body-centered cubic geometry to three equivalent Sc, one Ti, and four Sn atoms. There are three shorter (2.60 Å) and one longer (2.76 Å) Ni–Sn bond lengths. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 10-coordinate geometry to three equivalent Sc, three equivalent Ti, and four Ni atoms. In the second Sn site, Sn is bonded in a distorted q6 geometry to three equivalent Sc, three equivalent Ti, and four Ni atoms.

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Materials Data on InSn3 by Materials Project

InSn3 is beta-derived structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. In is bonded to six equivalent In and six equivalent Sn atoms to form InIn6Sn6 cuboctahedra that share corners with six equivalent InIn6Sn6 cuboctahedra, corners with twelve equivalent SnSn12 cuboctahedra, edges with six equivalent InIn6Sn6 cuboctahedra, edges with twelve equivalent SnIn3Sn9 cuboctahedra, faces with six equivalent InIn6Sn6 cuboctahedra, and faces with fourteen SnSn12 cuboctahedra. All In–In bond lengths are 3.37 Å. All In–Sn bond lengths are 3.41 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded to twelve Sn atoms to form SnSn12 cuboctahedra that share corners with six equivalent SnSn12 cuboctahedra, corners with twelve equivalent InIn6Sn6 cuboctahedra, edges with eighteen SnSn12 cuboctahedra, faces with two equivalent InIn6Sn6 cuboctahedra, and faces with eighteen SnSn12 cuboctahedra. There are six shorter (3.37 Å) and six longer (3.42 Å) Sn–Sn bond lengths. In the second Sn site, Sn is bonded to three equivalent In and nine Sn atoms to form distorted SnIn3Sn9 cuboctahedra that share corners with eighteen equivalent SnIn3Sn9 cuboctahedra, edges with six equivalent InIn6Sn6 cuboctahedra, edges with twelve SnSn12 cuboctahedra, faces with six equivalent InIn6Sn6 cuboctahedra, and faces with fourteen SnSn12 cuboctahedra. All Sn–Sn bond lengths are 3.37 Å.

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Materials Data on Dy5(Sn3Rh)6 by Materials Project

Dy5Rh6Sn17Sn crystallizes in the cubic F-43m space group. The structure is three-dimensional and consists of four 7440-31-5 molecules and one Dy5Rh6Sn17 framework. In the Dy5Rh6Sn17 framework, there are two inequivalent Dy sites. In the first Dy site, Dy is bonded in a 12-coordinate geometry to six equivalent Rh and twelve equivalent Sn atoms. All Dy–Rh bond lengths are 3.56 Å. All Dy–Sn bond lengths are 3.47 Å. In the second Dy site, Dy is bonded in a 1-coordinate geometry to three equivalent Rh and ten Sn atoms. All Dy–Rh bond lengths are 3.05 Å. There are a spread of Dy–Sn bond distances ranging from 2.91–3.41 Å. Rh is bonded in a 9-coordinate geometry to three Dy and six Sn atoms. There are four shorter (2.69 Å) and two longer (2.82 Å) Rh–Sn bond lengths. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a tetrahedral geometry to four equivalent Dy atoms. In the second Sn site, Sn is bonded in a hexagonal planar geometry to three equivalent Dy and three equivalent Rh atoms. In the third Sn site, Sn is bonded in a 2-coordinate geometry to three Dy and two equivalent Rh atoms.

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Materials Data on Sm3Sn13Ir4 by Materials Project

Sm3Ir4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Sm is bonded in a 12-coordinate geometry to four equivalent Ir and twelve equivalent Sn atoms. All Sm–Ir bond lengths are 3.47 Å. There are eight shorter (3.44 Å) and four longer (3.46 Å) Sm–Sn bond lengths. Ir is bonded in a 6-coordinate geometry to three equivalent Sm and six equivalent Sn atoms. All Ir–Sn bond lengths are 2.69 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent Sm, two equivalent Ir, and one Sn atom. The Sn–Sn bond length is 3.35 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on LiPrSn by Materials Project

LiPrSn crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded in a distorted trigonal planar geometry to six Pr and three Sn atoms. There are a spread of Li–Pr bond distances ranging from 3.23–3.54 Å. There are one shorter (2.78 Å) and two longer (2.81 Å) Li–Sn bond lengths. In the second Li site, Li is bonded in a 4-coordinate geometry to six equivalent Pr and four Sn atoms. There are three shorter (3.25 Å) and three longer (3.65 Å) Li–Pr bond lengths. There are three shorter (2.82 Å) and one longer (3.03 Å) Li–Sn bond lengths. There are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 12-coordinate geometry to six Li and six Sn atoms. There are a spread of Pr–Sn bond distances ranging from 3.33–3.46 Å. In the second Pr site, Pr is bonded in a 12-coordinate geometry to six equivalent Li and six equivalent Sn atoms. There are three shorter (3.29 Å) and three longer (3.50 Å) Pr–Sn bond lengths. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 3-coordinate geometry to three Li and six Pr atoms. In the second Sn site, Sn is bonded in a 4-coordinate geometry to four Li and six equivalent Pr atoms.

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Materials Data on MgSn by Materials Project

MgSn crystallizes in the monoclinic Cm space group. The structure is two-dimensional and consists of one MgSn sheet oriented in the (0, 0, 1) direction. there are three inequivalent Mg sites. In the first Mg site, Mg is bonded in a 5-coordinate geometry to five Sn atoms. There are a spread of Mg–Sn bond distances ranging from 3.05–3.20 Å. In the second Mg site, Mg is bonded in a 6-coordinate geometry to six Sn atoms. There are a spread of Mg–Sn bond distances ranging from 3.10–3.19 Å. In the third Mg site, Mg is bonded in a 11-coordinate geometry to four Sn atoms. There are two shorter (3.12 Å) and two longer (3.22 Å) Mg–Sn bond lengths. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 11-coordinate geometry to four Mg atoms. In the second Sn site, Sn is bonded in a 6-coordinate geometry to six Mg atoms. In the third Sn site, Sn is bonded in a 5-coordinate geometry to five Mg atoms.

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Materials Data on Pr3Sn13Ir4 by Materials Project

Pr3Ir4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Pr is bonded in a 12-coordinate geometry to four equivalent Ir and twelve equivalent Sn atoms. All Pr–Ir bond lengths are 3.48 Å. All Pr–Sn bond lengths are 3.46 Å. Ir is bonded in a 6-coordinate geometry to three equivalent Pr and six equivalent Sn atoms. All Ir–Sn bond lengths are 2.70 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent Pr, two equivalent Ir, and one Sn atom. The Sn–Sn bond length is 3.36 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on TiMn(Ni2Sn)2 by Materials Project

TiMn(Ni2Sn)2 is Tungsten-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Ti is bonded in a body-centered cubic geometry to eight Ni and six equivalent Sn atoms. There are two shorter (2.58 Å) and six longer (2.62 Å) Ti–Ni bond lengths. All Ti–Sn bond lengths are 3.06 Å. Mn is bonded in a distorted body-centered cubic geometry to eight Ni and six equivalent Sn atoms. There are six shorter (2.65 Å) and two longer (2.67 Å) Mn–Ni bond lengths. All Mn–Sn bond lengths are 3.02 Å. There are four inequivalent Ni sites. In the first Ni site, Ni is bonded in a distorted body-centered cubic geometry to one Ti, three equivalent Mn, and four equivalent Sn atoms. There are three shorter (2.61 Å) and one longer (2.63 Å) Ni–Sn bond lengths. In the second Ni site, Ni is bonded in a distorted body-centered cubic geometry to three equivalent Ti, one Mn, and four equivalent Sn atoms. There are one shorter (2.62 Å) and three longer (2.66 Å) Ni–Sn bond lengths. In the third Ni site, Ni is bonded in a distorted body-centered cubic geometry to one Ti, three equivalent Mn, and four equivalent Sn atoms. There are three shorter (2.61 Å) and one longer (2.63 Å) Ni–Sn bond lengths. In the fourth Ni site, Ni is bonded in a distorted body-centered cubic geometry to three equivalent Ti, one Mn, and four equivalent Sn atoms. All Ni–Ti bond lengths are 2.62 Å. There are one shorter (2.62 Å) and three longer (2.66 Å) Ni–Sn bond lengths. Sn is bonded in a 8-coordinate geometry to three equivalent Ti, three equivalent Mn, and eight Ni atoms.

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Materials Data on Yb3Co4Sn13 by Materials Project

Yb3Co4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Yb is bonded in a 12-coordinate geometry to four equivalent Co and twelve equivalent Sn atoms. All Yb–Co bond lengths are 3.38 Å. There are four shorter (3.32 Å) and eight longer (3.39 Å) Yb–Sn bond lengths. Co is bonded in a 6-coordinate geometry to three equivalent Yb and six equivalent Sn atoms. All Co–Sn bond lengths are 2.60 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 9-coordinate geometry to three equivalent Yb, two equivalent Co, and four Sn atoms. There are a spread of Sn–Sn bond distances ranging from 3.01–3.27 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on USnIr by Materials Project

UIrSn crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent U sites. In the first U site, U is bonded in a 11-coordinate geometry to five Ir and six Sn atoms. There are four shorter (3.01 Å) and one longer (3.06 Å) U–Ir bond lengths. There are two shorter (3.17 Å) and four longer (3.36 Å) U–Sn bond lengths. In the second U site, U is bonded in a 11-coordinate geometry to five Ir and six Sn atoms. There are a spread of U–Ir bond distances ranging from 3.00–3.08 Å. There are two shorter (3.17 Å) and four longer (3.36 Å) U–Sn bond lengths. There are two inequivalent Ir sites. In the first Ir site, Ir is bonded in a 9-coordinate geometry to six U and three Sn atoms. All Ir–Sn bond lengths are 2.80 Å. In the second Ir site, Ir is bonded in a 9-coordinate geometry to three U and six Sn atoms. All Ir–Sn bond lengths are 2.76 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 12-coordinate geometry to six U and four Ir atoms. In the second Sn site, Sn is bonded in a 12-coordinate geometry to six U and four Ir atoms.

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Materials Data on CuSnPd2 by Materials Project

Pd2CuSn crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are two inequivalent Pd sites. In the first Pd site, Pd is bonded to four equivalent Pd, four equivalent Cu, and four Sn atoms to form distorted PdCu4Sn4Pd4 cuboctahedra that share corners with twelve equivalent PdCu4Sn4Pd4 cuboctahedra, edges with eight equivalent PdCu2Sn4Pd6 cuboctahedra, edges with eight equivalent CuCu2Sn4Pd6 cuboctahedra, edges with eight SnCu4Pd8 cuboctahedra, faces with four equivalent CuCu2Sn4Pd6 cuboctahedra, faces with four SnCu4Pd8 cuboctahedra, and faces with ten PdCu4Sn4Pd4 cuboctahedra. All Pd–Pd bond lengths are 2.88 Å. All Pd–Cu bond lengths are 2.76 Å. There are a spread of Pd–Sn bond distances ranging from 2.70–2.94 Å. In the second Pd site, Pd is bonded to six Pd, two equivalent Cu, and four Sn atoms to form distorted PdCu2Sn4Pd6 cuboctahedra that share corners with four equivalent PdCu2Sn4Pd6 cuboctahedra, corners with eight equivalent CuCu2Sn4Pd6 cuboctahedra, edges with four equivalent CuCu2Sn4Pd6 cuboctahedra, edges with eight SnCu4Pd8 cuboctahedra, edges with twelve PdCu4Sn4Pd4 cuboctahedra, faces with four equivalent CuCu2Sn4Pd6 cuboctahedra, faces with four SnCu4Pd8 cuboctahedra, and faces with ten PdCu4Sn4Pd4 cuboctahedra. Both Pd–Pd bond lengths are 2.92 Å. Both Pd–Cu bond lengths are 2.80 Å. There are two shorter (2.77 Å) and two longer (2.87 Å) Pd–Sn bond lengths. Cu is bonded to six Pd, two equivalent Cu, and four Sn atoms to form CuCu2Sn4Pd6 cuboctahedra that share corners with four equivalent CuCu2Sn4Pd6 cuboctahedra, corners with eight equivalent PdCu2Sn4Pd6 cuboctahedra, edges with four equivalent CuCu2Sn4Pd6 cuboctahedra, edges with eight SnCu4Pd8 cuboctahedra, edges with twelve PdCu4Sn4Pd4 cuboctahedra, faces with four SnCu4Pd8 cuboctahedra, faces with six equivalent CuCu2Sn4Pd6 cuboctahedra, and faces with eight PdCu4Sn4Pd4 cuboctahedra. Both Cu–Cu bond lengths are 2.76 Å. There are two shorter (2.79 Å) and two longer (2.85 Å) Cu–Sn bond lengths. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded to eight Pd and four equivalent Cu atoms to form SnCu4Pd8 cuboctahedra that share corners with twelve SnCu4Pd8 cuboctahedra, edges with eight equivalent CuCu2Sn4Pd6 cuboctahedra, edges with sixteen PdCu4Sn4Pd4 cuboctahedra, faces with four equivalent CuCu2Sn4Pd6 cuboctahedra, faces with six SnCu4Pd8 cuboctahedra, and faces with eight PdCu4Sn4Pd4 cuboctahedra. In the second Sn site, Sn is bonded to four equivalent Pd and eight equivalent Cu atoms to form SnCu8Pd4 cuboctahedra that share corners with twelve SnCu4Pd8 cuboctahedra, edges with twenty-four PdCu4Sn4Pd4 cuboctahedra, faces with four equivalent PdCu4Sn4Pd4 cuboctahedra, faces with six SnCu4Pd8 cuboctahedra, and faces with eight equivalent CuCu2Sn4Pd6 cuboctahedra. In the third Sn site, Sn is bonded to twelve Pd atoms to form SnPd12 cuboctahedra that share corners with twelve SnCu4Pd8 cuboctahedra, edges with eight equivalent PdCu4Sn4Pd4 cuboctahedra, edges with sixteen equivalent CuCu2Sn4Pd6 cuboctahedra, faces with six SnCu4Pd8 cuboctahedra, and faces with twelve PdCu4Sn4Pd4 cuboctahedra.

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