Literature DB >> 21201566

BaCo(2)(AsO(4))(2).

Tamara Dordević1.   

Abstract

Suitable single crystals of the title compound, barium dicobalt(II) bis-[orthoarsenate(V)], were prepared under hydro-thermal conditions. This phase belongs to a series of compounds with general formula AM(2)(XO(4))(2), where A = alkaline earth metal, M = Mg or a divalent first-row transition element, and X = P, As or V. BaCo(2)(AsO(4))(2) is isotypic with BaNi(2)(XO(4))(2) (X = P, V or As) and is characterized by brucite-like sheets of edge-sharing CoO(6) octa-hedra (3 symmetry) parallel to (001), with one-third of the octa-hedral positions being vacant. The sheets are capped above and below by AsO(4) tetra-hedra (3 symmetry) and are inter-connected by distorted BaO(12) cubocta-hedra ( symmetry).

Entities:  

Year:  2008        PMID: 21201566      PMCID: PMC2960660          DOI: 10.1107/S1600536808025865

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


Related literature

For isostructural compounds, see: Eymond et al. (1969a ▶,b ▶); Bircsak & Harrison (1998 ▶); El-Bali et al. (1999 ▶); Faza et al. (2001 ▶); Rogado et al. (2002 ▶); Wichmann, & Müller-Buschbaum (1984 ▶). For magnetic properties of BaCo2(AsO4)2, see: Dojčilović et al. (1994 ▶); Regnault et al. (2006 ▶). For related compounds, see: Effenberger & Pertlik (1993 ▶); El-Bali et al. (1993a ▶,b ▶); Hemon & Courbion (1990 ▶); Kreidler & Hummel (1961 ▶); Lucas et al. (1998 ▶); Mihajlović et al. (2004 ▶); Moquine et al. (1993 ▶); Osterloh & Müller-Buschbaum (1994 ▶). For general background, see: Brese & O’Keeffe (1991 ▶).

Experimental

Crystal data

BaCo2(AsO4)2 M = 533.04 Hexagonal, a = 5.007 (1) Å c = 23.491 (5) Å V = 510.02 (18) Å3 Z = 3 Mo Kα radiation μ = 20.22 mm−1 T = 293 (2) K 0.09 × 0.05 × 0.05 mm

Data collection

Nonius KappaCCD diffractometer Absorption correction: multi-scan (Otwinowski & Minor, 1997 ▶; Otwinowski et al., 2003 ▶) T min = 0.221, T max = 0.362 681 measured reflections 341 independent reflections 336 reflections with I > 2σ(I) R int = 0.009

Refinement

R[F 2 > 2σ(F 2)] = 0.014 wR(F 2) = 0.038 S = 1.30 341 reflections 22 parameters Δρmax = 0.96 e Å−3 Δρmin = −1.09 e Å−3 Data collection: COLLECT (Nonius, 2002 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO-SMN (Otwinowski et al., 2003 ▶); method used to solve structure: starting parameters from an isostructural compound (Eymond et al., 1969a ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶) and WinGX (Farrugia, 1999 ▶); molecular graphics: ATOMS (Dowty, 2000 ▶); software used to prepare material for publication: publCIF (Westrip, 2008 ▶). Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808025865/wm2189sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808025865/wm2189Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
BaCo2(AsO4)2Z = 3
Mr = 533.04F000 = 720
Hexagonal, R3Dx = 5.206 Mg m3
Hall symbol: -R 3Mo Kα radiation λ = 0.71073 Å
a = 5.007 (1) ÅCell parameters from 675 reflections
b = 5.007 (1) Åθ = 1.0–30.0º
c = 23.491 (5) ŵ = 20.22 mm1
α = 90ºT = 293 (2) K
β = 90ºPseudo-hexagonal plate, pink
γ = 120º0.09 × 0.05 × 0.05 mm
V = 510.02 (18) Å3
Nonius KappaCCD diffractometer341 independent reflections
Radiation source: fine-focus sealed tube336 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.009
T = 293(2) Kθmax = 30.0º
φ and ω scansθmin = 2.6º
Absorption correction: multi-scan(Otwinowski & Minor, 1997; Otwinowski et al., 2003)h = −7→7
Tmin = 0.221, Tmax = 0.362k = −5→5
681 measured reflectionsl = −33→33
Refinement on F2Primary atom site location: isomorphous structure methods
Least-squares matrix: full  w = 1/[σ2(Fo2) + (0.0133P)2 + 3.104P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.014(Δ/σ)max < 0.001
wR(F2) = 0.038Δρmax = 0.96 e Å3
S = 1.30Δρmin = −1.09 e Å3
341 reflectionsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
22 parametersExtinction coefficient: 0.0118 (5)
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
Ba10.00000.00000.00000.01170 (15)
Co10.00000.00000.17014 (2)0.00614 (16)
As10.33330.66670.091941 (18)0.00473 (15)
O10.33330.66670.02145 (13)0.0118 (6)
O20.0163 (4)0.3375 (4)0.11476 (7)0.0077 (3)
U11U22U33U12U13U23
Ba10.01138 (17)0.01138 (17)0.0124 (2)0.00569 (8)0.0000.000
Co10.00474 (19)0.00474 (19)0.0089 (3)0.00237 (9)0.0000.000
As10.00414 (16)0.00414 (16)0.0059 (2)0.00207 (8)0.0000.000
O10.0149 (9)0.0149 (9)0.0055 (13)0.0075 (5)0.0000.000
O20.0055 (7)0.0050 (7)0.0116 (8)0.0019 (6)0.0017 (6)0.0020 (6)
Ba1—O1i2.9344 (8)Ba1—O2ix3.1611 (17)
Ba1—O1ii2.9344 (8)Co1—O2x2.0791 (17)
Ba1—O1iii2.9344 (8)Co1—O2xi2.0791 (17)
Ba1—O12.9344 (8)Co1—O2xii2.0792 (17)
Ba1—O1iv2.9344 (8)Co1—O2vii2.1017 (17)
Ba1—O1v2.9344 (8)Co1—O22.1017 (17)
Ba1—O2vi3.1611 (17)Co1—O2vi2.1017 (17)
Ba1—O23.1611 (17)As1—O11.656 (3)
Ba1—O2vii3.1611 (17)As1—O2xiii1.7050 (17)
Ba1—O2iii3.1611 (17)As1—O21.7050 (17)
Ba1—O2viii3.1611 (17)As1—O2xiv1.7050 (17)
O1i—Ba1—O1ii180.00 (12)O2vii—Ba1—O2iii126.22 (5)
O1i—Ba1—O1iii117.11 (3)O1i—Ba1—O2viii52.94 (6)
O1ii—Ba1—O1iii62.89 (3)O1ii—Ba1—O2viii127.06 (6)
O1i—Ba1—O162.89 (3)O1iii—Ba1—O2viii82.85 (6)
O1ii—Ba1—O1117.11 (3)O1—Ba1—O2viii97.15 (6)
O1iii—Ba1—O1180.00 (12)O1iv—Ba1—O2viii106.72 (6)
O1i—Ba1—O1iv117.11 (3)O1v—Ba1—O2viii73.28 (6)
O1ii—Ba1—O1iv62.89 (3)O2vi—Ba1—O2viii180.00 (7)
O1iii—Ba1—O1iv117.11 (3)O2—Ba1—O2viii126.22 (5)
O1—Ba1—O1iv62.89 (3)O2vii—Ba1—O2viii126.22 (5)
O1i—Ba1—O1v62.89 (3)O2iii—Ba1—O2viii53.78 (5)
O1ii—Ba1—O1v117.11 (3)O1i—Ba1—O2ix82.85 (6)
O1iii—Ba1—O1v62.89 (3)O1ii—Ba1—O2ix97.15 (6)
O1—Ba1—O1v117.11 (3)O1iii—Ba1—O2ix106.72 (6)
O1iv—Ba1—O1v180.00 (12)O1—Ba1—O2ix73.28 (6)
O1i—Ba1—O2vi127.06 (6)O1iv—Ba1—O2ix52.94 (6)
O1ii—Ba1—O2vi52.94 (6)O1v—Ba1—O2ix127.06 (6)
O1iii—Ba1—O2vi97.15 (6)O2vi—Ba1—O2ix126.22 (5)
O1—Ba1—O2vi82.85 (6)O2—Ba1—O2ix126.22 (5)
O1iv—Ba1—O2vi73.28 (6)O2vii—Ba1—O2ix180.00 (3)
O1v—Ba1—O2vi106.72 (6)O2iii—Ba1—O2ix53.78 (5)
O1i—Ba1—O273.28 (6)O2viii—Ba1—O2ix53.78 (5)
O1ii—Ba1—O2106.72 (6)O2x—Co1—O2xi92.91 (7)
O1iii—Ba1—O2127.06 (6)O2x—Co1—O2xii92.91 (7)
O1—Ba1—O252.94 (6)O2xi—Co1—O2xii92.91 (7)
O1iv—Ba1—O297.15 (6)O2x—Co1—O2vii92.34 (6)
O1v—Ba1—O282.85 (6)O2xi—Co1—O2vii174.36 (6)
O2vi—Ba1—O253.78 (5)O2xii—Co1—O2vii88.86 (9)
O1i—Ba1—O2vii97.15 (6)O2x—Co1—O2174.36 (6)
O1ii—Ba1—O2vii82.85 (6)O2xi—Co1—O288.86 (9)
O1iii—Ba1—O2vii73.28 (6)O2xii—Co1—O292.34 (6)
O1—Ba1—O2vii106.72 (6)O2vii—Co1—O285.72 (7)
O1iv—Ba1—O2vii127.06 (6)O2x—Co1—O2vi88.86 (9)
O1v—Ba1—O2vii52.94 (6)O2xi—Co1—O2vi92.34 (6)
O2vi—Ba1—O2vii53.78 (5)O2xii—Co1—O2vi174.36 (6)
O2—Ba1—O2vii53.78 (5)O2vii—Co1—O2vi85.72 (7)
O1i—Ba1—O2iii106.72 (6)O2—Co1—O2vi85.72 (7)
O1ii—Ba1—O2iii73.28 (6)O1—As1—O2xiii108.33 (6)
O1iii—Ba1—O2iii52.94 (6)O1—As1—O2108.33 (6)
O1—Ba1—O2iii127.06 (6)O2xiii—As1—O2110.59 (5)
O1iv—Ba1—O2iii82.85 (6)O1—As1—O2xiv108.33 (6)
O1v—Ba1—O2iii97.15 (6)O2xiii—As1—O2xiv110.59 (5)
O2vi—Ba1—O2iii126.22 (5)O2—As1—O2xiv110.59 (5)
O2—Ba1—O2iii180.00 (7)
Table 1

Selected bond lengths (Å)

Ba1—O12.9344 (8)
Ba1—O23.1611 (17)
Co1—O2i2.0791 (17)
Co1—O22.1017 (17)
As1—O11.656 (3)
As1—O21.7050 (17)

Symmetry code: (i) .

  2 in total

1.  Multiparametric scaling of diffraction intensities.

Authors:  Zbyszek Otwinowski; Dominika Borek; Wladyslaw Majewski; Wladek Minor
Journal:  Acta Crystallogr A       Date:  2003-04-25       Impact factor: 2.290

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

  2 in total
  1 in total

1.  Polarized-neutron investigation of magnetic ordering and spin dynamics in BaCo2(AsO4)2 frustrated honeycomb-lattice magnet.

Authors:  L-P Regnault; C Boullier; J E Lorenzo
Journal:  Heliyon       Date:  2018-01-12
  1 in total

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