Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620014576/ky3201sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S2053229620014576/ky3201Isup2.hkl | |
Portable Document Format (PDF) file https://doi.org/10.1107/S2053229620014576/ky3201sup3.pdf |
CCDC reference: 2031718
Data collection: APEX2 (Bruker, 2017); cell refinement: SAINT (Bruker, 2017); data reduction: SAINT (Bruker, 2017); program(s) used to solve structure: SHELXS (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015b); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2020).
CsNa2Sm2(BO3)(PO4)2 | Dx = 4.177 Mg m−3 |
Mr = 728.34 | Mo Kα radiation, λ = 0.71073 Å |
Orthorhombic, Cmcm | Cell parameters from 1320 reflections |
a = 7.0631 (6) Å | θ = 2.3–24.4° |
b = 15.2881 (15) Å | µ = 13.54 mm−1 |
c = 10.725 (1) Å | T = 296 K |
V = 1158.10 (19) Å3 | Block, colorless |
Z = 4 | 0.15 × 0.15 × 0.10 mm |
F(000) = 1296 |
Bruker SMART APEXII CCD area detector diffractometer | 812 independent reflections |
Radiation source: fine-focus sealed tube | 727 reflections with I > 2σ(I) |
Detector resolution: 83.33 pixels mm-1 | Rint = 0.037 |
ω scans | θmax = 28.3°, θmin = 2.7° |
Absorption correction: multi-scan (SADABS; Bruker, 2017) | h = −9→4 |
Tmin = 0.158, Tmax = 0.590 | k = −19→19 |
3854 measured reflections | l = −14→14 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.0233P)2 + 0.2713P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.022 | (Δ/σ)max = 0.001 |
wR(F2) = 0.048 | Δρmax = 1.09 e Å−3 |
S = 1.05 | Δρmin = −1.54 e Å−3 |
812 reflections | Extinction correction: SHELXL2018 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
59 parameters | Extinction coefficient: 0.00072 (6) |
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. A suitable single crystal with dimensions of 0.15 × 0.15 × 0.05 mm was selected and mounted on a glass fiber for the single-crystal X-ray diffraction (SC-XRD) experiments. Data collection was performed using a Bruker Smart Apex2 CCD diffractometer with graphite-monochromated Mo-Ka (λ = 0.71073 Å) radiation at a temperature of 293 K. The data set was corrected for Lorentz and polarization factors and for absorption by applying the ω-scan technique (Bruker, 2017). The structure was solved by direct method and refined by full-matrix least-squares fitting on F2 by Shelx-2017 (Sheldrick, 2015). The observed intensities are consistent with an orthorhombic C-centered space group Cmcm. The final refined solution obtained was checked with the Addsym algorithm in the program PLATON (Spek, 2020), and no higher symmetry was found. Crystallographic data and structural refinement were summarized in Table 1. The atomic coordinates and thermal parameters are given as supporting information (Table S1, S2), and some important bond distances are summarized in Table S3. Further details of the crystal structure investigations can be obtained from the CCDC database on quoting the depository number of 2031718 |
x | y | z | Uiso*/Ueq | ||
Cs1 | 0.500000 | 0.48636 (5) | 0.750000 | 0.0370 (2) | |
Na1 | 0.7563 (3) | 0.74620 (18) | 0.750000 | 0.0248 (6) | |
Sm1 | 1.000000 | 0.61983 (2) | 0.52841 (3) | 0.00667 (11) | |
B1 | 1.000000 | 0.5156 (7) | 0.750000 | 0.0109 (19) | |
P1 | 0.500000 | 0.68276 (10) | 0.52246 (13) | 0.0083 (3) | |
O1 | 1.000000 | 0.4772 (3) | 0.6361 (4) | 0.0167 (10) | |
O2 | 1.000000 | 0.6087 (4) | 0.750000 | 0.0183 (14) | |
O3 | 0.500000 | 0.7613 (3) | 0.6133 (4) | 0.0127 (9) | |
O4 | 0.500000 | 0.7240 (3) | 0.3918 (4) | 0.0141 (9) | |
O5 | 0.6758 (4) | 0.62691 (19) | 0.5449 (3) | 0.0196 (7) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cs1 | 0.0384 (4) | 0.0263 (4) | 0.0463 (5) | 0.000 | 0.000 | 0.000 |
Na1 | 0.0134 (13) | 0.0473 (19) | 0.0138 (13) | −0.0010 (12) | 0.000 | 0.000 |
Sm1 | 0.00608 (16) | 0.00696 (17) | 0.00696 (17) | 0.000 | 0.000 | −0.00011 (11) |
B1 | 0.008 (4) | 0.023 (5) | 0.002 (4) | 0.000 | 0.000 | 0.000 |
P1 | 0.0050 (7) | 0.0097 (7) | 0.0101 (7) | 0.000 | 0.000 | 0.0016 (6) |
O1 | 0.031 (3) | 0.007 (2) | 0.012 (2) | 0.000 | 0.000 | −0.0042 (17) |
O2 | 0.038 (4) | 0.009 (3) | 0.008 (3) | 0.000 | 0.000 | 0.000 |
O3 | 0.015 (2) | 0.013 (2) | 0.010 (2) | 0.000 | 0.000 | −0.0034 (17) |
O4 | 0.017 (2) | 0.017 (2) | 0.008 (2) | 0.000 | 0.000 | −0.0008 (17) |
O5 | 0.0075 (15) | 0.0171 (17) | 0.034 (2) | 0.0028 (11) | −0.0006 (14) | 0.0071 (14) |
Cs1—O5i | 3.316 (3) | Na1—O5i | 2.913 (4) |
Cs1—O5ii | 3.316 (3) | Sm1—O5x | 2.299 (3) |
Cs1—O5iii | 3.316 (3) | Sm1—O5 | 2.299 (3) |
Cs1—O5 | 3.316 (3) | Sm1—O1xi | 2.305 (4) |
Cs1—O4iv | 3.557 (4) | Sm1—O3ix | 2.369 (4) |
Cs1—O4v | 3.557 (4) | Sm1—O2 | 2.3826 (5) |
Cs1—O1 | 3.7393 (14) | Sm1—O1 | 2.468 (4) |
Cs1—O1vi | 3.7393 (14) | Sm1—O4ix | 2.537 (4) |
Cs1—O1i | 3.7393 (14) | B1—O1 | 1.355 (6) |
Cs1—O1vii | 3.7393 (14) | B1—O1i | 1.355 (6) |
Na1—O3i | 2.341 (3) | B1—O2 | 1.423 (11) |
Na1—O3 | 2.341 (3) | P1—O5 | 1.526 (3) |
Na1—O4viii | 2.342 (3) | P1—O5iii | 1.526 (3) |
Na1—O4ix | 2.342 (3) | P1—O4 | 1.537 (4) |
Na1—O2 | 2.717 (5) | P1—O3 | 1.546 (4) |
Na1—O5 | 2.913 (4) | ||
O1—B1—O1i | 128.6 (9) | O5iii—P1—O4 | 111.92 (16) |
O1—B1—O2 | 115.7 (4) | O5—P1—O3 | 109.57 (16) |
O1i—B1—O2 | 115.7 (4) | O5iii—P1—O3 | 109.57 (16) |
O5—P1—O5iii | 108.9 (2) | O4—P1—O3 | 104.8 (2) |
O5—P1—O4 | 111.92 (16) |
Symmetry codes: (i) x, y, −z+3/2; (ii) −x+1, y, −z+3/2; (iii) −x+1, y, z; (iv) −x+1, −y+1, −z+1; (v) −x+1, −y+1, z+1/2; (vi) x−1, y, z; (vii) x−1, y, −z+3/2; (viii) −x+3/2, −y+3/2, z+1/2; (ix) −x+3/2, −y+3/2, −z+1; (x) −x+2, y, z; (xi) −x+2, −y+1, −z+1. |