Crystal structure of di-μ-chlorido-bis­[di­chlorido(l-histidinium-κO)cadmium(II)]

Mohamedi, N.; Elleuch, S.; Boufas, S.; Legouira, M.; Djazi, F.

doi:10.1107/S205698901900690X

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ISSN: 2056-9890

Volume 75| Part 6| June 2019| Pages 823-825

https://doi.org/10.1107/S205698901900690X

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Crystal structure of di-μ-chlorido-bis[dichlorido(L-histidinium-κO)cadmium(II)]

Nacira Mohamedi,^a Slim Elleuch,^b Sihem Boufas,^a ^* Messaoud Legouira ^a and Faiçal Djazi ^c

^aLaboratoire de Géni-méncanique et Matériaux, Faculté de Technologie, Université de Skikda, 21000, Algeria, ^bLaboratoire de Physique Appliquée, Faculté des Sciences de Sfax, Université de Sfax, BP 1171, 3000 Sfax, Tunisia, and ^cLaboratoire de Recherche sur la Physico-chimie des Surfaces et Interfaces, Université de Skikda, 21000, Algeria
^*Correspondence e-mail: boufas_sihem@yahoo.fr

Edited by W. T. A. Harrison, University of Aberdeen, Scotland (Received 2 April 2019; accepted 13 May 2019; online 17 May 2019)

In the title compound, [Cd₂(C₆H₉N₃O₂)₂Cl₆], the coordination polyhedra around the Cd^II cations are distorted trigonal bipyramids. Two of the chloride ions (one axial and one equatorial) are bridging to the other metal atom, leading to a Cd⋯Cd separation of 3.9162 (4) Å. The O atom of the L-histidinium cation lies in an axial site. In the crystal, numerous N—H⋯Cl, N—H⋯O, C—H⋯O and C—H⋯Cl hydrogen bonds link the molecules into a three-dimensional network. Theoretical calculations and spectroscopic data are available as supporting information.

Keywords: X-ray diffraction; hybrid materials; dinuclear cadmium compounds; hydrogen bonds; electronic properties; crystal structure.

CCDC reference: 1915915

1. Chemical context

As a natural amino acid, L-histidine occurs in all organisms. It is a metal chelator in plants accumulating nickel from the soil (Krämer et al., 1996 ) and a part of the copper-transport system in human blood (Deschamps et al., 2005 ). Considerable efforts have been made to combine amino acids with organic and inorganic matrices to produce materials having a non-centrosymmetric cell, large polarizabilities and a strong non-linear optical coefficient (Ben Ahmed et al., 2008 ). As a chelating ligand, L-histidine provides up to three potential binding sites, as has been shown in complexes with nickel(II) (Sakurai et al., 1978 ), chromium(III) (Pennington et al., 1984 ), cobalt(III) (Herak et al., 1981 ), molybdenum(V) (Wu et al., 2005 ), vanadium(IV) (Islam et al., 2007 ) and copper(II) (Deschamps et al., 2005). In this work, we report the synthesis and structure of the title cadmium complex with L-histidine, (I). Cadmium is structurally interesting as it exhibits a number of coordination numbers and geometries such as those in [CdCl₄] (Boufas et al., 2009 ), [Cd₃Cl₁₁] (Kurawa et al., 2008 ), [CdCl₆]_n (Jarboui et al., 2011 ) and [CdCl₄]_n (Loseva et al., 2010 ).

2. Structural commentary

The molecular structure of the title compound is shown in Fig. 1. The asymmetric unit contains a [Cd₂Cl₆]²⁻ anionic core bridging a pair of histidinium cations via Cd—O bonds. Each cadmium atom is five-coordinated within a CdCl₄O environment, where atoms Cl3, Cl4 and Cl5 define the equatorial plane for Cd1, and Cl2 and O1 are in axial positions [O1—Cd1—Cl2 = 166.2 (1)°]. A similar coordination is observed for Cd2, and in this case the equatorial plane is formed by atoms Cl1, Cl2 and Cl6, while O3 and Cl5 are in equatorial positions [O3—Cd2—Cl5 = 165.2 (1)°]. Two μ-Cl atoms lead to a Cd₂Cl₂ square with a Cd1⋯Cd2 distance of 3.9162 (4) Å. The Cd—Cl distances lie in the range 2.4662 (12) to 2.7244 (14) Å for Cd1 and 2.4812 (11) to 2.7344 (14) Å for Cd2. The Cl—Cd—Cl angles are in the range of 82.61 (4) to 121.93 (3)°.

Figure 1
The asymmetric unit of (I)

, with displacement ellipsoids drawn at the 50% probability level.

In the histidinium cation, the α-amino and imidazole groups are protonated and positively charged, while the carboxyl group is deprotonated and negatively charged, which confirms that cations occur in their zwitterionic forms and carry a net positive charge. As expected, the imidazol rings are almost planar with r.m.s deviations for the non-H atoms of 0.003 Å in each molecule. The imidazol group is trans to the carboxyl group and gauche to the amino N atom.

The conformation of the histidine side chain can be described by the two torsion angles, χ₁ and χ₂₁ (IUPAC–IUB Commission on Biochemical Nomenclature, 1970 ). Angle χ₁, which defines the disposition of the side chain with respect to the main chain, can take values in the neighbourhood of −60, +60 or 180°, corresponding to the open conformation I (g⁻), closed conformation (g⁺) and open conformation II (t), respectively (Krause et al., 1991 ). The χ₂₁ values lie near −90 or +90° but the angle often deviates from these ideal values, as a result of interactions between the imidazole ring and other groups in the structure. In the title compound, the following values are seen: χ₁ = −52.9 (6); χ_1′ = −52.3 (5); χ₂₁ = −72.2 (7); χ_21′ = −82.5 (7)°. Hence, both histidinium cations adopt the sterically favourable open conformation in (I).

3. Supramolecular features

The extended structure of (I) is consolidated by a number of hydrogen-bonding (N—H⋯Cl and N—H⋯O) interactions (Table 1). The chloride anions and oxygen atoms play an important role in accepting hydrogen bonds from the amine N atom and the N atoms of the imidazolium ring. These interactions, together with weak C—H⋯Cl and C—H⋯O interactions, generate a three-dimensional network (Fig. 2).

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N1—H1A⋯O3ⁱ	0.89	2.01	2.881 (5)	167
N1—H1C⋯Cl6ⁱ	0.89	2.44	3.070 (4)	128
N2—H2⋯Cl4ⁱ	0.86	2.37	3.215 (5)	167
N3—H3⋯O4ⁱⁱ	0.86	1.99	2.751 (6)	146
N4—H11A⋯Cl1ⁱⁱⁱ	0.89	2.38	3.229 (4)	160
N4—H11B⋯Cl3^iv	0.89	2.70	3.426 (5)	140
N4—H11C⋯O1^v	0.89	1.96	2.846 (6)	171
N5—H22A⋯O2^iv	0.86	1.94	2.699 (6)	147
N6—H33⋯Cl6^v	0.86	2.28	3.137 (5)	174
C2—H2A⋯O4ⁱⁱ	0.98	2.56	3.252 (7)	128
C5—H5⋯Cl2ⁱ	0.93	2.79	3.424 (6)	126
C9—H33B⋯Cl3^vi	0.97	2.81	3.686 (6)	151
C11—H55⋯Cl5^v	0.93	2.71	3.405 (6)	132
C11—H55⋯O1^v	0.93	2.53	3.245 (7)	134
C12—H66⋯Cl1^iv	0.93	2.78	3.618 (6)	151
Symmetry codes: (i) x-1, y, z-1; (ii) x-1, y-1, z-1; (iii) x+1, y, z; (iv) x+1, y, z+1; (v) x+1, y+1, z+1; (vi) x, y, z+1.

Figure 2
Packing diagram for (I)

. Red dashed lines indicate hydrogen bonds.

4. Database survey

A search of the Cambridge Structural Database (Version 5.38, update May 2017; Groom et al., 2016 ) revealed that the geometric parameters of the title compound are similar to those found in bis(creatininium) tetrachloridocadmate(II) (Boufas et al., 2009). The imidazol group conformation of the title compound is in contrast to the bent gauche conformation found in the structure of L-HisH⁺·Cl⁻·H₂O (Donohue et al., 1956 , 1964 ), but similar to the trans conformation observed in DL-HisH⁺·Cl⁻·2H₂O (Steiner, 1996 )

5. Synthesis and crystallization

The title compound was prepared by dissolving 1 mmol (155.16 mg) of L-histidine in 50.0 ml of water with a mixture of CdCl₂·2H₂O (1 mmol) and HCl (8 mmol). The resulting mixture was capped and then heated at 353 K in a water bath for 1 h under continuous stirring and then left to slowly evaporate at room temperature. After two weeks, colourless crystals were obtained, which appear to be indefinitely stable when stored in air. Theoretical calculations and spectroscopic data are available as supporting information.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2. All H atoms were located in difference-Fourier maps and subsequently treated as riding atoms in geometrically idealized positions: N—H = 0.86 (NH) or 0.89 (NH₃) Å, C—H = 0.93 (cyclic), 0.97 (CH₂) or 0.98 (aliphatic C—H) Å with U_iso(H) = kU_eq(N,C), where k = 1.5 for the NH₃ and methyl groups (which were permitted to rotate but not to tilt) and 1.2 for all other H atoms.

Table 2
Experimental details

Crystal data
Chemical formula	[Cd₂(C₆H₉N₃O₂)₂Cl₆]
M_r	749.87
Crystal system, space group	Triclinic, P1
Temperature (K)	100
a, b, c (Å)	7.1540 (6), 8.2591 (6), 10.4459 (8)
α, β, γ (°)	108.502 (2), 97.499 (2), 94.512 (2)
V (Å³)	575.54 (8)
Z	1
Radiation type	Mo Kα
μ (mm⁻¹)	2.58
Crystal size (mm)	0.08 × 0.03 × 0.02

Data collection
Diffractometer	Bruker Nonius KappaCCD
Absorption correction	Multi-scan (SADABS; Sheldrick, 2003 )
T_min, T_max	0.820, 0.950
No. of measured, independent and observed [I > 2σ(I)] reflections	7735, 4856, 4799
R_int	0.025
(sin θ/λ)_max (Å⁻¹)	0.651

Refinement
R[F² > 2σ(F²)], wR(F²), S	0.024, 0.057, 1.08
No. of reflections	4856
No. of parameters	274
No. of restraints	3
H-atom treatment	H-atom parameters constrained
Δρ_max, Δρ_min (e Å⁻³)	1.33, −0.44
Absolute structure	Flack & Bernardinelli (2000 )
Absolute structure parameter	0.02 (2)
Computer programs: COLLECT(Nonius, 2002 ), DENZO and SCALEPACK (Otwinowski & Minor, 1997 ), SIR2014 (Burla et al., 2015 ), SHELXL2018 (Sheldrick, 2015 ), Mercury (Macrae et al., 2006 ), WinGX (Farrugia, 2012 ) and PARST (Nardelli, 1995 ).

Supporting information

CCDC reference: 1915915

Crystal structure: contains datablocks I, _Global. DOI: https://doi.org/10.1107/S205698901900690X/hb7815sup1.cif

Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S205698901900690X/hb7815Isup2.hkl

experimental and theoritical data of the title compound. DOI: https://doi.org/10.1107/S205698901900690X/hb7815sup3.docx

checkCIF report

Computing details top

Data collection: COLLECT(Nonius, 2002); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR2014 (Burla et al., 2015); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: WinGX (Farrugia, 2012) and PARST (Nardelli, 1995).

Di-µ-chlorido-bis[dichlorido(L-histidinium-κO)cadmium(II)] top

Crystal data top

[Cd₂(C₆H₉N₃O₂)₂Cl₆]	Z = 1
M_r = 749.87	F(000) = 364
Triclinic, P1	D_x = 2.163 Mg m⁻³
Hall symbol: P 1	Mo Kα radiation, λ = 0.71073 Å
a = 7.1540 (6) Å	Cell parameters from 6833 reflections
b = 8.2591 (6) Å	θ = 2.6–27.6°
c = 10.4459 (8) Å	µ = 2.58 mm⁻¹
α = 108.502 (2)°	T = 100 K
β = 97.499 (2)°	Block, colourless
γ = 94.512 (2)°	0.08 × 0.03 × 0.02 mm
V = 575.54 (8) Å³

Data collection top

Bruker Nonius KappaCCD diffractometer	4856 independent reflections
Radiation source: fine-focus sealed tube	4799 reflections with I > 2σ(I)
Graphite monochromator	R_int = 0.025
Detector resolution: 8.2632 pixels mm^-1	θ_max = 27.6°, θ_min = 2.6°
ω scans	h = −9→9
Absorption correction: multi-scan (SADABS; Sheldrick, 2003)	k = −10→10
T_min = 0.820, T_max = 0.950	l = −13→13
7735 measured reflections

Refinement top

Refinement on F²	Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full	H-atom parameters constrained
R[F² > 2σ(F²)] = 0.024	w = 1/[σ²(F_o²) + (0.0263P)²] where P = (F_o² + 2F_c²)/3
wR(F²) = 0.057	(Δ/σ)_max < 0.001
S = 1.08	Δρ_max = 1.33 e Å⁻³
4856 reflections	Δρ_min = −0.43 e Å⁻³
274 parameters	Absolute structure: Flack & Bernardinelli (2000)
3 restraints	Absolute structure parameter: 0.02 (2)

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.

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

	x	y	z	U_iso*/U_eq
Cd2	0.32732 (4)	0.13067 (3)	0.53489 (3)	0.00958 (10)
Cd1	0.21319 (4)	−0.04006 (3)	0.13444 (3)	0.00944 (10)
Cl2	0.5118 (2)	0.10427 (15)	0.34159 (13)	0.0111 (3)
Cl4	0.38809 (19)	−0.29705 (15)	0.05541 (13)	0.0118 (2)
Cl5	0.0240 (2)	0.02992 (15)	0.32637 (13)	0.0107 (3)
Cl1	0.25293 (19)	0.42775 (14)	0.63993 (13)	0.0131 (3)
Cl6	0.18541 (19)	−0.11633 (15)	0.59302 (13)	0.0138 (3)
Cl3	0.2694 (2)	0.17319 (16)	0.01896 (15)	0.0161 (3)
O3	0.5872 (5)	0.1400 (4)	0.6964 (4)	0.0117 (7)
C4	−0.3126 (9)	−0.3001 (7)	−0.4445 (6)	0.0096 (12)
O4	0.7438 (5)	0.3680 (4)	0.6649 (4)	0.0133 (8)
O1	−0.0490 (5)	−0.2181 (4)	−0.0211 (4)	0.0115 (7)
N1	−0.4829 (6)	−0.1360 (5)	−0.1962 (4)	0.0126 (9)
H1A	−0.447402	−0.043754	−0.218017	0.019*
H1B	−0.522967	−0.102932	−0.115773	0.019*
H1C	−0.576801	−0.202840	−0.260150	0.019*
O2	−0.2172 (6)	0.0068 (4)	0.0144 (4)	0.0133 (8)
C8	0.8474 (9)	0.3019 (6)	0.8662 (6)	0.0101 (11)
H22	0.891581	0.194267	0.870762	0.012*
N5	0.8879 (7)	0.3255 (6)	1.1983 (5)	0.0115 (10)
H22A	0.860404	0.215366	1.170454	0.014*
N2	−0.4575 (7)	−0.3273 (6)	−0.6510 (5)	0.0124 (10)
H2	−0.502332	−0.302327	−0.721887	0.015*
N3	−0.3875 (7)	−0.4694 (6)	−0.5153 (5)	0.0130 (10)
H3	−0.378659	−0.553255	−0.483665	0.016*
N4	1.0146 (6)	0.4309 (5)	0.8826 (4)	0.0107 (9)
H11A	1.054037	0.413115	0.802492	0.013*
H11B	1.108038	0.420170	0.943384	0.013*
H11C	0.981433	0.536510	0.911830	0.013*
C3	−0.2016 (8)	−0.2381 (6)	−0.3028 (5)	0.0097 (11)
H3A	−0.138831	−0.122866	−0.284998	0.012*
H3B	−0.103314	−0.311671	−0.298755	0.012*
C6	−0.4754 (9)	−0.4837 (7)	−0.6399 (6)	0.0135 (12)
H6	−0.537559	−0.584164	−0.706536	0.016*
C9	0.7299 (8)	0.3710 (6)	0.9811 (6)	0.0097 (11)
H33A	0.669343	0.465858	0.966065	0.012*
H33B	0.630052	0.280691	0.974320	0.012*
C1	−0.1857 (10)	−0.1393 (7)	−0.0503 (6)	0.0117 (13)
C5	−0.3564 (9)	−0.2120 (7)	−0.5316 (6)	0.0147 (13)
H5	−0.323972	−0.094758	−0.513781	0.018*
C2	−0.3185 (8)	−0.2340 (6)	−0.1874 (6)	0.0090 (11)
H2A	−0.362841	−0.351433	−0.192256	0.011*
C10	0.8396 (9)	0.4311 (7)	1.1223 (6)	0.0095 (12)
N6	0.9961 (7)	0.5842 (6)	1.3260 (5)	0.0129 (10)
H33	1.051801	0.670205	1.395165	0.015*
C12	0.9823 (9)	0.4198 (7)	1.3198 (6)	0.0137 (12)
H66	1.030715	0.378824	1.388932	0.016*
C7	0.7185 (9)	0.2673 (7)	0.7288 (6)	0.0086 (12)
C11	0.9078 (9)	0.5944 (6)	1.2053 (6)	0.0136 (12)
H55	0.896359	0.694526	1.183723	0.016*

Atomic displacement parameters (Å²) top

	U¹¹	U²²	U³³	U¹²	U¹³	U²³
Cd2	0.0101 (2)	0.00984 (15)	0.0073 (2)	−0.00029 (13)	−0.00021 (15)	0.00184 (13)
Cd1	0.0105 (2)	0.00944 (15)	0.0071 (2)	0.00022 (13)	−0.00009 (15)	0.00171 (13)
Cl2	0.0106 (7)	0.0129 (5)	0.0080 (6)	−0.0004 (5)	−0.0004 (5)	0.0020 (5)
Cl4	0.0112 (7)	0.0124 (5)	0.0097 (6)	0.0026 (5)	0.0001 (5)	0.0013 (4)
Cl5	0.0106 (7)	0.0127 (5)	0.0071 (6)	0.0004 (5)	0.0007 (5)	0.0016 (5)
Cl1	0.0155 (7)	0.0120 (5)	0.0111 (6)	0.0024 (5)	0.0040 (6)	0.0021 (5)
Cl6	0.0123 (7)	0.0171 (5)	0.0111 (6)	−0.0051 (5)	−0.0026 (5)	0.0069 (5)
Cl3	0.0145 (7)	0.0195 (5)	0.0185 (7)	0.0018 (5)	0.0022 (6)	0.0123 (5)
O3	0.012 (2)	0.0110 (14)	0.0090 (18)	−0.0013 (13)	−0.0035 (15)	0.0016 (13)
C4	0.008 (3)	0.013 (2)	0.007 (3)	0.001 (2)	0.002 (2)	0.001 (2)
O4	0.015 (2)	0.0168 (16)	0.0083 (19)	0.0010 (15)	−0.0007 (16)	0.0057 (14)
O1	0.012 (2)	0.0102 (14)	0.0091 (18)	0.0019 (14)	−0.0026 (15)	0.0000 (13)
N1	0.012 (2)	0.0147 (18)	0.011 (2)	0.0012 (17)	0.0015 (19)	0.0044 (17)
O2	0.016 (2)	0.0105 (14)	0.0098 (19)	0.0018 (13)	−0.0032 (16)	0.0005 (13)
C8	0.012 (3)	0.009 (2)	0.009 (3)	−0.003 (2)	−0.002 (2)	0.004 (2)
N5	0.011 (3)	0.0110 (18)	0.010 (3)	0.0024 (17)	0.003 (2)	0.0005 (17)
N2	0.014 (3)	0.019 (2)	0.006 (2)	0.0066 (19)	0.004 (2)	0.0040 (19)
N3	0.011 (3)	0.017 (2)	0.012 (2)	0.0009 (17)	0.001 (2)	0.0072 (18)
N4	0.014 (2)	0.0109 (16)	0.007 (2)	0.0009 (16)	0.0019 (18)	0.0030 (15)
C3	0.010 (3)	0.012 (2)	0.006 (3)	0.0005 (19)	0.001 (2)	0.0022 (19)
C6	0.010 (3)	0.016 (2)	0.012 (3)	−0.002 (2)	0.001 (2)	0.003 (2)
C9	0.009 (3)	0.009 (2)	0.010 (3)	0.0004 (18)	0.003 (2)	0.0012 (19)
C1	0.013 (3)	0.010 (2)	0.012 (3)	−0.001 (2)	0.001 (2)	0.005 (2)
C5	0.017 (3)	0.014 (2)	0.013 (3)	0.004 (2)	0.002 (3)	0.004 (2)
C2	0.009 (3)	0.012 (2)	0.006 (3)	0.003 (2)	0.002 (2)	0.002 (2)
C10	0.009 (3)	0.010 (2)	0.009 (3)	0.001 (2)	0.003 (2)	0.003 (2)
N6	0.012 (3)	0.015 (2)	0.008 (3)	−0.0009 (19)	0.001 (2)	−0.0014 (19)
C12	0.014 (3)	0.016 (3)	0.009 (3)	0.002 (2)	0.001 (2)	0.002 (2)
C7	0.010 (3)	0.008 (2)	0.006 (3)	0.001 (2)	0.002 (2)	−0.001 (2)
C11	0.017 (3)	0.012 (2)	0.012 (3)	0.000 (2)	0.003 (2)	0.004 (2)

Geometric parameters (Å, º) top

Cd1—O1	2.361 (4)	N5—C10	1.388 (6)
Cd1—Cl3	2.4662 (12)	N5—H22A	0.8600
Cd1—Cl5	2.5061 (14)	N2—C6	1.331 (7)
Cd1—Cl4	2.5155 (12)	N2—C5	1.374 (8)
Cd1—Cl2	2.7244 (14)	N2—H2	0.8600
Cd2—O3	2.320 (3)	N3—C6	1.335 (7)
Cd2—Cl1	2.4812 (11)	N3—H3	0.8600
Cd2—Cl6	2.4864 (12)	N4—H11A	0.8900
Cd2—Cl2	2.5155 (14)	N4—H11B	0.8900
Cd2—Cl5	2.7344 (14)	N4—H11C	0.8900
Cd2—Cd1	3.9162 (5)	C3—C2	1.548 (8)
O3—C7	1.280 (7)	C3—H3A	0.9700
C4—C5	1.355 (7)	C3—H3B	0.9700
C4—N3	1.383 (7)	C6—H6	0.9300
C4—C3	1.494 (8)	C9—C10	1.486 (8)
O4—C7	1.236 (6)	C9—H33A	0.9700
O1—C1	1.274 (7)	C9—H33B	0.9700
N1—C2	1.489 (6)	C1—C2	1.543 (9)
N1—H1A	0.8900	C5—H5	0.9300
N1—H1B	0.8900	C2—H2A	0.9800
N1—H1C	0.8900	C10—C11	1.362 (8)
O2—C1	1.236 (7)	N6—C12	1.334 (7)
C8—N4	1.492 (7)	N6—C11	1.366 (7)
C8—C7	1.531 (8)	N6—H33	0.8600
C8—C9	1.542 (8)	C12—H66	0.9300
C8—H22	0.9800	C11—H55	0.9300
N5—C12	1.319 (8)

O1—Cd1—Cl3	99.31 (8)	C8—N4—H11A	109.5
O1—Cd1—Cl5	91.97 (9)	C8—N4—H11B	109.5
Cl3—Cd1—Cl5	118.96 (4)	H11A—N4—H11B	109.5
O1—Cd1—Cl4	84.88 (8)	C8—N4—H11C	109.5
Cl3—Cd1—Cl4	113.33 (4)	H11A—N4—H11C	109.5
Cl5—Cd1—Cl4	127.41 (4)	H11B—N4—H11C	109.5
O1—Cd1—Cl2	166.16 (8)	C4—C3—C2	115.5 (5)
Cl3—Cd1—Cl2	94.41 (4)	C4—C3—H3A	108.4
Cl5—Cd1—Cl2	82.99 (4)	C2—C3—H3A	108.4
Cl4—Cd1—Cl2	87.97 (4)	C4—C3—H3B	108.4
O3—Cd2—Cl1	97.93 (9)	C2—C3—H3B	108.4
O3—Cd2—Cl6	85.65 (9)	H3A—C3—H3B	107.5
Cl1—Cd2—Cl6	121.93 (4)	N2—C6—N3	107.2 (5)
O3—Cd2—Cl2	95.70 (10)	N2—C6—H6	126.4
Cl1—Cd2—Cl2	112.59 (4)	N3—C6—H6	126.4
Cl6—Cd2—Cl2	124.74 (4)	C10—C9—C8	115.2 (5)
O3—Cd2—Cl5	165.13 (8)	C10—C9—H33A	108.5
Cl1—Cd2—Cl5	96.33 (4)	C8—C9—H33A	108.5
Cl6—Cd2—Cl5	83.27 (4)	C10—C9—H33B	108.5
Cl2—Cd2—Cl5	82.61 (4)	C8—C9—H33B	108.5
Cd2—Cl2—Cd1	96.64 (5)	H33A—C9—H33B	107.5
Cd1—Cl5—Cd2	96.62 (5)	O2—C1—O1	127.5 (6)
C7—O3—Cd2	117.6 (3)	O2—C1—C2	116.9 (5)
C5—C4—N3	105.7 (5)	O1—C1—C2	115.5 (5)
C5—C4—C3	129.8 (5)	C4—C5—N2	107.6 (5)
N3—C4—C3	124.5 (4)	C4—C5—H5	126.2
C1—O1—Cd1	114.9 (3)	N2—C5—H5	126.2
C2—N1—H1A	109.5	N1—C2—C1	108.2 (4)
C2—N1—H1B	109.5	N1—C2—C3	110.9 (4)
H1A—N1—H1B	109.5	C1—C2—C3	107.0 (5)
C2—N1—H1C	109.5	N1—C2—H2A	110.2
H1A—N1—H1C	109.5	C1—C2—H2A	110.2
H1B—N1—H1C	109.5	C3—C2—H2A	110.2
N4—C8—C7	110.6 (4)	C11—C10—N5	105.7 (5)
N4—C8—C9	109.8 (4)	C11—C10—C9	129.2 (4)
C7—C8—C9	108.1 (5)	N5—C10—C9	125.1 (5)
N4—C8—H22	109.4	C12—N6—C11	109.2 (5)
C7—C8—H22	109.4	C12—N6—H33	125.4
C9—C8—H22	109.4	C11—N6—H33	125.4
C12—N5—C10	109.6 (5)	N5—C12—N6	108.0 (5)
C12—N5—H22A	125.2	N5—C12—H66	126.0
C10—N5—H22A	125.2	N6—C12—H66	126.0
C6—N2—C5	109.5 (5)	O4—C7—O3	126.8 (6)
C6—N2—H2	125.3	O4—C7—C8	118.0 (5)
C5—N2—H2	125.3	O3—C7—C8	115.0 (4)
C6—N3—C4	110.1 (4)	C10—C11—N6	107.4 (4)
C6—N3—H3	125.0	C10—C11—H55	126.3
C4—N3—H3	125.0	N6—C11—H55	126.3

C5—C4—N3—C6	−0.7 (7)	C4—C3—C2—N1	−52.9 (6)
C3—C4—N3—C6	−178.8 (5)	C4—C3—C2—C1	−170.8 (4)
C5—C4—C3—C2	110.2 (7)	C12—N5—C10—C11	−0.8 (7)
N3—C4—C3—C2	−72.2 (7)	C12—N5—C10—C9	−179.0 (6)
C5—N2—C6—N3	0.1 (7)	C8—C9—C10—C11	99.8 (7)
C4—N3—C6—N2	0.4 (7)	C8—C9—C10—N5	−82.5 (7)
N4—C8—C9—C10	−52.3 (5)	C10—N5—C12—N6	0.5 (7)
C7—C8—C9—C10	−173.0 (4)	C11—N6—C12—N5	0.1 (7)
Cd1—O1—C1—O2	−18.4 (8)	Cd2—O3—C7—O4	−16.1 (8)
Cd1—O1—C1—C2	157.2 (3)	Cd2—O3—C7—C8	159.6 (4)
N3—C4—C5—N2	0.7 (7)	N4—C8—C7—O4	−13.9 (7)
C3—C4—C5—N2	178.7 (6)	C9—C8—C7—O4	106.4 (6)
C6—N2—C5—C4	−0.5 (7)	N4—C8—C7—O3	169.9 (4)
O2—C1—C2—N1	−11.4 (7)	C9—C8—C7—O3	−69.8 (5)
O1—C1—C2—N1	172.5 (5)	N5—C10—C11—N6	0.9 (7)
O2—C1—C2—C3	108.2 (6)	C9—C10—C11—N6	178.9 (6)
O1—C1—C2—C3	−67.8 (6)	C12—N6—C11—C10	−0.6 (7)

Hydrogen-bond geometry (Å, º) top

D—H···A	D—H	H···A	D···A	D—H···A
N1—H1A···O3ⁱ	0.89	2.01	2.881 (5)	167
N1—H1C···Cl6ⁱ	0.89	2.44	3.070 (4)	128
N2—H2···Cl4ⁱ	0.86	2.37	3.215 (5)	167
N3—H3···O4ⁱⁱ	0.86	1.99	2.751 (6)	146
N4—H11A···Cl1ⁱⁱⁱ	0.89	2.38	3.229 (4)	160
N4—H11B···Cl3^iv	0.89	2.70	3.426 (5)	140
N4—H11C···O1^v	0.89	1.96	2.846 (6)	171
N5—H22A···O2^iv	0.86	1.94	2.699 (6)	147
N6—H33···Cl6^v	0.86	2.28	3.137 (5)	174
C2—H2A···O4ⁱⁱ	0.98	2.56	3.252 (7)	128
C5—H5···Cl2ⁱ	0.93	2.79	3.424 (6)	126
C9—H33B···Cl3^vi	0.97	2.81	3.686 (6)	151
C11—H55···Cl5^v	0.93	2.71	3.405 (6)	132
C11—H55···O1^v	0.93	2.53	3.245 (7)	134
C12—H66···Cl1^iv	0.93	2.78	3.618 (6)	151

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

Acknowledgements

The authors thank Patricia Bénard-Rocherullé and Roisnel Thierry, Sciences Chimiques de Rennes (UMR CNRS 6226)University Rennes 1, France, for providing diffraction facilities.

Funding information

Funding for this research was provided by: 20 Aout 1955 University and LGMM Laboratory .

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