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Materials Data on Ba2TlZn by Materials Project

Ba2ZnTl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ba is bonded in a body-centered cubic geometry to four equivalent Zn and four equivalent Tl atoms. All Ba–Zn bond lengths are 3.66 Å. All Ba–Tl bond lengths are 3.66 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Ba atoms. Tl is bonded in a body-centered cubic geometry to eight equivalent Ba atoms.

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Materials Data on Ca3Tl by Materials Project

Ca3Tl is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ca is bonded in a 12-coordinate geometry to four equivalent Tl atoms. There are two shorter (3.49 Å) and two longer (3.69 Å) Ca–Tl bond lengths. Tl is bonded to twelve equivalent Ca atoms to form a mixture of corner and face-sharing TlCa12 cuboctahedra.

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Materials Data on Ba6Tl2NCl by Materials Project

Ba6Tl2NCl is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ba is bonded in a linear geometry to four equivalent Tl, one N, and one Cl atom. All Ba–Tl bond lengths are 4.15 Å. The Ba–N bond length is 2.73 Å. The Ba–Cl bond length is 3.14 Å. Tl is bonded to twelve equivalent Ba atoms to form TlBa12 cuboctahedra that share corners with twelve equivalent TlBa12 cuboctahedra, faces with six equivalent TlBa12 cuboctahedra, faces with four equivalent NBa6 octahedra, and faces with four equivalent ClBa6 octahedra. N is bonded to six equivalent Ba atoms to form NBa6 octahedra that share corners with six equivalent ClBa6 octahedra and faces with eight equivalent TlBa12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. Cl is bonded to six equivalent Ba atoms to form ClBa6 octahedra that share corners with six equivalent NBa6 octahedra and faces with eight equivalent TlBa12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on Ti3TlN by Materials Project

Ti3TlN is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Ti is bonded in a linear geometry to four equivalent Tl and two equivalent N atoms. All Ti–Tl bond lengths are 2.98 Å. Both Ti–N bond lengths are 2.11 Å. Tl is bonded to twelve equivalent Ti atoms to form TlTi12 cuboctahedra that share corners with twelve equivalent TlTi12 cuboctahedra, faces with six equivalent TlTi12 cuboctahedra, and faces with eight equivalent NTi6 octahedra. N is bonded to six equivalent Ti atoms to form NTi6 octahedra that share corners with six equivalent NTi6 octahedra and faces with eight equivalent TlTi12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on CsTlF3 by Materials Project

CsTlF3 is (Cubic) Perovskite structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Cs is bonded to twelve equivalent F atoms to form CsF12 cuboctahedra that share corners with twelve equivalent CsF12 cuboctahedra, faces with six equivalent CsF12 cuboctahedra, and faces with eight equivalent TlF6 octahedra. There are a spread of Cs–F bond distances ranging from 3.31–3.45 Å. Tl is bonded to six equivalent F atoms to form TlF6 octahedra that share corners with six equivalent TlF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 1°. All Tl–F bond lengths are 2.39 Å. F is bonded in a distorted linear geometry to four equivalent Cs and two equivalent Tl atoms.

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Materials Data on RbTlBr3 by Materials Project

RbTlBr3 is Ilmenite-like structured and crystallizes in the trigonal R3c space group. The structure is three-dimensional. Rb is bonded in a 6-coordinate geometry to six equivalent Br atoms. There are three shorter (3.54 Å) and three longer (3.76 Å) Rb–Br bond lengths. Tl is bonded to six equivalent Br atoms to form corner-sharing TlBr6 octahedra. The corner-sharing octahedral tilt angles are 24°. There are three shorter (2.95 Å) and three longer (2.99 Å) Tl–Br bond lengths. Br is bonded to two equivalent Rb and two equivalent Tl atoms to form a mixture of distorted edge and corner-sharing BrRb2Tl2 trigonal pyramids.

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Materials Data on Ba6YTl3(Cu2O7)3 by Materials Project

Ba6YTl3(Cu2O7)3 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.71–3.07 Å. In the second Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.74–3.05 Å. In the third Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.74–3.05 Å. In the fourth Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.72–3.07 Å. In the fifth Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.74–3.06 Å. In the sixth Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.74–3.04 Å. Y3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.35–2.38 Å. There are six inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.83–2.07 Å. In the second Cu3+ site, Cu3+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.84–2.07 Å. In the third Cu3+ site, Cu3+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.85–1.90 Å. In the fourth Cu3+ site, Cu3+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.83–2.07 Å. In the fifth Cu3+ site, Cu3+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.84–1.90 Å. In the sixth Cu3+ site, Cu3+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.85–2.06 Å. There are three inequivalent Tl3+ sites. In the first Tl3+ site, Tl3+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing TlO6 octahedra. The corner-sharing octahedra tilt angles range from 0–5°. There are a spread of Tl–O bond distances ranging from 2.09–2.71 Å. In the second Tl3+ site, Tl3+ is bonded to six O2- atoms to form a mixture of distorted edge and corner-sharing TlO6 octahedra. The corner-sharing octahedra tilt angles range from 0–8°. There are a spread of Tl–O bond distances ranging from 2.10–2.79 Å. In the third Tl3+ site, Tl3+ is bonded to six O2- atoms to form a mixture of distorted edge and corner-sharing TlO6 octahedra. The corner-sharing octahedra tilt angles range from 1–8°. There are a spread of Tl–O bond distances ranging from 2.06–2.83 Å. There are twenty-one inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to four Ba2+ and one Tl3+ atom. In the second O2- site, O2- is bonded to four Ba2+ and one Tl3+ atom to form distorted OBa4Tl trigonal bipyramids that share a cornercorner with one OBa4Tl trigonal bipyramid, edges with four OBa2Tl4 octahedra, and edges with two equivalent OBa4Tl trigonal bipyramids. In the third O2- site, O2- is bonded in a 5-coordinate geometry to four Ba2+ and one Tl3+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to two Ba2+, one Y3+, and two equivalent Cu3+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to two Ba2+, one Y3+, and two equivalent Cu3+ atoms. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Ba2+ and two equivalent Cu3+ atoms. In the seventh O2- site, O2- is bonded in a distorted see-saw-like geometry to two equivalent Ba2+, two equivalent Y3+, and two Cu3+ atoms. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent Ba2+ and two Cu3+ atoms. In the ninth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent Ba2+ and two Cu3+ atoms. In the tenth O2- site, O2- is bonded in a distorted see-saw-like geometry to two equivalent Ba2+, two equivalent Y3+, and two Cu3+ atoms. In the eleventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent Ba2+ and two Cu3+ atoms. In the twelfth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent Ba2+ and two Cu3+ atoms. In the thirteenth O2- site, O2- is bonded to two Ba2+ and four Tl3+ atoms to form OBa2Tl4 octahedra that share corners with four OBa2Tl4 octahedra, edges with four OBa2Tl4 octahedra, and edges with four OBa4Tl trigonal bipyramids. The corner-sharing octahedra tilt angles range from 1–7°. In the fourteenth O2- site, O2- is bonded to two Ba2+ and four Tl3+ atoms to form OBa2Tl4 octahedra that share corners with four OBa2Tl4 octahedra, edges with four OBa2Tl4 octahedra, and edges with four OBa4Tl trigonal bipyramids. The corner-sharing octahedra tilt angles range from 1–7°. In the fifteenth O2- site, O2- is bonded to two Ba2+ and four Tl3+ atoms to form a mixture of edge and corner-sharing OBa2Tl4 octahedra. The corner-sharing octahedra tilt angles range from 2–5°. In the sixteenth O2- site, O2- is bonded in a 3-coordinate geometry to two Ba2+, one Y3+, and two equivalent Cu3+ atoms. In the seventeenth O2- site, O2- is bonded in a 3-coordinate geometry to two Ba2+, one Y3+, and two equivalent Cu3+ atoms. In the eighteenth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Ba2+ and two equivalent Cu3+ atoms. In the nineteenth O2- site, O2- is bonded in a 5-coordinate geometry to four Ba2+ and one Tl3+ atom. In the twentieth O2- site, O2- is bonded to four Ba2+ and one Tl3+ atom to form distorted OBa4Tl trigonal bipyramids that share a cornercorner with one OBa4Tl trigonal bipyramid, edges with four OBa2Tl4 octahedra, and edges with two equivalent OBa4Tl trigonal bipyramids. In the twenty-first O2- site, O2- is bonded in a 5-coordinate geometry to four Ba2+ and one Tl3+ atom.

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Materials Data on Hf2Tl by Materials Project

Hf2Tl crystallizes in the tetragonal I4/mmm space group. The structure is two-dimensional and consists of two Hf2Tl sheets oriented in the (0, 0, 1) direction. Hf is bonded in a 8-coordinate geometry to four equivalent Tl atoms. All Hf–Tl bond lengths are 3.09 Å. Tl is bonded in a body-centered cubic geometry to eight equivalent Hf atoms.

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Materials Data on Pm2TlSn by Materials Project

Pm2TlSn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pm is bonded in a body-centered cubic geometry to four equivalent Tl and four equivalent Sn atoms. All Pm–Tl bond lengths are 3.36 Å. All Pm–Sn bond lengths are 3.36 Å. Tl is bonded in a body-centered cubic geometry to eight equivalent Pm atoms. Sn is bonded in a body-centered cubic geometry to eight equivalent Pm atoms.

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Materials Data on Sc2TlCo by Materials Project

Sc2CoTl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Sc2CoTl ribbons oriented in the (1, 0, 0) direction. Sc is bonded in a linear geometry to one Co and one Tl atom. The Sc–Co bond length is 2.11 Å. The Sc–Tl bond length is 3.01 Å. Co is bonded in a linear geometry to two equivalent Sc atoms. Tl is bonded in a linear geometry to two equivalent Sc atoms.

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Materials Data on LiY2Tl by Materials Project

LiY2Tl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two LiY2Tl ribbons oriented in the (1, 0, 0) direction. Li is bonded in a linear geometry to two equivalent Y atoms. Both Li–Y bond lengths are 3.40 Å. Y is bonded in a linear geometry to one Li and one Tl atom. The Y–Tl bond length is 3.02 Å. Tl is bonded in a linear geometry to two equivalent Y atoms.

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Materials Data on TlAgPSe3 by Materials Project

AgTlPSe3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Ag1+ sites. In the first Ag1+ site, Ag1+ is bonded in a 4-coordinate geometry to one Tl1+ and four Se2- atoms. The Ag–Tl bond length is 3.43 Å. There are a spread of Ag–Se bond distances ranging from 2.64–2.78 Å. In the second Ag1+ site, Ag1+ is bonded in a 4-coordinate geometry to four Se2- atoms. There are a spread of Ag–Se bond distances ranging from 2.74–2.79 Å. There are two inequivalent Tl1+ sites. In the first Tl1+ site, Tl1+ is bonded in a 1-coordinate geometry to one Ag1+ and nine Se2- atoms. There are a spread of Tl–Se bond distances ranging from 3.15–3.87 Å. In the second Tl1+ site, Tl1+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Tl–Se bond distances ranging from 3.31–3.94 Å. There are two inequivalent P4+ sites. In the first P4+ site, P4+ is bonded in a trigonal non-coplanar geometry to three Se2- atoms. There are a spread of P–Se bond distances ranging from 2.22–2.27 Å. In the second P4+ site, P4+ is bonded in a trigonal non-coplanar geometry to three Se2- atoms. There are a spread of P–Se bond distances ranging from 2.21–2.23 Å. There are six inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 2-coordinate geometry to one Ag1+, four Tl1+, and one P4+ atom. In the second Se2- site, Se2- is bonded in a 5-coordinate geometry to two equivalent Ag1+, two Tl1+, and one P4+ atom. In the third Se2- site, Se2- is bonded in a 1-coordinate geometry to two Ag1+, two equivalent Tl1+, and one P4+ atom. In the fourth Se2- site, Se2- is bonded in a 3-coordinate geometry to two Ag1+, three equivalent Tl1+, and one P4+ atom. In the fifth Se2- site, Se2- is bonded in a 1-coordinate geometry to two Tl1+ and one P4+ atom. In the sixth Se2- site, Se2- is bonded in a 2-coordinate geometry to one Ag1+, four Tl1+, and one P4+ atom.

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Materials Data on Dy2TlIn by Materials Project

Dy2TlIn 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 Tl and four equivalent In atoms. All Dy–Tl bond lengths are 3.28 Å. All Dy–In bond lengths are 3.28 Å. Tl 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 Nb2TlO7 by Materials Project

(NbO3)2TlO crystallizes in the orthorhombic Imma space group. The structure is three-dimensional and consists of two TlO ribbons oriented in the (1, 0, 0) direction and one NbO3 framework. In each TlO ribbon, Tl is bonded in a distorted linear geometry to two equivalent O atoms. Both Tl–O bond lengths are 2.08 Å. O is bonded in a bent 120 degrees geometry to two equivalent Tl atoms. In the NbO3 framework, there are two inequivalent Nb sites. In the first Nb site, Nb is bonded to six O atoms to form corner-sharing NbO6 octahedra. The corner-sharing octahedra tilt angles range from 39–40°. There is two shorter (1.97 Å) and four longer (2.02 Å) Nb–O bond length. In the second Nb site, Nb is bonded to six O atoms to form corner-sharing NbO6 octahedra. The corner-sharing octahedra tilt angles range from 38–39°. There are four shorter (2.00 Å) and two longer (2.01 Å) Nb–O bond lengths. There are three inequivalent O sites. In the first O site, O is bonded in a distorted bent 150 degrees geometry to two equivalent Nb atoms. In the second O site, O is bonded in a bent 150 degrees geometry to two equivalent Nb atoms. In the third O site, O is bonded in a distorted bent 150 degrees geometry to two Nb atoms.

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Materials Data on LiSc2Tl by Materials Project

LiSc2Tl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two LiSc2Tl ribbons oriented in the (1, 0, 0) direction. Li is bonded in a linear geometry to two equivalent Sc atoms. Both Li–Sc bond lengths are 3.22 Å. Sc is bonded in a linear geometry to one Li and one Tl atom. The Sc–Tl bond length is 2.92 Å. Tl is bonded in a linear geometry to two equivalent Sc atoms.

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Materials Data on TlHgPb2 by Materials Project

HgTlPb2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two HgTlPb2 ribbons oriented in the (1, 0, 0) direction. Hg is bonded in a linear geometry to two equivalent Pb atoms. Both Hg–Pb bond lengths are 2.91 Å. Tl is bonded in a linear geometry to two equivalent Pb atoms. Both Tl–Pb bond lengths are 2.84 Å. Pb is bonded in a linear geometry to one Hg and one Tl atom.

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Materials Data on TlHg2Pb by Materials Project

Hg2TlPb crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Hg2TlPb ribbons oriented in the (1, 0, 0) direction. Hg is bonded in a linear geometry to one Tl and one Pb atom. The Hg–Tl bond length is 3.09 Å. The Hg–Pb bond length is 2.95 Å. Tl is bonded in a linear geometry to two equivalent Hg atoms. Pb is bonded in a linear geometry to two equivalent Hg atoms.

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Materials Data on Sr2MgTl by Materials Project

Sr2MgTl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Sr2MgTl ribbons oriented in the (1, 0, 0) direction. Sr is bonded in a linear geometry to one Mg and one Tl atom. The Sr–Mg bond length is 3.71 Å. The Sr–Tl bond length is 3.20 Å. Mg is bonded in a linear geometry to two equivalent Sr atoms. Tl is bonded in a linear geometry to two equivalent Sr atoms.

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