Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “Pr”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

At least 145 records · Page 8

Structural changes induced by electric currents in a single crystal of Pr 2 CuO 4

We demonstrate an approach to the structural and electronic property modification of perovskites, focusing on Pr 2 CuO 4 , an undoped parent compound of a class of electron-doped copper-oxide superconductors. Currents were passed parallel or perpendicular to the copper oxygen layers with the voltage ramped up until a rapid drop in the resistivity was achieved, a process referred to as “flash.” The current was then further increased tenfold in current-control mode. This state was quenched by immersion into liquid nitrogen. Flash can drive many compounds into different atomic structures with new properties, whereas the quench freezes them into a long-lived state. Single-crystal neutron diffraction of as-grown and modified Pr 2 CuO 4 revealed a √10 ×√10 superlattice due to oxygen-vacancy order. The diffraction peak intensities of the superlattice of the modified sample were significantly enhanced relative to the pristine sample. Raman-active phonons in the modified sample were considerably sharper. Measurements of electrical resistivity, magnetization, and two-magnon Raman scattering indicate that the modification affected only the Pr-O layers, but not the Cu-O planes. These results point to enhanced oxygen-vacancy order in the modified samples well beyond what can be achieved without passing electrical current. Our work opens a new avenue toward electric field/quench control of structure and properties of layered perovskite oxides.

36 MATERIALS SCIENCE↗

Nanoscale Superconducting States in the Fe-Based Filamentary Superconductor of Pr-Doped CaFe 2 As 2

The low-temperature scanning tunneling microscope and spectroscopy (STM/STS) are used to visualize superconducting states in the cleaved single crystal of 9% praseodymium-doped CaFe 2 As 2 (Pr-Ca122) with Tc ≈ 30 K. The spectroscopy shows strong spatial variations in the density of states (DOS), and the superconducting map constructed from spectroscopy discloses a localized superconducting phase, as small as a single unit cell. The comparison of the spectra taken at 4.2 K and 22 K (below vs. close to the bulk superconducting transition temperature) from the exact same area confirms the superconducting behavior. Nanoscale superconducting states have been found near Pr dopants, which can be identified using dI/dV conductance maps at +300 mV. There is no correlation of the local superconductivity to the surface reconstruction domain and surface defects, which reflects its intrinsic bulk behavior. We, therefore, suggest that the local strain of Pr dopants is competing with defects induced local magnetic moments; this competition is responsible for the local superconducting states observed in this Fe-based filamentary superconductor.

77 NANOSCIENCE AND NANOTECHNOLOGY↗

Materials Data on Pr(PdO2)2 by Materials Project

Pr(PdO2)2 crystallizes in the tetragonal I4_1/a space group. The structure is three-dimensional. Pr4+ is bonded in a 8-coordinate geometry to eight equivalent O2- atoms. There are four shorter (2.46 Å) and four longer (2.55 Å) Pr–O bond lengths. Pd2+ is bonded in a square co-planar geometry to four equivalent O2- atoms. There are two shorter (2.03 Å) and two longer (2.04 Å) Pd–O bond lengths. O2- is bonded to two equivalent Pr4+ and two equivalent Pd2+ atoms to form a mixture of distorted edge and corner-sharing OPr2Pd2 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Pr(PO3)3 by Materials Project

Pr(PO3)3 crystallizes in the orthorhombic C222_1 space group. The structure is three-dimensional. Pr3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Pr–O bond distances ranging from 2.42–2.74 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form corner-sharing PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.49–1.62 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form corner-sharing PO4 tetrahedra. There is two shorter (1.52 Å) and two longer (1.59 Å) P–O bond length. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent P5+ atoms. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Pr3+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted linear geometry to one Pr3+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Pr3+ and one P5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Pr(IO3)3 by Materials Project

Pr(O3I)3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Pr3+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Pr–O bond distances ranging from 2.44–2.87 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Pr3+ and one I5+ atom. The O–I bond length is 1.87 Å. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Pr3+ and two I5+ atoms. There are one shorter (1.85 Å) and one longer (2.85 Å) O–I bond lengths. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two I5+ atoms. There are one shorter (1.83 Å) and one longer (2.84 Å) O–I bond lengths. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to one Pr3+ and one I5+ atom. The O–I bond length is 1.85 Å. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Pr3+ and one I5+ atom. The O–I bond length is 1.84 Å. In the sixth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Pr3+ and one I5+ atom. The O–I bond length is 1.83 Å. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to three I5+ atoms. There are a spread of O–I bond distances ranging from 1.87–2.78 Å. In the eighth O2- site, O2- is bonded in a distorted water-like geometry to one Pr3+ and one I5+ atom. The O–I bond length is 1.84 Å. In the ninth O2- site, O2- is bonded in a 2-coordinate geometry to one Pr3+ and one I5+ atom. The O–I bond length is 1.84 Å. There are three inequivalent I5+ sites. In the first I5+ site, I5+ is bonded in a 6-coordinate geometry to six O2- atoms. In the second I5+ site, I5+ is bonded in a 3-coordinate geometry to four O2- atoms. In the third I5+ site, I5+ is bonded in a 3-coordinate geometry to three O2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr(MoO2)6 by Materials Project

Pr(MoO2)6 crystallizes in the tetragonal I4/m space group. The structure is three-dimensional. Pr3+ is bonded in a distorted square co-planar geometry to four equivalent O2- atoms. All Pr–O bond lengths are 2.45 Å. There are two inequivalent Mo+3.50+ sites. In the first Mo+3.50+ site, Mo+3.50+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing MoO6 octahedra. The corner-sharing octahedra tilt angles range from 49–57°. There are a spread of Mo–O bond distances ranging from 2.06–2.23 Å. In the second Mo+3.50+ site, Mo+3.50+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing MoO6 octahedra. The corner-sharing octahedra tilt angles range from 49–52°. There are a spread of Mo–O bond distances ranging from 1.95–2.23 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Pr3+ and three Mo+3.50+ atoms. In the second O2- site, O2- is bonded in a trigonal planar geometry to three Mo+3.50+ atoms. In the third O2- site, O2- is bonded in a distorted T-shaped geometry to three Mo+3.50+ atoms. In the fourth O2- site, O2- is bonded in a trigonal planar geometry to three Mo+3.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr(SiPt)2 by Materials Project

Pr(PtSi)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Pr4+ is bonded in a 8-coordinate geometry to eight equivalent Pt2- atoms. All Pr–Pt bond lengths are 3.28 Å. Pt2- is bonded in a 4-coordinate geometry to four equivalent Pr4+ and four equivalent Si atoms. All Pt–Si bond lengths are 2.49 Å. Si is bonded in a 5-coordinate geometry to four equivalent Pt2- and one Si atom. The Si–Si bond length is 2.41 Å.

36 MATERIALS SCIENCE↗

Materials Data on Pr(C2N3)3 by Materials Project

Pr(C2N3)3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Pr3+ is bonded in a 9-coordinate geometry to nine N3- atoms. There are a spread of Pr–N bond distances ranging from 2.54–2.98 Å. There are two inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.18 Å) and one longer (1.30 Å) C–N bond length. In the second C4+ site, C4+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.18 Å) and one longer (1.30 Å) C–N bond length. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded in a bent 120 degrees geometry to one Pr3+ and two equivalent C4+ atoms. In the second N3- site, N3- is bonded in a bent 120 degrees geometry to one Pr3+ and two equivalent C4+ atoms. In the third N3- site, N3- is bonded in a distorted bent 150 degrees geometry to one Pr3+ and one C4+ atom. In the fourth N3- site, N3- is bonded in a distorted bent 150 degrees geometry to one Pr3+ and one C4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Pr(HO)3 by Materials Project

Pr(OH)3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. Pr3+ is bonded in a 9-coordinate geometry to nine equivalent O2- atoms. There are three shorter (2.55 Å) and six longer (2.57 Å) Pr–O bond lengths. H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.97 Å. O2- is bonded in a single-bond geometry to three equivalent Pr3+ and one H1+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Pr(HO)3 by Materials Project

Pr(OH)3 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. Pr3+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Pr–O bond distances ranging from 2.54–2.59 Å. There are three inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.97 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.97 Å. In the third H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.97 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to three equivalent Pr3+ and one H1+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to three equivalent Pr3+ and one H1+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to three equivalent Pr3+ and one H1+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Pr(WO3)5 by Materials Project

Pr(WO3)5 crystallizes in the orthorhombic Pmmm space group. The structure is three-dimensional. Pr3+ is bonded in a distorted square co-planar geometry to four equivalent O2- atoms. All Pr–O bond lengths are 3.06 Å. There are two inequivalent W+5.40+ sites. In the first W+5.40+ site, W+5.40+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedra tilt angles range from 4–50°. There are a spread of W–O bond distances ranging from 1.92–2.03 Å. In the second W+5.40+ site, W+5.40+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedra tilt angles range from 0–37°. There is two shorter (1.92 Å) and four longer (1.94 Å) W–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent W+5.40+ atoms. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Pr3+ and two equivalent W+5.40+ atoms. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent W+5.40+ atoms. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to two W+5.40+ atoms. In the fifth O2- site, O2- is bonded in a linear geometry to two equivalent W+5.40+ atoms. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent W+5.40+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr(BOs)2 by Materials Project

Pr(OsB)2 crystallizes in the orthorhombic Fddd space group. The structure is three-dimensional. Pr3+ is bonded in a 4-coordinate geometry to four equivalent Os+1.50- atoms. All Pr–Os bond lengths are 3.06 Å. Os+1.50- is bonded in a 4-coordinate geometry to two equivalent Pr3+ and four equivalent B atoms. There are two shorter (2.10 Å) and two longer (2.18 Å) Os–B bond lengths. B is bonded to four equivalent Os+1.50- atoms to form a mixture of distorted corner and edge-sharing BOs4 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Pr(CoO3)2 by Materials Project

Pr(CoO3)2 crystallizes in the monoclinic Pc space group. The structure is three-dimensional. Pr4+ is bonded in a 10-coordinate geometry to eight O2- atoms. There are a spread of Pr–O bond distances ranging from 2.44–2.68 Å. There are two inequivalent Co4+ sites. In the first Co4+ site, Co4+ is bonded to six O2- atoms to form corner-sharing CoO6 octahedra. The corner-sharing octahedra tilt angles range from 14–23°. There are a spread of Co–O bond distances ranging from 1.78–2.09 Å. In the second Co4+ site, Co4+ is bonded to six O2- atoms to form corner-sharing CoO6 octahedra. The corner-sharing octahedra tilt angles range from 14–23°. There are a spread of Co–O bond distances ranging from 1.78–2.09 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted T-shaped geometry to one Pr4+ and two Co4+ atoms. In the second O2- site, O2- is bonded in a distorted T-shaped geometry to one Pr4+ and two Co4+ atoms. In the third O2- site, O2- is bonded in a distorted T-shaped geometry to one Pr4+ and two Co4+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Pr4+ and two Co4+ atoms. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Pr4+ and two Co4+ atoms. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Pr4+ and two Co4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr(LuS2)3 by Materials Project

Pr(LuS2)3 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are three inequivalent Lu3+ sites. In the first Lu3+ site, Lu3+ is bonded to seven S2- atoms to form distorted LuS7 pentagonal bipyramids that share corners with three LuS6 octahedra, edges with two equivalent LuS6 octahedra, and edges with four equivalent LuS7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 39–51°. There are a spread of Lu–S bond distances ranging from 2.65–2.88 Å. In the second Lu3+ site, Lu3+ is bonded to six S2- atoms to form LuS6 octahedra that share corners with three equivalent LuS6 octahedra, a cornercorner with one LuS7 pentagonal bipyramid, edges with four equivalent LuS6 octahedra, and edges with two equivalent LuS7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 53–62°. There are a spread of Lu–S bond distances ranging from 2.64–2.74 Å. In the third Lu3+ site, Lu3+ is bonded to six S2- atoms to form LuS6 octahedra that share corners with three equivalent LuS6 octahedra, corners with two equivalent LuS7 pentagonal bipyramids, and edges with four equivalent LuS6 octahedra. The corner-sharing octahedra tilt angles range from 53–62°. There are a spread of Lu–S bond distances ranging from 2.62–2.75 Å. Pr3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Pr–S bond distances ranging from 2.91–3.04 Å. There are six inequivalent S2- sites. In the first S2- site, S2- is bonded in a 4-coordinate geometry to four Lu3+ atoms. In the second S2- site, S2- is bonded to three Lu3+ and one Pr3+ atom to form distorted SPrLu3 trigonal pyramids that share corners with two equivalent SPr2Lu3 square pyramids, corners with four SPr2Lu3 trigonal bipyramids, corners with two equivalent SPrLu3 trigonal pyramids, edges with three equivalent SPr2Lu3 square pyramids, and edges with two equivalent SPr3Lu2 trigonal bipyramids. In the third S2- site, S2- is bonded in a rectangular see-saw-like geometry to four Lu3+ atoms. In the fourth S2- site, S2- is bonded to three equivalent Lu3+ and two equivalent Pr3+ atoms to form distorted SPr2Lu3 square pyramids that share corners with six SPr2Lu3 trigonal bipyramids, corners with two equivalent SPrLu3 trigonal pyramids, edges with four equivalent SPr2Lu3 square pyramids, edges with two SPr2Lu3 trigonal bipyramids, and edges with three equivalent SPrLu3 trigonal pyramids. In the fifth S2- site, S2- is bonded to three Lu3+ and two equivalent Pr3+ atoms to form distorted SPr2Lu3 trigonal bipyramids that share corners with two equivalent SPr2Lu3 square pyramids, corners with two equivalent SPr3Lu2 trigonal bipyramids, corners with three equivalent SPrLu3 trigonal pyramids, an edgeedge with one SPr2Lu3 square pyramid, and edges with five SPr2Lu3 trigonal bipyramids. In the sixth S2- site, S2- is bonded to two equivalent Lu3+ and three equivalent Pr3+ atoms to form distorted SPr3Lu2 trigonal bipyramids that share corners with four equivalent SPr2Lu3 square pyramids, corners with two equivalent SPr2Lu3 trigonal bipyramids, a cornercorner with one SPrLu3 trigonal pyramid, an edgeedge with one SPr2Lu3 square pyramid, edges with seven SPr2Lu3 trigonal bipyramids, and edges with two equivalent SPrLu3 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Pr(TmS2)3 by Materials Project

Pr(TmS2)3 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are three inequivalent Tm3+ sites. In the first Tm3+ site, Tm3+ is bonded to seven S2- atoms to form distorted TmS7 pentagonal bipyramids that share corners with three TmS6 octahedra, edges with two equivalent TmS6 octahedra, and edges with four equivalent TmS7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 39–51°. There are a spread of Tm–S bond distances ranging from 2.67–2.90 Å. In the second Tm3+ site, Tm3+ is bonded to six S2- atoms to form TmS6 octahedra that share corners with three equivalent TmS6 octahedra, a cornercorner with one TmS7 pentagonal bipyramid, edges with four equivalent TmS6 octahedra, and edges with two equivalent TmS7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 55–61°. There are a spread of Tm–S bond distances ranging from 2.65–2.76 Å. In the third Tm3+ site, Tm3+ is bonded to six S2- atoms to form TmS6 octahedra that share corners with three equivalent TmS6 octahedra, corners with two equivalent TmS7 pentagonal bipyramids, and edges with four equivalent TmS6 octahedra. The corner-sharing octahedra tilt angles range from 55–61°. There are a spread of Tm–S bond distances ranging from 2.64–2.77 Å. Pr3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Pr–S bond distances ranging from 2.91–3.04 Å. There are six inequivalent S2- sites. In the first S2- site, S2- is bonded in a 4-coordinate geometry to four Tm3+ atoms. In the second S2- site, S2- is bonded to three Tm3+ and one Pr3+ atom to form distorted SPrTm3 trigonal pyramids that share corners with two equivalent SPr2Tm3 square pyramids, corners with four SPr2Tm3 trigonal bipyramids, corners with two equivalent SPrTm3 trigonal pyramids, edges with three equivalent SPr2Tm3 square pyramids, and edges with two equivalent SPr3Tm2 trigonal bipyramids. In the third S2- site, S2- is bonded in a rectangular see-saw-like geometry to four Tm3+ atoms. In the fourth S2- site, S2- is bonded to three equivalent Tm3+ and two equivalent Pr3+ atoms to form distorted SPr2Tm3 square pyramids that share corners with six SPr2Tm3 trigonal bipyramids, corners with two equivalent SPrTm3 trigonal pyramids, edges with four equivalent SPr2Tm3 square pyramids, edges with two SPr2Tm3 trigonal bipyramids, and edges with three equivalent SPrTm3 trigonal pyramids. In the fifth S2- site, S2- is bonded to three Tm3+ and two equivalent Pr3+ atoms to form distorted SPr2Tm3 trigonal bipyramids that share corners with two equivalent SPr2Tm3 square pyramids, corners with two equivalent SPr3Tm2 trigonal bipyramids, corners with three equivalent SPrTm3 trigonal pyramids, an edgeedge with one SPr2Tm3 square pyramid, and edges with five SPr2Tm3 trigonal bipyramids. In the sixth S2- site, S2- is bonded to two equivalent Tm3+ and three equivalent Pr3+ atoms to form distorted SPr3Tm2 trigonal bipyramids that share corners with four equivalent SPr2Tm3 square pyramids, corners with two equivalent SPr2Tm3 trigonal bipyramids, a cornercorner with one SPrTm3 trigonal pyramid, an edgeedge with one SPr2Tm3 square pyramid, edges with seven SPr2Tm3 trigonal bipyramids, and edges with two equivalent SPrTm3 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Pr(PPt)2 by Materials Project

Pr(PtP)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Pr3+ is bonded in a 8-coordinate geometry to eight P3- atoms. There are four shorter (3.23 Å) and four longer (3.24 Å) Pr–P bond lengths. There are two inequivalent Pt+1.50+ sites. In the first Pt+1.50+ site, Pt+1.50+ is bonded in a 5-coordinate geometry to five P3- atoms. There are one shorter (2.40 Å) and four longer (2.42 Å) Pt–P bond lengths. In the second Pt+1.50+ site, Pt+1.50+ is bonded in a distorted rectangular see-saw-like geometry to four equivalent P3- atoms. All Pt–P bond lengths are 2.54 Å. There are two inequivalent P3- sites. In the first P3- site, P3- is bonded in a 10-coordinate geometry to four equivalent Pr3+, five Pt+1.50+, and one P3- atom. The P–P bond length is 2.69 Å. In the second P3- site, P3- is bonded in a 8-coordinate geometry to four equivalent Pr3+ and four equivalent Pt+1.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr(CrB3)2 by Materials Project

Pr(CrB3)2 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Pr3+ is bonded in a 12-coordinate geometry to sixteen B2- atoms. There are a spread of Pr–B bond distances ranging from 2.85–2.96 Å. Cr+4.50+ is bonded in a 10-coordinate geometry to ten B2- atoms. There are a spread of Cr–B bond distances ranging from 2.14–2.23 Å. There are two inequivalent B2- sites. In the first B2- site, B2- is bonded in a 6-coordinate geometry to three equivalent Pr3+, three equivalent Cr+4.50+, and three B2- atoms. There is one shorter (1.77 Å) and two longer (1.80 Å) B–B bond length. In the second B2- site, B2- is bonded in a 9-coordinate geometry to two equivalent Pr3+, four equivalent Cr+4.50+, and three B2- atoms. The B–B bond length is 1.82 Å.

36 MATERIALS SCIENCE↗

Materials Data on Pr(CoP3)4 by Materials Project

Pr(CoP3)4 crystallizes in the cubic Im-3 space group. The structure is three-dimensional. Pr3+ is bonded to twelve equivalent P1- atoms to form PrP12 cuboctahedra that share faces with eight equivalent CoP6 octahedra. All Pr–P bond lengths are 3.00 Å. Co+2.25+ is bonded to six equivalent P1- atoms to form CoP6 octahedra that share corners with six equivalent CoP6 octahedra and faces with two equivalent PrP12 cuboctahedra. The corner-sharing octahedral tilt angles are 60°. All Co–P bond lengths are 2.26 Å. P1- is bonded in a 2-coordinate geometry to one Pr3+, two equivalent Co+2.25+, and two equivalent P1- atoms. There are one shorter (2.29 Å) and one longer (2.31 Å) P–P bond lengths.

36 MATERIALS SCIENCE↗