Literature DB >> 21578032

Tripraseodymium penta-iron(III) dodeca-oxide, Pr(3)Fe(5)O(12): a synchrotron radiation study.

Takashi Komori, Terutoshi Sakakura, Yasuyuki Takenaka, Kiyoaki Tanaka, Takashi Okuda.   

Abstract

The title compound, penta-iron tripraseodymium dodeca-oxide (PrIG), has an iron garnet structure. There are two Fe site symmetries. One of the Fe atoms is coordinated by six O atoms, forming a slightly distorted octa-hedron, and has site symmetry. The other Fe atom is coordinated by four O atoms, forming a slightly distorted tetra-hedron, and has site symmetry. FeO(6) octa-hedra and FeO(4) tetra-hedra are linked together by corners. The Pr atom is coordinated by eight O atoms, forming a distorted dodeca-hedron, and has 222 site symmetry. The O atoms occupy the general positions.

Entities:  

Year:  2009        PMID: 21578032      PMCID: PMC2971448          DOI: 10.1107/S1600536809038100

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


Related literature

The title compound is isotypic with the Ia d form of Y3Fe5O12 (YIG). For related structures, see: Bonnet et al. (1975 ▶). For details of the crystal growth from low-temperature liquid-phase epitaxy, see: Fratello et al. (1986 ▶). For the extinction correction, see: Becker & Coppens (1975 ▶). X-ray intensities were measured avoiding multiple diffraction, see: Takenaka et al. (2008 ▶).

Experimental

Crystal data

Pr3Fe5O12 M = 893.98 Cubic, a = 12.6302 (3) Å V = 2014.79 (8) Å3 Z = 8 Synchrotron radiation λ = 0.67171 Å μ = 17.41 mm−1 T = 298 K 0.035 mm (radius)

Data collection

Rigaku AFC four-circle diffractometer Absorption correction: for a sphere [transmission coefficients for spheres tabulated in International Tables C (1992), Table 6.3.3.3, were interpolated with Lagrange’s method (four-point interpolation; Yamauchi et al., 1965 ▶)] T min = 0.413, T max = 0.441 9351 measured reflections 1728 independent reflections 1728 reflections with F > 3σ(F) R int = 0.016

Refinement

R[F 2 > 2σ(F 2)] = 0.019 wR(F 2) = 0.021 S = 1.06 9351 reflections 17 parameters Δρmax = 2.52 e Å−3 Δρmin = −3.16 e Å−3 Data collection: AFC-5, specially designed for PF-BL14A (Rigaku, 1984 ▶) 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/S1600536809038100/br2121sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809038100/br2121Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Pr3Fe5O12Dx = 5.894 Mg m3
Mr = 893.98Synchrotron radiation, λ = 0.67171 Å
Cubic, Ia3dCell parameters from 9 reflections
Hall symbol: -I 4bd 2c 3θ = 17.5–52.3°
a = 12.6302 (3) ŵ = 17.41 mm1
V = 2014.79 (8) Å3T = 298 K
Z = 8Sphere, black
F(000) = 32240.04 mm (radius)
Rigaku AFC four-circle diffractometer1728 independent reflections
Si 1111728 reflections with F > 3σ(F)
Detector resolution: 1.25 × 1.25° pixels mm-1Rint = 0.016
ω/2θ scansθmax = 68.3°, θmin = 3.7°
Absorption correction: for a sphere [Transmission coefficients for spheres tabulated in International Tables C (1992), Table 6.3.3.3, were interpolated with Lagrange's method (four-point interpolation (Yamauchi et al., 1965)]h = −9→34
Tmin = 0.413, Tmax = 0.441k = −9→32
9351 measured reflectionsl = −9→34
Refinement on FPrimary atom site location: isomorphous structure methods
Least-squares matrix: fullWeighting scheme based on measured s.u.'s
R[F2 > 2σ(F2)] = 0.019(Δ/σ)max = 0.003
wR(F2) = 0.021Δρmax = 2.52 e Å3
S = 1.06Δρmin = −3.16 e Å3
9351 reflectionsExtinction correction: B–C type 1 Gaussian isotropic (Becker & Coppens, 1975)
17 parametersExtinction coefficient: 0.255 (5)
xyzUiso*/Ueq
Pr10.1250000.0000000.2500000.00531 (1)
Fe10.0000000.0000000.0000000.00512 (1)
Fe20.3750000.0000000.2500000.00533 (1)
O1−0.029622 (2)0.052553 (2)0.149166 (2)0.00711 (5)
U11U22U33U12U13U23
Pr10.00406 (2)0.00594 (2)0.00594 (2)000.00111 (1)
Fe10.00512 (2)0.00512 (2)0.00512 (2)−0.00023 (1)−0.00023 (1)−0.00023 (1)
Fe20.00411 (3)0.00594 (2)0.00594 (2)000
O10.00718 (8)0.00829 (8)0.00587 (7)−0.00004 (6)0.00080 (6)0.00038 (6)
Pr1—O12.42410 (10)Fe1—O1i2.03220 (10)
Pr1—O1i2.54010 (10)Fe1—O1viii2.03220 (10)
Pr1—O1ii2.42410 (10)Fe1—O1ix2.03220 (10)
Pr1—O1iii2.54010 (10)Fe1—O1x2.03220 (10)
Pr1—O1iv2.42410 (10)Fe1—O1xi2.03220 (10)
Pr1—O1v2.54010 (10)Fe2—O1xii1.87450 (10)
Pr1—O1vi2.42410 (10)Fe2—O1iv1.87450 (10)
Pr1—O1vii2.54010 (10)Fe2—O1xiii1.87450 (10)
Fe1—O12.03220 (10)Fe2—O1vi1.87450 (10)
O1—Pr1—O1i67.75 (1)O1—Fe1—O1viii85.87 (1)
O1—Pr1—O1ii72.66 (1)O1—Fe1—O1ix180.00
O1—Pr1—O1iii124.91 (1)O1—Fe1—O1x94.13 (1)
O1—Pr1—O1iv111.18 (1)O1—Fe1—O1xi94.13 (1)
O1—Pr1—O1v73.25 (1)O1xii—Fe2—O1vi114.39 (1)
O1—Pr1—O1vi159.51 (1)O1xii—Fe2—O1iv114.39 (1)
O1—Pr1—O1vii95.43 (1)O1xii—Fe2—O1xiii100.02 (1)
O1—Fe1—O1i85.87 (1)
Pr1—O12.42410 (10)
Pr1—O1i2.54010 (10)
Fe1—O12.03220 (10)
Fe2—O1ii1.87450 (10)
O1—Fe1—O1i85.87 (1)
O1ii—Fe2—O1iii114.39 (1)
O1ii—Fe2—O1iv100.02 (1)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) .

  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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