Literature DB >> 21200981

Redetermination of the perovskite-type compound YRh(3)B revealing a Rh deficiency.

Ryoko Makita, Koutarou Tanizawa, Kiyoaki Tanaka, Humihiko Takei.   

Abstract

In contrast with previous structural studies of ytterbium trirhodium boride, YbRh(3)B, that suggest a boron deficiency, the current redetermination of the crystal structure of YbRh(3)B revealed instead a rhodium deficiency with a refined composition of YbRh(2.67 (2))B. In the ABX(3) perovskite-type structure, Yb, B and Rh are located on the A, B and X positions, respectively, with site symmetries of mm for the A and B sites, and 4/mm.m for the X site.

Entities:  

Year:  2008        PMID: 21200981      PMCID: PMC2959336          DOI: 10.1107/S1600536808030754

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


Related literature

For a previous powder diffraction study of YbRh3B, see: Takei & Shishido (1984 ▶). For general background, see: Becker & Coppens (1975 ▶); Libermann et al. (1971 ▶); Mann (1968 ▶).

Experimental

Crystal data

YbRh2.67B M = 458.61 Cubic, a = 4.12992 (7) Å V = 70.44 (1) Å3 Z = 1 Mo Kα radiation μ = 47.90 mm−1 T = 109 (1) K Radius: 0.041 mm

Data collection

MacScience M06XHF22 four-circle diffractometer Absorption correction: for a sphere [transmission coefficients for spheres tabulated in International Tables for X-ray Crystallography (Vol. II, 1972, Table 5.3.6B) were interpolated with Lagrange’s method (four point interpolation; Yamauchi et al., 1965 ▶)] T min = 0.069, T max = 0.169 953 measured reflections 193 independent reflections 193 reflections with F > 3σ(F) R int = 0.018

Refinement

R[F 2 > 2σ(F 2)] = 0.014 wR(F 2) = 0.029 S = 1.15 193 reflections 11 parameters 3 restraints Δρmax = 1.86 e Å−3 Δρmin = −1.98 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 & Ōnuki, 2002 ▶; 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/S1600536808030754/wm2195sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808030754/wm2195Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
YbRh2.67BDx = 10.81 Mg m3
Mr = 458.61Mo Kα radiation, λ = 0.71073 Å
Cubic, Pm3mCell parameters from 30 reflections
Hall symbol: -P 4 2 3θ = 36.5–38.3°
a = 4.12992 (7) ŵ = 47.90 mm1
V = 70.44 (1) Å3T = 109 K
Z = 1Sphere, black
F(000) = 195.140.08 × 0.08 × 0.08 × 0.04 (radius) mm
MacScience M06XHF22 four-circle diffractometer193 independent reflections
Radiation source: fine-focus rotating anode193 reflections with F > 3σ(F)
graphiteRint = 0.019
Detector resolution: 1.25 x 1.25° pixels mm-1θmax = 74.9°, θmin = 4.9°
ω/2θ scansh = −7→9
Absorption correction: for a sphere [transmission coefficients for spheres tabulated in International Tables for X-ray Crystallography (Vol. II, 1972, Table 5.3.6B) were interpolated with Lagrange's method (four point interpolation; Yamauchi et al., 1965)]k = −11→11
Tmin = 0.069, Tmax = 0.169l = −11→11
953 measured reflections
Refinement on F3 restraints
Least-squares matrix: fullWeighting scheme based on measured s.u.'s
R[F2 > 2σ(F2)] = 0.014(Δ/σ)max = 0.0001
wR(F2) = 0.029Δρmax = 1.86 e Å3
S = 1.15Δρmin = −1.98 e Å3
193 reflectionsExtinction correction: B-C type 1 Gaussian anisotropic (Becker & Coppens, 1975)
11 parametersExtinction coefficient: 0.052 (2) times 104
Experimental. Multiple diffraction was avoided by using ψ-scans. Intensities was measured at the equi-temperature region of combinaion of angles ω and χ of a four-circle diffractometer.
xyzUiso*/UeqOcc. (<1)
Yb0.50000.50000.50000.212 (1)
Rh0.00000.00000.50000.143 (2)0.891 (6)
B0.00000.00000.00000.291 (6)
U11U22U33U12U13U23
Yb0.00269 (4)0.00269 (4)0.00269 (4)000
Rh0.00202 (6)0.00202 (6)0.00139 (6)000
B0.0037 (2)0.0037 (2)0.0037 (2)000
Rhi—Rhii2.92029 (7)Bi—Yb3.57662 (7)
Bi—Rhi2.06496 (7)Rhi—Yb2.92029 (7)
?···??
Rhi—Bi—Rhii90.000Rhi—Yb—Bi35.264
Rhi—Yb—Rhii60.000Yb—Bi—Rhii54.736
Table 1

Selected bond lengths (Å)

Rhi—Rhii2.92029 (7)
Bi—Rhi2.06496 (7)
Bi—Yb3.57662 (7)
Rhi—Yb2.92029 (7)

Symmetry codes: (i) ; (ii) .

  2 in total

1.  Observation of 4f electron transfer from Ce to B6 in the Kondo crystal CeB6 and its mechanism by multi-temperature X-ray diffraction.

Authors:  Kiyoaki Tanaka; Yoshichika Onuki
Journal:  Acta Crystallogr B       Date:  2002-05-29

2.  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

  2 in total

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