Literature DB >> 21579592

Filled skutterudite structure of europium ruthenium polyphosphide, EuRu(4)P(12).

Isao Kagomiya1, Shiro Funahashi, Terutoshi Sakakura, Takashi Komori, Kiyoaki Tanaka.   

Abstract

The crystal structure of EuRu(4)P(12) is isotypic with filled skutterudite structures of rare earth transition metal poly-phosphides: RFe(4)P(12) (R = Ce, Pr, Nd, Sm and Eu), RRu(4)P(12) (R = La, Ce, Pr and Nd) and ROs(4)P(12) (R = La, Ce, Pr and Nd). The Ru cation is coordinated by six P anions in a distorted octa-hedral manner. The partially occupied Eu position (site occupancy 0.97) is enclosed by a cage formed by the corner-shared framework of the eight RuP(6) octa-hedra.

Entities:  

Year:  2010        PMID: 21579592      PMCID: PMC2979920          DOI: 10.1107/S1600536810000589

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

The title compound is isotypic with the Im form of LaFe4P12, see: Jeitschko & Braun (1977 ▶). For the single-crystal preparation and magnetic and electrical properties of EuRu4P12, see: Sekine et al. (2000 ▶). For hyperfine inter­action in EuRu4P12, see: Grandjean et al. (1983 ▶); Indoh et al. (2002 ▶). For the method used to avoid multiple diffraction, see: Takenaka et al. (2008 ▶).

Experimental

Crystal data

Eu0.97Ru4P12 M = 923.37 Cubic, a = 8.04163 (10) Å V = 520.04 (1) Å3 Z = 2 Mo Kα radiation μ = 13.37 mm−1 T = 100 K 0.04 mm (radius)

Data collection

MacScience M06XHF22 four-circle diffractometer Absorption correction: for a sphere [transmission coefficients for spheres tabulated in International Tables Vol. C (1992), Table 6.3.3.3, were interpolated with Lagrange’s method (four-point interpolation; Yamauchi et al., 1965 ▶)] T min = 0.486, T max = 0.526 1564 measured reflections 769 independent reflections 625 reflections with F > 3σ(F) R int = 0.016

Refinement

R[F 2 > 2σ(F 2)] = 0.020 wR(F 2) = 0.024 S = 1.54 1304 reflections 30 parameters Δρmax = 2.08 e Å−3 Δρmin = −1.14 e Å−3 Data collection: MXCSYS (MacScience, 1995 ▶) and IUANGLE (Tanaka et al., 1994 ▶); cell refinement: RSLC-3 UNICS system (Sakurai & Kobayashi, 1979 ▶); data reduction: RDEDIT (Tanaka, 2008 ▶); program(s) used to solve structure: QNTAO (Tanaka et al., 2008 ▶); program(s) used to refine structure: QNTAO; molecular graphics: ATOMS for Windows (Dowty, 2000 ▶); software used to prepare material for publication: RDEDIT. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810000589/br2130sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810000589/br2130Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Eu0.97Ru4P12Dx = 5.925 Mg m3
Mr = 923.37Mo Kα radiation, λ = 0.71073 Å
Cubic, Im3Cell parameters from 37 reflections
Hall symbol: -I 2 2 3θ = 36.0–37.7°
a = 8.04163 (10) ŵ = 13.37 mm1
V = 520.04 (1) Å3T = 100 K
Z = 2Sphere, black
F(000) = 828.40.04 mm (radius)
MacScience M06XHF22 four-circle diffractometer769 independent reflections
Radiation source: fine-focus rotating anode625 reflections with F > 3σ(F)
graphiteRint = 0.016
Detector resolution: 1.25 x 1.25° pixels mm-1θmax = 74.2°, θmin = 3.6°
ω/2θ scansh = −18→20
Absorption correction: for a sphere [transmission coefficients for spheres tabulated in International Tables Vol. C (1992), Table 6.3.3.3, were interpolated with Lagrange's method (four-point interpolation; Yamauchi et al., 1965)]k = −21→21
Tmin = 0.486, Tmax = 0.526l = −18→20
1564 measured reflections
Refinement on FWeighting scheme based on measured s.u.'s
Least-squares matrix: full(Δ/σ)max = 0.018
R[F2 > 2σ(F2)] = 0.020Δρmax = 2.08 e Å3
wR(F2) = 0.024Δρmin = −1.14 e Å3
S = 1.54Extinction correction: B–C type 1 Gaussian isotropic (Becker & Coppens, 1975)
1304 reflectionsExtinction coefficient: 0.068 (6)
30 parameters
xyzUiso*/UeqOcc. (<1)
Eu10.0000000.0000000.0000000.00270 (2)0.970 (4)
Ru10.2500000.2500000.2500000.001840 (15)
P10.0000000.3593290.1433860.00283 (4)
U11U22U33U12U13U23
Eu10.00271 (3)0.00271 (3)0.00271 (3)000
Ru10.00185 (3)0.00185 (3)0.00185 (3)0.000108 (17)0.000108 (17)0.000108 (17)
P10.00268 (10)0.00301 (10)0.00285 (10)00−0.00009 (7)
Eu1—P13.1112 (3)Ru1—P1i2.3558 (1)
Eu1—Ru13.4821 (1)P1—P1ii2.3061 (1)
Ru1—P12.3558 (1)P1—P1i3.0829 (1)
Eu1—P1—Ru177.78Ru1—P1—P1i49.13
Eu1—P1—P1ii68.25P1—Ru1—P1i81.74
Eu1—P1—P1i109.77P1ii—P1—P1i89.59
Ru1—P1—P1ii111.34
Table 1

Selected bond lengths (Å)

Eu1—P13.1112 (3)
Eu1—Ru13.4821 (1)
Ru1—P12.3558 (1)
P1—P1i2.3061 (1)
P1—P1ii3.0829 (1)

Symmetry codes: (i) ; (ii) .

  1 in total

1.  X-ray atomic orbital analysis. I. Quantum-mechanical and crystallographic framework of the method.

Authors:  Kiyoaki Tanaka; Ryoko Makita; Shiro Funahashi; Takashi Komori; Zaw Win
Journal:  Acta Crystallogr A       Date:  2008-06-17       Impact factor: 2.290

  1 in total

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