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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Apr 14;66(Pt 5):o1081. doi: 10.1107/S1600536810013012

4-(5-Phenyl-1,2,4-triazolo[3,4-a]isoquinolin-3-yl)benzonitrile

F Nawaz Khan a, P Manivel a, K Prabakaran a, Venkatesha R Hathwar b, Mehmet Akkurt c,*
PMCID: PMC2979274  PMID: 21579135

Abstract

In the title mol­ecule, C23H14N4, the triazoloisoquinoline ring system is nearly planar, with an r.m.s. deviation of 0.038 (2) Å and a maximum deviation of −0.030 (2) Å from the mean plane of the triazole ring C atom which is bonded to the benzene ring. The benzene and phenyl rings are twisted by 57.65 (8) and 53.60 (9)°, respectively, with respect to the mean plane of the triazoloisoquinoline ring system. In the crystal structure, mol­ecules are linked by weak aromatic π–π inter­actions [centroid–centroid distance = 3.8074 (12) Å]. In addition, the crystal structure exhibits a nonclassical inter­molecular C—H⋯N hydrogen bond.

Related literature

For a related crystal structure, see: Khan et al. (2010).graphic file with name e-66-o1081-scheme1.jpg

Experimental

Crystal data

  • C23H14N4

  • M r = 346.38

  • Orthorhombic, Inline graphic

  • a = 7.1614 (3) Å

  • b = 18.0957 (7) Å

  • c = 26.4021 (9) Å

  • V = 3421.5 (2) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 290 K

  • 0.25 × 0.21 × 0.17 mm

Data collection

  • Oxford Xcalibur Eos (Nova) CCD detector diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO RED; Oxford Diffraction, 2009) T min = 0.959, T max = 0.986

  • 14977 measured reflections

  • 3164 independent reflections

  • 1490 reflections with I > 2σ(I)

  • R int = 0.070

Refinement

  • R[F 2 > 2σ(F 2)] = 0.046

  • wR(F 2) = 0.100

  • S = 0.81

  • 3164 reflections

  • 244 parameters

  • H-atom parameters constrained

  • Δρmax = 0.15 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: CrysAlis PRO CCD (Oxford Diffraction, 2009); cell refinement: CrysAlis PRO CCD; data reduction: CrysAlis PRO RED (Oxford Diffraction, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810013012/rk2199sup1.cif

e-66-o1081-sup1.cif (20.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810013012/rk2199Isup2.hkl

e-66-o1081-Isup2.hkl (152.2KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C11—H11⋯N3i 0.93 2.50 3.418 (3) 170

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank the FIST program for data collection on the Oxford single-crystal diffractometer at SSCU, IISc, Bangalore. The authors also thank Professor T. N. Guru Row, IISc, Bangalore, for his help with the data collection. FNK thanks the DST for Fast Track Proposal funding.

supplementary crystallographic information

Comment

As part of our search for new isoquinoline analogues (Khan et al., 2010), we focused on synthesis of titled compounds and the crystal structure is reported.

In the title molecule, Fig. 1, the triazoloisoquinoline ring system (N1-N3/C1-C9/C16) is nearly planar, with an r.m.s. deviation of 0.038 (2)Å and a maximum deviation of -0.030 (2)Å from the mean plane for the triazole ring C16 atom which is bonded to the benzene ring (C17-C22). The benzene (C17-C22) and phenyl (C10-C15) rings are twisted by 57.65 (8)° and 53.60 (9)°, respectively, with respect to the mean plane of the triazoloisoquinoline ring system. The benzene (C17-C22) and phenyl (C10-C15) rings make a dihedral angle of 29.10 (11)° with each other.

Molecular conformation is stabilized by a weak π–π interaction [Cg4···Cg5 = 3.8229 (14)Å, where are Cg4 and Cg5 are centroids of the C10-C15 and C17-C22 rings, respectively]. In the crystal structure, the molecules are linked by weak aromatic π–π interactions [Cg1···Cg1ii = 3.8074 (12)Å, symmetry code: (ii) x-1/2, 1/2-y, -z. Cg1 is the centroid of the N1-N3/C1/C16 ring]. In addition, the crystal structure exhibits an intermolecular non-classical C–H···N hydrogen bond (Table 1, Fig. 2).

Experimental

2-(3-Phenylisoquinolin-1-yl)hydrazine (1 mmol) was condensed with 4-formylbenzonitrile (1.1 mmol) under refluxing conditions isopropanol (10 ml) solvent to give the corresponding hydrazone in high yield. After removal of solvent the compound was then oxidatively cyclized in nitrobenzene (10 ml) at 473 K. The product was recrystallized from dichlomethane to give block-shaped crystals.

Refinement

All H atoms were placed in calculated positions with C–H = 0.93Å and were included in the refinement in the riding model approximation, with Uiso(H) = 1.2Ueq(C).

Pure diffraction experiment (ratio observed/unique reflections 47%) we explain by weak diffraction of the crystal.

Figures

Fig. 1.

Fig. 1.

The view of the title molecule with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are presented as a small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

The packing diagram and the hydrogen bonding in the title crystal structure viewed down the [1 0 0] direction. H atoms not involved in the motif shown have been omitted for clarity.

Crystal data

C23H14N4 F(000) = 1440
Mr = 346.38 Dx = 1.345 Mg m3
Orthorhombic, Pbca Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2ab Cell parameters from 1235 reflections
a = 7.1614 (3) Å θ = 1.6–20.4°
b = 18.0957 (7) Å µ = 0.08 mm1
c = 26.4021 (9) Å T = 290 K
V = 3421.5 (2) Å3 Block, colourless
Z = 8 0.25 × 0.21 × 0.17 mm

Data collection

Oxford Xcalibur Eos (Nova) CCD detector diffractometer 3164 independent reflections
Radiation source: Enhance (Mo) X-ray Source 1490 reflections with I > 2σ(I)
graphite Rint = 0.070
ω scans θmax = 25.5°, θmin = 3.1°
Absorption correction: multi-scan (CrysAlis PRO RED; Oxford Diffraction, 2009) h = −8→7
Tmin = 0.959, Tmax = 0.986 k = −21→21
14977 measured reflections l = −31→31

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.046 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100 H-atom parameters constrained
S = 0.81 w = 1/[σ2(Fo2) + (0.0413P)2] where P = (Fo2 + 2Fc2)/3
3164 reflections (Δ/σ)max < 0.001
244 parameters Δρmax = 0.15 e Å3
0 restraints Δρmin = −0.20 e Å3

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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
N1 0.6627 (2) 0.33099 (9) 0.03366 (6) 0.0370 (4)
N2 0.5820 (3) 0.22467 (10) −0.00072 (7) 0.0510 (5)
N3 0.6063 (2) 0.27481 (11) −0.03950 (7) 0.0495 (5)
N4 0.5390 (3) 0.08980 (15) 0.27259 (9) 0.0927 (9)
C1 0.6539 (3) 0.33812 (13) −0.01851 (8) 0.0395 (5)
C2 0.6915 (3) 0.40722 (12) −0.04237 (8) 0.0407 (6)
C3 0.6888 (3) 0.41638 (14) −0.09495 (8) 0.0490 (6)
H3 0.6586 0.3766 −0.1157 0.059*
C4 0.7302 (3) 0.48368 (15) −0.11611 (9) 0.0570 (7)
H4 0.7297 0.4894 −0.1511 0.068*
C5 0.7728 (3) 0.54308 (14) −0.08507 (9) 0.0581 (7)
H5 0.8002 0.5887 −0.0996 0.070*
C6 0.7754 (3) 0.53585 (13) −0.03328 (9) 0.0526 (6)
H6 0.8030 0.5764 −0.0130 0.063*
C7 0.7364 (3) 0.46741 (12) −0.01110 (8) 0.0416 (6)
C8 0.7527 (3) 0.45523 (12) 0.04249 (8) 0.0454 (6)
H8 0.7853 0.4952 0.0628 0.054*
C9 0.7238 (3) 0.38972 (12) 0.06498 (8) 0.0387 (6)
C10 0.7671 (3) 0.37673 (11) 0.11909 (8) 0.0374 (5)
C11 0.8907 (3) 0.32192 (12) 0.13406 (8) 0.0456 (6)
H11 0.9426 0.2903 0.1101 0.055*
C12 0.9365 (3) 0.31454 (14) 0.18466 (9) 0.0562 (7)
H12 1.0180 0.2774 0.1948 0.067*
C13 0.8625 (4) 0.36161 (15) 0.22007 (9) 0.0645 (8)
H13 0.8935 0.3561 0.2541 0.077*
C14 0.7438 (4) 0.41647 (15) 0.20553 (9) 0.0595 (7)
H14 0.6960 0.4490 0.2295 0.071*
C15 0.6944 (3) 0.42380 (13) 0.15537 (9) 0.0478 (6)
H15 0.6114 0.4608 0.1458 0.057*
C16 0.6137 (3) 0.25837 (12) 0.04252 (8) 0.0406 (6)
C17 0.5906 (3) 0.22246 (12) 0.09194 (8) 0.0403 (5)
C18 0.6918 (3) 0.15870 (13) 0.10218 (8) 0.0480 (6)
H18 0.7701 0.1391 0.0775 0.058*
C19 0.6771 (3) 0.12414 (12) 0.14857 (9) 0.0523 (6)
H19 0.7474 0.0821 0.1554 0.063*
C20 0.5575 (3) 0.15217 (13) 0.18497 (8) 0.0480 (6)
C21 0.4514 (3) 0.21414 (13) 0.17476 (8) 0.0524 (6)
H21 0.3693 0.2324 0.1990 0.063*
C22 0.4678 (3) 0.24882 (13) 0.12834 (8) 0.0503 (6)
H22 0.3957 0.2903 0.1214 0.060*
C23 0.5459 (3) 0.11720 (15) 0.23405 (10) 0.0629 (8)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0393 (10) 0.0337 (11) 0.0381 (11) −0.0026 (8) −0.0031 (8) −0.0012 (9)
N2 0.0631 (13) 0.0439 (12) 0.0459 (12) −0.0068 (10) −0.0062 (10) −0.0041 (11)
N3 0.0614 (13) 0.0457 (13) 0.0414 (11) −0.0057 (10) −0.0054 (9) 0.0003 (10)
N4 0.0964 (19) 0.124 (2) 0.0576 (16) 0.0151 (16) 0.0099 (14) 0.0261 (16)
C1 0.0394 (14) 0.0404 (15) 0.0387 (13) −0.0003 (11) −0.0054 (10) −0.0027 (12)
C2 0.0357 (13) 0.0443 (15) 0.0421 (14) 0.0023 (11) −0.0010 (10) 0.0016 (12)
C3 0.0463 (15) 0.0544 (17) 0.0463 (15) 0.0062 (13) 0.0002 (11) 0.0032 (13)
C4 0.0515 (17) 0.0687 (19) 0.0507 (15) 0.0085 (14) 0.0028 (12) 0.0160 (15)
C5 0.0464 (16) 0.0584 (19) 0.0695 (19) −0.0011 (13) −0.0002 (13) 0.0241 (15)
C6 0.0500 (15) 0.0465 (16) 0.0613 (17) −0.0003 (12) −0.0016 (13) 0.0076 (13)
C7 0.0344 (14) 0.0413 (15) 0.0490 (14) 0.0004 (11) −0.0046 (11) 0.0072 (12)
C8 0.0461 (14) 0.0387 (15) 0.0513 (15) −0.0011 (11) −0.0052 (12) −0.0054 (12)
C9 0.0347 (14) 0.0368 (15) 0.0445 (13) −0.0002 (10) −0.0019 (11) −0.0060 (11)
C10 0.0399 (14) 0.0336 (13) 0.0386 (13) −0.0029 (11) −0.0012 (10) −0.0018 (11)
C11 0.0441 (14) 0.0436 (15) 0.0492 (15) −0.0011 (12) −0.0005 (11) −0.0047 (12)
C12 0.0519 (16) 0.0604 (18) 0.0563 (17) 0.0036 (13) −0.0129 (13) 0.0072 (15)
C13 0.075 (2) 0.077 (2) 0.0416 (15) −0.0091 (16) −0.0111 (14) 0.0000 (15)
C14 0.0721 (18) 0.0580 (18) 0.0483 (16) −0.0068 (15) 0.0073 (14) −0.0115 (14)
C15 0.0507 (15) 0.0429 (15) 0.0497 (15) 0.0013 (12) 0.0008 (12) −0.0051 (13)
C16 0.0436 (14) 0.0361 (14) 0.0423 (13) −0.0039 (11) −0.0025 (11) −0.0031 (12)
C17 0.0400 (13) 0.0351 (14) 0.0458 (14) −0.0048 (11) −0.0039 (11) −0.0015 (11)
C18 0.0586 (15) 0.0392 (15) 0.0463 (15) 0.0034 (13) 0.0039 (12) −0.0031 (12)
C19 0.0637 (17) 0.0400 (15) 0.0532 (16) 0.0085 (12) 0.0004 (13) 0.0023 (13)
C20 0.0498 (15) 0.0497 (16) 0.0446 (14) −0.0053 (13) −0.0014 (12) 0.0051 (13)
C21 0.0516 (16) 0.0559 (17) 0.0497 (16) 0.0024 (14) 0.0067 (12) −0.0002 (13)
C22 0.0516 (16) 0.0417 (15) 0.0575 (16) 0.0052 (12) −0.0014 (13) 0.0000 (13)
C23 0.0591 (18) 0.075 (2) 0.0546 (18) 0.0052 (14) 0.0030 (14) 0.0043 (16)

Geometric parameters (Å, °)

N1—C16 1.380 (2) C10—C11 1.387 (3)
N1—C1 1.385 (2) C11—C12 1.382 (3)
N1—C9 1.416 (2) C11—H11 0.9300
N2—C16 1.314 (2) C12—C13 1.371 (3)
N2—N3 1.379 (2) C12—H12 0.9300
N3—C1 1.318 (3) C13—C14 1.362 (3)
N4—C23 1.133 (3) C13—H13 0.9300
C1—C2 1.426 (3) C14—C15 1.377 (3)
C2—C3 1.398 (3) C14—H14 0.9300
C2—C7 1.404 (3) C15—H15 0.9300
C3—C4 1.372 (3) C16—C17 1.467 (3)
C3—H3 0.9300 C17—C22 1.387 (3)
C4—C5 1.386 (3) C17—C18 1.389 (3)
C4—H4 0.9300 C18—C19 1.379 (3)
C5—C6 1.374 (3) C18—H18 0.9300
C5—H5 0.9300 C19—C20 1.384 (3)
C6—C7 1.398 (3) C19—H19 0.9300
C6—H6 0.9300 C20—C21 1.381 (3)
C7—C8 1.437 (3) C20—C23 1.445 (3)
C8—C9 1.342 (3) C21—C22 1.382 (3)
C8—H8 0.9300 C21—H21 0.9300
C9—C10 1.481 (3) C22—H22 0.9300
C10—C15 1.384 (3)
C16—N1—C1 104.23 (17) C12—C11—H11 120.1
C16—N1—C9 133.97 (18) C10—C11—H11 120.1
C1—N1—C9 121.67 (19) C13—C12—C11 120.5 (2)
C16—N2—N3 108.54 (17) C13—C12—H12 119.7
C1—N3—N2 107.01 (17) C11—C12—H12 119.7
N3—C1—N1 110.4 (2) C14—C13—C12 120.1 (2)
N3—C1—C2 128.7 (2) C14—C13—H13 119.9
N1—C1—C2 120.8 (2) C12—C13—H13 119.9
C3—C2—C7 119.7 (2) C13—C14—C15 120.1 (2)
C3—C2—C1 122.7 (2) C13—C14—H14 120.0
C7—C2—C1 117.6 (2) C15—C14—H14 120.0
C4—C3—C2 120.4 (2) C14—C15—C10 120.7 (2)
C4—C3—H3 119.8 C14—C15—H15 119.7
C2—C3—H3 119.8 C10—C15—H15 119.7
C3—C4—C5 119.7 (2) N2—C16—N1 109.78 (18)
C3—C4—H4 120.2 N2—C16—C17 123.23 (19)
C5—C4—H4 120.2 N1—C16—C17 126.94 (19)
C6—C5—C4 121.2 (2) C22—C17—C18 118.8 (2)
C6—C5—H5 119.4 C22—C17—C16 122.4 (2)
C4—C5—H5 119.4 C18—C17—C16 118.8 (2)
C5—C6—C7 119.9 (2) C19—C18—C17 120.6 (2)
C5—C6—H6 120.0 C19—C18—H18 119.7
C7—C6—H6 120.0 C17—C18—H18 119.7
C6—C7—C2 119.1 (2) C18—C19—C20 119.9 (2)
C6—C7—C8 122.1 (2) C18—C19—H19 120.1
C2—C7—C8 118.6 (2) C20—C19—H19 120.1
C9—C8—C7 124.0 (2) C21—C20—C19 120.2 (2)
C9—C8—H8 118.0 C21—C20—C23 119.9 (2)
C7—C8—H8 118.0 C19—C20—C23 119.9 (2)
C8—C9—N1 116.90 (19) C20—C21—C22 119.7 (2)
C8—C9—C10 122.32 (19) C20—C21—H21 120.2
N1—C9—C10 120.61 (19) C22—C21—H21 120.2
C15—C10—C11 118.9 (2) C21—C22—C17 120.8 (2)
C15—C10—C9 119.4 (2) C21—C22—H22 119.6
C11—C10—C9 121.49 (19) C17—C22—H22 119.6
C12—C11—C10 119.7 (2) N4—C23—C20 179.2 (3)
C16—N2—N3—C1 0.5 (2) N1—C9—C10—C15 −131.8 (2)
N2—N3—C1—N1 0.3 (2) C8—C9—C10—C11 −121.8 (2)
N2—N3—C1—C2 −178.9 (2) N1—C9—C10—C11 53.2 (3)
C16—N1—C1—N3 −0.9 (2) C15—C10—C11—C12 1.0 (3)
C9—N1—C1—N3 175.46 (16) C9—C10—C11—C12 176.0 (2)
C16—N1—C1—C2 178.40 (18) C10—C11—C12—C13 −0.9 (3)
C9—N1—C1—C2 −5.2 (3) C11—C12—C13—C14 −0.4 (4)
N3—C1—C2—C3 −2.5 (3) C12—C13—C14—C15 1.4 (4)
N1—C1—C2—C3 178.35 (17) C13—C14—C15—C10 −1.3 (4)
N3—C1—C2—C7 178.8 (2) C11—C10—C15—C14 0.0 (3)
N1—C1—C2—C7 −0.4 (3) C9—C10—C15—C14 −175.0 (2)
C7—C2—C3—C4 0.2 (3) N3—N2—C16—N1 −1.0 (2)
C1—C2—C3—C4 −178.5 (2) N3—N2—C16—C17 176.63 (18)
C2—C3—C4—C5 −0.8 (3) C1—N1—C16—N2 1.2 (2)
C3—C4—C5—C6 0.4 (3) C9—N1—C16—N2 −174.51 (19)
C4—C5—C6—C7 0.7 (3) C1—N1—C16—C17 −176.38 (19)
C5—C6—C7—C2 −1.2 (3) C9—N1—C16—C17 7.9 (4)
C5—C6—C7—C8 174.57 (19) N2—C16—C17—C22 −120.5 (2)
C3—C2—C7—C6 0.8 (3) N1—C16—C17—C22 56.7 (3)
C1—C2—C7—C6 179.55 (19) N2—C16—C17—C18 57.8 (3)
C3—C2—C7—C8 −175.16 (18) N1—C16—C17—C18 −125.0 (2)
C1—C2—C7—C8 3.6 (3) C22—C17—C18—C19 −3.0 (3)
C6—C7—C8—C9 −177.2 (2) C16—C17—C18—C19 178.6 (2)
C2—C7—C8—C9 −1.5 (3) C17—C18—C19—C20 1.4 (3)
C7—C8—C9—N1 −3.9 (3) C18—C19—C20—C21 0.7 (3)
C7—C8—C9—C10 171.32 (18) C18—C19—C20—C23 −178.3 (2)
C16—N1—C9—C8 −177.6 (2) C19—C20—C21—C22 −1.2 (3)
C1—N1—C9—C8 7.3 (3) C23—C20—C21—C22 177.8 (2)
C16—N1—C9—C10 7.0 (3) C20—C21—C22—C17 −0.4 (3)
C1—N1—C9—C10 −168.06 (17) C18—C17—C22—C21 2.5 (3)
C8—C9—C10—C15 53.1 (3) C16—C17—C22—C21 −179.2 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C11—H11···N3i 0.93 2.50 3.418 (3) 170

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RK2199).

References

  1. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  2. Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
  3. Khan, F. N., Manivel, P., Prabakaran, K., Hathwar, V. R. & Ng, S. W. (2010). Acta Cryst. E66, o488. [DOI] [PMC free article] [PubMed]
  4. Oxford Diffraction (2009). CrysAlis PRO CCD and CrysAlis PRO RED Oxford Diffraction Ltd, Yarnton, Oxfordshire, England.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S1600536810013012/rk2199sup1.cif

e-66-o1081-sup1.cif (20.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810013012/rk2199Isup2.hkl

e-66-o1081-Isup2.hkl (152.2KB, 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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