Crystal structure of di-μ-hydroxido-bis­[aqua­(1,10-phenanthroline-κ2N,N′)copper(II)] naphthalene-2,6-di­carboxyl­ate hexa­hydrate

Arias-Zárate, D.; Ballesteros-Rivas, M.F.; Toscano, R.A.; Valdés-Martínez, J.

doi:10.1107/S2056989015004338

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ISSN: 2056-9890

Volume 71| Part 4| April 2015| Pages 360-362

doi:10.1107/S2056989015004338

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Crystal structure of di-μ-hydroxido-bis[aqua(1,10-phenanthroline-κ²N,N′)copper(II)] naphthalene-2,6-dicarboxylate hexahydrate

Daniela Arias-Zárate,^a María Fernanda Ballesteros-Rivas,^b Rubén A. Toscano ^b and Jesús Valdés-Martínez ^b ^*

^aUVM Campus Toluca, Avenida las Palmas Poniente No. 439 San Jorge Pueblo Nuevo, CP 52164, Metepec, Estado de México, Mexico, and ^bInstituto de Química, Universidad Nacional Autónoma de México, Circuito Exterior s/n, Ciudad Universitaria, Cd. México, 04510, Coyoacán, México D.F., Mexico
^*Correspondence e-mail: jvaldes@unam.mx

Edited by D.-J. Xu, Zhejiang University (Yuquan Campus), China (Received 27 January 2015; accepted 2 March 2015; online 14 March 2015)

In the title compound, [Cu₂(OH)₂(C₁₂H₈N₂)₂(H₂O)₂](C₁₂H₆O₄)·6H₂O, the two hydroxide groups bridge the two Cu^II cations, forming a centrosymmetric binuclear complex cation, in which the Cu^II cation is coordinated by a 1,10-phenanthroline (phen) molecule, one water molecule and two bridging hydroxide O atoms in a distorted N₂O₃ square-pyramidal coordination geometry. The naphthalene-2,6-dicarboxylate anion is also located on an inversion centre. In the crystal, O—H⋯O hydrogen bonds link the cations, anions and lattice water molecules into a three-dimensional supramolecular architecture. Extensive π–π stacking is observed between the parallel or nearly parallel aromatic rings of adjacent phen ligands and naphthalenedicarboxylate anions, the centroid-to-centroid distances ranging from 3.4990 (16) to 3.8895 (16) Å.

Keywords: crystal structure; binuclear copper(II) complex; crystal engineering; hydrogen bonding; π–π stacking.

CCDC reference: 1051837

1. Chemical context

The designed arrangement of molecules through intermolecular interactions is one of the main purposes of crystal engineering. Among these interactions are hydrogen bonds and π–π stacking (Hunter & Sanders, 1990 ). π–π stacking interactions are ubiquitous in biological systems, and organic molecules (Riley & Hobza, 2013 ; Klärner & Schrader, 2013 ), and are present in many metal complexes (Janiak, 2000 ). Nevertheless, relatively few systems have been designed to be organized mainly by π–π interactions (Putta et al., 2014 ; Sebaoun et al., 2014 ; Valdés-Martínez et al., 2005 ). In most cases, they are secondary interactions helping to stabilize the network, not the main tool in the organization of the molecules in the crystal. We have proved that it is possible to obtain designed non-centrosymmetric crystals through π–π stacking interactions (Serrano-Becerra et al., 2009 ).

As part of a systematic study of the possible organization of copper coordination compounds controlled by π–π stacking interactions, we decided to use aromatic amines, as blocking ligands, and naphthalene-2,6-dicarboxylate as a possible bridging ligand between the [Cu(ammine)] moieties, as long as all of them may form π–π interactions. The reactions were done in water – the tendency of carboxylates to form hydrogen bonds with water is well known, as is their tendency to coordinate to Cu^II complexes – so these structures will give us an opportunity to evaluate the importance of water⋯ hydrogen bonding versus π–π interactions as the main interaction controlling the organization of the molecules in the crystal.

During these studies, the title compound was unexpectedly obtained. Its molecular and crystal structure are described herein.

2. Structural commentary

The asymmetric unit of the title compound contains half of a [(phen)(H₂O)Cu(OH)₂Cu(H₂O)(phen)] (phen is 1,10-phenanthroline) dimer, half of an naphthalene-2,6-dicarboxylate anion and three lattice water molecules. The Cu^II cation is pentacoordinated with a square-pyramidal geometry, the phen coordinates as a bidentate ligand through the N atoms, the hydroxide groups bridge the two Cu^II cations and a water molecule is coordinated in the apical position (Fig. 1). The carboxylate group of the naphthalene-2,6-dicarboxylate anion is twisted at 12.4 (3)° with respect to the naphthalene ring system.

Figure 1
The structure of the title compound showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are shown as circles of arbitrary radius.

3. Supramolecular features

An extensive network of hydrogen bonds is formed (Table 1) in the crystal. Atom O4 of the coordinating water molecule acts as a hydrogen-bond donor to O6 of a water molecule and carboxylate atom O1. The bridging hydroxide group hydrogen bonds to atom O5 of a water molecule and acts as a hydrogen-bond acceptor with water oxygen atom O7. The carboxylate atom O1 forms three hydrogen bonds while carboxylate atom O2 forms two hydrogen bonds. Water oxygen atoms O6 and O7 form hydrogen bonds with each other as well as with the carboxylate O atoms. The hydrogen-bond network extends into a three-dimensional structure, see Fig. 2. The presence of a free naphthalene-2,6-dicarboxylate with four hydrogen-bond acceptors requires the presence of water molecules, but the tendency of the aromatic rings in the ligands to form interactions may also observed and this is an important factor in the organization of the molecules in the crystal (Fig. 2). Two phenanthroline units from two adjacent cations lie parallel, on top of each other, the distance between the centroids of the ligand rings N7–C8–C10–C17–C18 and C15–C19–C20–N16—C14–C13 being 3.4990 (16) Å.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
O3—H3A⋯O5ⁱ	0.76 (1)	2.24 (2)	2.977 (3)	166 (3)
O4—H4A⋯O6	0.76 (1)	2.07 (2)	2.821 (3)	168 (4)
O4—H4B⋯O1ⁱ	0.76 (1)	2.01 (1)	2.769 (3)	176 (4)
O5—H5A⋯O1	0.76 (1)	2.27 (2)	2.993 (3)	159 (4)
O5—H5B⋯O2ⁱⁱ	0.76 (1)	2.13 (2)	2.846 (3)	156 (4)
O6—H6A⋯O1	0.76 (1)	2.13 (2)	2.882 (3)	167 (4)
O6—H6B⋯O7	0.77 (1)	2.04 (2)	2.782 (4)	164 (4)
O7—H7A⋯O3ⁱⁱⁱ	0.76 (1)	2.07 (1)	2.820 (3)	171 (4)
O7—H7B⋯O2^iv	0.76 (1)	2.00 (2)	2.744 (3)	165 (4)
Symmetry codes: (i) -x+1, -y+1, -z+1; (ii) $[-x+1, y+{\script{1\over 2}}, -z+{\script{1\over 2}}]$ ; (iii) -x+1, -y, -z+1; (iv) $[-x+1, y-{\script{1\over 2}}, -z+{\script{1\over 2}}]$ .

Figure 2
Crystal structure of the title compound viewed along the b axis, showing the hydrogen bonding, as dashed lines, and π–π stacking.

4. Database survey

There are reports of structures with naphthalene-2,6-dicarboxylate coordinating to Cu^II ions (Kanoo et al., 2009 ; Zhao et al., 2005 ; Gomez et al., 2007 ; He et al., 2005 ; Chen et al., 2010 ) as well as compounds with the naphthalene-2,6-dicarboxylate not coordinating (Tao et al., 2003 ; Han et al., 2012 ).

5. Synthesis and crystallization

Naphthalene-2,6-dicarboxylic acid (0.021 g, 0.10 mmol) was suspended in 10 ml of water; while stirring and heating, a concentrated solution of KOH was added until a transparent solution was obtained. A second solution was prepared by mixing 1,10-phenanthroline (0.018 g, 0.10 mmol) in MeOH (5 ml) and Cu(NO₃)₂·3H₂0 (0.018 g, 0.21 mmol) dissolved in water (5 ml). Both solutions were mixed and stirred under reflux for a period of 3 h. The clear-blue solution was slowly evaporated at room temperature. Blue crystals of the title compound were obtained after several days. The yield was not determined due to the poor stability of the compound out of solution.

6. Refinement

Crystal data, data collection and crystal structure refinement details are summarized in Table 2. The hydroxide H and water H atoms were located in a difference Fourier map and positional parameters were refined with U_iso(H) = 1.5U_eq(O). Aromatic H atoms were placed in calculated positions and refined in riding mode, C—H = 0.93 Å and U_iso(H) = 1.2U_eq(C).

Table 2
Experimental details

Crystal data
Chemical formula	[Cu₂(OH)₂(C₁₂H₈N₂)₂(H₂O)₂](C₁₂H₆O₄)·6H₂O
M_r	879.80
Crystal system, space group	Monoclinic, P2₁/c
Temperature (K)	298
a, b, c (Å)	9.3626 (16), 10.5812 (18), 18.648 (3)
β (°)	100.961 (3)
V (Å³)	1813.7 (5)
Z	2
Radiation type	Mo Kα
μ (mm⁻¹)	1.25
Crystal size (mm)	0.32 × 0.14 × 0.13

Data collection
Diffractometer	Bruker SMART APEX CCD
Absorption correction	Multi-scan (SADABS; Bruker, 2012 )
T_min, T_max	0.691, 0.858
No. of measured, independent and observed [I > 2σ(I)] reflections	12102, 4168, 3164
R_int	0.040
(sin θ/λ)_max (Å⁻¹)	0.651

Refinement
R[F² > 2σ(F²)], wR(F²), S	0.037, 0.087, 1.03
No. of reflections	4168
No. of parameters	280
No. of restraints	36
H-atom treatment	H atoms treated by a mixture of independent and constrained refinement
Δρ_max, Δρ_min (e Å⁻³)	0.41, −0.30
Computer programs: APEX2 and SAINT (Bruker, 2012), SHELXS2012 (Sheldrick, 2008 ), SHELXL2014 (Sheldrick, 2015 ), XP in SHELXTL (Sheldrick, 2008) and CIFTAB (Sheldrick, 2013 ).

Supporting information

CCDC reference: 1051837

Crystal structure: contains datablocks I, global. DOI: 10.1107/S2056989015004338/xu5835sup1.cif

Structure factors: contains datablock I. DOI: 10.1107/S2056989015004338/xu5835Isup2.hkl

checkCIF report

Computing details top

Data collection: APEX2 (Bruker, 2012); cell refinement: SAINT (Bruker, 2012); data reduction: SAINT (Bruker, 2012); program(s) used to solve structure: SHELXS2012 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: CIFTAB (Sheldrick, 2013).

Di-µ-hydroxido-bis[aqua(1,10-phenanthroline-κ²N,N')copper(II)] naphthalene-2,6-dicarboxylate hexahydrate top

Crystal data top

[Cu₂(OH)₂(C₁₂H₈N₂)₂(H₂O)₂](C₁₂H₆O₄)·6H₂O	F(000) = 908
M_r = 879.80	D_x = 1.611 Mg m⁻³
Monoclinic, P2₁/c	Mo Kα radiation, λ = 0.71073 Å
a = 9.3626 (16) Å	Cell parameters from 4729 reflections
b = 10.5812 (18) Å	θ = 2.2–27.5°
c = 18.648 (3) Å	µ = 1.25 mm⁻¹
β = 100.961 (3)°	T = 298 K
V = 1813.7 (5) Å³	Prism-hexagonal, blue
Z = 2	0.32 × 0.14 × 0.13 mm

Data collection top

Bruker SMART APEX CCD diffractometer	4168 independent reflections
Radiation source: fine-focus sealed tube	3164 reflections with I > 2σ(I)
Graphite monochromator	R_int = 0.040
Detector resolution: 8.333 pixels mm^-1	θ_max = 27.6°, θ_min = 2.2°
φ and ω scans	h = −12→12
Absorption correction: multi-scan (SADABS; Bruker, 2012)	k = −13→13
T_min = 0.691, T_max = 0.858	l = −24→24
12102 measured reflections

Refinement top

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)] = 0.037	Hydrogen site location: inferred from neighbouring sites
wR(F²) = 0.087	H atoms treated by a mixture of independent and constrained refinement
S = 1.03	w = 1/[σ²(F_o²) + (0.0327P)² + 0.9957P] where P = (F_o² + 2F_c²)/3
4168 reflections	(Δ/σ)_max = 0.001
280 parameters	Δρ_max = 0.41 e Å⁻³
36 restraints	Δρ_min = −0.30 e Å⁻³

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.

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

	x	y	z	U_iso*/U_eq
Cu1	0.36968 (3)	0.07336 (3)	0.50127 (2)	0.02290 (10)
O1	0.5472 (2)	0.60808 (19)	0.36776 (11)	0.0381 (5)
O2	0.6367 (2)	0.5229 (2)	0.27719 (11)	0.0495 (6)
O3	0.52734 (18)	−0.00259 (17)	0.57091 (9)	0.0261 (4)
H3A	0.571 (3)	0.047 (2)	0.5945 (15)	0.039*
O4	0.4830 (2)	0.26261 (19)	0.50689 (11)	0.0349 (5)
H4A	0.456 (4)	0.303 (3)	0.4734 (12)	0.052*
H4B	0.472 (4)	0.301 (3)	0.5401 (13)	0.052*
O5	0.3358 (3)	0.8164 (2)	0.31710 (13)	0.0498 (6)
H5A	0.387 (4)	0.760 (3)	0.319 (2)	0.075*
H5B	0.341 (4)	0.855 (3)	0.2833 (14)	0.075*
O6	0.3821 (3)	0.3788 (2)	0.37053 (15)	0.0525 (6)
H6A	0.414 (4)	0.4451 (19)	0.371 (2)	0.079*
H6B	0.428 (4)	0.333 (3)	0.352 (2)	0.079*
O7	0.5308 (3)	0.1767 (2)	0.32376 (12)	0.0459 (6)
H7A	0.519 (4)	0.135 (3)	0.3554 (15)	0.069*
H7B	0.491 (4)	0.140 (3)	0.2907 (14)	0.069*
C1	0.7904 (3)	0.5295 (2)	0.39346 (14)	0.0266 (6)
C2	0.9135 (3)	0.4941 (3)	0.36397 (14)	0.0306 (6)
H2	0.9045	0.4853	0.3137	0.037*
C3	1.0446 (3)	0.4728 (3)	0.40805 (14)	0.0304 (6)
H3	1.1242	0.4512	0.3874	0.036*
C4	0.9383 (3)	0.5169 (2)	0.51493 (14)	0.0255 (5)
C5	0.8052 (3)	0.5398 (2)	0.46729 (14)	0.0280 (6)
H5	0.7247	0.5627	0.4869	0.034*
C6	0.6480 (3)	0.5557 (3)	0.34251 (15)	0.0308 (6)
N7	0.1858 (2)	0.11609 (19)	0.43037 (11)	0.0232 (5)
C8	0.1602 (3)	0.1156 (3)	0.35799 (14)	0.0290 (6)
H8	0.2362	0.0970	0.3341	0.035*
C9	0.0233 (3)	0.1419 (3)	0.31650 (15)	0.0332 (6)
H9	0.0093	0.1403	0.2658	0.040*
C10	−0.0906 (3)	0.1702 (3)	0.35005 (15)	0.0320 (6)
H10	−0.1821	0.1876	0.3225	0.038*
C11	−0.1773 (3)	0.2011 (2)	0.46792 (16)	0.0314 (6)
H11	−0.2711	0.2198	0.4435	0.038*
C12	−0.1477 (3)	0.2013 (2)	0.54136 (15)	0.0304 (6)
H12	−0.2214	0.2205	0.5667	0.037*
C13	0.0330 (3)	0.1719 (3)	0.65763 (15)	0.0328 (6)
H13	−0.0365	0.1890	0.6859	0.039*
C14	0.1731 (3)	0.1457 (3)	0.69029 (15)	0.0341 (7)
H14	0.1999	0.1467	0.7409	0.041*
C15	0.2761 (3)	0.1174 (3)	0.64738 (14)	0.0290 (6)
H15	0.3708	0.0985	0.6704	0.035*
N16	0.2434 (2)	0.11657 (19)	0.57492 (11)	0.0230 (5)
C17	0.0737 (2)	0.1444 (2)	0.46436 (14)	0.0217 (5)
C18	−0.0673 (3)	0.1726 (2)	0.42647 (14)	0.0251 (5)
C19	0.1051 (2)	0.1448 (2)	0.54237 (13)	0.0215 (5)
C20	−0.0055 (3)	0.1728 (2)	0.58126 (14)	0.0256 (6)

Atomic displacement parameters (Å²) top

	U¹¹	U²²	U³³	U¹²	U¹³	U²³
Cu1	0.01878 (16)	0.02928 (18)	0.02090 (16)	0.00393 (13)	0.00440 (11)	0.00009 (14)
O1	0.0302 (10)	0.0441 (12)	0.0373 (11)	0.0069 (9)	−0.0002 (9)	−0.0061 (9)
O2	0.0487 (13)	0.0674 (16)	0.0277 (11)	0.0166 (12)	−0.0042 (10)	−0.0074 (11)
O3	0.0238 (9)	0.0330 (11)	0.0208 (9)	0.0057 (8)	0.0022 (7)	−0.0031 (8)
O4	0.0370 (11)	0.0312 (12)	0.0372 (12)	0.0013 (9)	0.0087 (10)	−0.0018 (9)
O5	0.0523 (14)	0.0594 (17)	0.0414 (14)	0.0069 (12)	0.0186 (12)	0.0011 (12)
O6	0.0476 (14)	0.0491 (15)	0.0640 (16)	−0.0027 (12)	0.0191 (12)	0.0028 (14)
O7	0.0475 (13)	0.0484 (15)	0.0392 (14)	−0.0100 (11)	0.0014 (11)	0.0018 (11)
C1	0.0296 (14)	0.0209 (13)	0.0275 (14)	−0.0008 (11)	0.0008 (11)	0.0012 (11)
C2	0.0365 (15)	0.0322 (15)	0.0234 (13)	0.0000 (12)	0.0064 (11)	0.0002 (12)
C3	0.0314 (14)	0.0313 (15)	0.0298 (15)	0.0036 (12)	0.0089 (12)	−0.0016 (12)
C4	0.0285 (13)	0.0197 (13)	0.0281 (14)	0.0028 (11)	0.0052 (11)	−0.0008 (11)
C5	0.0296 (14)	0.0258 (14)	0.0298 (14)	0.0055 (11)	0.0090 (11)	−0.0011 (11)
C6	0.0349 (15)	0.0251 (14)	0.0306 (14)	0.0007 (12)	0.0016 (12)	0.0001 (12)
N7	0.0212 (10)	0.0248 (11)	0.0238 (11)	0.0006 (9)	0.0051 (9)	0.0010 (9)
C8	0.0284 (14)	0.0328 (15)	0.0263 (14)	0.0013 (11)	0.0069 (11)	0.0026 (12)
C9	0.0389 (16)	0.0334 (16)	0.0244 (14)	−0.0006 (13)	−0.0015 (12)	0.0050 (12)
C10	0.0265 (14)	0.0296 (15)	0.0355 (15)	0.0007 (12)	−0.0049 (12)	0.0039 (12)
C11	0.0179 (12)	0.0284 (15)	0.0468 (17)	0.0033 (11)	0.0032 (12)	−0.0039 (13)
C12	0.0229 (13)	0.0282 (15)	0.0425 (17)	0.0005 (11)	0.0122 (12)	−0.0039 (12)
C13	0.0340 (15)	0.0335 (15)	0.0348 (15)	−0.0025 (13)	0.0166 (12)	−0.0080 (13)
C14	0.0397 (16)	0.0379 (17)	0.0261 (14)	−0.0018 (13)	0.0096 (12)	−0.0050 (12)
C15	0.0284 (14)	0.0307 (15)	0.0266 (14)	−0.0011 (11)	0.0023 (11)	−0.0034 (11)
N16	0.0194 (10)	0.0239 (11)	0.0257 (11)	0.0003 (9)	0.0042 (9)	−0.0011 (9)
C17	0.0188 (12)	0.0171 (12)	0.0292 (13)	−0.0001 (10)	0.0047 (10)	0.0008 (10)
C18	0.0210 (12)	0.0195 (13)	0.0334 (14)	−0.0014 (10)	0.0012 (10)	0.0017 (11)
C19	0.0186 (12)	0.0195 (13)	0.0269 (13)	−0.0016 (10)	0.0053 (10)	−0.0018 (10)
C20	0.0233 (13)	0.0210 (13)	0.0344 (15)	−0.0030 (10)	0.0106 (11)	−0.0050 (11)

Geometric parameters (Å, º) top

Cu1—O3	1.9448 (17)	C4—C4ⁱⁱ	1.420 (5)
Cu1—O3ⁱ	1.9482 (17)	C5—H5	0.9300
Cu1—N7	2.012 (2)	N7—C8	1.325 (3)
Cu1—N16	2.028 (2)	N7—C17	1.358 (3)
Cu1—O4	2.259 (2)	C8—C9	1.394 (4)
Cu1—Cu1ⁱ	2.9002 (7)	C8—H8	0.9300
O1—C6	1.261 (3)	C9—C10	1.368 (4)
O2—C6	1.251 (3)	C9—H9	0.9300
O3—Cu1ⁱ	1.9481 (17)	C10—C18	1.400 (4)
O3—H3A	0.757 (13)	C10—H10	0.9300
O4—H4A	0.762 (13)	C11—C12	1.345 (4)
O4—H4B	0.762 (13)	C11—C18	1.432 (4)
O5—H5A	0.760 (13)	C11—H11	0.9300
O5—H5B	0.763 (13)	C12—C20	1.429 (3)
O6—H6A	0.763 (13)	C12—H12	0.9300
O6—H6B	0.766 (13)	C13—C14	1.365 (4)
O7—H7A	0.762 (13)	C13—C20	1.401 (4)
O7—H7B	0.761 (13)	C13—H13	0.9300
C1—C5	1.362 (4)	C14—C15	1.398 (4)
C1—C2	1.419 (4)	C14—H14	0.9300
C1—C6	1.508 (4)	C15—N16	1.328 (3)
C2—C3	1.359 (4)	C15—H15	0.9300
C2—H2	0.9300	N16—C19	1.355 (3)
C3—C4ⁱⁱ	1.419 (4)	C17—C18	1.406 (3)
C3—H3	0.9300	C17—C19	1.428 (3)
C4—C5	1.407 (4)	C19—C20	1.404 (3)
C4—C3ⁱⁱ	1.419 (4)

O3—Cu1—O3ⁱ	83.69 (8)	C8—N7—C17	118.0 (2)
O3—Cu1—N7	167.78 (8)	C8—N7—Cu1	129.39 (17)
O3ⁱ—Cu1—N7	96.11 (8)	C17—N7—Cu1	112.53 (16)
O3—Cu1—N16	96.16 (8)	N7—C8—C9	122.3 (2)
O3ⁱ—Cu1—N16	169.61 (8)	N7—C8—H8	118.9
N7—Cu1—N16	81.84 (8)	C9—C8—H8	118.9
O3—Cu1—O4	92.59 (8)	C10—C9—C8	120.3 (3)
O3ⁱ—Cu1—O4	94.76 (8)	C10—C9—H9	119.9
N7—Cu1—O4	99.61 (8)	C8—C9—H9	119.9
N16—Cu1—O4	95.62 (8)	C9—C10—C18	119.0 (2)
O3—Cu1—Cu1ⁱ	41.89 (5)	C9—C10—H10	120.5
O3ⁱ—Cu1—Cu1ⁱ	41.80 (5)	C18—C10—H10	120.5
N7—Cu1—Cu1ⁱ	136.62 (6)	C12—C11—C18	121.3 (2)
N16—Cu1—Cu1ⁱ	137.11 (6)	C12—C11—H11	119.3
O4—Cu1—Cu1ⁱ	94.93 (6)	C18—C11—H11	119.3
Cu1—O3—Cu1ⁱ	96.31 (8)	C11—C12—C20	121.4 (2)
Cu1—O3—H3A	111 (2)	C11—C12—H12	119.3
Cu1ⁱ—O3—H3A	112 (2)	C20—C12—H12	119.3
Cu1—O4—H4A	112 (3)	C14—C13—C20	119.6 (2)
Cu1—O4—H4B	112 (3)	C14—C13—H13	120.2
H4A—O4—H4B	107 (4)	C20—C13—H13	120.2
H5A—O5—H5B	108 (4)	C13—C14—C15	119.8 (3)
H6A—O6—H6B	109 (4)	C13—C14—H14	120.1
H7A—O7—H7B	102 (4)	C15—C14—H14	120.1
C5—C1—C2	118.6 (2)	N16—C15—C14	122.2 (2)
C5—C1—C6	122.0 (2)	N16—C15—H15	118.9
C2—C1—C6	119.4 (2)	C14—C15—H15	118.9
C3—C2—C1	121.1 (2)	C15—N16—C19	118.1 (2)
C3—C2—H2	119.5	C15—N16—Cu1	129.74 (17)
C1—C2—H2	119.5	C19—N16—Cu1	112.16 (16)
C2—C3—C4ⁱⁱ	121.0 (2)	N7—C17—C18	123.2 (2)
C2—C3—H3	119.5	N7—C17—C19	116.7 (2)
C4ⁱⁱ—C3—H3	119.5	C18—C17—C19	120.2 (2)
C5—C4—C3ⁱⁱ	122.8 (2)	C10—C18—C17	117.2 (2)
C5—C4—C4ⁱⁱ	119.0 (3)	C10—C18—C11	124.3 (2)
C3ⁱⁱ—C4—C4ⁱⁱ	118.2 (3)	C17—C18—C11	118.4 (2)
C1—C5—C4	122.1 (2)	N16—C19—C20	123.4 (2)
C1—C5—H5	118.9	N16—C19—C17	116.7 (2)
C4—C5—H5	118.9	C20—C19—C17	119.9 (2)
O2—C6—O1	123.7 (3)	C13—C20—C19	116.8 (2)
O2—C6—C1	117.6 (2)	C13—C20—C12	124.4 (2)
O1—C6—C1	118.7 (2)	C19—C20—C12	118.8 (2)

C5—C1—C2—C3	−1.1 (4)	C9—C10—C18—C17	−0.5 (4)
C6—C1—C2—C3	178.3 (3)	C9—C10—C18—C11	179.9 (3)
C1—C2—C3—C4ⁱⁱ	1.1 (4)	N7—C17—C18—C10	0.3 (4)
C2—C1—C5—C4	0.2 (4)	C19—C17—C18—C10	−179.9 (2)
C6—C1—C5—C4	−179.2 (2)	N7—C17—C18—C11	−180.0 (2)
C3ⁱⁱ—C4—C5—C1	−180.0 (3)	C19—C17—C18—C11	−0.2 (4)
C4ⁱⁱ—C4—C5—C1	0.6 (5)	C12—C11—C18—C10	179.8 (3)
C5—C1—C6—O2	−167.8 (3)	C12—C11—C18—C17	0.1 (4)
C2—C1—C6—O2	12.9 (4)	C15—N16—C19—C20	−1.1 (4)
C5—C1—C6—O1	11.8 (4)	Cu1—N16—C19—C20	177.23 (19)
C2—C1—C6—O1	−167.6 (3)	C15—N16—C19—C17	179.4 (2)
C17—N7—C8—C9	−0.5 (4)	Cu1—N16—C19—C17	−2.3 (3)
Cu1—N7—C8—C9	176.7 (2)	N7—C17—C19—N16	−0.2 (3)
N7—C8—C9—C10	0.3 (4)	C18—C17—C19—N16	179.9 (2)
C8—C9—C10—C18	0.2 (4)	N7—C17—C19—C20	−179.8 (2)
C18—C11—C12—C20	−0.2 (4)	C18—C17—C19—C20	0.4 (4)
C20—C13—C14—C15	−1.4 (4)	C14—C13—C20—C19	0.6 (4)
C13—C14—C15—N16	1.0 (4)	C14—C13—C20—C12	−178.7 (3)
C14—C15—N16—C19	0.3 (4)	N16—C19—C20—C13	0.6 (4)
C14—C15—N16—Cu1	−177.7 (2)	C17—C19—C20—C13	−179.8 (2)
C8—N7—C17—C18	0.2 (4)	N16—C19—C20—C12	180.0 (2)
Cu1—N7—C17—C18	−177.50 (19)	C17—C19—C20—C12	−0.5 (4)
C8—N7—C17—C19	−179.7 (2)	C11—C12—C20—C13	179.7 (3)
Cu1—N7—C17—C19	2.7 (3)	C11—C12—C20—C19	0.4 (4)

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

Hydrogen-bond geometry (Å, º) top

D—H···A	D—H	H···A	D···A	D—H···A
O3—H3A···O5ⁱⁱⁱ	0.76 (1)	2.24 (2)	2.977 (3)	166 (3)
O4—H4A···O6	0.76 (1)	2.07 (2)	2.821 (3)	168 (4)
O4—H4B···O1ⁱⁱⁱ	0.76 (1)	2.01 (1)	2.769 (3)	176 (4)
O5—H5A···O1	0.76 (1)	2.27 (2)	2.993 (3)	159 (4)
O5—H5B···O2^iv	0.76 (1)	2.13 (2)	2.846 (3)	156 (4)
O6—H6A···O1	0.76 (1)	2.13 (2)	2.882 (3)	167 (4)
O6—H6B···O7	0.77 (1)	2.04 (2)	2.782 (4)	164 (4)
O7—H7A···O3ⁱ	0.76 (1)	2.07 (1)	2.820 (3)	171 (4)
O7—H7B···O2^v	0.76 (1)	2.00 (2)	2.744 (3)	165 (4)

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

Acknowledgements

DAZ acknowledges CONACYT–México for the SNI scholarship.

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