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Materials Data on InPt by Materials Project

PtIn crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Pt2- sites. In the first Pt2- site, Pt2- is bonded to six In2+ atoms to form distorted edge-sharing PtIn6 octahedra. There are four shorter (2.82 Å) and two longer (2.83 Å) Pt–In bond lengths. In the second Pt2- site, Pt2- is bonded in a 11-coordinate geometry to seven In2+ atoms. There are a spread of Pt–In bond distances ranging from 2.70–3.24 Å. In the third Pt2- site, Pt2- is bonded in a 7-coordinate geometry to seven In2+ atoms. There are a spread of Pt–In bond distances ranging from 2.81–2.99 Å. There are three inequivalent In2+ sites. In the first In2+ site, In2+ is bonded in a distorted hexagonal planar geometry to six Pt2- atoms. In the second In2+ site, In2+ is bonded in a distorted hexagonal planar geometry to six Pt2- atoms. In the third In2+ site, In2+ is bonded in a 8-coordinate geometry to eight Pt2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ce(InPt)2 by Materials Project

CePt2In2 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are two inequivalent Ce sites. In the first Ce site, Ce is bonded in a 1-coordinate geometry to five Pt and nine In atoms. There are a spread of Ce–Pt bond distances ranging from 2.92–3.23 Å. There are a spread of Ce–In bond distances ranging from 3.33–3.57 Å. In the second Ce site, Ce is bonded in a 7-coordinate geometry to seven Pt atoms. There are a spread of Ce–Pt bond distances ranging from 2.95–3.22 Å. There are four inequivalent Pt sites. In the first Pt site, Pt is bonded in a 10-coordinate geometry to two equivalent Ce and six In atoms. There are four shorter (2.82 Å) and two longer (2.95 Å) Pt–In bond lengths. In the second Pt site, Pt is bonded in a 10-coordinate geometry to three Ce and five In atoms. There are a spread of Pt–In bond distances ranging from 2.87–2.96 Å. In the third Pt site, Pt is bonded in a 9-coordinate geometry to four Ce and five In atoms. There are a spread of Pt–In bond distances ranging from 2.71–2.83 Å. In the fourth Pt site, Pt is bonded in a 10-coordinate geometry to three equivalent Ce and three equivalent In atoms. There are two shorter (2.81 Å) and one longer (2.84 Å) Pt–In bond lengths. There are four inequivalent In sites. In the first In site, In is bonded in a 4-coordinate geometry to two equivalent Ce and four Pt atoms. In the second In site, In is bonded in a 4-coordinate geometry to three equivalent Ce and four Pt atoms. In the third In site, In is bonded in a 5-coordinate geometry to three equivalent Ce and five Pt atoms. In the fourth In site, In is bonded in a 6-coordinate geometry to one Ce and six Pt atoms.

36 MATERIALS SCIENCE↗

Materials Data on InPt by Materials Project

PtIn is alpha-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Pt2- is bonded in a 12-coordinate geometry to six equivalent In2+ atoms. All Pt–In bond lengths are 2.83 Å. In2+ is bonded in a distorted hexagonal planar geometry to six equivalent Pt2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ba(InPt)2 by Materials Project

Ba(PtIn)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ba2+ is bonded in a distorted body-centered cubic geometry to eight equivalent Pt2- atoms. All Ba–Pt bond lengths are 3.55 Å. Pt2- is bonded in a 9-coordinate geometry to four equivalent Ba2+, one Pt2-, and four equivalent In1+ atoms. The Pt–Pt bond length is 2.74 Å. All Pt–In bond lengths are 2.80 Å. In1+ is bonded to four equivalent Pt2- atoms to form a mixture of corner and edge-sharing InPt4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Pr(InPt)2 by Materials Project

PrPt2In2 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 7-coordinate geometry to seven Pt atoms. There are a spread of Pr–Pt bond distances ranging from 3.04–3.24 Å. In the second Pr site, Pr is bonded in a 1-coordinate geometry to five Pt and nine In atoms. There are a spread of Pr–Pt bond distances ranging from 2.94–3.28 Å. There are a spread of Pr–In bond distances ranging from 3.34–3.58 Å. There are four inequivalent Pt sites. In the first Pt site, Pt is bonded in a 10-coordinate geometry to two equivalent Pr, two Pt, and six In atoms. There are one shorter (2.88 Å) and one longer (3.04 Å) Pt–Pt bond lengths. There are a spread of Pt–In bond distances ranging from 2.81–2.96 Å. In the second Pt site, Pt is bonded in a 10-coordinate geometry to three Pr, one Pt, and five In atoms. There are a spread of Pt–In bond distances ranging from 2.89–2.98 Å. In the third Pt site, Pt is bonded in a 9-coordinate geometry to four Pr and five In atoms. There are a spread of Pt–In bond distances ranging from 2.76–2.84 Å. In the fourth Pt site, Pt is bonded in a 10-coordinate geometry to three equivalent Pr, one Pt, and three equivalent In atoms. There are two shorter (2.78 Å) and one longer (2.84 Å) Pt–In bond lengths. There are four inequivalent In sites. In the first In site, In is bonded in a 3-coordinate geometry to three equivalent Pr and five Pt atoms. In the second In site, In is bonded in a 4-coordinate geometry to two equivalent Pr and four Pt atoms. In the third In site, In is bonded in a 6-coordinate geometry to one Pr and six Pt atoms. In the fourth In site, In is bonded in a 4-coordinate geometry to three equivalent Pr and four Pt atoms.

36 MATERIALS SCIENCE↗

Materials Data on Dy(InPt)4 by Materials Project

DyPt4In4 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Dy3+ is bonded in a 8-coordinate geometry to eight Pt2- atoms. There are six shorter (3.01 Å) and two longer (3.14 Å) Dy–Pt bond lengths. There are two inequivalent Pt2- sites. In the first Pt2- site, Pt2- is bonded in a distorted body-centered cubic geometry to one Dy3+ and seven In+1.25+ atoms. There are a spread of Pt–In bond distances ranging from 2.76–2.88 Å. In the second Pt2- site, Pt2- is bonded in a 8-coordinate geometry to three equivalent Dy3+ and four In+1.25+ atoms. There are three shorter (2.78 Å) and one longer (2.82 Å) Pt–In bond lengths. There are two inequivalent In+1.25+ sites. In the first In+1.25+ site, In+1.25+ is bonded in a distorted pentagonal planar geometry to five Pt2- atoms. In the second In+1.25+ site, In+1.25+ is bonded in a distorted hexagonal planar geometry to six Pt2- atoms.

36 MATERIALS SCIENCE↗

First-order structural phase transition at low temperature in GaPt 5 P and its rapid enhancement with pressure

Single crystals of X Pt 5 ⁢P (X = Al, Ga, and In), belonging to the 1-5-1 family of compounds, were grown from a Pt-P solution at high temperatures, and measurements of the ambient pressure, temperature-dependent magnetization, resistivity, and x-ray diffraction were made. Additionally, the ambient-pressure Hall resistivity and temperature-dependent resistance under pressure were measured on GaPt 5 ⁢P. All three compounds have a tetragonal P4/mmm crystal structure at room temperature with metallic transport and weak diamagnetism over the 2–300 K temperature range. Surprisingly, at ambient pressure, both the transport and magnetization measurements on GaPt 5 ⁢P show a steplike feature in the 70–90 K region, suggesting a possible structural phase transition. Neither AlPt 5 ⁢P nor InPt 5 ⁢P have any signatures of a phase transition in their temperature-dependent electrical resistance and magnetization data. Both the hysteretic nature and sharpness of the features in the GaPt 5 ⁢P data suggest that the transition is first-order. Further, single-crystal x-ray diffraction measurements provided further details of the structural transition with a possibility of a crystal symmetry different from P⁢4/mmm below the transition temperature. The transition is characterized by anisotropic changes in the lattice parameters and a volume collapse with respect to the high-temperature tetragonal crystal structure. Furthermore, satellite peaks are observed at two distinct and nonequivalent wave vectors (0, 0, 0.5) and (0.5, 0.5, 0.5), and density functional theory calculations present phonon softening, especially at (0.5, 0.5, 0.5), as a possible driving mechanism. Additionally, we find that the structural transition temperature increases rapidly with increasing pressure, reaching room temperature by ~2.2 GPa, highlighting the high degree of pressure sensitivity of GaPt 5 ⁢P and fragile nature of its room-temperature structure. Even though the volume collapse and extreme pressure sensitivity suggest chemical pressure should drive a similar structural change in AlPt 5⁢ P, where both unit-cell dimensions and volume are smaller, its structure is found to be the same as that of the room-temperature GaPt 5 ⁢P. Overall, GaPt 5 ⁢P stands out as a sole member of the 1-5-1 family of compounds for which a temperature-driven structural change has been observed.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗