Literature DB >> 21580811

K(2)Ho(PO(4))(WO(4)).

Katherina V Terebilenko, Igor V Zatovsky, Vyacheslav N Baumer, Nikolay S Slobodyanik, Oleg V Shishkin.   

Abstract

A new compound, dipotassium holmium(III) phosphate(V) tungstate(VI), K(2)Ho(PO(4))(WO(4)), has been obtained during investigation of the K(2)O-P(2)O(5)-WO(3)-HoF(3) phase system using the flux technique. The compound is isotypic with K(2)Bi(PO(4))(WO(4)). Its framework structure consists of flat (∞) (2)[HoPO(4)] layers parallel to (100) that are made up of (∞) (1)[HoO(8)] zigzag chains inter-linked via slightly distorted PO(4) tetra-hedra. WO(4) tetra-hedra are attached above and below these layers, leaving space for the K(+) counter-cations. The HoO(8), PO(4) and WO(4) units exhibit 2 symmetry.

Entities:  

Year:  2008        PMID: 21580811      PMCID: PMC2959528          DOI: 10.1107/S160053680803287X

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


Related literature

For related structures, see: Ben Amara & Dabbabi (1987 ▶); Marsh (1987 ▶); Zatovsky, Terebilenko, Slobodyanik & Baumer (2006 ▶); Zatovsky, Terebilenko, Slobodyanik, Baumer & Shishkin (2006 ▶).

Experimental

Crystal data

K2Ho(PO4)(WO4) M = 585.95 Orthorhombic, a = 6.8820 (10) Å b = 12.1485 (18) Å c = 19.695 (3) Å V = 1646.6 (4) Å3 Z = 8 Mo Kα radiation μ = 24.72 mm−1 T = 293 (2) K 0.10 × 0.09 × 0.07 mm

Data collection

Oxford Diffraction Xcalibur-3 CCD diffractometer Absorption correction: multi-scan based on the method by Blessing (1995 ▶) T min = 0.102, T max = 0.177 8608 measured reflections 1561 independent reflections 1257 reflections with I > 2σ(I) R int = 0.055

Refinement

R[F 2 > 2σ(F 2)] = 0.029 wR(F 2) = 0.071 S = 1.15 1561 reflections 62 parameters Δρmax = 1.90 e Å−3 Δρmin = −1.73 e Å−3 Data collection: CrysAlis CCD (Oxford Diffraction, 2005 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2005 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053680803287X/wm2196sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053680803287X/wm2196Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
K2Ho(PO4)(WO4)F(000) = 2064
Mr = 585.95Dx = 4.727 Mg m3
Orthorhombic, IbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -I 2b 2cCell parameters from 8608 reflections
a = 6.882 (1) Åθ = 3.4–33.0°
b = 12.1485 (18) ŵ = 24.72 mm1
c = 19.695 (3) ÅT = 293 K
V = 1646.6 (4) Å3Prism, pale beige
Z = 80.10 × 0.09 × 0.07 mm
Oxford Diffraction XCalibur-3 CCD diffractometer1561 independent reflections
Radiation source: fine-focus sealed tube1257 reflections with I > 2σ(I)
graphiteRint = 0.055
φ and ω scansθmax = 33.0°, θmin = 3.4°
Absorption correction: multi-scan based on the method by Blessing (1995)h = −10→10
Tmin = 0.102, Tmax = 0.177k = −18→18
8608 measured reflectionsl = −30→29
Refinement on F20 restraints
Least-squares matrix: fullw = 1/[σ2(Fo2) + (0.0397P)2 + 3.2575P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.029(Δ/σ)max < 0.001
wR(F2) = 0.071Δρmax = 1.90 e Å3
S = 1.15Δρmin = −1.73 e Å3
1561 reflectionsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
62 parametersExtinction coefficient: 0.00010 (2)
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
xyzUiso*/Ueq
W10.50.250.334530 (12)0.01088 (5)
Ho10.750.325113 (17)0.50.00662 (5)
K10.96872 (15)0.07992 (10)0.34389 (5)0.0196 (2)
P10.750.07042 (10)0.50.0065 (2)
O10.7088 (4)0.2796 (3)0.38536 (17)0.0146 (7)
O20.4420 (6)0.3643 (4)0.2845 (2)0.0269 (8)
O30.7308 (4)−0.0047 (2)0.43834 (16)0.0102 (6)
O40.9229 (4)0.1514 (2)0.49215 (17)0.0105 (6)
U11U22U33U12U13U23
W10.01432 (9)0.01167 (9)0.00666 (9)−0.00095 (8)00
Ho10.00652 (9)0.00523 (9)0.00811 (10)0−0.00005 (9)0
K10.0204 (4)0.0248 (5)0.0137 (4)−0.0002 (4)0.0021 (3)0.0039 (4)
P10.0064 (5)0.0034 (5)0.0098 (6)00.0000 (5)0
O10.0154 (14)0.0171 (14)0.0113 (14)−0.0035 (11)−0.0012 (11)−0.0031 (11)
O20.0308 (17)0.0296 (19)0.0203 (17)−0.0008 (17)0.0013 (15)0.0126 (16)
O30.0126 (13)0.0079 (11)0.0101 (13)−0.0018 (10)−0.0002 (11)−0.0010 (9)
O40.0052 (10)0.0066 (11)0.0198 (16)−0.0017 (9)0.0011 (10)−0.0016 (11)
W1—O2i1.749 (4)Ho1—K1vii3.8119 (11)
W1—O21.749 (4)Ho1—K1vi3.8119 (12)
W1—O11.788 (3)K1—O32.683 (3)
W1—O1i1.788 (3)K1—O2v2.689 (4)
W1—K13.8352 (12)K1—O3x2.747 (3)
W1—K1i3.8352 (12)K1—O1vi2.916 (3)
W1—K1ii4.0181 (13)K1—O2xi2.934 (5)
W1—K1iii4.0181 (13)K1—O43.063 (3)
W1—K1iv4.0821 (12)K1—O13.122 (4)
W1—K1v4.0821 (12)K1—O2i3.133 (4)
Ho1—O4vi2.274 (3)K1—P13.4251 (11)
Ho1—O4vii2.274 (3)K1—Ho1vi3.8119 (11)
Ho1—O12.342 (3)K1—K1iii3.9511 (13)
Ho1—O1viii2.342 (3)P1—O31.525 (3)
Ho1—O3ix2.401 (3)P1—O3viii1.525 (3)
Ho1—O3ii2.401 (3)P1—O41.552 (3)
Ho1—O4viii2.428 (3)P1—O4viii1.552 (3)
Ho1—O42.428 (3)P1—Ho1xii2.9802 (13)
Ho1—P1ix2.9802 (13)P1—K1viii3.4251 (11)
Ho1—P13.0941 (13)
O2i—W1—O2111.4 (3)O3x—K1—O461.07 (8)
O2i—W1—O1106.94 (17)O1vi—K1—O469.23 (9)
O2—W1—O1109.83 (19)O2xi—K1—O4130.90 (10)
O2i—W1—O1i109.83 (19)O3—K1—O176.52 (9)
O2—W1—O1i106.94 (17)O2v—K1—O1100.44 (12)
O1—W1—O1i111.9 (2)O3x—K1—O1117.21 (9)
O4vi—Ho1—O4vii165.59 (15)O1vi—K1—O184.72 (10)
O4vi—Ho1—O194.81 (11)O2xi—K1—O1156.62 (10)
O4vii—Ho1—O188.59 (11)O4—K1—O158.09 (8)
O4vi—Ho1—O1viii88.59 (11)O3—K1—O2i77.94 (10)
O4vii—Ho1—O1viii94.81 (11)O2v—K1—O2i78.50 (9)
O1—Ho1—O1viii152.68 (18)O3x—K1—O2i156.48 (11)
O4vi—Ho1—O3ix88.91 (10)O1vi—K1—O2i131.64 (12)
O4vii—Ho1—O3ix78.65 (10)O2xi—K1—O2i103.49 (13)
O1—Ho1—O3ix133.18 (11)O4—K1—O2i101.64 (9)
O1viii—Ho1—O3ix73.88 (12)O1—K1—O2i54.04 (10)
O4vi—Ho1—O3ii78.65 (10)O3—P1—O3viii106.4 (2)
O4vii—Ho1—O3ii88.91 (10)O3—P1—O4111.52 (16)
O1—Ho1—O3ii73.88 (12)O3viii—P1—O4113.10 (16)
O1viii—Ho1—O3ii133.18 (12)O3—P1—O4viii113.10 (16)
O3ix—Ho1—O3ii61.17 (15)O3viii—P1—O4viii111.52 (16)
O4vi—Ho1—O4viii126.77 (7)O4—P1—O4viii101.3 (2)
O4vii—Ho1—O4viii67.63 (12)W1—O1—Ho1133.20 (16)
O1—Ho1—O4viii78.27 (12)W1—O1—K1vi124.93 (16)
O1viii—Ho1—O4viii78.03 (12)Ho1—O1—K1vi92.27 (11)
O3ix—Ho1—O4viii133.56 (10)W1—O1—K199.08 (14)
O3ii—Ho1—O4viii143.86 (10)Ho1—O1—K1111.49 (12)
O4vi—Ho1—O467.63 (12)K1vi—O1—K186.88 (9)
O4vii—Ho1—O4126.77 (8)W1—O2—K1v132.6 (2)
O1—Ho1—O478.03 (12)W1—O2—K1ii115.89 (19)
O1viii—Ho1—O478.27 (12)K1v—O2—K1ii95.86 (13)
O3ix—Ho1—O4143.86 (10)W1—O2—K1i99.64 (16)
O3ii—Ho1—O4133.56 (10)K1v—O2—K1i120.18 (15)
O4viii—Ho1—O459.26 (13)K1ii—O2—K1i81.21 (11)
O3—K1—O2v152.62 (12)P1—O3—Ho1xii96.20 (15)
O3—K1—O3x78.69 (8)P1—O3—K1105.64 (14)
O2v—K1—O3x124.78 (11)Ho1xii—O3—K1130.32 (12)
O3—K1—O1vi119.65 (10)P1—O3—K1iii142.66 (16)
O2v—K1—O1vi86.67 (12)Ho1xii—O3—K1iii95.30 (9)
O3x—K1—O1vi60.35 (9)K1—O3—K1iii93.37 (11)
O3—K1—O2xi93.55 (11)P1—O4—Ho1vi146.28 (18)
O2v—K1—O2xi78.59 (14)P1—O4—Ho199.72 (13)
O3x—K1—O2xi80.53 (10)Ho1vi—O4—Ho1111.83 (11)
O1vi—K1—O2xi118.34 (11)P1—O4—K189.66 (13)
O3—K1—O452.05 (8)Ho1vi—O4—K189.92 (10)
O2v—K1—O4148.06 (12)Ho1—O4—K1110.96 (11)
Table 1

Selected bond lengths (Å)

W1—O21.749 (4)
W1—O11.788 (3)
Ho1—O4i2.274 (3)
Ho1—O12.342 (3)
Ho1—O3ii2.401 (3)
Ho1—O42.428 (3)
P1—O31.525 (3)
P1—O41.552 (3)

Symmetry codes: (i) ; (ii) .

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2.  An empirical correction for absorption anisotropy.

Authors:  R H Blessing
Journal:  Acta Crystallogr A       Date:  1995-01-01       Impact factor: 2.290

  2 in total
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1.  Cs(2)Bi(PO(4))(WO(4)).

Authors:  Kateryna V Terebilenko; Igor V Zatovsky; Vyacheslav N Baumer; Nikolay S Slobodyanik
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2009-08-15

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Journal:  RSC Adv       Date:  2022-03-22       Impact factor: 3.361

  2 in total

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