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Materials Data on CsEuS2 by Materials Project

CsEuS2 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 3.53 Å. Eu3+ is bonded to six equivalent S2- atoms to form edge-sharing EuS6 octahedra. All Eu–S bond lengths are 2.87 Å. S2- is bonded to three equivalent Cs1+ and three equivalent Eu3+ atoms to form a mixture of distorted edge, face, and corner-sharing SCs3Eu3 octahedra. The corner-sharing octahedra tilt angles range from 0–41°.

36 MATERIALS SCIENCE↗

Materials Data on GaMo2C by Materials Project

Mo2GaC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Mo is bonded in a 6-coordinate geometry to three equivalent Ga and three equivalent C atoms. All Mo–Ga bond lengths are 2.77 Å. All Mo–C bond lengths are 2.13 Å. Ga is bonded in a 12-coordinate geometry to six equivalent Mo atoms. C is bonded to six equivalent Mo atoms to form edge-sharing CMo6 octahedra.

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Materials Data on Cr2SiC by Materials Project

Cr2SiC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cr3+ is bonded in a 6-coordinate geometry to three equivalent Si4- and three equivalent C2- atoms. All Cr–Si bond lengths are 2.53 Å. All Cr–C bond lengths are 1.97 Å. Si4- is bonded in a 12-coordinate geometry to six equivalent Cr3+ atoms. C2- is bonded to six equivalent Cr3+ atoms to form edge-sharing CCr6 octahedra.

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Materials Data on BaTiN2 by Materials Project

BaTiN2 is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ba2+ is bonded in a 6-coordinate geometry to six equivalent N3- atoms. All Ba–N bond lengths are 2.74 Å. Ti4+ is bonded to six equivalent N3- atoms to form edge-sharing TiN6 octahedra. All Ti–N bond lengths are 2.18 Å. N3- is bonded to three equivalent Ba2+ and three equivalent Ti4+ atoms to form a mixture of distorted edge, face, and corner-sharing NBa3Ti3 octahedra. The corner-sharing octahedra tilt angles range from 0–40°.

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Materials Data on In(BiSe2)3 by Materials Project

InBiSe3Bi2Se3 is MAX Phase-like structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three Bi2Se3 sheets oriented in the (0, 0, 1) direction and three InBiSe3 sheets oriented in the (0, 0, 1) direction. In each Bi2Se3 sheet, there are two inequivalent Bi3+ sites. In the first Bi3+ site, Bi3+ is bonded to six Se2- atoms to form a mixture of edge and corner-sharing BiSe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (2.88 Å) and three longer (3.09 Å) Bi–Se bond lengths. In the second Bi3+ site, Bi3+ is bonded to six Se2- atoms to form a mixture of edge and corner-sharing BiSe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (2.88 Å) and three longer (3.11 Å) Bi–Se bond lengths. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the second Se2- site, Se2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the third Se2- site, Se2- is bonded to six Bi3+ atoms to form edge-sharing SeBi6 octahedra. In each InBiSe3 sheet, In3+ is bonded to six Se2- atoms to form InSe6 octahedra that share corners with three equivalent BiSe6 octahedra, edges with three equivalent BiSe6 octahedra, and edges with six equivalent InSe6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (2.73 Å) and three longer (3.01 Å) In–Se bond lengths. Bi3+ is bonded to six Se2- atoms to form BiSe6 octahedra that share corners with three equivalent InSe6 octahedra, edges with three equivalent InSe6 octahedra, and edges with six equivalent BiSe6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (2.88 Å) and three longer (3.12 Å) Bi–Se bond lengths. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the second Se2- site, Se2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent In3+ atoms. In the third Se2- site, Se2- is bonded to three equivalent In3+ and three equivalent Bi3+ atoms to form edge-sharing SeIn3Bi3 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on Ti3S4 by Materials Project

Ti3S4 is MAX Phase-derived structured and crystallizes in the trigonal P3m1 space group. The structure is two-dimensional and consists of one Ti3S4 sheet oriented in the (0, 0, 1) direction. there are three inequivalent Ti+2.67+ sites. In the first Ti+2.67+ site, Ti+2.67+ is bonded to six S2- atoms to form a mixture of face, edge, and corner-sharing TiS6 octahedra. The corner-sharing octahedral tilt angles are 46°. There are three shorter (2.42 Å) and three longer (2.54 Å) Ti–S bond lengths. In the second Ti+2.67+ site, Ti+2.67+ is bonded to six S2- atoms to form a mixture of face, edge, and corner-sharing TiS6 octahedra. The corner-sharing octahedra tilt angles range from 3–46°. There are three shorter (2.38 Å) and three longer (2.58 Å) Ti–S bond lengths. In the third Ti+2.67+ site, Ti+2.67+ is bonded to six S2- atoms to form a mixture of edge and corner-sharing TiS6 octahedra. The corner-sharing octahedral tilt angles are 3°. There are three shorter (2.43 Å) and three longer (2.46 Å) Ti–S bond lengths. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded to six Ti+2.67+ atoms to form a mixture of distorted edge and corner-sharing STi6 pentagonal pyramids. The corner-sharing octahedral tilt angles are 6°. In the second S2- site, S2- is bonded in a distorted T-shaped geometry to three equivalent Ti+2.67+ atoms. In the third S2- site, S2- is bonded in a distorted T-shaped geometry to three equivalent Ti+2.67+ atoms. In the fourth S2- site, S2- is bonded to six Ti+2.67+ atoms to form a mixture of edge and corner-sharing STi6 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on GeSbTe3 by Materials Project

GeSbTe3 is MAX Phase-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Ge3+ is bonded to six Te2- atoms to form GeTe6 octahedra that share corners with three equivalent SbTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with six equivalent GeTe6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (2.86 Å) and three longer (3.14 Å) Ge–Te bond lengths. Sb3+ is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with three equivalent GeTe6 octahedra, edges with three equivalent GeTe6 octahedra, and edges with six equivalent SbTe6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (3.04 Å) and three longer (3.12 Å) Sb–Te bond lengths. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Ge3+ and three equivalent Sb3+ atoms to form edge-sharing TeGe3Sb3 octahedra. In the second Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Sb3+ and three equivalent Te2- atoms. All Te–Te bond lengths are 3.55 Å. In the third Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Ge3+ and three equivalent Te2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on AlW2C by Materials Project

W2AlC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. W is bonded to three equivalent Al and three equivalent C atoms to form a mixture of distorted face, edge, and corner-sharing WAl3C3 octahedra. The corner-sharing octahedra tilt angles range from 0–36°. All W–Al bond lengths are 2.80 Å. All W–C bond lengths are 2.13 Å. Al is bonded in a 12-coordinate geometry to six equivalent W atoms. C is bonded to six equivalent W atoms to form edge-sharing CW6 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on Hf2PbC by Materials Project

Hf2PbC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Hf is bonded in a 6-coordinate geometry to three equivalent Pb and three equivalent C atoms. All Hf–Pb bond lengths are 3.15 Å. All Hf–C bond lengths are 2.29 Å. Pb is bonded in a 12-coordinate geometry to six equivalent Hf atoms. C is bonded to six equivalent Hf atoms to form edge-sharing CHf6 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on Tb2CI by Materials Project

Tb2CI is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Tb is bonded to three equivalent C and three equivalent I atoms to form a mixture of distorted face, edge, and corner-sharing TbC3I3 octahedra. The corner-sharing octahedra tilt angles range from 0–39°. All Tb–C bond lengths are 2.53 Å. All Tb–I bond lengths are 3.27 Å. C is bonded to six equivalent Tb atoms to form edge-sharing CTb6 octahedra. I is bonded in a 6-coordinate geometry to six equivalent Tb atoms.

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Materials Data on InGe2SbTe5 by Materials Project

Ge2SbInTe5 is MAX Phase-derived structured and crystallizes in the trigonal P3m1 space group. The structure is two-dimensional and consists of one Ge2SbInTe5 sheet oriented in the (0, 0, 1) direction. In3+ is bonded to six Te2- atoms to form InTe6 octahedra that share corners with three equivalent GeTe6 octahedra, corners with three equivalent SbTe6 octahedra, edges with three equivalent GeTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with six equivalent InTe6 octahedra. The corner-sharing octahedra tilt angles range from 1–11°. There are three shorter (2.92 Å) and three longer (3.15 Å) In–Te bond lengths. There are two inequivalent Ge4+ sites. In the first Ge4+ site, Ge4+ is bonded to six Te2- atoms to form distorted GeTe6 octahedra that share corners with three equivalent InTe6 octahedra, edges with three equivalent InTe6 octahedra, and edges with six equivalent GeTe6 octahedra. The corner-sharing octahedral tilt angles are 11°. There are three shorter (2.84 Å) and three longer (3.37 Å) Ge–Te bond lengths. In the second Ge4+ site, Ge4+ is bonded to six Te2- atoms to form GeTe6 octahedra that share corners with three equivalent SbTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with six equivalent GeTe6 octahedra. The corner-sharing octahedral tilt angles are 6°. There are three shorter (2.85 Å) and three longer (3.30 Å) Ge–Te bond lengths. Sb1- is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with three equivalent InTe6 octahedra, corners with three equivalent GeTe6 octahedra, edges with three equivalent InTe6 octahedra, edges with three equivalent GeTe6 octahedra, and edges with six equivalent SbTe6 octahedra. The corner-sharing octahedra tilt angles range from 1–6°. There are three shorter (3.02 Å) and three longer (3.18 Å) Sb–Te bond lengths. There are five inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Ge4+ atoms. In the second Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Ge4+ atoms. In the third Te2- site, Te2- is bonded to three equivalent In3+ and three equivalent Sb1- atoms to form a mixture of corner and edge-sharing TeIn3Sb3 octahedra. The corner-sharing octahedra tilt angles range from 4–6°. In the fourth Te2- site, Te2- is bonded to three equivalent Ge4+ and three equivalent Sb1- atoms to form a mixture of corner and edge-sharing TeGe3Sb3 octahedra. The corner-sharing octahedral tilt angles are 4°. In the fifth Te2- site, Te2- is bonded to three equivalent In3+ and three equivalent Ge4+ atoms to form distorted TeIn3Ge3 octahedra that share corners with three equivalent TeIn3Sb3 octahedra and edges with nine TeIn3Ge3 octahedra. The corner-sharing octahedral tilt angles are 6°.

36 MATERIALS SCIENCE↗

Materials Data on LiTaN2 by Materials Project

LiTaN2 is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Li1+ is bonded to six equivalent N3- atoms to form LiN6 octahedra that share corners with six equivalent TaN6 pentagonal pyramids, edges with six equivalent LiN6 octahedra, and edges with six equivalent TaN6 pentagonal pyramids. All Li–N bond lengths are 2.24 Å. Ta5+ is bonded to six equivalent N3- atoms to form distorted TaN6 pentagonal pyramids that share corners with six equivalent LiN6 octahedra, edges with six equivalent LiN6 octahedra, and edges with six equivalent TaN6 pentagonal pyramids. The corner-sharing octahedral tilt angles are 3°. All Ta–N bond lengths are 2.14 Å. N3- is bonded to three equivalent Li1+ and three equivalent Ta5+ atoms to form a mixture of edge, face, and corner-sharing NLi3Ta3 octahedra. The corner-sharing octahedra tilt angles range from 0–48°.

36 MATERIALS SCIENCE↗

Materials Data on Bi(SbTe2)3 by Materials Project

BiSbTe3Sb2Te3 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 and three Sb2Te3 sheets oriented in the (0, 0, 1) direction. In each BiSbTe3 sheet, 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 (3.26 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 (3.19 Å) Sb–Te bond lengths. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Sb3+ atoms. In the second Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Bi3+ atoms. In the third Te2- site, Te2- is bonded to three equivalent Bi3+ and three equivalent Sb3+ atoms to form edge-sharing TeBi3Sb3 octahedra. In each Sb2Te3 sheet, there are two inequivalent Sb3+ sites. In the first Sb3+ site, Sb3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SbTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (3.04 Å) and three longer (3.21 Å) Sb–Te bond lengths. In the second Sb3+ site, Sb3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SbTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (3.04 Å) and three longer (3.21 Å) Sb–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to six Sb3+ atoms to form edge-sharing TeSb6 octahedra. In the second Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Sb3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ti5Al2C3 by Materials Project

Ti5Al2C3 is H-Phase-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. there are five inequivalent Ti sites. In the first Ti site, Ti is bonded to six C atoms to form edge-sharing TiC6 octahedra. There are three shorter (2.19 Å) and three longer (2.20 Å) Ti–C bond lengths. In the second Ti site, Ti is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ti–Al bond lengths are 2.92 Å. All Ti–C bond lengths are 2.07 Å. In the third Ti site, Ti is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ti–Al bond lengths are 2.90 Å. All Ti–C bond lengths are 2.11 Å. In the fourth Ti site, Ti is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ti–Al bond lengths are 2.89 Å. All Ti–C bond lengths are 2.11 Å. In the fifth Ti site, Ti is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ti–Al bond lengths are 2.91 Å. All Ti–C bond lengths are 2.07 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded to six Ti and six equivalent Al atoms to form distorted AlTi6Al6 cuboctahedra that share corners with six equivalent AlTi6Al6 cuboctahedra, corners with six CTi6 octahedra, edges with six equivalent AlTi6Al6 cuboctahedra, edges with six CTi6 octahedra, and faces with six equivalent AlTi6Al6 cuboctahedra. The corner-sharing octahedra tilt angles range from 19–21°. All Al–Al bond lengths are 3.07 Å. In the second Al site, Al is bonded to six Ti and six equivalent Al atoms to form distorted AlTi6Al6 cuboctahedra that share corners with six equivalent AlTi6Al6 cuboctahedra, corners with six CTi6 octahedra, edges with six equivalent AlTi6Al6 cuboctahedra, edges with six CTi6 octahedra, and faces with six equivalent AlTi6Al6 cuboctahedra. The corner-sharing octahedra tilt angles range from 19–21°. All Al–Al bond lengths are 3.07 Å. There are three inequivalent C sites. In the first C site, C is bonded to six Ti atoms to form CTi6 octahedra that share corners with three equivalent AlTi6Al6 cuboctahedra, corners with three equivalent CTi6 octahedra, edges with three equivalent AlTi6Al6 cuboctahedra, and edges with nine CTi6 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second C site, C is bonded to six Ti atoms to form CTi6 octahedra that share corners with three equivalent AlTi6Al6 cuboctahedra, corners with three equivalent CTi6 octahedra, edges with three equivalent AlTi6Al6 cuboctahedra, and edges with nine CTi6 octahedra. The corner-sharing octahedral tilt angles are 0°. In the third C site, C is bonded to six Ti atoms to form CTi6 octahedra that share corners with six AlTi6Al6 cuboctahedra, edges with six AlTi6Al6 cuboctahedra, and edges with six equivalent CTi6 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on CsTmS2 by Materials Project

CsTmS2 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. Tm3+ is bonded to six equivalent S2- atoms to form edge-sharing TmS6 octahedra. All Tm–S bond lengths are 2.75 Å. S2- is bonded to three equivalent Cs1+ and three equivalent Tm3+ atoms to form a mixture of distorted face, edge, and corner-sharing SCs3Tm3 octahedra. The corner-sharing octahedra tilt angles range from 0–39°.

36 MATERIALS SCIENCE↗

Materials Data on Ta2Al3V4C3 by Materials Project

Ta2V4Al3C3 is H-Phase-derived structured and crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. there are four inequivalent Ta sites. In the first Ta site, Ta is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ta–Al bond lengths are 2.84 Å. All Ta–C bond lengths are 2.16 Å. In the second Ta site, Ta is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ta–Al bond lengths are 2.89 Å. All Ta–C bond lengths are 2.18 Å. In the third Ta site, Ta is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ta–Al bond lengths are 2.88 Å. All Ta–C bond lengths are 2.17 Å. In the fourth Ta site, Ta is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All Ta–Al bond lengths are 2.84 Å. All Ta–C bond lengths are 2.16 Å. There are eight inequivalent V sites. In the first V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.78 Å. All V–C bond lengths are 2.04 Å. In the second V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.78 Å. All V–C bond lengths are 2.04 Å. In the third V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.72 Å. All V–C bond lengths are 2.04 Å. In the fourth V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.77 Å. All V–C bond lengths are 2.05 Å. In the fifth V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.78 Å. All V–C bond lengths are 2.04 Å. In the sixth V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.72 Å. All V–C bond lengths are 2.04 Å. In the seventh V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.75 Å. All V–C bond lengths are 2.04 Å. In the eighth V site, V is bonded in a 3-coordinate geometry to three equivalent Al and three equivalent C atoms. All V–Al bond lengths are 2.74 Å. All V–C bond lengths are 2.04 Å. There are six inequivalent Al sites. In the first Al site, Al is bonded to three equivalent Ta, three equivalent V, and six equivalent Al atoms to form distorted AlTa3Al6V3 cuboctahedra that share corners with six equivalent AlTa3Al6V3 cuboctahedra, corners with six CTa6 octahedra, edges with six equivalent AlTa3Al6V3 cuboctahedra, edges with six CTa6 octahedra, and faces with six equivalent AlTa3Al6V3 cuboctahedra. The corner-sharing octahedra tilt angles range from 16–19°. All Al–Al bond lengths are 2.99 Å. In the second Al site, Al is bonded to six V and six equivalent Al atoms to form AlAl6V6 cuboctahedra that share corners with six equivalent AlAl6V6 cuboctahedra, corners with six CTa3V3 octahedra, edges with six equivalent AlAl6V6 cuboctahedra, edges with six CTa3V3 octahedra, and faces with six equivalent AlAl6V6 cuboctahedra. The corner-sharing octahedra tilt angles range from 19–20°. All Al–Al bond lengths are 2.99 Å. In the third Al site, Al is bonded to six V and six equivalent Al atoms to form AlAl6V6 cuboctahedra that share corners with six equivalent AlAl6V6 cuboctahedra, corners with six CTa3V3 octahedra, edges with six equivalent AlAl6V6 cuboctahedra, edges with six CTa3V3 octahedra, and faces with six equivalent AlAl6V6 cuboctahedra. The corner-sharing octahedra tilt angles range from 19–20°. All Al–Al bond lengths are 2.99 Å. In the fourth Al site, Al is bonded to three equivalent Ta, three equivalent V, and six equivalent Al atoms to form distorted AlTa3Al6V3 cuboctahedra that share corners with six equivalent AlTa3Al6V3 cuboctahedra, corners with six CTa6 octahedra, edges with six equivalent AlTa3Al6V3 cuboctahedra, edges with six CTa6 octahedra, and faces with six equivalent AlTa3Al6V3 cuboctahedra. The corner-sharing octahedra tilt angles range from 16–18°. All Al–Al bond lengths are 2.99 Å. In the fifth Al site, Al is bonded to three equivalent Ta, three equivalent V, and six equivalent Al atoms to form AlTa3Al6V3 cuboctahedra that share corners with six equivalent AlTa3Al6V3 cuboctahedra, corners with six CTa3V3 octahedra, edges with six equivalent AlTa3Al6V3 cuboctahedra, edges with six CTa3V3 octahedra, and faces with six equivalent AlTa3Al6V3 cuboctahedra. The corner-sharing octahedra tilt angles range from 16–19°. All Al–Al bond lengths are 2.99 Å. In the sixth Al site, Al is bonded to three equivalent Ta, three equivalent V, and six equivalent Al atoms to form distorted AlTa3Al6V3 cuboctahedra that share corners with six equivalent AlTa3Al6V3 cuboctahedra, corners with six CTa3V3 octahedra, edges with six equivalent AlTa3Al6V3 cuboctahedra, edges with six CTa3V3 octahedra, and faces with six equivalent AlTa3Al6V3 cuboctahedra. The corner-sharing octahedra tilt angles range from 16–19°. All Al–Al bond lengths are 2.99 Å. There are six inequivalent C sites. In the first C site, C is bonded to six Ta atoms to form CTa6 octahedra that share corners with six AlTa3Al6V3 cuboctahedra, edges with six AlTa3Al6V3 cuboctahedra, and edges with six equivalent CTa6 octahedra. In the second C site, C is bonded to three equivalent Ta and three equivalent V atoms to form CTa3V3 octahedra that share corners with six AlTa3Al6V3 cuboctahedra, edges with six AlTa3Al6V3 cuboctahedra, and edges with six equivalent CTa3V3 octahedra. In the third C site, C is bonded to three equivalent Ta and three equivalent V atoms to form CTa3V3 octahedra that share corners with six AlTa3Al6V3 cuboctahedra, edges with six AlTa3Al6V3 cuboctahedra, and edges with six equivalent CTa3V3 octahedra. In the fourth C site, C is bonded to six V atoms to form CV6 octahedra that share corners with six AlTa3Al6V3 cuboctahedra, edges with six AlTa3Al6V3 cuboctahedra, and edges with six equivalent CV6 octahedra. In the fifth C site, C is bonded to six V atoms to form CV6 octahedra that share corners with six AlAl6V6 cuboctahedra, edges with six AlAl6V6 cuboctahedra, and edges with six equivalent CV6 octahedra. In the sixth C site, C is bonded to six V atoms to form CV6 octahedra that share corners with six AlTa3Al6V3 cuboctahedra, edges with six AlTa3Al6V3 cuboctahedra, and edges with six equivalent CV6 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on Hf2TlC by Materials Project

Hf2TlC is H-Phase structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Hf is bonded in a 3-coordinate geometry to three equivalent Tl and three equivalent C atoms. All Hf–Tl bond lengths are 3.16 Å. All Hf–C bond lengths are 2.28 Å. Tl is bonded to six equivalent Hf atoms to form distorted TlHf6 cuboctahedra that share corners with six equivalent CHf6 octahedra, edges with six equivalent TlHf6 cuboctahedra, and edges with six equivalent CHf6 octahedra. The corner-sharing octahedral tilt angles are 20°. C is bonded to six equivalent Hf atoms to form CHf6 octahedra that share corners with six equivalent TlHf6 cuboctahedra, edges with six equivalent TlHf6 cuboctahedra, and edges with six equivalent CHf6 octahedra.

36 MATERIALS SCIENCE↗

Sensitivity of an early dark matter search using the electromagnetic calorimeter as a target for the Light Dark Matter eXperiment

The Light Dark Matter eXperiment (LDMX) is proposed to employ a thin tungsten target and a multi-GeV electron beam to carry out a missing momentum search for the production of dark matter candidate particles. We study the sensitivity for a complementary missing-energy-based search using the LDMX Electromagnetic Calorimeter as an active target with a focus on early running. In this context, we construct an event selection from a limited set of variables that projects sensitivity into previously-unexplored regions of light dark matter phase space — down to an effective dark photon interaction strength y of approximately 2 × 10 −13 (5 × 10 −12 ) for a 1 MeV (10 MeV) dark matter candidate mass.

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