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The title compound, C25H20Cl2O2, was synthesized by the reaction of 3,4-dihydro­naphthalen-1(2H)-one with 3-(3,4-dichloro­phen­yl)-1-phenyl­prop-2-en-1-one under solvent-free conditions at room temperature. X-ray analysis reveals that the cyclo­hexa­none ring adopts an envelope conformation

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805039449/ci6714sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805039449/ci6714Isup2.hkl
Contains datablock I

CCDC reference: 296537

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.053
  • wR factor = 0.148
  • Data-to-parameter ratio = 10.7

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C12 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C13 PLAT340_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 5 PLAT480_ALERT_4_C Long H...A H-Bond Reported H9 .. CG1 .. 2.97 Ang.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

1,5-Diketones are extremely important synthetic intermediates and are desirable starting materials for preparing many heterocyclic (Arigan or Ariyan & Suschitiky, 1961) and polyfunctional compounds (Edwin & Alexanden, 1992; Gill et al., 1952). The solvent-free reaction has attracted much attention in recent years (Tanaka & Toda, 2000) and has been proved to have many advantages: reduced pollution, low costs, and simplicity in process and handling. The solid-state Michael addition has been performed well recently (Goud et al., 1995; Annunziata et al., 1997; Li et al., 1999). We report here the crystal structure of the title compound, (I), which was synthesized by the solvent-free Michael addition reaction of 3,4-dihydronaphthalen-1(2H)-one and 3-(3,4-dichlorophenyl)-1-phenylprop-2-en-1-one at room temperature.

In (I), the fused cyclohexanone ring adopts an envelope conformation (Fig.1), with the atom C25 deviating from the C16/C17/C18/C23/C24 plane by 0.684 (4) Å. The C4–C9 and C10–C15 planes form dihedral angles of 85.6 (1) and 74.6 (1)°, respectively, with respect to the C16–C24 plane. The crystal packing is stablized by C—H···π interactions involving the C18–C23 phenyl ring (centroid Cg1) (Table 2).

Experimental top

Compound (I) was prepared by the reaction of 3,4-dihydronaphthalen-1(2H)-one (2 mmol) with 3-(3,4-dichlorophenyl)-1-phenylprop-2-en-1-one (2 mmol) catalysed by NaOH (0.2 g) under solvent-free condition (m.p. 469–470 K). Single crystals suitable for X-ray diffraction were obtained by slow evaporation of an ethanol solution.

Refinement top

H atoms were located in a difference map and refined isotropically. The C—H distances range from 0.89 (3) to 1.04 (3) Å.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1999); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The structure of (I), showing 30% probability displacement ellipsoids.
2-[1-(3,4-Dichlorophenyl)-3-oxo-3-phenylpropyl]-3,4-dihydro-2H- naphthalen-1-one top
Crystal data top
C25H20Cl2O2F(000) = 880
Mr = 423.31Dx = 1.348 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 2344 reflections
a = 9.9826 (19) Åθ = 2.3–21.1°
b = 17.858 (3) ŵ = 0.33 mm1
c = 11.703 (2) ÅT = 298 K
β = 91.667 (3)°Block, colourless
V = 2085.4 (6) Å30.42 × 0.37 × 0.29 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
3669 independent reflections
Radiation source: fine-focus sealed tube2008 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
ϕ and ω scansθmax = 25.0°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1111
Tmin = 0.874, Tmax = 0.910k = 1621
10745 measured reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.053Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.148All H-atom parameters refined
S = 1.00 w = 1/[σ2(Fo2) + (0.074P)2]
where P = (Fo2 + 2Fc2)/3
3669 reflections(Δ/σ)max = 0.001
342 parametersΔρmax = 0.46 e Å3
4 restraintsΔρmin = 0.58 e Å3
Crystal data top
C25H20Cl2O2V = 2085.4 (6) Å3
Mr = 423.31Z = 4
Monoclinic, P21/nMo Kα radiation
a = 9.9826 (19) ŵ = 0.33 mm1
b = 17.858 (3) ÅT = 298 K
c = 11.703 (2) Å0.42 × 0.37 × 0.29 mm
β = 91.667 (3)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
3669 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2008 reflections with I > 2σ(I)
Tmin = 0.874, Tmax = 0.910Rint = 0.038
10745 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0534 restraints
wR(F2) = 0.148All H-atom parameters refined
S = 1.00Δρmax = 0.46 e Å3
3669 reflectionsΔρmin = 0.58 e Å3
342 parameters
Special details top

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) top
xyzUiso*/Ueq
Cl10.60289 (12)0.94496 (7)0.09359 (14)0.1434 (6)
Cl20.86756 (12)1.00483 (5)0.19962 (8)0.0974 (4)
O10.8679 (2)0.65171 (12)0.07565 (18)0.0733 (6)
O20.7770 (2)0.65610 (12)0.30267 (16)0.0706 (6)
C10.8762 (3)0.73942 (16)0.1209 (2)0.0501 (7)
C20.9834 (3)0.68126 (18)0.0988 (3)0.0556 (8)
C30.9667 (3)0.64200 (16)0.0155 (2)0.0540 (8)
C41.0748 (3)0.58997 (15)0.0512 (2)0.0538 (7)
C51.1766 (4)0.56655 (19)0.0213 (3)0.0677 (9)
C61.2723 (4)0.5164 (2)0.0160 (4)0.0824 (11)
C71.2677 (5)0.4908 (2)0.1250 (4)0.0853 (11)
C81.1680 (5)0.5146 (2)0.1987 (4)0.0886 (12)
C91.0726 (4)0.5633 (2)0.1621 (3)0.0769 (10)
C100.8753 (3)0.80494 (16)0.0377 (2)0.0519 (7)
C110.7566 (4)0.84144 (18)0.0114 (3)0.0626 (9)
C120.7534 (3)0.90283 (18)0.0610 (3)0.0688 (9)
C130.8703 (4)0.92844 (16)0.1086 (2)0.0619 (8)
C140.9871 (4)0.89229 (19)0.0846 (3)0.0701 (9)
C150.9897 (4)0.8315 (2)0.0130 (3)0.0664 (9)
C160.8851 (3)0.76833 (17)0.2450 (2)0.0514 (7)
C170.8430 (3)0.71060 (16)0.3308 (2)0.0515 (7)
C180.8804 (3)0.72456 (16)0.4529 (2)0.0510 (7)
C190.8354 (3)0.67466 (19)0.5357 (3)0.0606 (8)
C200.8583 (4)0.6883 (2)0.6488 (3)0.0741 (10)
C210.9271 (4)0.7509 (3)0.6826 (3)0.0827 (11)
C220.9760 (4)0.7997 (2)0.6031 (3)0.0754 (10)
C230.9549 (3)0.78684 (16)0.4863 (2)0.0572 (8)
C241.0121 (5)0.8382 (2)0.3985 (3)0.0688 (10)
C251.0214 (3)0.8009 (2)0.2830 (3)0.0624 (9)
H10.790 (3)0.7166 (13)0.114 (2)0.047 (8)*
H20.980 (2)0.6412 (16)0.156 (2)0.057 (8)*
H31.074 (3)0.7036 (15)0.101 (2)0.056 (8)*
H41.185 (3)0.5857 (16)0.094 (2)0.066 (9)*
H51.341 (4)0.5037 (18)0.041 (3)0.087 (12)*
H61.338 (3)0.4534 (18)0.156 (3)0.084 (10)*
H71.168 (4)0.501 (2)0.2777 (18)0.116 (14)*
H81.001 (3)0.5799 (17)0.208 (3)0.076 (11)*
H90.679 (3)0.8232 (16)0.040 (2)0.063 (9)*
H101.0628 (16)0.9183 (13)0.115 (2)0.087 (11)*
H111.070 (4)0.8055 (18)0.009 (3)0.086 (11)*
H120.821 (3)0.8110 (16)0.250 (2)0.063 (8)*
H130.792 (3)0.6279 (15)0.508 (2)0.054 (8)*
H140.826 (3)0.6590 (17)0.702 (3)0.070 (10)*
H150.943 (3)0.7639 (17)0.760 (3)0.078 (10)*
H161.021 (3)0.8432 (18)0.619 (3)0.069 (10)*
H170.949 (3)0.8800 (17)0.386 (2)0.066 (9)*
H181.095 (3)0.8524 (17)0.423 (3)0.073 (11)*
H191.053 (3)0.8372 (16)0.223 (2)0.068 (9)*
H201.094 (3)0.7599 (18)0.286 (2)0.073 (9)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0794 (8)0.1264 (10)0.2243 (15)0.0274 (7)0.0026 (8)0.0879 (10)
Cl20.1310 (9)0.0719 (7)0.0890 (7)0.0047 (5)0.0013 (6)0.0306 (5)
O10.0724 (16)0.0862 (17)0.0606 (13)0.0086 (12)0.0080 (12)0.0068 (11)
O20.0828 (16)0.0711 (15)0.0580 (13)0.0271 (12)0.0041 (11)0.0014 (11)
C10.0515 (19)0.0530 (18)0.0458 (17)0.0029 (15)0.0026 (14)0.0016 (14)
C20.062 (2)0.0536 (19)0.0511 (19)0.0044 (17)0.0023 (15)0.0035 (15)
C30.062 (2)0.0528 (19)0.0475 (17)0.0046 (15)0.0055 (15)0.0039 (14)
C40.064 (2)0.0448 (17)0.0533 (18)0.0053 (15)0.0080 (15)0.0005 (14)
C50.080 (3)0.064 (2)0.060 (2)0.0104 (18)0.0053 (19)0.0061 (18)
C60.085 (3)0.074 (3)0.088 (3)0.012 (2)0.004 (2)0.005 (2)
C70.098 (3)0.067 (3)0.092 (3)0.011 (2)0.018 (3)0.018 (2)
C80.110 (3)0.083 (3)0.073 (3)0.015 (2)0.006 (3)0.020 (2)
C90.090 (3)0.074 (2)0.067 (2)0.015 (2)0.004 (2)0.0158 (19)
C100.0566 (19)0.0519 (18)0.0473 (16)0.0025 (15)0.0024 (14)0.0025 (14)
C110.055 (2)0.061 (2)0.072 (2)0.0003 (17)0.0054 (17)0.0091 (17)
C120.062 (2)0.064 (2)0.079 (2)0.0089 (17)0.0076 (17)0.0109 (18)
C130.078 (2)0.0519 (19)0.0559 (18)0.0087 (17)0.0018 (17)0.0037 (14)
C140.070 (2)0.072 (2)0.069 (2)0.0076 (19)0.0094 (18)0.0129 (18)
C150.057 (2)0.075 (2)0.068 (2)0.0037 (18)0.0056 (17)0.0174 (18)
C160.0541 (19)0.0488 (18)0.0517 (17)0.0012 (15)0.0049 (14)0.0019 (14)
C170.0498 (18)0.0544 (19)0.0505 (18)0.0009 (14)0.0054 (14)0.0016 (14)
C180.0486 (17)0.0545 (18)0.0500 (17)0.0023 (14)0.0044 (13)0.0021 (14)
C190.057 (2)0.069 (2)0.056 (2)0.0013 (17)0.0027 (15)0.0053 (17)
C200.076 (2)0.090 (3)0.057 (2)0.004 (2)0.0010 (19)0.012 (2)
C210.099 (3)0.104 (3)0.045 (2)0.006 (2)0.001 (2)0.002 (2)
C220.090 (3)0.072 (3)0.064 (2)0.007 (2)0.0035 (19)0.015 (2)
C230.063 (2)0.059 (2)0.0498 (18)0.0054 (15)0.0052 (15)0.0025 (15)
C240.083 (3)0.057 (2)0.066 (2)0.014 (2)0.004 (2)0.0092 (18)
C250.071 (2)0.059 (2)0.057 (2)0.0137 (19)0.0077 (17)0.0016 (17)
Geometric parameters (Å, º) top
Cl1—C121.714 (3)C11—H90.91 (3)
Cl2—C131.730 (3)C12—C131.386 (4)
O1—C31.207 (3)C13—C141.355 (4)
O2—C171.215 (3)C14—C151.371 (4)
C1—C21.518 (4)C14—H100.966 (13)
C1—C101.522 (4)C15—H110.96 (3)
C1—C161.541 (4)C16—C171.508 (4)
C1—H10.95 (3)C16—C251.534 (4)
C2—C31.515 (4)C16—H121.00 (3)
C2—H20.98 (3)C17—C181.487 (4)
C2—H30.99 (3)C18—C231.387 (4)
C3—C41.492 (4)C18—C191.401 (4)
C4—C51.370 (4)C19—C201.358 (4)
C4—C91.382 (4)C19—H130.99 (3)
C5—C61.389 (5)C20—C211.365 (5)
C5—H40.91 (3)C20—H140.89 (3)
C6—C71.355 (5)C21—C221.374 (5)
C6—H50.97 (4)C21—H150.94 (3)
C7—C81.365 (6)C22—C231.396 (4)
C7—H61.04 (3)C22—H160.91 (3)
C8—C91.368 (5)C23—C241.502 (4)
C8—H70.956 (19)C24—C251.512 (4)
C9—H80.93 (3)C24—H170.98 (3)
C10—C111.379 (4)C24—H180.91 (3)
C10—C151.386 (4)C25—H191.02 (3)
C11—C121.385 (4)C25—H201.03 (3)
C2—C1—C10114.1 (2)C13—C14—C15120.4 (3)
C2—C1—C16111.6 (2)C13—C14—H10111.8 (13)
C10—C1—C16110.1 (2)C15—C14—H10127.4 (13)
C2—C1—H1109.3 (15)C14—C15—C10122.0 (3)
C10—C1—H1106.8 (15)C14—C15—H11123 (2)
C16—C1—H1104.4 (15)C10—C15—H11115 (2)
C3—C2—C1114.0 (3)C17—C16—C25109.2 (2)
C3—C2—H2105.0 (15)C17—C16—C1112.9 (2)
C1—C2—H2110.1 (15)C25—C16—C1115.3 (2)
C3—C2—H3106.9 (15)C17—C16—H12107.0 (16)
C1—C2—H3111.6 (15)C25—C16—H12105.2 (16)
H2—C2—H3109 (2)C1—C16—H12106.7 (16)
O1—C3—C4120.8 (3)O2—C17—C18120.9 (3)
O1—C3—C2121.0 (3)O2—C17—C16121.8 (3)
C4—C3—C2118.3 (3)C18—C17—C16117.3 (2)
C5—C4—C9117.9 (3)C23—C18—C19119.7 (3)
C5—C4—C3123.1 (3)C23—C18—C17121.5 (3)
C9—C4—C3119.0 (3)C19—C18—C17118.8 (3)
C4—C5—C6120.5 (4)C20—C19—C18120.8 (3)
C4—C5—H4120.6 (19)C20—C19—H13122.2 (15)
C6—C5—H4118.9 (19)C18—C19—H13116.8 (15)
C7—C6—C5120.5 (4)C19—C20—C21119.9 (4)
C7—C6—H5125 (2)C19—C20—H14122 (2)
C5—C6—H5115 (2)C21—C20—H14118 (2)
C6—C7—C8119.6 (4)C20—C21—C22120.6 (4)
C6—C7—H6122.7 (18)C20—C21—H15123.2 (19)
C8—C7—H6117.7 (18)C22—C21—H15116.2 (19)
C7—C8—C9120.1 (4)C21—C22—C23120.9 (4)
C7—C8—H7121 (2)C21—C22—H16125.7 (19)
C9—C8—H7119 (2)C23—C22—H16113 (2)
C8—C9—C4121.4 (4)C18—C23—C22118.1 (3)
C8—C9—H8123 (2)C18—C23—C24120.5 (3)
C4—C9—H8115 (2)C22—C23—C24121.3 (3)
C11—C10—C15117.2 (3)C23—C24—C25112.2 (3)
C11—C10—C1119.7 (3)C23—C24—H17108.2 (17)
C15—C10—C1123.2 (3)C25—C24—H17104.8 (17)
C10—C11—C12121.0 (3)C23—C24—H18109 (2)
C10—C11—H9118.8 (19)C25—C24—H18109 (2)
C12—C11—H9120.2 (19)H17—C24—H18114 (3)
C11—C12—C13120.2 (3)C24—C25—C16110.4 (3)
C11—C12—Cl1119.2 (3)C24—C25—H19111.7 (16)
C13—C12—Cl1120.6 (3)C16—C25—H19109.2 (16)
C14—C13—C12119.3 (3)C24—C25—H20110.1 (17)
C14—C13—Cl2120.1 (3)C16—C25—H20111.0 (17)
C12—C13—Cl2120.6 (3)H19—C25—H20104 (2)
C10—C1—C2—C363.4 (4)C11—C10—C15—C141.3 (5)
C16—C1—C2—C3171.0 (3)C1—C10—C15—C14177.6 (3)
C1—C2—C3—O17.6 (4)C2—C1—C16—C1770.5 (3)
C1—C2—C3—C4173.4 (3)C10—C1—C16—C17161.8 (2)
O1—C3—C4—C5168.0 (3)C2—C1—C16—C2555.9 (4)
C2—C3—C4—C511.1 (4)C10—C1—C16—C2571.9 (3)
O1—C3—C4—C911.5 (4)C25—C16—C17—O2147.7 (3)
C2—C3—C4—C9169.4 (3)C1—C16—C17—O218.1 (4)
C9—C4—C5—C61.3 (5)C25—C16—C17—C1834.9 (3)
C3—C4—C5—C6178.2 (3)C1—C16—C17—C18164.5 (2)
C4—C5—C6—C71.0 (6)O2—C17—C18—C23179.5 (3)
C5—C6—C7—C80.0 (6)C16—C17—C18—C232.1 (4)
C6—C7—C8—C90.7 (6)O2—C17—C18—C191.6 (4)
C7—C8—C9—C40.4 (6)C16—C17—C18—C19175.8 (2)
C5—C4—C9—C80.6 (5)C23—C18—C19—C203.1 (4)
C3—C4—C9—C8178.9 (3)C17—C18—C19—C20174.9 (3)
C2—C1—C10—C11150.2 (3)C18—C19—C20—C210.6 (5)
C16—C1—C10—C1183.4 (3)C19—C20—C21—C221.4 (6)
C2—C1—C10—C1530.9 (4)C20—C21—C22—C230.9 (6)
C16—C1—C10—C1595.5 (3)C19—C18—C23—C223.5 (4)
C15—C10—C11—C121.2 (5)C17—C18—C23—C22174.4 (3)
C1—C10—C11—C12177.8 (3)C19—C18—C23—C24175.8 (3)
C10—C11—C12—C130.2 (5)C17—C18—C23—C246.3 (5)
C10—C11—C12—Cl1178.5 (3)C21—C22—C23—C181.6 (5)
C11—C12—C13—C140.7 (5)C21—C22—C23—C24177.7 (4)
Cl1—C12—C13—C14177.5 (3)C18—C23—C24—C2519.9 (5)
C11—C12—C13—Cl2179.7 (2)C22—C23—C24—C25159.3 (3)
Cl1—C12—C13—Cl21.5 (4)C23—C24—C25—C1653.4 (5)
C12—C13—C14—C150.6 (5)C17—C16—C25—C2460.5 (4)
Cl2—C13—C14—C15179.6 (3)C1—C16—C25—C24171.2 (3)
C13—C14—C15—C100.4 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H9···Cg1i0.91 (3)2.97 (3)3.855 (6)166 (3)
Symmetry code: (i) x1/2, y+3/2, z1/2.

Experimental details

Crystal data
Chemical formulaC25H20Cl2O2
Mr423.31
Crystal system, space groupMonoclinic, P21/n
Temperature (K)298
a, b, c (Å)9.9826 (19), 17.858 (3), 11.703 (2)
β (°) 91.667 (3)
V3)2085.4 (6)
Z4
Radiation typeMo Kα
µ (mm1)0.33
Crystal size (mm)0.42 × 0.37 × 0.29
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.874, 0.910
No. of measured, independent and
observed [I > 2σ(I)] reflections
10745, 3669, 2008
Rint0.038
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.053, 0.148, 1.00
No. of reflections3669
No. of parameters342
No. of restraints4
H-atom treatmentAll H-atom parameters refined
Δρmax, Δρmin (e Å3)0.46, 0.58

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1999), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1999), SHELXTL.

Selected geometric parameters (Å, º) top
Cl1—C121.714 (3)O1—C31.207 (3)
Cl2—C131.730 (3)O2—C171.215 (3)
C10—C1—C16110.1 (2)C11—C10—C15117.2 (3)
C3—C2—C1114.0 (3)C15—C10—C1123.2 (3)
C5—C4—C9117.9 (3)C17—C16—C1112.9 (2)
C5—C4—C3123.1 (3)C25—C16—C1115.3 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H9···Cg1i0.91 (3)2.97 (3)3.855 (6)166 (3)
Symmetry code: (i) x1/2, y+3/2, z1/2.
 

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