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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2017 Feb 10;73(Pt 3):341–344. doi: 10.1107/S2056989017001888

Synthesis and structure of the mercury chloride complex of 2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole)

Varsha Rani a, Harkesh B Singh a, Ray J Butcher b,*
PMCID: PMC5347049  PMID: 28316804

In the title mercury complex, the HgII atom is coordinated by two Cl atoms and by two N atoms from two 2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole) ligands, which gives rise to a zigzag helical 1-D polymer propagating along the b-axis direction.

Keywords: crystal structure, mercury coordination polymer, (benzimidazol-2-yl)benzene ligands

Abstract

In the title mercury complex, catena-poly[[di­chlorido­mercury(II)]-μ-2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole)-κ2 N 3:N 3′], [HgCl2(C26H25BrN4)]n, the HgII atom is coordinated by two Cl atoms and by two N atoms from two 2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole) ligands. The metal cation adopts a distorted tetrahedral coordination geometry with with bond angles around mercury of 100.59 (15)° [N—Hg—N] and 126.35 (7)° [Cl—Hg—Cl]. This arrangement gives rise to a zigzag helical 1-D polymer propagating along the b-axis direction.

Chemical context  

In the last one decade, 1,3-bis­(benzimidazol-2-yl)benzene-based ligands have been studied extensively due to the presence of active sites for binding of metal atoms (Yang et al., 2012; Tam et al., 2011; Dorazco-Gonzalez, 2014). Very recently, dinuclear zinc complexes containing (benzimidazol-2-yl)benzene-based ligands have shown remarkable anti­cancer activities (Xie et al., 2014). Helical and non-helical complexes with copper(I) have been reported by Ruettimann et al. (1992). Palladium complexes with bromo-functionalized benzimid­azole derivatives have been utilized for Heck reactions (Reddy & Krishna, 2005).

A survey of the structural investigations of mercury halide complexes with benzimidazole derivatives have shown that they come in two main types, viz. polymeric, bridging either through the halide (Zhang et al., 2015; Li et al., 2007; Shen et al., 2005) or through alternative N atoms from the benzimidazole moieties (Xiao et al., 2009, 2011; Huang et al., 2006; Li et al., 2007, 2012a ,b ; Dey et al., 2013; Du et al., 2011; Chen et al., 2013; Su et al., 2003; Xu et al., 2011), or discrete mol­ecules, i.e. non-polymeric (Xiao et al., 2011; Wu et al., 2009; Zhao et al., 2012; Lou et al., 2012; Zhu et al., 2009; Carballo et al., 1993; Yan et al., 2012; Hu et al., 2012, 2015; Ding et al., 2012; Matthews et al., 1998; Manjunatha et al., 2011; Wang et al., 2007, 2009, 2012, 2015; Chen et al., 2014; Su et al., 2003; Quiroz-Castro et al., 2000; Yang & Luo, 2012; He et al., 2012; Bouchouit et al., 2015).

In the present case, during the attempted synthesis of the C-2 mercurated derivative 3 from 2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole), 1, using n-BuLi and mercuric chloride, the mercury complex 2 was isolated unexpectedly (Fig. 1).

Figure 1.

Figure 1

Diagram showing the the starting compound, 1, the title compound, 2, and the expected product, 3.

Structural commentary  

The structure of 2 with empirical formula, C26H25BrCl2HgN4, is reported in this paper. As a result of the presence of the Br and t-butyl substituents on the central ring, coordination of the HgII atom to this ring is prevented and thus a monomeric complex is formed, as has previously been observed for an HgCl2 complex with a similar ligand but with a central pyridine ring rather than a phenyl ring (Liu et al., 2007).

Another related structure has recently been reported of a dinuclear structure of HgCl2 with a similar ligand to 1 where there is a methyl substituent on the C1 atom of the imidazole ring (Hu et al., 2015). In the case of 2, however, a zigzag polymeric structure forms in the b-axis direction, in which the HgCl2 moiety is linked by atoms N1 from one ligand and N3 from an adjoining ligand. The coordination environment around the mercury atom is distorted tetra­hedral with bond angles ranging from 100.6 (2) to 126.35 (7)° (Fig. 2). The two Hg—N bond lengths are equivalent at 2.333 (4) and 2.338 (4) Å. However, the metal–halogen bonds are not similar [Hg—Cl1 = 2.4424 (13) and Hg—Cl2 = 2.4020 (15) Å]. The ligand adopts a conformation whereby the two benzimidazole moieties are not coplanar with each other or the central phenyl ring. The dihedral angles between the benzimidazole moieties N1/N2/C1–C7 and N3/N4/C19–C24 are 60.9 (2)° while they make dihedral angles of 55.6 (2) and 84.2 (2)°, respectively, with the central ring.graphic file with name e-73-00341-scheme1.jpg

Figure 2.

Figure 2

Diagram showing the three units which assemble to form a coordination polymer and illustrating its zigzag helical nature (with H atoms omitted for clarity). Displacement parameters are drawn at the 30% probability level. [Symmetry codes: (A) 1 − x, Inline graphic + y, z − Inline graphic; (B) 1 − x, y − Inline graphic, z − Inline graphic.]

Supra­molecular features  

The combination of HgCl2 with 2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole) results in a zigzag helical 1-D coordination polymer that propagates along the b-axis direction. This is mediated by the HgCl2 moiety, which is linked by atoms N1 from one ligand and N3 from an adjoining ligand (Fig. 2). Although helices are inherently chiral in nature, the overall structure is not chiral as the individual helices are related by a center of inversion. The inter­nal structure of this polymer is stabilized by both C—H⋯Cl and C—H⋯N inter­actions (Table 1). In addition, there are both C—H⋯π (Table 1) and π–π inter­actions [Cg6⋯Cg6(1 − x, −y, −z) = 3.531 (2) Å, where Cg6 is the centroid of the benzimidazole ring system N3/N4/C19–C24 and C25]. There are no halogen bonds or C—H⋯Br inter­actions present. Apart from van der Waals inter­actions, there are no significant inter­actions between the zigzag chains of the coordination polymer (Fig. 3).

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

Cg1 is the centroid of the imidazole ring N1/N2/C1/C2/C7.

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3A⋯N3i 0.95 2.65 3.459 (7) 144
C8—H8A⋯Cl2ii 0.98 2.71 3.643 (6) 160
C8—H8B⋯Cl1iii 0.98 2.82 3.719 (6) 152
C21—H21B⋯Cl1ii 0.95 2.77 3.616 (3) 149
C16—H16BCg1ii 0.98 2.91 3.671 (8) 135

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Figure 3.

Figure 3

Packing diagram showing two units of the polymer, which repeat in the b-axis direction, viewed along the a axis.

Database survey  

A search of the Cambridge Structural Database (Version 5.37 with updates May 2016; Groom et al., 2016) reveals that there is no report in the literature for a mercury complex with 2,2′-(2-bromo-5-tert-butyl-1,3-phenyl­ene)bis­(1-methyl-1H-benzimidazole) that has been structurally characterized. A cadmium complex, bis­[1,3-bis­(benzimidazol-2-yl)benzene]­dichlorido­cadmium(II), in which the Cd is coordinated by two Cl atoms and two N atoms in a distorted tetra­hedral configuration has been reported (Jiang et al., 2010). In the title complex 2, cadmium is replaced by an HgII atom along with a slight modification of the ligand.

Synthesis and crystallization  

To a solution of 1 (0.2 g, 0.42 mmol) in THF (15 ml) was added dropwise a solution of n-BuLi (0.3 ml, 0.47 mmol) at 195 K. The synthesis of compound 1 will be published elsewhere. The reaction mixture turned blue after immediate addition of n-BuLi. The reaction mixture was stirred for 30 min at 195 K followed by the addition of HgCl2 (0.126 g, 0.466 mmol). The reaction mixture was warmed to room temperature and stirred for 16 h. The reaction mixture was then filtered through Whatman filter paper and the solvent was evaporated on a rotary evaporator. Colourless plate-shaped crystals were obtained by the slow evaporation of an ethyl acetate solution of the compound at room temperature.

Yield 44% (0.138 g), 1H NMR (400 MHz, CDCl3): δ 7.88–7.86 (m, 3H), 7.45–7.34 (m, 7H), 3.98 (s, 6H), 1.46 (s, 9H). 13C NMR (100 MHz, DMSO): 152.3, 151.2, 141.6, 135.2, 131.8, 131.4, 123.3, 122.7, 121.6, 119.1, 111.0, 34.9, 31.1, 30.8. Analysis calculated for C26H25N4Cl2BrHg: C, 41.92; H, 3.38; N, 7.52. Found C, 42.68; H, 4.14; N, 6.29.

Refinement  

Crystal data, data collection and structure refinement details are summarized in Table 2. H atoms were positioned geomet­ric­ally and refined as riding: C—H = 0.95–0.98 Å with U iso(H) = 1.2U eq(C) or 1.5U eq(C) for methyl H atoms.

Table 2. Experimental details.

Crystal data
Chemical formula [HgCl2(C26H25BrN4)]
M r 744.90
Crystal system, space group Monoclinic, P21/c
Temperature (K) 123
a, b, c (Å) 9.50481 (18), 13.3872 (2), 20.3322 (4)
β (°) 93.0955 (19)
V3) 2583.36 (9)
Z 4
Radiation type Cu Kα
μ (mm−1) 14.57
Crystal size (mm) 0.37 × 0.09 × 0.03
 
Data collection
Diffractometer Agilent Xcalibur, Ruby, Gemini
Absorption correction Analytical [CrysAlis PRO (Agilent, 2012) based on expressions derived by Clark & Reid (1995)]
T min, T max 0.331, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 9778, 5217, 4596
R int 0.034
(sin θ/λ)max−1) 0.628
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.038, 0.104, 1.07
No. of reflections 5217
No. of parameters 300
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 1.34, −1.88

Computer programs: CrysAlis PRO (Agilent, 2012), SHELXS2013 (Sheldrick, 2008), SHELXL2016 (Sheldrick, 2015) and SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989017001888/zl2694sup1.cif

e-73-00341-sup1.cif (359KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017001888/zl2694Isup2.hkl

e-73-00341-Isup2.hkl (415.2KB, hkl)

CCDC reference: 1530778

Additional supporting information: crystallographic information; 3D view; checkCIF report

Acknowledgments

RJB is grateful for funding from NSF (award 1205608) and the Partnership for Reduced Dimensional Materials for partial funding of this research, to Howard University Nanoscience Facility for access to liquid nitro­gen, and the NSF–MRI program (grant No. CHE0619278) for funds to purchase the X-ray diffractometer. HBS is grateful to the DST, New Delhi, for a J. C. Bose National Fellowship. VR gratefully acknowledges the Council of Scientific and Industrial Research (CSIR), New Delhi, for a Senior Research Fellowship.

supplementary crystallographic information

Crystal data

[HgCl2(C26H25BrN4)] F(000) = 1432
Mr = 744.90 Dx = 1.915 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54184 Å
a = 9.50481 (18) Å Cell parameters from 4457 reflections
b = 13.3872 (2) Å θ = 3.9–74.8°
c = 20.3322 (4) Å µ = 14.57 mm1
β = 93.0955 (19)° T = 123 K
V = 2583.36 (9) Å3 Plate, colorless
Z = 4 0.37 × 0.09 × 0.03 mm

Data collection

Agilent Xcalibur, Ruby, Gemini diffractometer 5217 independent reflections
Radiation source: Enhance (Cu) X-ray Source 4596 reflections with I > 2σ(I)
Detector resolution: 10.5081 pixels mm-1 Rint = 0.034
ω scans θmax = 75.6°, θmin = 4.0°
Absorption correction: analytical [CrysAlis PRO (Agilent, 2012) based on expressions derived by Clark & Reid (1995)] h = −11→11
Tmin = 0.331, Tmax = 1.000 k = −10→16
9778 measured reflections l = −25→20

Refinement

Refinement on F2 0 restraints
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038 H-atom parameters constrained
wR(F2) = 0.104 w = 1/[σ2(Fo2) + (0.0583P)2] where P = (Fo2 + 2Fc2)/3
S = 1.07 (Δ/σ)max = 0.001
5217 reflections Δρmax = 1.34 e Å3
300 parameters Δρmin = −1.88 e Å3

Special details

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.

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

x y z Uiso*/Ueq
Hg 0.26669 (2) 0.15196 (2) 0.17398 (2) 0.03689 (9)
Br1 0.78523 (7) 0.01223 (6) 0.26403 (4) 0.05807 (19)
Cl1 0.07681 (12) 0.04507 (10) 0.12894 (8) 0.0455 (3)
Cl2 0.3350 (3) 0.17449 (13) 0.28849 (7) 0.0680 (5)
N1 0.4632 (4) 0.0840 (3) 0.12648 (19) 0.0297 (8)
N2 0.6469 (4) −0.0168 (3) 0.1125 (2) 0.0332 (8)
C1 0.5402 (5) 0.0084 (4) 0.1512 (2) 0.0290 (9)
C2 0.5243 (5) 0.1104 (4) 0.0687 (2) 0.0325 (10)
C3 0.4867 (6) 0.1831 (4) 0.0214 (2) 0.0380 (11)
H3A 0.407599 0.225411 0.026176 0.046*
C4 0.5690 (7) 0.1912 (5) −0.0326 (3) 0.0443 (13)
H4A 0.546152 0.239743 −0.065535 0.053*
C5 0.6869 (7) 0.1279 (5) −0.0392 (3) 0.0462 (13)
H5A 0.742376 0.136244 −0.076319 0.055*
C6 0.7235 (6) 0.0557 (4) 0.0054 (3) 0.0415 (12)
H6A 0.801480 0.012676 −0.000153 0.050*
C7 0.6402 (5) 0.0478 (4) 0.0599 (2) 0.0336 (10)
C8 0.7432 (5) −0.1007 (4) 0.1193 (3) 0.0412 (11)
H8A 0.706934 −0.149329 0.150248 0.062*
H8B 0.835960 −0.077071 0.136067 0.062*
H8C 0.751825 −0.132519 0.076325 0.062*
C9 0.5103 (5) −0.0449 (4) 0.2128 (2) 0.0295 (9)
C10 0.6114 (5) −0.0530 (4) 0.2651 (2) 0.0328 (9)
C11 0.5801 (5) −0.1064 (4) 0.3208 (2) 0.0347 (10)
C12 0.4486 (6) −0.1492 (4) 0.3257 (2) 0.0340 (10)
H12A 0.429536 −0.186816 0.363769 0.041*
C13 0.3436 (5) −0.1382 (4) 0.2757 (2) 0.0326 (10)
C14 0.3774 (5) −0.0858 (4) 0.2192 (2) 0.0301 (9)
H14A 0.307701 −0.078004 0.184253 0.036*
C15 0.1946 (6) −0.1774 (5) 0.2844 (3) 0.0446 (13)
C16 0.1931 (7) −0.2560 (6) 0.3375 (3) 0.0569 (16)
H16A 0.250243 −0.313200 0.325066 0.085*
H16B 0.096006 −0.277900 0.342884 0.085*
H16C 0.232117 −0.227992 0.379161 0.085*
C17 0.1086 (9) −0.0864 (7) 0.3074 (4) 0.069 (2)
H17A 0.014973 −0.108654 0.319073 0.103*
H17B 0.098912 −0.037282 0.271679 0.103*
H17C 0.157701 −0.055702 0.345930 0.103*
C18 0.1272 (7) −0.2131 (5) 0.2188 (3) 0.0504 (14)
H18A 0.189918 −0.261007 0.198742 0.076*
H18B 0.111504 −0.155783 0.189316 0.076*
H18C 0.036859 −0.245312 0.226242 0.076*
N3 0.7624 (4) −0.2007 (3) 0.3870 (2) 0.0334 (8)
N4 0.7052 (7) −0.0512 (4) 0.4249 (3) 0.0574 (15)
C19 0.6851 (6) −0.1200 (4) 0.3764 (3) 0.0389 (11)
C20 0.8389 (4) −0.1846 (3) 0.44605 (14) 0.0393 (11)
C21 0.9323 (4) −0.2448 (2) 0.48302 (18) 0.0436 (12)
H21B 0.958442 −0.308251 0.466606 0.052*
C22 0.9875 (5) −0.2123 (3) 0.54401 (18) 0.0604 (18)
H22B 1.051354 −0.253523 0.569280 0.073*
C23 0.9493 (6) −0.1196 (4) 0.56803 (19) 0.085 (3)
H23B 0.987023 −0.097343 0.609714 0.102*
C24 0.8559 (6) −0.0593 (3) 0.5311 (2) 0.092 (4)
H24B 0.829779 0.004111 0.547474 0.111*
C25 0.8007 (5) −0.0918 (3) 0.4701 (2) 0.0562 (17)
C26 0.6419 (11) 0.0482 (6) 0.4279 (4) 0.080 (3)
H26D 0.560680 0.052189 0.396154 0.121*
H26E 0.711628 0.098707 0.417059 0.121*
H26F 0.610913 0.060333 0.472366 0.121*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Hg 0.03625 (13) 0.03134 (14) 0.04333 (13) 0.00299 (7) 0.00463 (8) 0.00013 (8)
Br1 0.0463 (3) 0.0589 (4) 0.0671 (4) −0.0147 (3) −0.0146 (3) 0.0142 (3)
Cl1 0.0290 (5) 0.0381 (7) 0.0696 (8) −0.0006 (5) 0.0036 (5) 0.0048 (6)
Cl2 0.1242 (16) 0.0414 (8) 0.0383 (6) 0.0101 (9) 0.0035 (8) −0.0041 (6)
N1 0.0269 (18) 0.030 (2) 0.0319 (17) −0.0004 (15) 0.0016 (14) 0.0021 (15)
N2 0.0281 (18) 0.034 (2) 0.0383 (19) −0.0019 (16) 0.0042 (15) −0.0003 (17)
C1 0.0243 (19) 0.030 (2) 0.033 (2) −0.0040 (17) 0.0014 (16) −0.0013 (18)
C2 0.034 (2) 0.034 (3) 0.0289 (19) −0.0077 (19) −0.0034 (17) −0.0009 (19)
C3 0.044 (3) 0.034 (3) 0.035 (2) −0.010 (2) −0.002 (2) 0.005 (2)
C4 0.061 (3) 0.039 (3) 0.033 (2) −0.018 (3) −0.001 (2) 0.003 (2)
C5 0.051 (3) 0.053 (3) 0.035 (2) −0.023 (3) 0.009 (2) −0.006 (2)
C6 0.041 (3) 0.042 (3) 0.042 (2) −0.011 (2) 0.010 (2) −0.008 (2)
C7 0.032 (2) 0.032 (2) 0.037 (2) −0.0111 (19) 0.0068 (18) −0.0054 (19)
C8 0.030 (2) 0.037 (3) 0.057 (3) 0.002 (2) 0.008 (2) −0.003 (2)
C9 0.030 (2) 0.026 (2) 0.032 (2) 0.0013 (17) −0.0007 (17) 0.0030 (17)
C10 0.029 (2) 0.026 (2) 0.042 (2) −0.0050 (18) −0.0071 (18) 0.0024 (19)
C11 0.039 (2) 0.032 (3) 0.032 (2) 0.001 (2) −0.0086 (18) −0.0024 (19)
C12 0.039 (3) 0.032 (3) 0.030 (2) 0.0009 (19) 0.0011 (19) 0.0045 (18)
C13 0.031 (2) 0.036 (3) 0.032 (2) 0.0023 (19) 0.0047 (18) −0.0002 (18)
C14 0.027 (2) 0.033 (2) 0.0302 (19) 0.0032 (18) 0.0007 (16) −0.0002 (17)
C15 0.032 (3) 0.060 (4) 0.042 (3) −0.003 (2) 0.006 (2) 0.015 (3)
C16 0.057 (4) 0.061 (4) 0.053 (3) −0.016 (3) 0.005 (3) 0.009 (3)
C17 0.060 (4) 0.073 (5) 0.075 (5) 0.013 (4) 0.027 (3) 0.007 (4)
C18 0.047 (3) 0.050 (4) 0.054 (3) −0.020 (3) −0.004 (2) 0.011 (3)
N3 0.0333 (19) 0.027 (2) 0.0393 (19) −0.0024 (16) −0.0082 (16) 0.0031 (16)
N4 0.074 (4) 0.044 (3) 0.051 (3) 0.019 (3) −0.027 (3) −0.016 (2)
C19 0.045 (3) 0.034 (3) 0.037 (2) −0.001 (2) −0.011 (2) 0.003 (2)
C20 0.043 (3) 0.039 (3) 0.035 (2) −0.001 (2) −0.004 (2) 0.002 (2)
C21 0.042 (3) 0.042 (3) 0.045 (3) 0.004 (2) −0.006 (2) 0.007 (2)
C22 0.055 (4) 0.077 (5) 0.048 (3) 0.012 (3) −0.018 (3) 0.002 (3)
C23 0.106 (7) 0.090 (6) 0.055 (4) 0.031 (5) −0.043 (5) −0.027 (4)
C24 0.124 (8) 0.075 (6) 0.070 (5) 0.039 (5) −0.057 (5) −0.037 (4)
C25 0.070 (4) 0.049 (4) 0.048 (3) 0.013 (3) −0.021 (3) −0.005 (3)
C26 0.110 (7) 0.047 (4) 0.079 (5) 0.035 (4) −0.042 (5) −0.021 (4)

Geometric parameters (Å, º)

Hg—N1 2.333 (4) C13—C15 1.530 (7)
Hg—N3i 2.338 (4) C14—H14A 0.9500
Hg—Cl2 2.4020 (15) C15—C16 1.508 (8)
Hg—Cl1 2.4424 (13) C15—C18 1.525 (8)
Br1—C10 1.870 (5) C15—C17 1.553 (10)
N1—C1 1.331 (6) C16—H16A 0.9800
N1—C2 1.383 (6) C16—H16B 0.9800
N2—C1 1.359 (6) C16—H16C 0.9800
N2—C7 1.374 (7) C17—H17A 0.9800
N2—C8 1.452 (7) C17—H17B 0.9800
C1—C9 1.483 (6) C17—H17C 0.9800
C2—C3 1.401 (7) C18—H18A 0.9800
C2—C7 1.404 (7) C18—H18B 0.9800
C3—C4 1.387 (8) C18—H18C 0.9800
C3—H3A 0.9500 N3—C19 1.318 (7)
C4—C5 1.417 (10) N3—C20 1.387 (4)
C4—H4A 0.9500 N4—C19 1.355 (7)
C5—C6 1.358 (9) N4—C25 1.369 (6)
C5—H5A 0.9500 N4—C26 1.463 (9)
C6—C7 1.401 (7) C20—C21 1.3900
C6—H6A 0.9500 C20—C25 1.3900
C8—H8A 0.9800 C21—C22 1.3900
C8—H8B 0.9800 C21—H21B 0.9500
C8—H8C 0.9800 C22—C23 1.3900
C9—C14 1.389 (7) C22—H22B 0.9500
C9—C10 1.398 (6) C23—C24 1.3900
C10—C11 1.387 (7) C23—H23B 0.9500
C11—C12 1.383 (8) C24—C25 1.3900
C11—C19 1.478 (6) C24—H24B 0.9500
C12—C13 1.392 (7) C26—H26D 0.9800
C12—H12A 0.9500 C26—H26E 0.9800
C13—C14 1.399 (7) C26—H26F 0.9800
N1—Hg—N3i 100.59 (15) C16—C15—C18 112.8 (6)
N1—Hg—Cl2 105.64 (11) C16—C15—C13 111.5 (5)
N3i—Hg—Cl2 115.22 (11) C18—C15—C13 110.7 (5)
N1—Hg—Cl1 102.02 (10) C16—C15—C17 107.9 (6)
N3i—Hg—Cl1 103.38 (10) C18—C15—C17 107.8 (6)
Cl2—Hg—Cl1 126.35 (7) C13—C15—C17 105.7 (6)
C1—N1—C2 105.5 (4) C15—C16—H16A 109.5
C1—N1—Hg 125.2 (3) C15—C16—H16B 109.5
C2—N1—Hg 129.3 (3) H16A—C16—H16B 109.5
C1—N2—C7 106.8 (4) C15—C16—H16C 109.5
C1—N2—C8 128.6 (4) H16A—C16—H16C 109.5
C7—N2—C8 124.4 (4) H16B—C16—H16C 109.5
N1—C1—N2 112.5 (4) C15—C17—H17A 109.5
N1—C1—C9 123.9 (4) C15—C17—H17B 109.5
N2—C1—C9 123.5 (4) H17A—C17—H17B 109.5
N1—C2—C3 131.1 (5) C15—C17—H17C 109.5
N1—C2—C7 108.9 (4) H17A—C17—H17C 109.5
C3—C2—C7 120.0 (5) H17B—C17—H17C 109.5
C4—C3—C2 117.6 (6) C15—C18—H18A 109.5
C4—C3—H3A 121.2 C15—C18—H18B 109.5
C2—C3—H3A 121.2 H18A—C18—H18B 109.5
C3—C4—C5 120.8 (5) C15—C18—H18C 109.5
C3—C4—H4A 119.6 H18A—C18—H18C 109.5
C5—C4—H4A 119.6 H18B—C18—H18C 109.5
C6—C5—C4 122.5 (5) C19—N3—C20 106.0 (4)
C6—C5—H5A 118.7 C19—N3—Hgii 123.8 (3)
C4—C5—H5A 118.7 C20—N3—Hgii 129.2 (3)
C5—C6—C7 116.5 (6) C19—N4—C25 106.3 (5)
C5—C6—H6A 121.7 C19—N4—C26 127.3 (5)
C7—C6—H6A 121.7 C25—N4—C26 126.4 (5)
N2—C7—C6 131.2 (5) N3—C19—N4 112.5 (4)
N2—C7—C2 106.3 (4) N3—C19—C11 125.0 (5)
C6—C7—C2 122.5 (5) N4—C19—C11 122.4 (5)
N2—C8—H8A 109.5 N3—C20—C21 131.9 (3)
N2—C8—H8B 109.5 N3—C20—C25 108.0 (3)
H8A—C8—H8B 109.5 C21—C20—C25 120.0
N2—C8—H8C 109.5 C20—C21—C22 120.0
H8A—C8—H8C 109.5 C20—C21—H21B 120.0
H8B—C8—H8C 109.5 C22—C21—H21B 120.0
C14—C9—C10 119.3 (4) C23—C22—C21 120.0
C14—C9—C1 119.0 (4) C23—C22—H22B 120.0
C10—C9—C1 121.6 (4) C21—C22—H22B 120.0
C11—C10—C9 119.5 (4) C22—C23—C24 120.0
C11—C10—Br1 118.6 (3) C22—C23—H23B 120.0
C9—C10—Br1 121.8 (4) C24—C23—H23B 120.0
C12—C11—C10 120.4 (4) C23—C24—C25 120.0
C12—C11—C19 118.0 (5) C23—C24—H24B 120.0
C10—C11—C19 121.6 (5) C25—C24—H24B 120.0
C11—C12—C13 121.3 (5) N4—C25—C24 132.8 (3)
C11—C12—H12A 119.4 N4—C25—C20 107.2 (3)
C13—C12—H12A 119.4 C24—C25—C20 120.0
C12—C13—C14 117.7 (5) N4—C26—H26D 109.5
C12—C13—C15 120.7 (5) N4—C26—H26E 109.5
C14—C13—C15 121.5 (4) H26D—C26—H26E 109.5
C9—C14—C13 121.6 (4) N4—C26—H26F 109.5
C9—C14—H14A 119.2 H26D—C26—H26F 109.5
C13—C14—H14A 119.2 H26E—C26—H26F 109.5
C2—N1—C1—N2 −0.7 (5) C11—C12—C13—C15 −174.2 (5)
Hg—N1—C1—N2 178.9 (3) C10—C9—C14—C13 −2.4 (8)
C2—N1—C1—C9 −178.7 (4) C1—C9—C14—C13 179.1 (5)
Hg—N1—C1—C9 0.8 (6) C12—C13—C14—C9 −0.7 (8)
C7—N2—C1—N1 1.1 (5) C15—C13—C14—C9 176.1 (5)
C8—N2—C1—N1 −173.1 (5) C12—C13—C15—C16 −20.5 (8)
C7—N2—C1—C9 179.1 (4) C14—C13—C15—C16 162.8 (5)
C8—N2—C1—C9 4.9 (8) C12—C13—C15—C18 −147.0 (5)
C1—N1—C2—C3 178.3 (5) C14—C13—C15—C18 36.3 (8)
Hg—N1—C2—C3 −1.2 (8) C12—C13—C15—C17 96.5 (6)
C1—N1—C2—C7 0.0 (5) C14—C13—C15—C17 −80.2 (7)
Hg—N1—C2—C7 −179.5 (3) C20—N3—C19—N4 −0.1 (7)
N1—C2—C3—C4 −179.2 (5) Hgii—N3—C19—N4 169.2 (4)
C7—C2—C3—C4 −1.1 (7) C20—N3—C19—C11 −176.2 (5)
C2—C3—C4—C5 −0.1 (8) Hgii—N3—C19—C11 −6.9 (8)
C3—C4—C5—C6 1.4 (8) C25—N4—C19—N3 −1.0 (8)
C4—C5—C6—C7 −1.4 (8) C26—N4—C19—N3 177.1 (8)
C1—N2—C7—C6 −179.8 (5) C25—N4—C19—C11 175.2 (6)
C8—N2—C7—C6 −5.3 (8) C26—N4—C19—C11 −6.6 (12)
C1—N2—C7—C2 −1.0 (5) C12—C11—C19—N3 80.3 (8)
C8—N2—C7—C2 173.5 (4) C10—C11—C19—N3 −99.4 (7)
C5—C6—C7—N2 178.9 (5) C12—C11—C19—N4 −95.5 (7)
C5—C6—C7—C2 0.2 (7) C10—C11—C19—N4 84.8 (8)
N1—C2—C7—N2 0.6 (5) C19—N3—C20—C21 176.7 (4)
C3—C2—C7—N2 −177.9 (4) Hgii—N3—C20—C21 8.2 (7)
N1—C2—C7—C6 179.5 (4) C19—N3—C20—C25 1.1 (5)
C3—C2—C7—C6 1.0 (7) Hgii—N3—C20—C25 −167.4 (3)
N1—C1—C9—C14 54.6 (7) N3—C20—C21—C22 −175.2 (5)
N2—C1—C9—C14 −123.2 (5) C25—C20—C21—C22 0.0
N1—C1—C9—C10 −123.9 (5) C20—C21—C22—C23 0.0
N2—C1—C9—C10 58.3 (7) C21—C22—C23—C24 0.0
C14—C9—C10—C11 3.6 (8) C22—C23—C24—C25 0.0
C1—C9—C10—C11 −177.8 (5) C19—N4—C25—C24 −175.9 (4)
C14—C9—C10—Br1 −173.0 (4) C26—N4—C25—C24 5.9 (12)
C1—C9—C10—Br1 5.5 (7) C19—N4—C25—C20 1.7 (7)
C9—C10—C11—C12 −1.8 (8) C26—N4—C25—C20 −176.5 (8)
Br1—C10—C11—C12 175.0 (4) C23—C24—C25—N4 177.4 (7)
C9—C10—C11—C19 177.9 (5) C23—C24—C25—C20 0.0
Br1—C10—C11—C19 −5.4 (7) N3—C20—C25—N4 −1.8 (5)
C10—C11—C12—C13 −1.4 (8) C21—C20—C25—N4 −178.0 (5)
C19—C11—C12—C13 178.9 (5) N3—C20—C25—C24 176.2 (4)
C11—C12—C13—C14 2.6 (8) C21—C20—C25—C24 0.0

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

Hydrogen-bond geometry (Å, º)

Cg1 is the centroid of the imidazole ring N1/N2/C1/C2/C7.

D—H···A D—H H···A D···A D—H···A
C3—H3A···N3i 0.95 2.65 3.459 (7) 144
C8—H8A···Cl2ii 0.98 2.71 3.643 (6) 160
C8—H8B···Cl1iii 0.98 2.82 3.719 (6) 152
C21—H21B···Cl1ii 0.95 2.77 3.616 (3) 149
C16—H16B···Cg1ii 0.98 2.91 3.671 (8) 135

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

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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 datablock(s) I. DOI: 10.1107/S2056989017001888/zl2694sup1.cif

e-73-00341-sup1.cif (359KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017001888/zl2694Isup2.hkl

e-73-00341-Isup2.hkl (415.2KB, hkl)

CCDC reference: 1530778

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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