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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Aug 6;64(Pt 9):m1106. doi: 10.1107/S1600536808023982

Poly[zinc(II)-[μ-1,4-bis­(imidazol-1-yl­methyl)benzene]-μ-4,4′-oxydibenzoato]

Chun-Hui Yu a,*
PMCID: PMC2960729  PMID: 21201572

Abstract

In the title compound, [Zn(C14H8O5)(C14H14N4)]n, the coordination polyhedron around each ZnII atom is a distorted tetra­hedron. The ligands bridge the Zn atoms to form a two-dimensional (4,4)-network.

Related literature

For related literature, see Batten & Robson (1998); Ma et al. (2003).graphic file with name e-64-m1106-scheme1.jpg

Experimental

Crystal data

  • [Zn(C14H8O5)(C14H14N4)]

  • M r = 559.87

  • Monoclinic, Inline graphic

  • a = 6.1608 (9) Å

  • b = 25.811 (4) Å

  • c = 16.185 (3) Å

  • β = 92.503 (2)°

  • V = 2571.2 (7) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.00 mm−1

  • T = 293 (2) K

  • 0.33 × 0.25 × 0.19 mm

Data collection

  • Bruker APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1998) T min = 0.718, T max = 0.826

  • 14194 measured reflections

  • 5057 independent reflections

  • 3906 reflections with I > 2σ(I)

  • R int = 0.047

Refinement

  • R[F 2 > 2σ(F 2)] = 0.061

  • wR(F 2) = 0.159

  • S = 1.07

  • 5057 reflections

  • 343 parameters

  • H-atom parameters constrained

  • Δρmax = 1.43 e Å−3

  • Δρmin = −0.31 e Å−3

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808023982/bt2755sup1.cif

e-64-m1106-sup1.cif (20.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023982/bt2755Isup2.hkl

e-64-m1106-Isup2.hkl (242.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Acknowledgments

The author thanks Beihua University for supporting this work.

supplementary crystallographic information

Comment

Metal–organic frameworks is currently of great interest because of their interesting structures and potential applications. As a good candidate for rigid rod-like spacers in the construction of metal–organic polymers, 4,4'-bipyridine has been relatively well known and has shown hundreds of interesting supramolecular architectures (Batten & Robson, 1998). However, the flexible ligands such as 1,4-bis(imidazol-1-ylmethyl)benzene (L) has not been well explored to date (Ma et al., 2003). In this work, I selected 4,4'-oxybis(benzoic acid) (H2oba) and L as linkers, generating a new coordination polymer, [Zn(oba)(L)], (I), which is reported here.

In compound (I) each ZnII atom is four-coordinated by two N atoms from one L ligand, and two O atoms from two oba carboxylate anions in a distorted tetrahedral coordination sphere (Fig. 1). The two neighbouring ZnII atoms are bridged by the oba and L ligands to form a two-dimensional (4,4) network (Fig. 2).

Experimental

A mixture of H2oba (0.5 mmol), L (0.5 mmol), NaOH (1 mmol) and ZnCl2.6H2O (0.5 mmol) was suspended in 12 ml of deionized water and sealed in a 20 ml Teflon-lined autoclave. Upon heating at 170°C for one week, the autoclave was slowly cooled to room temperature. The crystals were collected, washed with deionized water and dried.

Refinement

H atoms were generated geometrically and refined as riding atoms with C—H = 0.93 Å and Uiso(H) = 1.2 times Ueq(C).

Figures

Fig. 1.

Fig. 1.

The structure of (I), showing the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. Symmetry codes: (i) -1 - x, 1/2 + y, 1/2 - z; (ii) x, 1/2 - y, 1/2 + z.

Fig. 2.

Fig. 2.

View of the chain structure of (I).

Crystal data

[Zn(C14H8O5)(C14H14N4)] F000 = 1152
Mr = 559.87 Dx = 1.446 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 5057 reflections
a = 6.1608 (9) Å θ = 1.9–26.1º
b = 25.811 (4) Å µ = 1.00 mm1
c = 16.185 (3) Å T = 293 (2) K
β = 92.503 (2)º Block, colourless
V = 2571.2 (7) Å3 0.33 × 0.25 × 0.19 mm
Z = 4

Data collection

Bruker APEX CCD area-detector diffractometer 5057 independent reflections
Radiation source: fine-focus sealed tube 3906 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.047
T = 293(2) K θmax = 26.1º
φ and ω scans θmin = 1.5º
Absorption correction: multi-scan(SADABS; Bruker, 1998) h = −7→6
Tmin = 0.718, Tmax = 0.826 k = −31→27
14194 measured reflections l = −19→19

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.061 H-atom parameters constrained
wR(F2) = 0.159   w = 1/[σ2(Fo2) + (0.0761P)2 + 2.2361P] where P = (Fo2 + 2Fc2)/3
S = 1.07 (Δ/σ)max < 0.001
5057 reflections Δρmax = 1.43 e Å3
343 parameters Δρmin = −0.31 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

Special details

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.
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 > σ(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
C1 0.1661 (7) 0.04984 (15) 0.0495 (3) 0.0273 (9)
H1 0.0525 0.0275 0.0603 0.033*
C2 0.3029 (7) 0.04487 (16) −0.0136 (3) 0.0284 (9)
H2 0.3004 0.0190 −0.0537 0.034*
C3 0.3919 (7) 0.11368 (15) 0.0599 (3) 0.0281 (9)
H3 0.4643 0.1434 0.0784 0.034*
C4 0.6352 (8) 0.09401 (17) −0.0563 (3) 0.0384 (11)
H4A 0.6121 0.0764 −0.1089 0.046*
H4B 0.7623 0.0789 −0.0283 0.046*
C5 0.6768 (7) 0.15040 (16) −0.0719 (3) 0.0312 (10)
C6 0.5194 (8) 0.18139 (19) −0.1091 (3) 0.0416 (12)
H6 0.3861 0.1668 −0.1251 0.050*
C7 0.5531 (8) 0.23363 (19) −0.1233 (3) 0.0440 (12)
H7 0.4425 0.2537 −0.1476 0.053*
C8 0.7516 (7) 0.25584 (16) −0.1014 (3) 0.0274 (9)
C9 0.9128 (7) 0.22467 (18) −0.0648 (3) 0.0355 (11)
H9 1.0479 0.2388 −0.0502 0.043*
C10 0.8738 (8) 0.17265 (18) −0.0500 (3) 0.0379 (11)
H10 0.9828 0.1524 −0.0249 0.045*
C11 0.8036 (7) 0.31222 (17) −0.1168 (3) 0.0333 (10)
H11A 0.8759 0.3266 −0.0675 0.040*
H11B 0.9032 0.3145 −0.1614 0.040*
C12 0.4828 (8) 0.36811 (18) −0.0836 (3) 0.0393 (12)
H12 0.5095 0.3720 −0.0269 0.047*
C13 0.3094 (8) 0.38615 (17) −0.1294 (3) 0.0349 (11)
H13 0.1968 0.4057 −0.1091 0.042*
C14 0.5102 (7) 0.34527 (16) −0.2128 (3) 0.0272 (9)
H14 0.5639 0.3306 −0.2603 0.033*
C15 −0.2311 (7) 0.04825 (15) 0.2220 (3) 0.0269 (9)
C16 −0.3735 (7) 0.01450 (15) 0.2723 (3) 0.0272 (9)
C17 −0.5687 (7) −0.00464 (16) 0.2373 (3) 0.0312 (10)
H17 −0.6076 0.0032 0.1826 0.037*
C18 −0.7053 (7) −0.03508 (17) 0.2825 (3) 0.0332 (10)
H18 −0.8353 −0.0475 0.2587 0.040*
C19 −0.6446 (7) −0.04668 (15) 0.3635 (3) 0.0301 (10)
C20 −0.4550 (8) −0.02835 (16) 0.4000 (3) 0.0322 (10)
H20 −0.4174 −0.0366 0.4547 0.039*
C21 −0.3190 (7) 0.00262 (16) 0.3547 (3) 0.0305 (10)
H21 −0.1910 0.0155 0.3795 0.037*
C22 −0.8501 (7) −0.12400 (15) 0.3885 (3) 0.0291 (9)
C23 −0.7128 (7) −0.15793 (17) 0.3502 (3) 0.0370 (11)
H23 −0.5768 −0.1471 0.3344 0.044*
C24 −0.7814 (7) −0.20848 (16) 0.3356 (3) 0.0350 (11)
H24 −0.6888 −0.2318 0.3111 0.042*
C25 −0.9857 (7) −0.22472 (15) 0.3571 (3) 0.0268 (9)
C26 −1.0669 (7) −0.27912 (16) 0.3427 (3) 0.0294 (10)
C27 −1.1208 (7) −0.18936 (16) 0.3946 (3) 0.0333 (10)
H27 −1.2587 −0.1997 0.4090 0.040*
C28 −1.0534 (7) −0.13930 (17) 0.4106 (3) 0.0340 (10)
H28 −1.1446 −0.1161 0.4360 0.041*
N1 0.2223 (6) 0.09330 (12) 0.0948 (2) 0.0258 (8)
N2 0.4459 (6) 0.08575 (13) −0.0061 (2) 0.0270 (8)
N3 0.6107 (6) 0.34292 (13) −0.1381 (2) 0.0281 (8)
N4 0.3250 (6) 0.37110 (13) −0.2109 (2) 0.0282 (8)
O1 −0.0854 (5) 0.07421 (11) 0.26198 (18) 0.0326 (7)
O2 −0.2634 (5) 0.05027 (12) 0.14567 (18) 0.0353 (7)
O3 −1.2588 (5) −0.28926 (12) 0.3550 (2) 0.0393 (8)
O4 −0.9314 (5) −0.31274 (11) 0.31674 (19) 0.0331 (7)
O5 −0.7843 (5) −0.07438 (11) 0.41306 (19) 0.0380 (8)
Zn1 0.09373 (8) 0.120902 (17) 0.19746 (3) 0.02586 (17)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.028 (2) 0.022 (2) 0.032 (2) −0.0029 (17) −0.0013 (18) −0.0012 (17)
C2 0.030 (2) 0.026 (2) 0.029 (2) 0.0022 (18) −0.0012 (18) −0.0039 (17)
C3 0.032 (2) 0.020 (2) 0.032 (2) 0.0034 (17) 0.0039 (19) −0.0014 (17)
C4 0.039 (3) 0.028 (2) 0.049 (3) 0.004 (2) 0.023 (2) 0.004 (2)
C5 0.036 (3) 0.029 (2) 0.030 (2) 0.0011 (19) 0.011 (2) 0.0031 (18)
C6 0.030 (3) 0.042 (3) 0.052 (3) −0.008 (2) −0.004 (2) 0.011 (2)
C7 0.032 (3) 0.040 (3) 0.059 (3) −0.003 (2) −0.005 (2) 0.021 (2)
C8 0.026 (2) 0.031 (2) 0.026 (2) 0.0028 (18) 0.0033 (17) 0.0044 (17)
C9 0.025 (2) 0.038 (3) 0.044 (3) 0.001 (2) −0.003 (2) 0.001 (2)
C10 0.032 (3) 0.035 (3) 0.047 (3) 0.008 (2) −0.001 (2) 0.008 (2)
C11 0.024 (2) 0.037 (3) 0.038 (3) −0.0009 (19) −0.0014 (19) 0.005 (2)
C12 0.052 (3) 0.035 (3) 0.031 (2) 0.001 (2) 0.003 (2) −0.003 (2)
C13 0.040 (3) 0.029 (2) 0.036 (3) 0.003 (2) 0.010 (2) −0.0047 (19)
C14 0.026 (2) 0.029 (2) 0.027 (2) 0.0018 (18) 0.0003 (18) 0.0035 (17)
C15 0.027 (2) 0.017 (2) 0.037 (3) 0.0043 (17) 0.0066 (19) 0.0005 (17)
C16 0.032 (2) 0.018 (2) 0.033 (2) 0.0043 (17) 0.0065 (19) −0.0012 (17)
C17 0.040 (3) 0.026 (2) 0.028 (2) −0.0034 (19) 0.000 (2) 0.0000 (18)
C18 0.030 (3) 0.032 (2) 0.037 (3) −0.009 (2) −0.001 (2) −0.0031 (19)
C19 0.040 (3) 0.016 (2) 0.034 (2) −0.0043 (18) 0.009 (2) −0.0005 (17)
C20 0.048 (3) 0.024 (2) 0.025 (2) −0.001 (2) 0.003 (2) 0.0018 (17)
C21 0.032 (2) 0.025 (2) 0.033 (2) −0.0044 (18) −0.0035 (19) −0.0005 (18)
C22 0.041 (3) 0.021 (2) 0.026 (2) −0.0033 (19) 0.0050 (19) 0.0005 (17)
C23 0.031 (3) 0.033 (2) 0.048 (3) −0.011 (2) 0.013 (2) 0.000 (2)
C24 0.035 (3) 0.024 (2) 0.047 (3) 0.0005 (19) 0.019 (2) −0.0029 (19)
C25 0.028 (2) 0.022 (2) 0.031 (2) −0.0032 (17) 0.0027 (18) 0.0014 (17)
C26 0.035 (3) 0.021 (2) 0.032 (2) −0.0009 (18) 0.0055 (19) 0.0008 (17)
C27 0.030 (2) 0.027 (2) 0.043 (3) −0.0020 (19) 0.009 (2) −0.0003 (19)
C28 0.036 (3) 0.025 (2) 0.042 (3) 0.0024 (19) 0.013 (2) −0.0013 (19)
N1 0.030 (2) 0.0206 (17) 0.0268 (18) 0.0008 (15) 0.0026 (15) −0.0004 (14)
N2 0.029 (2) 0.0230 (18) 0.0299 (18) 0.0035 (15) 0.0051 (15) 0.0005 (14)
N3 0.029 (2) 0.0268 (19) 0.0286 (19) −0.0002 (15) 0.0015 (16) 0.0065 (15)
N4 0.030 (2) 0.0240 (18) 0.0303 (19) 0.0032 (15) 0.0033 (15) 0.0039 (15)
O1 0.0351 (18) 0.0278 (16) 0.0354 (17) −0.0094 (13) 0.0073 (14) 0.0003 (13)
O2 0.0397 (19) 0.0369 (18) 0.0300 (17) −0.0037 (14) 0.0068 (14) 0.0024 (13)
O3 0.0345 (19) 0.0294 (17) 0.055 (2) −0.0072 (14) 0.0087 (16) −0.0032 (15)
O4 0.0340 (18) 0.0234 (15) 0.0426 (18) −0.0012 (13) 0.0088 (14) −0.0021 (13)
O5 0.053 (2) 0.0251 (16) 0.0375 (18) −0.0140 (14) 0.0200 (16) −0.0062 (13)
Zn1 0.0284 (3) 0.0203 (3) 0.0292 (3) −0.0010 (2) 0.0048 (2) −0.00183 (19)

Geometric parameters (Å, °)

C1—C2 1.357 (6) C15—O2 1.243 (5)
C1—N1 1.376 (5) C15—O1 1.274 (5)
C1—H1 0.9300 C15—C16 1.502 (6)
C2—N2 1.377 (5) C16—C21 1.395 (6)
C2—H2 0.9300 C16—C17 1.397 (6)
C3—N1 1.319 (5) C17—C18 1.383 (6)
C3—N2 1.342 (5) C17—H17 0.9300
C3—H3 0.9300 C18—C19 1.381 (6)
C4—N2 1.466 (5) C18—H18 0.9300
C4—C5 1.501 (6) C19—C20 1.370 (6)
C4—H4A 0.9700 C19—O5 1.398 (5)
C4—H4B 0.9700 C20—C21 1.389 (6)
C5—C6 1.375 (6) C20—H20 0.9300
C5—C10 1.375 (6) C21—H21 0.9300
C6—C7 1.385 (6) C22—C28 1.375 (6)
C6—H6 0.9300 C22—C23 1.383 (6)
C7—C8 1.383 (6) C22—O5 1.396 (5)
C7—H7 0.9300 C23—C24 1.389 (6)
C8—C9 1.390 (6) C23—H23 0.9300
C8—C11 1.513 (6) C24—C25 1.385 (6)
C9—C10 1.387 (6) C24—H24 0.9300
C9—H9 0.9300 C25—C27 1.392 (6)
C10—H10 0.9300 C25—C26 1.505 (6)
C11—N3 1.457 (5) C26—O3 1.236 (5)
C11—H11A 0.9700 C26—O4 1.288 (5)
C11—H11B 0.9700 C27—C28 1.378 (6)
C12—C13 1.356 (7) C27—H27 0.9300
C12—N3 1.372 (6) C28—H28 0.9300
C12—H12 0.9300 N1—Zn1 2.002 (3)
C13—N4 1.383 (5) N4—Zn1i 2.021 (4)
C13—H13 0.9300 O1—Zn1 1.965 (3)
C14—N4 1.323 (5) O4—Zn1ii 1.992 (3)
C14—N3 1.336 (5) Zn1—O4iii 1.992 (3)
C14—H14 0.9300 Zn1—N4iv 2.021 (4)
C2—C1—N1 109.1 (4) C16—C17—H17 119.3
C2—C1—H1 125.4 C19—C18—C17 118.6 (4)
N1—C1—H1 125.4 C19—C18—H18 120.7
C1—C2—N2 106.1 (4) C17—C18—H18 120.7
C1—C2—H2 126.9 C20—C19—C18 121.6 (4)
N2—C2—H2 126.9 C20—C19—O5 117.7 (4)
N1—C3—N2 110.8 (4) C18—C19—O5 120.5 (4)
N1—C3—H3 124.6 C19—C20—C21 119.6 (4)
N2—C3—H3 124.6 C19—C20—H20 120.2
N2—C4—C5 112.3 (3) C21—C20—H20 120.2
N2—C4—H4A 109.1 C20—C21—C16 120.3 (4)
C5—C4—H4A 109.1 C20—C21—H21 119.8
N2—C4—H4B 109.1 C16—C21—H21 119.8
C5—C4—H4B 109.1 C28—C22—C23 121.1 (4)
H4A—C4—H4B 107.9 C28—C22—O5 116.5 (4)
C6—C5—C10 117.9 (4) C23—C22—O5 122.2 (4)
C6—C5—C4 121.0 (4) C22—C23—C24 118.9 (4)
C10—C5—C4 121.1 (4) C22—C23—H23 120.5
C5—C6—C7 122.1 (4) C24—C23—H23 120.5
C5—C6—H6 119.0 C25—C24—C23 121.0 (4)
C7—C6—H6 119.0 C25—C24—H24 119.5
C8—C7—C6 119.9 (4) C23—C24—H24 119.5
C8—C7—H7 120.1 C24—C25—C27 118.6 (4)
C6—C7—H7 120.1 C24—C25—C26 122.9 (4)
C7—C8—C9 118.5 (4) C27—C25—C26 118.5 (4)
C7—C8—C11 123.2 (4) O3—C26—O4 123.3 (4)
C9—C8—C11 118.3 (4) O3—C26—C25 119.1 (4)
C10—C9—C8 120.5 (4) O4—C26—C25 117.6 (4)
C10—C9—H9 119.7 C28—C27—C25 121.0 (4)
C8—C9—H9 119.7 C28—C27—H27 119.5
C5—C10—C9 121.2 (4) C25—C27—H27 119.5
C5—C10—H10 119.4 C22—C28—C27 119.4 (4)
C9—C10—H10 119.4 C22—C28—H28 120.3
N3—C11—C8 112.7 (4) C27—C28—H28 120.3
N3—C11—H11A 109.1 C3—N1—C1 106.4 (3)
C8—C11—H11A 109.1 C3—N1—Zn1 124.3 (3)
N3—C11—H11B 109.1 C1—N1—Zn1 129.2 (3)
C8—C11—H11B 109.1 C3—N2—C2 107.5 (3)
H11A—C11—H11B 107.8 C3—N2—C4 126.4 (4)
C13—C12—N3 105.8 (4) C2—N2—C4 125.8 (4)
C13—C12—H12 127.1 C14—N3—C12 107.7 (4)
N3—C12—H12 127.1 C14—N3—C11 125.4 (4)
C12—C13—N4 109.9 (4) C12—N3—C11 126.2 (4)
C12—C13—H13 125.1 C14—N4—C13 105.0 (4)
N4—C13—H13 125.1 C14—N4—Zn1i 128.0 (3)
N4—C14—N3 111.6 (4) C13—N4—Zn1i 126.5 (3)
N4—C14—H14 124.2 C15—O1—Zn1 116.9 (3)
N3—C14—H14 124.2 C26—O4—Zn1ii 106.7 (3)
O2—C15—O1 124.1 (4) C22—O5—C19 119.0 (3)
O2—C15—C16 119.5 (4) O1—Zn1—O4iii 107.32 (12)
O1—C15—C16 116.4 (4) O1—Zn1—N1 118.32 (13)
C21—C16—C17 118.5 (4) O4iii—Zn1—N1 115.16 (13)
C21—C16—C15 121.6 (4) O1—Zn1—N4iv 93.85 (13)
C17—C16—C15 119.9 (4) O4iii—Zn1—N4iv 109.34 (13)
C18—C17—C16 121.3 (4) N1—Zn1—N4iv 110.68 (14)
C18—C17—H17 119.3

Symmetry codes: (i) x, −y+1/2, z−1/2; (ii) −x−1, y−1/2, −z+1/2; (iii) −x−1, y+1/2, −z+1/2; (iv) x, −y+1/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2755).

References

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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 datablocks global, I. DOI: 10.1107/S1600536808023982/bt2755sup1.cif

e-64-m1106-sup1.cif (20.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023982/bt2755Isup2.hkl

e-64-m1106-Isup2.hkl (242.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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