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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2019 Jun 21;75(Pt 7):1041–1045. doi: 10.1107/S2056989019008685

Two new glaserite-type orthovanadates: Rb2KDy(VO4)2 and Cs1.52K1.48Gd(VO4)2

Lotfi Rghioui a, Lahcen El Ammari b,*, Abderrazzak Assani b, Mohamed Saadi b
PMCID: PMC6659331  PMID: 31392021

The title compounds have the glaserite structure type. The DyO6 or GdO6 octa­hedra share their three six vertices with six VO4 tetra­hedra, three of which are upward and the other three down. The remaining cations are localized between the sheets resulting from the tetra­hedra-octa­hedra linkage via common vertices.

Keywords: crystal structure, crystal growth, X-ray diffraction, Rb2KDy(VO4)2, Cs1.52K1.48Gd(VO4)2, orthovanadates, IR and Raman spectroscopy

Abstract

The crystal structures of dirubidium potassium dysprosium bis­(vanadate), Rb2KDy(VO4)2, and caesium potassium gadolinium bis­(vanadate), Cs1.52K1.48Gd(VO4)2, were solved from single-crystal X-ray diffraction data. Both compounds, synthesized by the reactive flux method, crystallize in the space group P Inline graphic m1 with the glaserite structure type. VO4 tetra­hedra are linked to DyO6 or GdO6 octa­hedra by common vertices to form sheets stacking along the c axis. The large twelve-coordinate Cs+ or Rb+ cations are sandwiched between these layers in tunnels along the a and b axes, while the K+ cations, surrounded by ten oxygen atoms, are localized in cavities.

Chemical context  

Many studies have been devoted to phosphates, vanadates and arsenates with the general formula (A,A′)3 Ln(XO4)2 (A,A′ = alkaline elements, Ln = rare-earth element and X = P, V, As) because of their outstanding optical properties. This type of compound has numerous possible applications, such as their use in the production of low- and high-pressure mercury lamps or colour television screens (Hong & Chinn, 1976). It has been shown that these optical properties are enhanced by the presence of either a rare-earth element or an XO4 group and are determined by the fine details of the crystal structures of those materials (Benarafa et al., 2005; Rghioui et al., 1996, 1999, 2006). For instance, Parent et al. (1980) studied the luminescence phenomenon in Na3La1–xNdx(PO4)2 and Na3La1–xNdx(VO4)2 and measured the life time of the excited state 4F 3/2 as a function of the Nd3+ concentration. From a detailed examination of the emission and excitation spectra, Srivastava et al. (1990) highlighted an energy transfer from Ce3+ to the Tb3+ ion in the K3La0.80Ce0.20(PO4)2, K3La0.80Tb0.20(PO4)2 and K3La1–xyTbxCey(PO4)2 phosphates. In addition, the band gaps and the life times of Ce3+ and Tb3+ were determined by Finke et al. (1992, 1994). The optical properties of the La atom in K3La(PO4)2; K2RbLa(PO4)2; Rb2KLa(PO4)2 and Rb3La(PO4)2 phosphates, investigated by FTIR and VUV spectroscopy, have allowed the determination of the values of band-gap energies for K3La(PO4)2 prepared by two different methods (Sasum et al., 1997). In addition, Guzik et al. (2007) concluded that the emission phenomenon occurs from the charge transfer state in Na3Lu1–xyYbx(PO4)2 and Na3Y1–xyYbx(PO4)2 compounds. More recently, the optical properties of the Eu3+ ion were widely investigated in K3Eu(XO4)2 where X = P, As and V, K2YbHo1–xyEux(PO4)2, K2CsLn(VO4)2 where Ln = La and Gd (Benarafa et al., 2009; Rghioui et al., 2015; Duke John David et al., 2016; Tao et al., 2014; Farmer et al., 2014, 2016). In the case of K3Eu(XO4)2, a vibronic coupling mechanism was proposed to explain the process of europium emission observed under 647.1 nm excitation.

From a crystallographic point of view, the related (A,A′)3 Ln(XO4)2 compounds with A,A′ = K, Rb and Cs adopt three structure types. The first is a monoclinic system, space group P21/m, represented by the phosphate K3Nd(PO4)2. The second one is trigonal, space group P Inline graphic, represented by K3Lu(PO4)2, while the third one is also trigonal but in space group P Inline graphic m1 and represented by the glaserite K3Na(SO4)2. The present work is a continuation of our structural investigations by X-ray diffraction of the (A,A′)3 Ln(XO4)2 system where A,A′ = K, Rb and Cs, Ln = rare earth and X = P, V, As (Rghioui et al., 1999, 2002, 2007). The present paper reports the synthesis and the crystal structure determination of the title compounds by X-ray diffraction at room temperature and vibrational spectroscopy.

Structural commentary  

Dirubidium potassium dysprosium bis­(vanadate), Rb2KDy(VO4)2, and caesium potassium gadolinium bis­(vanadate), Cs1.52K1.48Gd(VO4)2, both compounds crystallize in the space group P Inline graphic m1 with the common glaserite, K3Na(SO4)2, structure type (Moonre, 1973; Okada & Ossaka, 1980). The formulae determined by X-ray diffraction are consistent with the results of chemical analysis. In both structures, all atoms are in special positions of the P Inline graphic m1 space group, namely Dy1 in Wyckoff position 1a (Inline graphic m), Rb1 in 1b (Inline graphic m), K1/Rb2, V1 and O2 in 2d (3m) and O1 in 6i (m). The structures of the two vanadates are built up from two independent VO4 tetra­hedra sharing an apex with DyO6 or GdO6 octa­hedra in such a way as to form a layer parallel to the ab plane, as shown in Fig. 1. Three of the six VO4 tetra­hedra surrounding each DyO6 or GdO6 octa­hedron are oriented upwards and the other three down. The concatenation of these polyhedra delimits large tunnels and cavities of site symmetry Inline graphic m and 3m in which are located rubidium and a statistical mixture of rubidium and potassium atoms (Fig. 2).

Figure 1.

Figure 1

Layer of VO4 tetra­hedra linked to DyO6 octa­hedra by vertex sharing in the structure of Rb2KDy(VO4)2.

Figure 2.

Figure 2

Three-dimensional view along the a axis of the crystal structure showing Rb+ (or Cs+) in the channels.

The coordination polyhedron of the mixed site is formed by ten oxygen atoms belonging to three edges, one face and one vertex of five VO4 tetra­hedra as shown in Fig. 3. The K/Rb—O distances range from 2.681 (8) to 3.312 (7) Å. The twelve oxygen atoms surrounding the rubidium atom form an irregular cubocta­hedron with Rb—O distances varying between 3.133 (2) and 3.4649 (3) Å. The main inter­atomic distances and angles are compatible with the values quoted in the literature (Gagné & Hawthorne, 2016; Gagné, 2018).

Figure 3.

Figure 3

View along the c axis of a layer in the structure of the title compounds, showing the cavities in which the K/Rb+ (or K/Cs+) cations are located.

The three-dimensional structure consists of a basic tetra­hedral–octa­hedral framework, forming layers that stack along the c-axis direction, as shown in Fig. 4. In glaserite-like structures, the large cations are located between the layers in channels running along the a- and b-axis directions and the average size cations are located in the cavities (see Fig. 5).

Figure 4.

Figure 4

Three-dimensional view of the crystal structure showing Rb+ (or Cs+) cations between the layers stacked along the c axis.

Figure 5.

Figure 5

Three-dimensional perspective view along c axis of the crystal structure of Rb2KDy(VO4)2.

Vibrational spectroscopy  

The Raman and infrared spectra for Rb2KDy(VO4)2 are shown in Figs. 6 and 7, respectively. Their band assignments given in Table 1 are based on previous works for homologous vanadates (Rghioui et al., 1999, 2012; Benarafa et al., 2009). The stretching modes of (VO4)3− anions are usually found in the region 950–700 cm−1. The peaks observed in the Raman spectrum at 935, 875 and 740 cm−1 as well as the corres­ponding bands in the infrared spectrum at 925, 830 and 755 cm−1 are all attributed to the symmetric (VO4)3− and the asymmetric (VO4)3− vibration. The bending vibrations of (VO4)3− are seen in the range 390–310 cm−1. As in previous works (Rghioui et al., 2012), the separation between the symmetric and asymmetric bending can not be identified in the vibrational spectra. The bands lying between 230 and 95 cm−1 in the spectra are assigned to the lattice vibrations. They are due to the VO4 rotation and to the VO4, K+, Rb+ and Dy3+ translation modes. A comparison of the Raman and infrared bands shows that they are not coincident. This fact confirms the centrosymmetric structure of Rb2KDy(VO4)2 vanadate.

Figure 6.

Figure 6

Raman spectrum of Rb2KDy(VO4)2.

Figure 7.

Figure 7

Infrared spectrum of Rb2KDy(VO4)2.

Table 1. Raman and Infrared band assignments (cm−1) for Rb2KDy(VO4)2 .

Raman Infrared Attribution
935 925 Stretching vibrations of VO4 groups
875 830
740 755
     
385 377 Deformation modes of VO4 groups
370 365
340 311
     
200 230 External modes
160 177
125 130
95 120

Synthesis and crystallization  

Single crystals of Rb2KDy(VO4)2 and Cs1.52K1.48Gd(VO4)2 were synthesized by the flux method using a mixture of K2CO3, Rb2CO3 (or Cs2CO3 for the Gd compound), Dy2O3 (or Gd2O3) and V2O5 corresponding to 1 mol of K2RbDy(VO4)2 (or Cs1.52K1.48Gd(VO4)2 and 1 mol of Rb3VO4 (or Cs3VO4). The reagents were ground in an agate mortar and placed in a platinum crucible. The temperature was raised slowly to 873 K and maintained for 24 h, permitting the carbonates to decompose. A second treatment at the melting temperature of 1273 K was performed, followed by slow cooling at a rate of 4 K h−1 to 673 K and then quickly to ambient temperature. Each thermal treatment was inter­spersed with grinding. The obtained product was then washed with distilled water in order to eliminate the flux. The resulting product contained single crystals of a suitable size for the X-ray diffraction study.

Refinement  

Crystal data, data collection and structure refinement details are summarized in Table 2. In the refinement procedure, the substitutional occupation of the mixed sites was freely refined and restricted to the occupancy of one site for Cs1.52K1.48Gd(VO4)2 but restricted to 0.5:0.5 for Rb2KDy(VO4)2.

Table 2. Experimental details.

  Rb2KDy(VO4)2 Cs1.52K1.48Gd(VO4)2
Crystal data
M r 602.42 646.74
Crystal system, space group Trigonal, P Inline graphic m1 Trigonal, P Inline graphic m1
Temperature (K) 296 296
a, c (Å) 5.9728 (1), 7.7780 (1) 6.0321 (1), 7.9821 (2)
V3) 240.30 (1) 251.53 (1)
Z 1 1
Radiation type Mo Kα Mo Kα
μ (mm−1) 20.10 14.37
Crystal size (mm) 0.35 × 0.28 × 0.25 0.34 × 0.26 × 0.22
 
Data collection
Diffractometer Bruker X8 APEX Bruker X8 APEX
Absorption correction Multi-scan (SADABS; Krause et al., 2015) Multi-scan (SADABS; Krause et al., 2015)
T min, T max 0.357, 0.749 0.639, 0.747
No. of measured, independent and observed [I > 2σ(I)] reflections 10549, 647, 631 14472, 678, 666
R int 0.049 0.038
(sin θ/λ)max−1) 0.926 0.925
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.016, 0.042, 1.11 0.010, 0.028, 1.09
No. of reflections 647 678
No. of parameters 24 25
Δρmax, Δρmin (e Å−3) 1.35, −1.35 0.63, −0.94

Computer programs: APEX2 and SAINT-Plus (Bruker, 2009), SHELXT2014 (Sheldrick, 2015a ), SHELXL2018 (Sheldrick, 2015b ), ORTEP-3 for Windows (Farrugia, 2012), DIAMOND (Brandenburg, 2006), Mercury (Macrae et al., 2008) and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, II, global. DOI: 10.1107/S2056989019008685/vn2149sup1.cif

e-75-01041-sup1.cif (823.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989019008685/vn2149Isup2.hkl

e-75-01041-Isup2.hkl (54.3KB, hkl)

Structure factors: contains datablock(s) II. DOI: 10.1107/S2056989019008685/vn2149IIsup3.hkl

e-75-01041-IIsup3.hkl (56.8KB, hkl)

CCDC references: 1934723, 1934722

Additional supporting information: crystallographic information; 3D view; checkCIF report

Acknowledgments

The authors thank the Faculty of Science at the Mohammed V University in Rabat, Morocco, for the X-ray measurements.

supplementary crystallographic information

Dirubidium potassium dysprosium bis(vanadate) (I). Crystal data

Rb2KDy(VO4)2 Dx = 4.163 Mg m3
Mr = 602.42 Mo Kα radiation, λ = 0.71073 Å
Trigonal, P3m1 Cell parameters from 647 reflections
a = 5.9728 (1) Å θ = 2.6–41.1°
c = 7.7780 (1) Å µ = 20.10 mm1
V = 240.30 (1) Å3 T = 296 K
Z = 1 Block, colourless
F(000) = 269 0.35 × 0.28 × 0.25 mm

Dirubidium potassium dysprosium bis(vanadate) (I). Data collection

Bruker X8 APEX diffractometer 647 independent reflections
Radiation source: fine-focus sealed tube 631 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.049
φ and ω scans θmax = 41.1°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Krause et al., 2015) h = −11→11
Tmin = 0.357, Tmax = 0.749 k = −11→10
10549 measured reflections l = −14→14

Dirubidium potassium dysprosium bis(vanadate) (I). Refinement

Refinement on F2 0 restraints
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0239P)2 + 0.1252P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.016 (Δ/σ)max < 0.001
wR(F2) = 0.042 Δρmax = 1.35 e Å3
S = 1.11 Δρmin = −1.35 e Å3
647 reflections Extinction correction: SHELXL2018 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
24 parameters Extinction coefficient: 0.0124 (15)

Dirubidium potassium dysprosium bis(vanadate) (I). Special details

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.

Dirubidium potassium dysprosium bis(vanadate) (I). Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Rb1 0.000000 0.000000 0.500000 0.03556 (16)
Dy1 0.000000 0.000000 0.000000 0.00791 (6)
K1 0.333333 0.666667 0.8013 (9) 0.0098 (8) 0.5
Rb2 0.333333 0.666667 0.7969 (5) 0.0191 (6) 0.5
V1 0.333333 0.666667 0.24618 (6) 0.00765 (8)
O1 0.17571 (17) 0.82429 (17) 0.1720 (3) 0.0273 (4)
O2 0.333333 0.666667 0.4567 (4) 0.0389 (10)

Dirubidium potassium dysprosium bis(vanadate) (I). Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Rb1 0.0463 (3) 0.0463 (3) 0.0141 (2) 0.02314 (13) 0.000 0.000
Dy1 0.00565 (6) 0.00565 (6) 0.01243 (8) 0.00282 (3) 0.000 0.000
K1 0.0082 (10) 0.0082 (10) 0.0128 (18) 0.0041 (5) 0.000 0.000
Rb2 0.0194 (7) 0.0194 (7) 0.0185 (12) 0.0097 (4) 0.000 0.000
V1 0.00766 (10) 0.00766 (10) 0.00763 (16) 0.00383 (5) 0.000 0.000
O1 0.0219 (5) 0.0219 (5) 0.0424 (10) 0.0141 (6) −0.0081 (3) 0.0081 (3)
O2 0.0542 (15) 0.0542 (15) 0.0084 (10) 0.0271 (8) 0.000 0.000

Dirubidium potassium dysprosium bis(vanadate) (I). Geometric parameters (Å, º)

Rb1—O1i 3.133 (2) K1—O1xvii 2.9951 (5)
Rb1—O1ii 3.133 (2) K1—O1xviii 2.9951 (6)
Rb1—O1iii 3.133 (2) K1—O1iii 2.9951 (6)
Rb1—O1iv 3.133 (2) K1—O1xix 2.9951 (5)
Rb1—O1v 3.133 (2) K1—O1i 2.9951 (5)
Rb1—O1vi 3.133 (2) K1—O1xx 3.312 (7)
Rb1—O2vii 3.4648 (3) K1—O1xxi 3.312 (7)
Rb1—O2viii 3.4648 (3) K1—O1xxii 3.312 (7)
Rb1—O2ix 3.4648 (3) K1—V1xx 3.460 (7)
Rb1—O2 3.4648 (3) K1—V1vii 3.4681 (8)
Rb1—O2iii 3.4649 (3) Rb2—O2 2.647 (5)
Rb1—O2iv 3.4649 (3) Rb2—O1xvi 2.9976 (4)
Dy1—O1x 2.2569 (17) Rb2—O1xvii 2.9976 (4)
Dy1—O1vi 2.2569 (17) Rb2—O1xviii 2.9976 (4)
Dy1—O1xi 2.2569 (17) Rb2—O1iii 2.9976 (4)
Dy1—O1iv 2.2569 (17) Rb2—O1xix 2.9976 (4)
Dy1—O1xii 2.2569 (17) Rb2—O1i 2.9976 (4)
Dy1—O1ii 2.2569 (17) Rb2—O1xx 3.342 (4)
Dy1—K1xiii 3.779 (3) Rb2—O1xxi 3.342 (4)
Dy1—K1vii 3.779 (3) Rb2—O1xxii 3.342 (4)
Dy1—K1xiv 3.779 (3) Rb2—V1vii 3.4646 (4)
Dy1—K1ix 3.779 (3) Rb2—V1iii 3.4647 (4)
Dy1—K1xv 3.779 (3) V1—O2 1.637 (3)
Dy1—K1iii 3.779 (3) V1—O1 1.7297 (16)
K1—O2 2.681 (8) V1—O1vi 1.7297 (16)
K1—O1xvi 2.9951 (5) V1—O1xxiii 1.7297 (16)
O1i—Rb1—O1ii 180.0 O1xviii—K1—V1xx 86.02 (15)
O1i—Rb1—O1iii 60.33 (5) O1iii—K1—V1xx 86.02 (15)
O1ii—Rb1—O1iii 119.67 (5) O1xix—K1—V1xx 86.02 (15)
O1i—Rb1—O1iv 119.67 (5) O1i—K1—V1xx 86.02 (15)
O1ii—Rb1—O1iv 60.33 (5) O1xx—K1—V1xx 29.49 (7)
O1iii—Rb1—O1iv 180.0 O1xxi—K1—V1xx 29.49 (7)
O1i—Rb1—O1v 60.33 (5) O1xxii—K1—V1xx 29.49 (7)
O1ii—Rb1—O1v 119.67 (5) O2—K1—V1vii 83.89 (12)
O1iii—Rb1—O1v 60.33 (5) O1xvi—K1—V1vii 148.26 (4)
O1iv—Rb1—O1v 119.67 (5) O1xvii—K1—V1vii 148.26 (4)
O1i—Rb1—O1vi 119.67 (5) O1xviii—K1—V1vii 92.20 (4)
O1ii—Rb1—O1vi 60.33 (5) O1iii—K1—V1vii 92.20 (4)
O1iii—Rb1—O1vi 119.67 (5) O1xix—K1—V1vii 29.92 (3)
O1iv—Rb1—O1vi 60.33 (5) O1i—K1—V1vii 29.92 (3)
O1v—Rb1—O1vi 180.0 O1xx—K1—V1vii 125.60 (19)
O1i—Rb1—O2vii 48.95 (6) O1xxi—K1—V1vii 81.25 (8)
O1ii—Rb1—O2vii 131.05 (6) O1xxii—K1—V1vii 81.25 (8)
O1iii—Rb1—O2vii 102.09 (5) V1xx—K1—V1vii 96.11 (12)
O1iv—Rb1—O2vii 77.91 (5) O2—Rb2—O1xvi 94.63 (9)
O1v—Rb1—O2vii 102.09 (5) O2—Rb2—O1xvii 94.63 (9)
O1vi—Rb1—O2vii 77.91 (5) O1xvi—Rb2—O1xvii 63.36 (7)
O1i—Rb1—O2viii 131.05 (6) O2—Rb2—O1xviii 94.63 (9)
O1ii—Rb1—O2viii 48.95 (6) O1xvi—Rb2—O1xviii 56.21 (7)
O1iii—Rb1—O2viii 77.91 (5) O1xvii—Rb2—O1xviii 119.36 (3)
O1iv—Rb1—O2viii 102.09 (5) O2—Rb2—O1iii 94.63 (9)
O1v—Rb1—O2viii 77.91 (5) O1xvi—Rb2—O1iii 119.36 (3)
O1vi—Rb1—O2viii 102.09 (5) O1xvii—Rb2—O1iii 56.21 (7)
O2vii—Rb1—O2viii 180.00 (11) O1xviii—Rb2—O1iii 170.08 (18)
O1i—Rb1—O2ix 102.09 (5) O2—Rb2—O1xix 94.63 (9)
O1ii—Rb1—O2ix 77.91 (5) O1xvi—Rb2—O1xix 119.36 (3)
O1iii—Rb1—O2ix 102.09 (5) O1xvii—Rb2—O1xix 170.08 (18)
O1iv—Rb1—O2ix 77.91 (5) O1xviii—Rb2—O1xix 63.36 (7)
O1v—Rb1—O2ix 48.95 (6) O1iii—Rb2—O1xix 119.36 (3)
O1vi—Rb1—O2ix 131.05 (6) O2—Rb2—O1i 94.63 (9)
O2vii—Rb1—O2ix 119.065 (18) O1xvi—Rb2—O1i 170.08 (18)
O2viii—Rb1—O2ix 60.935 (18) O1xvii—Rb2—O1i 119.36 (3)
O1i—Rb1—O2 77.91 (5) O1xviii—Rb2—O1i 119.36 (3)
O1ii—Rb1—O2 102.09 (5) O1iii—Rb2—O1i 63.36 (7)
O1iii—Rb1—O2 77.91 (5) O1xix—Rb2—O1i 56.21 (7)
O1iv—Rb1—O2 102.09 (5) O2—Rb2—O1xx 150.80 (5)
O1v—Rb1—O2 131.05 (6) O1xvi—Rb2—O1xx 61.07 (8)
O1vi—Rb1—O2 48.95 (6) O1xvii—Rb2—O1xx 61.07 (8)
O2vii—Rb1—O2 60.935 (18) O1xviii—Rb2—O1xx 85.09 (8)
O2viii—Rb1—O2 119.065 (18) O1iii—Rb2—O1xx 85.09 (8)
O2ix—Rb1—O2 180.0 O1xix—Rb2—O1xx 110.99 (11)
O1i—Rb1—O2iii 102.09 (5) O1i—Rb2—O1xx 110.99 (11)
O1ii—Rb1—O2iii 77.91 (5) O2—Rb2—O1xxi 150.80 (5)
O1iii—Rb1—O2iii 48.95 (6) O1xvi—Rb2—O1xxi 85.09 (8)
O1iv—Rb1—O2iii 131.05 (6) O1xvii—Rb2—O1xxi 110.99 (11)
O1v—Rb1—O2iii 102.09 (5) O1xviii—Rb2—O1xxi 61.07 (8)
O1vi—Rb1—O2iii 77.91 (5) O1iii—Rb2—O1xxi 110.99 (11)
O2vii—Rb1—O2iii 119.064 (18) O1xix—Rb2—O1xxi 61.07 (8)
O2viii—Rb1—O2iii 60.936 (18) O1i—Rb2—O1xxi 85.09 (8)
O2ix—Rb1—O2iii 119.064 (18) O1xx—Rb2—O1xxi 49.99 (8)
O2—Rb1—O2iii 60.935 (18) O2—Rb2—O1xxii 150.80 (5)
O1i—Rb1—O2iv 77.91 (5) O1xvi—Rb2—O1xxii 110.99 (11)
O1ii—Rb1—O2iv 102.09 (5) O1xvii—Rb2—O1xxii 85.09 (8)
O1iii—Rb1—O2iv 131.05 (6) O1xviii—Rb2—O1xxii 110.99 (11)
O1iv—Rb1—O2iv 48.95 (6) O1iii—Rb2—O1xxii 61.07 (8)
O1v—Rb1—O2iv 77.91 (5) O1xix—Rb2—O1xxii 85.09 (8)
O1vi—Rb1—O2iv 102.09 (5) O1i—Rb2—O1xxii 61.07 (8)
O2vii—Rb1—O2iv 60.936 (18) O1xx—Rb2—O1xxii 49.99 (8)
O2viii—Rb1—O2iv 119.064 (18) O1xxi—Rb2—O1xxii 49.99 (8)
O2ix—Rb1—O2iv 60.936 (18) O2—Rb2—V1vii 84.45 (7)
O2—Rb1—O2iv 119.065 (18) O1xvi—Rb2—V1vii 148.32 (3)
O2iii—Rb1—O2iv 180.0 O1xvii—Rb2—V1vii 148.32 (3)
O1x—Dy1—O1vi 180.00 (12) O1xviii—Rb2—V1vii 92.23 (3)
O1x—Dy1—O1xi 88.46 (9) O1iii—Rb2—V1vii 92.23 (3)
O1vi—Dy1—O1xi 91.54 (9) O1xix—Rb2—V1vii 29.95 (3)
O1x—Dy1—O1iv 91.54 (9) O1i—Rb2—V1vii 29.95 (3)
O1vi—Dy1—O1iv 88.46 (9) O1xx—Rb2—V1vii 124.76 (11)
O1xi—Dy1—O1iv 180.00 (9) O1xxi—Rb2—V1vii 80.89 (5)
O1x—Dy1—O1xii 88.46 (9) O1xxii—Rb2—V1vii 80.89 (5)
O1vi—Dy1—O1xii 91.54 (9) O2—Rb2—V1iii 84.45 (7)
O1xi—Dy1—O1xii 88.46 (9) O1xvi—Rb2—V1iii 92.23 (3)
O1iv—Dy1—O1xii 91.54 (9) O1xvii—Rb2—V1iii 29.95 (3)
O1x—Dy1—O1ii 91.54 (9) O1xviii—Rb2—V1iii 148.32 (3)
O1vi—Dy1—O1ii 88.46 (9) O1iii—Rb2—V1iii 29.95 (3)
O1xi—Dy1—O1ii 91.54 (9) O1xix—Rb2—V1iii 148.32 (3)
O1iv—Dy1—O1ii 88.46 (9) O1i—Rb2—V1iii 92.23 (3)
O1xii—Dy1—O1ii 180.00 (10) O1xx—Rb2—V1iii 80.89 (5)
O1x—Dy1—K1xiii 52.42 (5) O1xxi—Rb2—V1iii 124.76 (11)
O1vi—Dy1—K1xiii 127.58 (5) O1xxii—Rb2—V1iii 80.89 (5)
O1xi—Dy1—K1xiii 52.42 (5) V1vii—Rb2—V1iii 119.07 (2)
O1iv—Dy1—K1xiii 127.58 (5) O2—V1—O1 109.49 (8)
O1xii—Dy1—K1xiii 119.51 (12) O2—V1—O1vi 109.49 (8)
O1ii—Dy1—K1xiii 60.49 (12) O1—V1—O1vi 109.45 (8)
O1x—Dy1—K1vii 127.58 (5) O2—V1—O1xxiii 109.49 (8)
O1vi—Dy1—K1vii 52.42 (5) O1—V1—O1xxiii 109.45 (8)
O1xi—Dy1—K1vii 127.58 (5) O1vi—V1—O1xxiii 109.45 (8)
O1iv—Dy1—K1vii 52.42 (5) O2—V1—K1xiv 180.0
O1xii—Dy1—K1vii 60.49 (12) O1—V1—K1xiv 70.51 (8)
O1ii—Dy1—K1vii 119.51 (12) O1vi—V1—K1xiv 70.51 (8)
K1xiii—Dy1—K1vii 180.0 O1xxiii—V1—K1xiv 70.51 (8)
O1x—Dy1—K1xiv 119.51 (12) O2—V1—K1vii 96.11 (12)
O1vi—Dy1—K1xiv 60.49 (12) O1—V1—K1vii 154.40 (15)
O1xi—Dy1—K1xiv 52.42 (5) O1vi—V1—K1vii 59.72 (4)
O1iv—Dy1—K1xiv 127.58 (5) O1xxiii—V1—K1vii 59.72 (4)
O1xii—Dy1—K1xiv 52.42 (5) K1xiv—V1—K1vii 83.89 (12)
O1ii—Dy1—K1xiv 127.58 (5) O2—V1—K1iii 96.11 (12)
K1xiii—Dy1—K1xiv 104.42 (12) O1—V1—K1iii 59.72 (4)
K1vii—Dy1—K1xiv 75.58 (12) O1vi—V1—K1iii 59.72 (4)
O1x—Dy1—K1ix 60.49 (12) O1xxiii—V1—K1iii 154.40 (15)
O1vi—Dy1—K1ix 119.51 (12) K1xiv—V1—K1iii 83.89 (12)
O1xi—Dy1—K1ix 127.58 (5) K1vii—V1—K1iii 118.88 (4)
O1iv—Dy1—K1ix 52.42 (5) O2—V1—K1xviii 96.11 (12)
O1xii—Dy1—K1ix 127.58 (5) O1—V1—K1xviii 59.72 (4)
O1ii—Dy1—K1ix 52.42 (5) O1vi—V1—K1xviii 154.40 (15)
K1xiii—Dy1—K1ix 75.58 (12) O1xxiii—V1—K1xviii 59.72 (4)
K1vii—Dy1—K1ix 104.42 (12) K1xiv—V1—K1xviii 83.89 (12)
K1xiv—Dy1—K1ix 180.0 K1vii—V1—K1xviii 118.88 (5)
O1x—Dy1—K1xv 52.42 (5) K1iii—V1—K1xviii 118.88 (4)
O1vi—Dy1—K1xv 127.58 (5) O2—V1—Rb1xxiv 60.209 (6)
O1xi—Dy1—K1xv 119.51 (12) O1—V1—Rb1xxiv 49.28 (8)
O1iv—Dy1—K1xv 60.49 (12) O1vi—V1—Rb1xxiv 125.09 (3)
O1xii—Dy1—K1xv 52.42 (5) O1xxiii—V1—Rb1xxiv 125.09 (3)
O1ii—Dy1—K1xv 127.58 (5) K1xiv—V1—Rb1xxiv 119.792 (6)
K1xiii—Dy1—K1xv 104.42 (12) K1vii—V1—Rb1xxiv 156.32 (12)
K1vii—Dy1—K1xv 75.58 (12) K1iii—V1—Rb1xxiv 67.75 (7)
K1xiv—Dy1—K1xv 104.42 (12) K1xviii—V1—Rb1xxiv 67.75 (7)
K1ix—Dy1—K1xv 75.58 (12) O2—V1—Rb1xxv 60.209 (6)
O1x—Dy1—K1iii 127.58 (5) O1—V1—Rb1xxv 125.09 (3)
O1vi—Dy1—K1iii 52.42 (5) O1vi—V1—Rb1xxv 125.09 (3)
O1xi—Dy1—K1iii 60.49 (12) O1xxiii—V1—Rb1xxv 49.28 (8)
O1iv—Dy1—K1iii 119.51 (12) K1xiv—V1—Rb1xxv 119.791 (6)
O1xii—Dy1—K1iii 127.58 (5) K1vii—V1—Rb1xxv 67.76 (7)
O1ii—Dy1—K1iii 52.42 (5) K1iii—V1—Rb1xxv 156.32 (12)
K1xiii—Dy1—K1iii 75.58 (12) K1xviii—V1—Rb1xxv 67.76 (7)
K1vii—Dy1—K1iii 104.42 (12) Rb1xxiv—V1—Rb1xxv 97.454 (8)
K1xiv—Dy1—K1iii 75.58 (12) O2—V1—Rb1 60.209 (6)
K1ix—Dy1—K1iii 104.42 (12) O1—V1—Rb1 125.09 (3)
K1xv—Dy1—K1iii 180.0 O1vi—V1—Rb1 49.28 (8)
O2—K1—O1xvi 93.98 (15) O1xxiii—V1—Rb1 125.09 (3)
O2—K1—O1xvii 93.98 (15) K1xiv—V1—Rb1 119.791 (6)
O1xvi—K1—O1xvii 63.42 (7) K1vii—V1—Rb1 67.76 (7)
O2—K1—O1xviii 93.98 (15) K1iii—V1—Rb1 67.76 (7)
O1xvi—K1—O1xviii 56.26 (7) K1xviii—V1—Rb1 156.32 (12)
O1xvii—K1—O1xviii 119.52 (4) Rb1xxiv—V1—Rb1 97.454 (8)
O2—K1—O1iii 93.98 (15) Rb1xxv—V1—Rb1 97.454 (8)
O1xvi—K1—O1iii 119.52 (4) O2—V1—Rb2 0.000 (1)
O1xvii—K1—O1iii 56.26 (7) O1—V1—Rb2 109.49 (8)
O1xviii—K1—O1iii 171.3 (3) O1vi—V1—Rb2 109.49 (8)
O2—K1—O1xix 93.98 (15) O1xxiii—V1—Rb2 109.49 (8)
O1xvi—K1—O1xix 119.52 (4) K1xiv—V1—Rb2 180.0
O1xvii—K1—O1xix 171.3 (3) K1vii—V1—Rb2 96.11 (12)
O1xviii—K1—O1xix 63.42 (7) K1iii—V1—Rb2 96.11 (12)
O1iii—K1—O1xix 119.52 (4) K1xviii—V1—Rb2 96.11 (12)
O2—K1—O1i 93.98 (15) Rb1xxiv—V1—Rb2 60.209 (6)
O1xvi—K1—O1i 171.3 (3) Rb1xxv—V1—Rb2 60.209 (6)
O1xvii—K1—O1i 119.52 (4) Rb1—V1—Rb2 60.209 (6)
O1xviii—K1—O1i 119.52 (4) V1—O1—Dy1xxiv 163.14 (14)
O1iii—K1—O1i 63.42 (7) V1—O1—K1xviii 90.36 (6)
O1xix—K1—O1i 56.26 (7) Dy1xxiv—O1—K1xviii 90.91 (9)
O2—K1—O1xx 150.51 (7) V1—O1—K1iii 90.36 (6)
O1xvi—K1—O1xx 61.46 (10) Dy1xxiv—O1—K1iii 90.91 (9)
O1xvii—K1—O1xx 61.46 (10) K1xviii—O1—K1iii 171.3 (3)
O1xviii—K1—O1xx 85.65 (13) V1—O1—Rb1xxiv 105.98 (10)
O1iii—K1—O1xx 85.65 (13) Dy1xxiv—O1—Rb1xxiv 90.88 (6)
O1xix—K1—O1xx 111.86 (19) K1xviii—O1—Rb1xxiv 85.72 (12)
O1i—K1—O1xx 111.86 (19) K1iii—O1—Rb1xxiv 85.72 (12)
O2—K1—O1xxi 150.51 (7) V1—O1—K1xiv 80.00 (10)
O1xvi—K1—O1xxi 85.65 (13) Dy1xxiv—O1—K1xiv 83.14 (9)
O1xvii—K1—O1xxi 111.86 (19) K1xviii—O1—K1xiv 94.35 (13)
O1xviii—K1—O1xxi 61.46 (10) K1iii—O1—K1xiv 94.35 (13)
O1iii—K1—O1xxi 111.86 (19) Rb1xxiv—O1—K1xiv 174.02 (9)
O1xix—K1—O1xxi 61.46 (10) V1—O2—Rb2 180.0
O1i—K1—O1xxi 85.65 (13) V1—O2—K1 180.0
O1xx—K1—O1xxi 50.47 (12) Rb2—O2—K1 0.000 (1)
O2—K1—O1xxii 150.51 (7) V1—O2—Rb1xxiv 95.58 (5)
O1xvi—K1—O1xxii 111.86 (19) Rb2—O2—Rb1xxiv 84.42 (5)
O1xvii—K1—O1xxii 85.65 (13) K1—O2—Rb1xxiv 84.42 (5)
O1xviii—K1—O1xxii 111.86 (19) V1—O2—Rb1xxv 95.58 (5)
O1iii—K1—O1xxii 61.46 (10) Rb2—O2—Rb1xxv 84.42 (5)
O1xix—K1—O1xxii 85.65 (13) K1—O2—Rb1xxv 84.42 (5)
O1i—K1—O1xxii 61.46 (10) Rb1xxiv—O2—Rb1xxv 119.065 (18)
O1xx—K1—O1xxii 50.47 (12) V1—O2—Rb1 95.58 (5)
O1xxi—K1—O1xxii 50.47 (12) Rb2—O2—Rb1 84.42 (5)
O2—K1—V1xx 180.0 K1—O2—Rb1 84.42 (5)
O1xvi—K1—V1xx 86.02 (15) Rb1xxiv—O2—Rb1 119.065 (18)
O1xvii—K1—V1xx 86.02 (15) Rb1xxv—O2—Rb1 119.065 (18)

Symmetry codes: (i) xy+1, x, −z+1; (ii) −x+y−1, −x, z; (iii) −x, −y+1, −z+1; (iv) x, y−1, z; (v) y−1, −x+y−1, −z+1; (vi) −y+1, xy+1, z; (vii) −x+1, −y+1, −z+1; (viii) x−1, y−1, z; (ix) −x, −y, −z+1; (x) y−1, −x+y−1, −z; (xi) −x, −y+1, −z; (xii) xy+1, x, −z; (xiii) x−1, y−1, z−1; (xiv) x, y, z−1; (xv) x, y−1, z−1; (xvi) xy+1, x+1, −z+1; (xvii) y−1, −x+y, −z+1; (xviii) −x+1, −y+2, −z+1; (xix) y, −x+y, −z+1; (xx) x, y, z+1; (xxi) −x+y, −x+1, z+1; (xxii) −y+1, xy+1, z+1; (xxiii) −x+y, −x+1, z; (xxiv) x, y+1, z; (xxv) x+1, y+1, z.

Caesium potassium gadolinium bis(vanadate) (II). Crystal data

Cs1.52K1.48Gd(VO4)2 Dx = 4.270 Mg m3
Mr = 646.74 Mo Kα radiation, λ = 0.71073 Å
Trigonal, P3m1 Cell parameters from 678 reflections
a = 6.0321 (1) Å θ = 3.9–41.1°
c = 7.9821 (2) Å µ = 14.37 mm1
V = 251.53 (1) Å3 T = 296 K
Z = 1 Block, colourless
F(000) = 286 0.34 × 0.26 × 0.22 mm

Caesium potassium gadolinium bis(vanadate) (II). Data collection

Bruker X8 APEX diffractometer 678 independent reflections
Radiation source: fine-focus sealed tube 666 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.038
φ and ω scans θmax = 41.1°, θmin = 3.9°
Absorption correction: multi-scan (SADABS; Krause et al., 2015) h = −11→11
Tmin = 0.639, Tmax = 0.747 k = −9→11
14472 measured reflections l = −14→14

Caesium potassium gadolinium bis(vanadate) (II). Refinement

Refinement on F2 0 restraints
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.014P)2 + 0.0871P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.010 (Δ/σ)max < 0.001
wR(F2) = 0.028 Δρmax = 0.63 e Å3
S = 1.09 Δρmin = −0.94 e Å3
678 reflections Extinction correction: SHELXL2018 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
25 parameters Extinction coefficient: 0.0022 (6)

Caesium potassium gadolinium bis(vanadate) (II). Special details

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.

Caesium potassium gadolinium bis(vanadate) (II). Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Cs1 0.000000 0.000000 0.500000 0.02453 (5)
Gd1 0.000000 0.000000 0.000000 0.00899 (4)
K1 0.333333 0.666667 0.7877 (3) 0.0113 (5) 0.7404 (18)
Cs2 0.333333 0.666667 0.7867 (4) 0.0230 (8) 0.2597 (18)
V1 0.333333 0.666667 0.23977 (4) 0.00899 (5)
O1 0.17704 (10) 0.82296 (10) 0.16910 (16) 0.0265 (2)
O2 0.333333 0.666667 0.4470 (3) 0.0317 (5)

Caesium potassium gadolinium bis(vanadate) (II). Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cs1 0.02979 (7) 0.02979 (7) 0.01402 (8) 0.01489 (3) 0.000 0.000
Gd1 0.00627 (4) 0.00627 (4) 0.01444 (6) 0.00313 (2) 0.000 0.000
K1 0.0091 (6) 0.0091 (6) 0.0156 (9) 0.0046 (3) 0.000 0.000
Cs2 0.0200 (9) 0.0200 (9) 0.0288 (14) 0.0100 (5) 0.000 0.000
V1 0.00756 (7) 0.00756 (7) 0.01186 (11) 0.00378 (3) 0.000 0.000
O1 0.0244 (4) 0.0244 (4) 0.0379 (6) 0.0177 (4) −0.00613 (19) 0.00613 (19)
O2 0.0404 (7) 0.0404 (7) 0.0144 (7) 0.0202 (4) 0.000 0.000

Caesium potassium gadolinium bis(vanadate) (II). Geometric parameters (Å, º)

Cs1—O1i 3.2245 (13) K1—O1xvii 3.0377 (4)
Cs1—O1ii 3.2245 (13) K1—O1xviii 3.0377 (4)
Cs1—O1iii 3.2245 (13) K1—O1iii 3.0377 (4)
Cs1—O1iv 3.2245 (13) K1—O1xix 3.0377 (4)
Cs1—O1v 3.2245 (13) K1—O1i 3.0377 (4)
Cs1—O1vi 3.2245 (13) K1—V1vii 3.4895 (2)
Cs1—O2vii 3.5082 (3) K1—V1iii 3.4895 (2)
Cs1—O2viii 3.5082 (3) K1—V1xviii 3.4895 (2)
Cs1—O2ix 3.5082 (3) K1—V1xx 3.609 (3)
Cs1—O2 3.5083 (3) Cs2—O2 2.712 (4)
Cs1—O2iii 3.5083 (3) Cs2—O1xvi 3.0386 (4)
Cs1—O2iv 3.5083 (2) Cs2—O1xvii 3.0386 (4)
Gd1—O1x 2.2898 (10) Cs2—O1xviii 3.0386 (4)
Gd1—O1vi 2.2898 (10) Cs2—O1iii 3.0386 (4)
Gd1—O1xi 2.2898 (10) Cs2—O1xix 3.0386 (4)
Gd1—O1iv 2.2898 (10) Cs2—O1i 3.0386 (4)
Gd1—O1xii 2.2898 (10) Cs2—O1xx 3.462 (3)
Gd1—O1ii 2.2898 (10) Cs2—O1xxi 3.462 (3)
Gd1—K1xiii 3.8732 (12) Cs2—O1xxii 3.462 (3)
Gd1—K1vii 3.8732 (12) Cs2—V1vii 3.4890 (2)
Gd1—K1xiv 3.8731 (12) Cs2—V1iii 3.4890 (2)
Gd1—K1ix 3.8731 (12) V1—O2 1.654 (2)
Gd1—K1xv 3.8732 (12) V1—O1 1.7276 (10)
Gd1—K1iii 3.8732 (12) V1—O1vi 1.7276 (10)
K1—O2 2.719 (3) V1—O1xxiii 1.7276 (10)
K1—O1xvi 3.0377 (4)
O1i—Cs1—O1ii 180.0 O1xvi—K1—V1xx 83.48 (6)
O1i—Cs1—O1iii 59.57 (3) O1xvii—K1—V1xx 83.48 (6)
O1ii—Cs1—O1iii 120.43 (3) O1xviii—K1—V1xx 83.48 (6)
O1i—Cs1—O1iv 120.43 (3) O1iii—K1—V1xx 83.48 (6)
O1ii—Cs1—O1iv 59.57 (3) O1xix—K1—V1xx 83.48 (6)
O1iii—Cs1—O1iv 180.0 O1i—K1—V1xx 83.48 (6)
O1i—Cs1—O1v 59.57 (3) V1vii—K1—V1xx 93.60 (4)
O1ii—Cs1—O1v 120.43 (3) V1iii—K1—V1xx 93.60 (4)
O1iii—Cs1—O1v 59.57 (3) V1xviii—K1—V1xx 93.60 (4)
O1iv—Cs1—O1v 120.43 (3) O2—K1—Gd1xxiv 115.95 (4)
O1i—Cs1—O1vi 120.43 (3) O1xvi—K1—Gd1xxiv 36.21 (2)
O1ii—Cs1—O1vi 59.57 (3) O1xvii—K1—Gd1xxiv 36.21 (2)
O1iii—Cs1—O1vi 120.43 (3) O1xviii—K1—Gd1xxiv 85.31 (3)
O1iv—Cs1—O1vi 59.57 (3) O1iii—K1—Gd1xxiv 85.31 (3)
O1v—Cs1—O1vi 180.0 O1xix—K1—Gd1xxiv 137.69 (7)
O1i—Cs1—O2vii 48.07 (4) O1i—K1—Gd1xxiv 137.69 (7)
O1ii—Cs1—O2vii 131.93 (4) V1vii—K1—Gd1xxiv 157.65 (8)
O1iii—Cs1—O2vii 100.71 (3) V1iii—K1—Gd1xxiv 65.087 (12)
O1iv—Cs1—O2vii 79.29 (3) V1xviii—K1—Gd1xxiv 65.087 (12)
O1v—Cs1—O2vii 100.71 (3) V1xx—K1—Gd1xxiv 64.05 (4)
O1vi—Cs1—O2vii 79.29 (3) O2—Cs2—O1xvi 96.67 (7)
O1i—Cs1—O2viii 131.93 (4) O2—Cs2—O1xvii 96.67 (7)
O1ii—Cs1—O2viii 48.07 (4) O1xvi—Cs2—O1xvii 63.63 (4)
O1iii—Cs1—O2viii 79.29 (3) O2—Cs2—O1xviii 96.67 (7)
O1iv—Cs1—O2viii 100.71 (3) O1xvi—Cs2—O1xviii 55.47 (4)
O1v—Cs1—O2viii 79.29 (3) O1xvii—Cs2—O1xviii 118.67 (3)
O1vi—Cs1—O2viii 100.71 (3) O2—Cs2—O1iii 96.67 (7)
O2vii—Cs1—O2viii 180.0 O1xvi—Cs2—O1iii 118.67 (3)
O1i—Cs1—O2ix 100.71 (3) O1xvii—Cs2—O1iii 55.47 (4)
O1ii—Cs1—O2ix 79.29 (3) O1xviii—Cs2—O1iii 166.04 (13)
O1iii—Cs1—O2ix 100.71 (3) O2—Cs2—O1xix 96.67 (7)
O1iv—Cs1—O2ix 79.29 (3) O1xvi—Cs2—O1xix 118.67 (3)
O1v—Cs1—O2ix 48.07 (4) O1xvii—Cs2—O1xix 166.04 (13)
O1vi—Cs1—O2ix 131.93 (4) O1xviii—Cs2—O1xix 63.63 (4)
O2vii—Cs1—O2ix 118.567 (13) O1iii—Cs2—O1xix 118.67 (3)
O2viii—Cs1—O2ix 61.433 (14) O2—Cs2—O1i 96.67 (7)
O1i—Cs1—O2 79.29 (3) O1xvi—Cs2—O1i 166.04 (13)
O1ii—Cs1—O2 100.71 (3) O1xvii—Cs2—O1i 118.67 (3)
O1iii—Cs1—O2 79.29 (3) O1xviii—Cs2—O1i 118.67 (3)
O1iv—Cs1—O2 100.71 (3) O1iii—Cs2—O1i 63.63 (4)
O1v—Cs1—O2 131.93 (4) O1xix—Cs2—O1i 55.47 (4)
O1vi—Cs1—O2 48.07 (4) O2—Cs2—O1xx 151.86 (3)
O2vii—Cs1—O2 61.434 (13) O1xvi—Cs2—O1xx 60.03 (5)
O2viii—Cs1—O2 118.566 (13) O1xvii—Cs2—O1xx 60.03 (5)
O2ix—Cs1—O2 180.0 O1xviii—Cs2—O1xx 83.15 (6)
O1i—Cs1—O2iii 100.71 (3) O1iii—Cs2—O1xx 83.15 (6)
O1ii—Cs1—O2iii 79.29 (3) O1xix—Cs2—O1xx 108.15 (8)
O1iii—Cs1—O2iii 48.07 (4) O1i—Cs2—O1xx 108.15 (8)
O1iv—Cs1—O2iii 131.93 (4) O2—Cs2—O1xxi 151.86 (3)
O1v—Cs1—O2iii 100.71 (3) O1xvi—Cs2—O1xxi 83.15 (6)
O1vi—Cs1—O2iii 79.29 (3) O1xvii—Cs2—O1xxi 108.15 (8)
O2vii—Cs1—O2iii 118.565 (14) O1xviii—Cs2—O1xxi 60.03 (5)
O2viii—Cs1—O2iii 61.435 (13) O1iii—Cs2—O1xxi 108.15 (8)
O2ix—Cs1—O2iii 118.565 (14) O1xix—Cs2—O1xxi 60.03 (5)
O2—Cs1—O2iii 61.434 (13) O1i—Cs2—O1xxi 83.15 (6)
O1i—Cs1—O2iv 79.29 (3) O1xx—Cs2—O1xxi 48.22 (5)
O1ii—Cs1—O2iv 100.71 (3) O2—Cs2—O1xxii 151.86 (3)
O1iii—Cs1—O2iv 131.93 (4) O1xvi—Cs2—O1xxii 108.15 (8)
O1iv—Cs1—O2iv 48.07 (4) O1xvii—Cs2—O1xxii 83.15 (6)
O1v—Cs1—O2iv 79.29 (3) O1xviii—Cs2—O1xxii 108.15 (8)
O1vi—Cs1—O2iv 100.71 (3) O1iii—Cs2—O1xxii 60.03 (5)
O2vii—Cs1—O2iv 61.435 (13) O1xix—Cs2—O1xxii 83.15 (6)
O2viii—Cs1—O2iv 118.565 (14) O1i—Cs2—O1xxii 60.03 (5)
O2ix—Cs1—O2iv 61.435 (13) O1xx—Cs2—O1xxii 48.22 (5)
O2—Cs1—O2iv 118.566 (14) O1xxi—Cs2—O1xxii 48.22 (5)
O2iii—Cs1—O2iv 180.0 O2—Cs2—V1vii 86.53 (5)
O1x—Gd1—O1vi 180.00 (5) O1xvi—Cs2—V1vii 147.92 (2)
O1x—Gd1—O1xi 88.78 (5) O1xvii—Cs2—V1vii 147.92 (2)
O1vi—Gd1—O1xi 91.22 (5) O1xviii—Cs2—V1vii 92.44 (2)
O1x—Gd1—O1iv 91.22 (5) O1iii—Cs2—V1vii 92.44 (2)
O1vi—Gd1—O1iv 88.78 (5) O1xix—Cs2—V1vii 29.680 (19)
O1xi—Gd1—O1iv 180.00 (6) O1i—Cs2—V1vii 29.680 (19)
O1x—Gd1—O1xii 88.78 (5) O1xx—Cs2—V1vii 121.61 (8)
O1vi—Gd1—O1xii 91.22 (5) O1xxi—Cs2—V1vii 79.51 (4)
O1xi—Gd1—O1xii 88.78 (5) O1xxii—Cs2—V1vii 79.51 (4)
O1iv—Gd1—O1xii 91.22 (5) O2—Cs2—V1iii 86.53 (5)
O1x—Gd1—O1ii 91.22 (5) O1xvi—Cs2—V1iii 92.44 (2)
O1vi—Gd1—O1ii 88.78 (5) O1xvii—Cs2—V1iii 29.680 (19)
O1xi—Gd1—O1ii 91.22 (5) O1xviii—Cs2—V1iii 147.91 (2)
O1iv—Gd1—O1ii 88.78 (5) O1iii—Cs2—V1iii 29.681 (19)
O1xii—Gd1—O1ii 180.00 (6) O1xix—Cs2—V1iii 147.92 (2)
O1x—Gd1—K1xiii 51.601 (16) O1i—Cs2—V1iii 92.44 (2)
O1vi—Gd1—K1xiii 128.399 (17) O1xx—Cs2—V1iii 79.51 (4)
O1xi—Gd1—K1xiii 51.602 (16) O1xxi—Cs2—V1iii 121.61 (8)
O1iv—Gd1—K1xiii 128.398 (16) O1xxii—Cs2—V1iii 79.51 (4)
O1xii—Gd1—K1xiii 117.93 (5) V1vii—Cs2—V1iii 119.638 (11)
O1ii—Gd1—K1xiii 62.07 (5) O2—V1—O1 109.06 (5)
O1x—Gd1—K1vii 128.399 (17) O2—V1—O1vi 109.06 (5)
O1vi—Gd1—K1vii 51.601 (16) O1—V1—O1vi 109.88 (5)
O1xi—Gd1—K1vii 128.398 (16) O2—V1—O1xxiii 109.06 (5)
O1iv—Gd1—K1vii 51.602 (16) O1—V1—O1xxiii 109.88 (5)
O1xii—Gd1—K1vii 62.07 (5) O1vi—V1—O1xxiii 109.88 (5)
O1ii—Gd1—K1vii 117.93 (5) O2—V1—K1vii 93.60 (4)
K1xiii—Gd1—K1vii 180.0 O1—V1—K1vii 157.34 (6)
O1x—Gd1—K1xiv 117.93 (5) O1vi—V1—K1vii 60.518 (16)
O1vi—Gd1—K1xiv 62.07 (5) O1xxiii—V1—K1vii 60.518 (16)
O1xi—Gd1—K1xiv 51.602 (16) O2—V1—K1iii 93.60 (4)
O1iv—Gd1—K1xiv 128.398 (16) O1—V1—K1iii 60.517 (16)
O1xii—Gd1—K1xiv 51.602 (16) O1vi—V1—K1iii 60.518 (16)
O1ii—Gd1—K1xiv 128.398 (16) O1xxiii—V1—K1iii 157.34 (6)
K1xiii—Gd1—K1xiv 102.28 (4) K1vii—V1—K1iii 119.610 (10)
K1vii—Gd1—K1xiv 77.72 (4) O2—V1—K1xviii 93.60 (4)
O1x—Gd1—K1ix 62.07 (5) O1—V1—K1xviii 60.517 (16)
O1vi—Gd1—K1ix 117.93 (5) O1vi—V1—K1xviii 157.34 (6)
O1xi—Gd1—K1ix 128.398 (16) O1xxiii—V1—K1xviii 60.518 (16)
O1iv—Gd1—K1ix 51.602 (16) K1vii—V1—K1xviii 119.610 (10)
O1xii—Gd1—K1ix 128.398 (16) K1iii—V1—K1xviii 119.609 (10)
O1ii—Gd1—K1ix 51.602 (16) O2—V1—K1xiv 180.0
K1xiii—Gd1—K1ix 77.72 (4) O1—V1—K1xiv 70.94 (5)
K1vii—Gd1—K1ix 102.28 (4) O1vi—V1—K1xiv 70.94 (5)
K1xiv—Gd1—K1ix 180.0 O1xxiii—V1—K1xiv 70.94 (5)
O1x—Gd1—K1xv 51.602 (16) K1vii—V1—K1xiv 86.40 (4)
O1vi—Gd1—K1xv 128.398 (16) K1iii—V1—K1xiv 86.40 (4)
O1xi—Gd1—K1xv 117.93 (5) K1xviii—V1—K1xiv 86.40 (4)
O1iv—Gd1—K1xv 62.07 (5) O2—V1—Cs1xxv 59.187 (4)
O1xii—Gd1—K1xv 51.602 (16) O1—V1—Cs1xxv 49.87 (5)
O1ii—Gd1—K1xv 128.398 (16) O1vi—V1—Cs1xxv 124.970 (19)
K1xiii—Gd1—K1xv 102.28 (4) O1xxiii—V1—Cs1xxv 124.970 (19)
K1vii—Gd1—K1xv 77.72 (4) K1vii—V1—Cs1xxv 152.79 (5)
K1xiv—Gd1—K1xv 102.28 (4) K1iii—V1—Cs1xxv 66.64 (3)
K1ix—Gd1—K1xv 77.72 (4) K1xviii—V1—Cs1xxv 66.64 (3)
O1x—Gd1—K1iii 128.398 (16) K1xiv—V1—Cs1xxv 120.814 (4)
O1vi—Gd1—K1iii 51.602 (16) O2—V1—Cs1xxvi 59.187 (4)
O1xi—Gd1—K1iii 62.07 (5) O1—V1—Cs1xxvi 124.969 (19)
O1iv—Gd1—K1iii 117.93 (5) O1vi—V1—Cs1xxvi 124.970 (19)
O1xii—Gd1—K1iii 128.398 (16) O1xxiii—V1—Cs1xxvi 49.87 (5)
O1ii—Gd1—K1iii 51.602 (16) K1vii—V1—Cs1xxvi 66.65 (3)
K1xiii—Gd1—K1iii 77.72 (4) K1iii—V1—Cs1xxvi 152.78 (5)
K1vii—Gd1—K1iii 102.28 (4) K1xviii—V1—Cs1xxvi 66.65 (3)
K1xiv—Gd1—K1iii 77.72 (4) K1xiv—V1—Cs1xxvi 120.813 (4)
K1ix—Gd1—K1iii 102.28 (4) Cs1xxv—V1—Cs1xxvi 96.109 (5)
K1xv—Gd1—K1iii 180.0 O2—V1—Cs1 59.187 (4)
O2—K1—O1xvi 96.52 (6) O1—V1—Cs1 124.969 (19)
O2—K1—O1xvii 96.52 (6) O1vi—V1—Cs1 49.87 (5)
O1xvi—K1—O1xvii 63.65 (4) O1xxiii—V1—Cs1 124.970 (19)
O2—K1—O1xviii 96.52 (6) K1vii—V1—Cs1 66.65 (3)
O1xvi—K1—O1xviii 55.49 (4) K1iii—V1—Cs1 66.65 (3)
O1xvii—K1—O1xviii 118.73 (2) K1xviii—V1—Cs1 152.78 (5)
O2—K1—O1iii 96.52 (6) K1xiv—V1—Cs1 120.813 (4)
O1xvi—K1—O1iii 118.73 (2) Cs1xxv—V1—Cs1 96.109 (5)
O1xvii—K1—O1iii 55.49 (4) Cs1xxvi—V1—Cs1 96.109 (5)
O1xviii—K1—O1iii 166.32 (11) O2—V1—Cs2 0.0
O2—K1—O1xix 96.52 (6) O1—V1—Cs2 109.06 (5)
O1xvi—K1—O1xix 118.73 (2) O1vi—V1—Cs2 109.06 (5)
O1xvii—K1—O1xix 166.32 (11) O1xxiii—V1—Cs2 109.06 (5)
O1xviii—K1—O1xix 63.65 (4) K1vii—V1—Cs2 93.60 (4)
O1iii—K1—O1xix 118.73 (2) K1iii—V1—Cs2 93.60 (4)
O2—K1—O1i 96.52 (6) K1xviii—V1—Cs2 93.60 (4)
O1xvi—K1—O1i 166.32 (11) K1xiv—V1—Cs2 180.0
O1xvii—K1—O1i 118.73 (2) Cs1xxv—V1—Cs2 59.187 (4)
O1xviii—K1—O1i 118.73 (2) Cs1xxvi—V1—Cs2 59.187 (4)
O1iii—K1—O1i 63.65 (4) Cs1—V1—Cs2 59.187 (4)
O1xix—K1—O1i 55.49 (4) V1—O1—Gd1xxv 162.94 (8)
O2—K1—V1vii 86.40 (4) V1—O1—K1xviii 89.81 (3)
O1xvi—K1—V1vii 147.94 (2) Gd1xxv—O1—K1xviii 92.19 (4)
O1xvii—K1—V1vii 147.94 (2) V1—O1—K1iii 89.81 (3)
O1xviii—K1—V1vii 92.45 (2) Gd1xxv—O1—K1iii 92.19 (4)
O1iii—K1—V1vii 92.45 (2) K1xviii—O1—K1iii 166.32 (11)
O1xix—K1—V1vii 29.676 (19) V1—O1—Cs1xxv 105.95 (5)
O1i—K1—V1vii 29.676 (19) Gd1xxv—O1—Cs1xxv 91.12 (4)
O2—K1—V1iii 86.40 (4) K1xviii—O1—Cs1xxv 83.48 (5)
O1xvi—K1—V1iii 92.45 (2) K1iii—O1—Cs1xxv 83.48 (5)
O1xvii—K1—V1iii 29.675 (19) V1—O2—Cs2 180.0
O1xviii—K1—V1iii 147.94 (2) V1—O2—K1 180.0
O1iii—K1—V1iii 29.676 (19) Cs2—O2—K1 0.0
O1xix—K1—V1iii 147.94 (2) V1—O2—Cs1xxv 96.93 (3)
O1i—K1—V1iii 92.45 (2) Cs2—O2—Cs1xxv 83.07 (3)
V1vii—K1—V1iii 119.610 (10) K1—O2—Cs1xxv 83.07 (3)
O2—K1—V1xviii 86.40 (4) V1—O2—Cs1xxvi 96.93 (3)
O1xvi—K1—V1xviii 29.675 (19) Cs2—O2—Cs1xxvi 83.07 (3)
O1xvii—K1—V1xviii 92.45 (2) K1—O2—Cs1xxvi 83.07 (3)
O1xviii—K1—V1xviii 29.676 (19) Cs1xxv—O2—Cs1xxvi 118.566 (13)
O1iii—K1—V1xviii 147.94 (2) V1—O2—Cs1 96.93 (3)
O1xix—K1—V1xviii 92.45 (2) Cs2—O2—Cs1 83.07 (3)
O1i—K1—V1xviii 147.94 (2) K1—O2—Cs1 83.07 (3)
V1vii—K1—V1xviii 119.610 (10) Cs1xxv—O2—Cs1 118.566 (13)
V1iii—K1—V1xviii 119.609 (10) Cs1xxvi—O2—Cs1 118.566 (13)
O2—K1—V1xx 180.0

Symmetry codes: (i) xy+1, x, −z+1; (ii) −x+y−1, −x, z; (iii) −x, −y+1, −z+1; (iv) x, y−1, z; (v) y−1, −x+y−1, −z+1; (vi) −y+1, xy+1, z; (vii) −x+1, −y+1, −z+1; (viii) x−1, y−1, z; (ix) −x, −y, −z+1; (x) y−1, −x+y−1, −z; (xi) −x, −y+1, −z; (xii) xy+1, x, −z; (xiii) x−1, y−1, z−1; (xiv) x, y, z−1; (xv) x, y−1, z−1; (xvi) xy+1, x+1, −z+1; (xvii) y−1, −x+y, −z+1; (xviii) −x+1, −y+2, −z+1; (xix) y, −x+y, −z+1; (xx) x, y, z+1; (xxi) −x+y, −x+1, z+1; (xxii) −y+1, xy+1, z+1; (xxiii) −x+y, −x+1, z; (xxiv) x, y+1, z+1; (xxv) x, y+1, z; (xxvi) x+1, y+1, z.

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, II, global. DOI: 10.1107/S2056989019008685/vn2149sup1.cif

e-75-01041-sup1.cif (823.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989019008685/vn2149Isup2.hkl

e-75-01041-Isup2.hkl (54.3KB, hkl)

Structure factors: contains datablock(s) II. DOI: 10.1107/S2056989019008685/vn2149IIsup3.hkl

e-75-01041-IIsup3.hkl (56.8KB, hkl)

CCDC references: 1934723, 1934722

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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