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A new caesium sodium samarium borate phosphate, CsNa2Sm2(BO3)(PO4)2, has been obtained successfully by the high-temperature solution growth (HTSG) method and single-crystal X-ray diffraction analysis reveals that it crystallizes in the ortho­rhom­bic space group Cmcm. The structure contains BO3, PO4, NaO7 and SmO7 polyhedra which are inter­connected via corner- or edge-sharing O atoms to form a three-dimensional [Na2Sm2(BO3)(PO4)2] network. This network delimits large cavities where large Cs+ cations reside to form the total structure. Under 402 nm light excitation, CsNa2Sm2(BO3)(PO4)2 exhibits three emission bands due to the 4f→4f transitions of Sm3+. Furthermore, we introduced Gd3+ into Sm3+ sites to optimize the Sm3+ concentration and improve the luminescence intensity. The optimal concentration is Gd/Sm = 98/2. The luminescent lifetime of a series of CsNa2Gd2(1–x)Sm2x(BO3)(PO4)2 phosphors shows a gradual degradation of lifetime from 2.196 to 0.872 ms for x = 0.01–0.10. The Commission Internationale de l'Eclairage (CIE) 1931 calculation reveals that CsNa2Gd1.96Sm0.04(BO3)(PO4)2 can emit orange light under 402 nm excitation.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620014576/ky3201sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620014576/ky3201Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229620014576/ky3201sup3.pdf
Additional geometry

CCDC reference: 2031718

Computing details top

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).

Caesium disodium disamarium borate bis(phosphate) top
Crystal data top
CsNa2Sm2(BO3)(PO4)2Dx = 4.177 Mg m3
Mr = 728.34Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, CmcmCell parameters from 1320 reflections
a = 7.0631 (6) Åθ = 2.3–24.4°
b = 15.2881 (15) ŵ = 13.54 mm1
c = 10.725 (1) ÅT = 296 K
V = 1158.10 (19) Å3Block, colorless
Z = 40.15 × 0.15 × 0.10 mm
F(000) = 1296
Data collection top
Bruker SMART APEXII CCD area detector
diffractometer
812 independent reflections
Radiation source: fine-focus sealed tube727 reflections with I > 2σ(I)
Detector resolution: 83.33 pixels mm-1Rint = 0.037
ω scansθmax = 28.3°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Bruker, 2017)
h = 94
Tmin = 0.158, Tmax = 0.590k = 1919
3854 measured reflectionsl = 1414
Refinement top
Refinement on F20 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) = 0.048Δρmax = 1.09 e Å3
S = 1.05Δρmin = 1.54 e Å3
812 reflectionsExtinction correction: SHELXL2018 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
59 parametersExtinction coefficient: 0.00072 (6)
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cs10.5000000.48636 (5)0.7500000.0370 (2)
Na10.7563 (3)0.74620 (18)0.7500000.0248 (6)
Sm11.0000000.61983 (2)0.52841 (3)0.00667 (11)
B11.0000000.5156 (7)0.7500000.0109 (19)
P10.5000000.68276 (10)0.52246 (13)0.0083 (3)
O11.0000000.4772 (3)0.6361 (4)0.0167 (10)
O21.0000000.6087 (4)0.7500000.0183 (14)
O30.5000000.7613 (3)0.6133 (4)0.0127 (9)
O40.5000000.7240 (3)0.3918 (4)0.0141 (9)
O50.6758 (4)0.62691 (19)0.5449 (3)0.0196 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cs10.0384 (4)0.0263 (4)0.0463 (5)0.0000.0000.000
Na10.0134 (13)0.0473 (19)0.0138 (13)0.0010 (12)0.0000.000
Sm10.00608 (16)0.00696 (17)0.00696 (17)0.0000.0000.00011 (11)
B10.008 (4)0.023 (5)0.002 (4)0.0000.0000.000
P10.0050 (7)0.0097 (7)0.0101 (7)0.0000.0000.0016 (6)
O10.031 (3)0.007 (2)0.012 (2)0.0000.0000.0042 (17)
O20.038 (4)0.009 (3)0.008 (3)0.0000.0000.000
O30.015 (2)0.013 (2)0.010 (2)0.0000.0000.0034 (17)
O40.017 (2)0.017 (2)0.008 (2)0.0000.0000.0008 (17)
O50.0075 (15)0.0171 (17)0.034 (2)0.0028 (11)0.0006 (14)0.0071 (14)
Geometric parameters (Å, º) top
Cs1—O5i3.316 (3)Na1—O5i2.913 (4)
Cs1—O5ii3.316 (3)Sm1—O5x2.299 (3)
Cs1—O5iii3.316 (3)Sm1—O52.299 (3)
Cs1—O53.316 (3)Sm1—O1xi2.305 (4)
Cs1—O4iv3.557 (4)Sm1—O3ix2.369 (4)
Cs1—O4v3.557 (4)Sm1—O22.3826 (5)
Cs1—O13.7393 (14)Sm1—O12.468 (4)
Cs1—O1vi3.7393 (14)Sm1—O4ix2.537 (4)
Cs1—O1i3.7393 (14)B1—O11.355 (6)
Cs1—O1vii3.7393 (14)B1—O1i1.355 (6)
Na1—O3i2.341 (3)B1—O21.423 (11)
Na1—O32.341 (3)P1—O51.526 (3)
Na1—O4viii2.342 (3)P1—O5iii1.526 (3)
Na1—O4ix2.342 (3)P1—O41.537 (4)
Na1—O22.717 (5)P1—O31.546 (4)
Na1—O52.913 (4)
O1—B1—O1i128.6 (9)O5iii—P1—O4111.92 (16)
O1—B1—O2115.7 (4)O5—P1—O3109.57 (16)
O1i—B1—O2115.7 (4)O5iii—P1—O3109.57 (16)
O5—P1—O5iii108.9 (2)O4—P1—O3104.8 (2)
O5—P1—O4111.92 (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) x1, y, z; (vii) x1, 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.
 

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