Literature DB >> 26090126

Crystal structure of an unknown solvate of bis-(tetra-n-butyl-ammonium) [N,N'-(4-tri-fluoro-methyl-1,2-phenyl-ene)bis-(oxamato)-κ(4) O,N,N',O']nickelate(II).

François Eya'ane Meva1, Dieter Schaarschmidt2, Tobias Rüffer2.   

Abstract

In the title compound, [N(C4H9)4]2[Ni(C11H3F3N2O6)] or [N(n-Bu)4]2[Ni(topbo)] [n-Bu = n-butyl and topbo = 4-tri-fluoro-methyl-1,2-phenyl-enebis(oxamate)], the Ni(2+) cation is coordinated by two deprotonated amido N atoms and two carboxyl-ate O atoms, setting up a slightly distorted square-planar coordination environment. The [Ni(topbo](2-) anion lies on a twofold rotation axis. Due to an incompatibility with the point-group symmetry of the complete mol-ecule, orientational disorder of the CF3 group is observed. The tetra-hedral ammonium cations and the anion are linked by weak inter-molecular C-H⋯O and C-H⋯F hydrogen-bonding inter-actions into a three-dimensional network. A region of electron density was treated with the SQUEEZE procedure in PLATON [Spek (2015). Acta Cryst. C71, 9-18] following unsuccessful attempts to model it as plausible solvent mol-ecule(s). The given chemical formula and other crystal data do not take into account the unknown solvent mol-ecule.

Entities:  

Keywords:  SQUEEZE procedure; crystal structure; disorder; nickel(II); non-symmetric compound; oxamate ligand

Year:  2015        PMID: 26090126      PMCID: PMC4459374          DOI: 10.1107/S205698901500835X

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

Oxamate-bridged polymetallic complexes are of inter­est in the discipline of supra­molecular magnetism as they exhibit diverse supra­molecular architectures and magnetic properties (Pardo et al., 2008 ▸; Kahn, 1987 ▸, 2000 ▸) and have been synthesized by, for example, Ruiz et al. (1997a ▸,b ▸), Berg et al. (2002 ▸), Martín et al. (2002 ▸) and Ottenwaelder et al. (2005 ▸). Over the last decade, we have been inter­ested in the synthesis of bis­(oxamates) and bis­(oxamate) complexes (Rüffer et al., 2007a ▸,b ▸, 2008 ▸, 2009 ▸; Eya’ane Meva et al., 2012 ▸), as well as their deposition as thin films (Bräuer et al., 2006 ▸, 2008 ▸, 2009 ▸). In order to optimize the deposition conditions and to increase the thin-film quality, the monometallic title compound, bis­(tetra-n-butyl­ammonium) [N,N′-(4-tri­fluoro­methyl-1,2-phenyl­ene)bis­(oxa­mato)-κ4 O,N,N′,O′]nickelate(II), (I), was prepared. The complex includes four sites of coordination and a CF3 group which provides a good solubility in organic solvents.

Structural commentary

The asymmetric unit of compound (I) contains one [N(n-Bu)4]+ cation and half of the complex anion [Ni(topbo)]2– (Fig. 1 ▸). The anion possesses point-group symmetry 2. This imposes orientational disorder of the CF3 group, which lies on both sides of the twofold rotation axis with 0.5 occupancy. The anion is essentially planar (root-mean-square deviation 0.145 Å), the highest deviation from planarity being observed for C6 [0.440 (5) Å]. The Ni2+ cation is coordinated by two deprotonated amido N atoms and two carboxyl­ate O atoms, resulting in a slightly distorted square-planar coordination geometry. In agreement with related nickel compounds, the Ni—N bonds are significantly shorter than the Ni—O bonds, which is due to the stronger donicity of the amido nitro­gens (Fettouhi et al., 1996 ▸; Rüffer et al., 2007a ▸,b ▸, 2008 ▸; Abdulmalic et al., 2013 ▸; Milek et al., 2013 ▸). Compared to the respective nickel complex without the CF3 group (Abdulmalic et al., 2013 ▸), compound (I) exhibits longer Ni—N and Ni—O bonds. It is instructive to note that for other complexes, the presence of electron-withdrawing substituents at the benzene moiety, e.g. Cl, NO2, causes a shortening of the Ni—N and Ni—O bonds (Fettouhi et al., 1996 ▸; Rüffer et al., 2008 ▸).
Figure 1

The mol­ecular components of (I) drawn with displacement ellipsoids at the 50% probability level. H atoms were omitted for clarity. Only one disordered part of the –CF3 group is shown. [Symmetry code: (A) −x + 2, y, −z + .]

Supra­molecular features

Five weak C—H⋯O and one weak C—H⋯F hydrogen bonds (Steiner, 2002 ▸) are observed in the crystal structure of (I) (Table 1 ▸), which connect the [N(n-Bu)4]+ cations and the [Ni(topbo)]2– anion, forming a three-dimensional network. A packing diagram is shown in Fig. 2 ▸.
Table 1

Hydrogen-bond geometry (, )

DHA DHHA D A DHA
C11H11AO10.972.423.347(2)160
C11H11BO1i 0.972.403.368(2)172
C15H15AO2ii 0.972.563.529(2)174
C17H17AO2iii 0.972.413.333(3)159
C19H19AO3i 0.972.553.441(2)152
C21H21BF10.972.293.208(4)156

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

Figure 2

Packing diagram of compound (I), with voids in the structure represented by yellow spheres [drawn using the CAVITYPLOT routine in PLATON (Spek, 2009 ▸)]. H atoms are omitted for clarity. Color code: black (C), blue (N), red (O), green (F), purple (Ni).

Synthesis and crystallization

4-Tri­fluoro­methyl-1,2-phenyl­enebis(ethyl oxamate) was prepared from ethyl oxalyl chloride and 4-tri­fluoro­methyl-1,2-phenyl­enedi­amine in analogy to Cervera et al. (1998 ▸). To a solution of 4-tri­fluoro­methyl-1,2-phenyl­enedi­amine (0.4 g, 2.22 mmol) dissolved in tetra­hydro­furan (50 ml) was added dropwise via a dropping funnel a solution of ethyl oxalyl chloride (5.05 g, 4.45 mmol) in tetra­hydro­furan (25 ml) within 20 min. The resulting mixture was refluxed for 30 min at 343 K, filtrated and concentrated to about one third on a rotary evaporator. The careful addition of water resulted in the precipitation of a brown solid which was filtered off and dried in air. To a solution of 4-tri­fluoro­methyl-1,2-phenyl­enebis(ethyl oxamate) (0.4 g, 1.06 mmol) in ethanol (40 ml) was added dropwise under stirring [N(n-Bu)4]OH (2.76 g, 4.25 mmol, 40 wt-% aqueous solution) in water (20 ml); the resulting mixture was refluxed for 30 min. After cooling to room temperature, an aqueous solution (20 ml) of NiCl2·6H2O (0.25 g, 1.05 mmol) was added dropwise under stirring. The yellow solution was filtered, concentrated to a volume of 20 ml on a rotatory evaporator, and extracted with di­chloro­methane (100 ml). The organic layer was separated, washed with water (3 x 25 ml) dried over Na2SO4 and concentrated to a volume of 10 ml. The title compound was precipitated by adding Et2O (100 ml). The yellow solid was filtered off, washed with Et2O and dried in air. Single crystals were obtained by the slow diffusion of Et2O into a saturated solution of the title compound in CH2Cl2/thf (1:1). The overall synthetic procedure is schematically shown in Fig. 3 ▸.
Figure 3

Scheme representing the synthesis of compound (I).

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▸. C-bonded H atoms were placed in calculated positions and constrained to ride on their parent atoms, with U iso(H) = 1.2U eq(C) and a C—H distance of 0.93 Å for aromatic and 0.97 Å for methyl­ene protons as well as U iso(H) = 1.5U eq(C) and a C—H distance of 0.96 Å for methyl protons.
Table 2

Experimental details

Crystal data
Chemical formula(C16H36N)2[Ni(C11H3F3N2O6)]
M r 859.78
Crystal system, space groupMonoclinic, C2/c
Temperature (K)110
a, b, c ()19.5285(3), 17.3370(3), 14.1484(3)
()92.136(2)
V (3)4786.83(15)
Z 4
Radiation typeCu K
(mm1)1.06
Crystal size (mm)0.10 0.08 0.06
 
Data collection
DiffractometerOxford Gemini S
Absorption correctionMulti-scan (CrysAlis RED; Oxford Diffraction, 2006)
T min, T max 0.807, 1.000
No. of measured, independent and observed [I > 2(I)] reflections15600, 3545, 3142
R int 0.023
max ()60.5
(sin /)max (1)0.564
 
Refinement
R[F 2 > 2(F 2)], wR(F 2), S 0.036, 0.102, 1.09
No. of reflections3545
No. of parameters277
H-atom treatmentH-atom parameters constrained
max, min (e 3)0.32, 0.20

Computer programs: CrysAlis CCD and CrysAlis RED (Oxford Diffraction, 2006 ▸), SHELXT (Sheldrick, 2015a ▸), SHELXL2013 (Sheldrick, 2015b ▸), SHELXTL (Sheldrick, 2008 ▸), ORTEP-3 for Windows and WinGX (Farrugia, 2012 ▸), PLATON (Spek, 2009 ▸), publCIF (Westrip, 2010 ▸) and SQUEEZE (Spek, 2015 ▸).

A small region of electron density at a distance of 1.6–3.7 Å from the tri­fluoro­methyl group indicates the presence of a disordered solvent mol­ecule. All attempts to model a disordered tetra­hydro­furan, di­chloro­methane or diethyl ether mol­ecule (solvents used for crystallization) failed. Therefore, the solvent contributions have been removed using the SQUEEZE procedure in PLATON (Spek, 2015 ▸). SQUEEZE calculated a void volume of approximately 310 Å3 occupied by 24 electrons per unit cell. Fig. 2 ▸ shows the positions of the voids within the unit cell. Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S205698901500835X/wm5144sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S205698901500835X/wm5144Isup2.hkl CCDC reference: 1062184 Additional supporting information: crystallographic information; 3D view; checkCIF report
(C16H36N)2[Ni(C11H3F3N2O6)]F(000) = 1856
Mr = 859.78Dx = 1.193 Mg m3
Monoclinic, C2/cCu Kα radiation, λ = 1.54184 Å
a = 19.5285 (3) ÅCell parameters from 5954 reflections
b = 17.3370 (3) Åθ = 4.5–60.4°
c = 14.1484 (3) ŵ = 1.06 mm1
β = 92.136 (2)°T = 110 K
V = 4786.83 (15) Å3Block, orange
Z = 40.1 × 0.08 × 0.06 mm
Oxford Gemini S diffractometerRint = 0.023
ω scansθmax = 60.5°, θmin = 3.4°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2006)h = −21→21
Tmin = 0.807, Tmax = 1.000k = −19→19
15600 measured reflectionsl = −15→15
3545 independent reflections2 standard reflections every 25 reflections
3142 reflections with I > 2σ(I) intensity decay: none
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.102w = 1/[σ2(Fo2) + (0.0577P)2 + 2.8029P] where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
3545 reflectionsΔρmax = 0.32 e Å3
277 parametersΔρmin = −0.20 e Å3
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.
xyzUiso*/UeqOcc. (<1)
C10.88594 (10)0.35368 (11)0.65544 (14)0.0356 (5)
C20.88021 (10)0.44362 (12)0.65187 (14)0.0370 (5)
C30.96883 (10)0.25942 (11)0.72161 (15)0.0371 (4)
C40.94040 (11)0.18979 (12)0.69174 (16)0.0454 (5)
H40.90110.18930.65250.055*
C50.97086 (14)0.12088 (13)0.72067 (18)0.0566 (6)
H50.95190.07430.70040.068*0.5
C70.68930 (10)0.16654 (11)0.76809 (14)0.0363 (4)
H7A0.66680.21050.79580.044*
H7B0.67290.12070.79930.044*
C80.76537 (10)0.17349 (11)0.79037 (14)0.0386 (5)
H8A0.78210.22200.76610.046*
H8B0.78950.13190.76000.046*
C90.77901 (12)0.16984 (13)0.89696 (15)0.0466 (5)
H9A0.75280.21000.92670.056*
H9B0.76310.12060.92010.056*
C100.85411 (13)0.17956 (14)0.92587 (17)0.0567 (6)
H10A0.85960.17680.99350.085*
H10B0.86990.22880.90450.085*
H10C0.88030.13930.89790.085*
C110.68357 (10)0.23650 (11)0.61193 (14)0.0356 (4)
H11A0.73210.24690.62240.043*
H11B0.67560.22770.54470.043*
C120.64405 (11)0.30812 (11)0.63902 (16)0.0412 (5)
H12A0.65070.31800.70620.049*
H12B0.59550.30060.62520.049*
C130.67014 (11)0.37655 (12)0.58245 (17)0.0466 (5)
H13A0.71960.37980.59120.056*
H13B0.65960.36790.51570.056*
C140.63858 (16)0.45253 (15)0.6120 (2)0.0789 (9)
H14A0.65580.49350.57390.118*
H14B0.65030.46230.67740.118*
H14C0.58970.44980.60320.118*
C150.59008 (10)0.14707 (11)0.66235 (14)0.0358 (4)
H15A0.58220.10010.69750.043*
H15B0.56840.18890.69560.043*
C160.55475 (10)0.13920 (11)0.56594 (14)0.0378 (5)
H16A0.56980.09220.53580.045*
H16B0.56680.18250.52650.045*
C170.47760 (10)0.13688 (13)0.57613 (16)0.0445 (5)
H17A0.46690.09990.62480.053*
H17B0.46220.18720.59660.053*
C180.43874 (11)0.11520 (15)0.48520 (17)0.0532 (6)
H18A0.39050.11470.49580.080*
H18B0.45290.06490.46530.080*
H18C0.44830.15220.43700.080*
C190.70443 (10)0.09850 (10)0.61375 (14)0.0348 (4)
H19A0.68710.09610.54870.042*
H19B0.75260.11210.61280.042*
C200.69831 (11)0.01936 (11)0.65738 (15)0.0390 (5)
H20A0.65090.00270.65300.047*
H20B0.71240.02170.72380.047*
C210.74277 (12)−0.03850 (12)0.60717 (17)0.0497 (6)
H21A0.7284−0.04100.54090.060*
H21B0.7901−0.02140.61110.060*
C220.73766 (14)−0.11826 (13)0.65073 (17)0.0544 (6)
H22A0.7661−0.15350.61760.082*
H22B0.6909−0.13560.64610.082*
H22C0.7527−0.11610.71610.082*
N10.94347 (8)0.33319 (9)0.70205 (12)0.0356 (4)
N20.66664 (8)0.16218 (9)0.66403 (11)0.0338 (4)
O10.84134 (7)0.31211 (8)0.61726 (10)0.0410 (3)
O20.92921 (7)0.48170 (7)0.69564 (10)0.0391 (3)
O30.83119 (7)0.47330 (8)0.60942 (10)0.0445 (4)
C60.9520 (2)0.0478 (2)0.6727 (4)0.0499 (11)0.5
F10.88379 (14)0.04371 (15)0.6729 (3)0.0760 (9)0.5
F20.96828 (17)0.03869 (15)0.5806 (2)0.0698 (8)0.5
F30.97597 (13)−0.01539 (13)0.7165 (2)0.0581 (7)0.5
Ni11.00000.41486 (2)0.75000.02432 (15)
U11U22U33U12U13U23
C10.0395 (11)0.0420 (11)0.0257 (11)0.0005 (9)0.0080 (8)0.0002 (8)
C20.0439 (11)0.0423 (11)0.0253 (11)0.0022 (9)0.0080 (9)0.0001 (9)
C30.0452 (10)0.0352 (10)0.0312 (11)0.0002 (8)0.0084 (8)0.0005 (8)
C40.0555 (13)0.0409 (12)0.0397 (13)−0.0012 (9)−0.0016 (10)−0.0032 (9)
C50.0773 (16)0.0352 (11)0.0563 (15)−0.0023 (11)−0.0124 (12)−0.0044 (11)
C70.0501 (11)0.0329 (10)0.0264 (11)−0.0015 (8)0.0098 (9)−0.0003 (8)
C80.0516 (12)0.0328 (10)0.0318 (12)−0.0029 (8)0.0068 (9)−0.0016 (8)
C90.0641 (14)0.0428 (12)0.0328 (13)−0.0020 (10)0.0028 (10)0.0022 (9)
C100.0729 (16)0.0570 (14)0.0396 (14)−0.0056 (12)−0.0062 (11)0.0000 (11)
C110.0407 (10)0.0342 (10)0.0322 (12)−0.0057 (8)0.0073 (8)0.0031 (8)
C120.0496 (12)0.0362 (11)0.0384 (13)−0.0024 (9)0.0106 (9)0.0017 (9)
C130.0521 (12)0.0381 (11)0.0505 (14)−0.0008 (9)0.0113 (10)0.0080 (10)
C140.097 (2)0.0411 (14)0.101 (3)0.0092 (14)0.0333 (18)0.0174 (14)
C150.0406 (11)0.0334 (10)0.0342 (12)−0.0024 (8)0.0120 (8)−0.0008 (8)
C160.0434 (11)0.0360 (10)0.0348 (12)−0.0025 (8)0.0108 (9)−0.0011 (8)
C170.0429 (11)0.0479 (12)0.0435 (13)−0.0054 (9)0.0114 (9)0.0027 (10)
C180.0421 (12)0.0666 (15)0.0510 (15)−0.0062 (10)0.0040 (10)0.0046 (11)
C190.0404 (10)0.0342 (10)0.0303 (11)−0.0004 (8)0.0087 (8)−0.0038 (8)
C200.0500 (12)0.0366 (10)0.0309 (12)−0.0019 (9)0.0079 (9)−0.0030 (8)
C210.0631 (14)0.0442 (12)0.0427 (14)0.0123 (10)0.0124 (11)0.0008 (10)
C220.0783 (16)0.0412 (12)0.0437 (14)0.0138 (11)0.0028 (12)−0.0010 (10)
N10.0391 (9)0.0356 (9)0.0324 (10)−0.0001 (7)0.0047 (7)−0.0002 (7)
N20.0427 (9)0.0326 (8)0.0266 (9)−0.0030 (7)0.0096 (7)−0.0009 (6)
O10.0432 (8)0.0456 (8)0.0344 (8)−0.0040 (6)0.0030 (6)−0.0010 (6)
O20.0435 (7)0.0365 (7)0.0376 (8)0.0027 (6)0.0048 (6)−0.0005 (6)
O30.0485 (8)0.0476 (8)0.0373 (9)0.0078 (7)0.0012 (7)0.0029 (6)
C60.050 (3)0.037 (2)0.062 (3)0.0017 (19)0.004 (2)−0.004 (2)
F10.0477 (16)0.0465 (15)0.134 (3)−0.0011 (12)0.0005 (16)−0.0231 (17)
F20.100 (2)0.0521 (16)0.0572 (19)0.0026 (15)−0.0005 (16)−0.0133 (14)
F30.0630 (17)0.0351 (13)0.076 (2)0.0013 (11)0.0042 (12)0.0005 (12)
Ni10.0293 (2)0.0226 (2)0.0215 (3)0.0000.00539 (16)0.000
C1—O11.239 (2)C14—H14B0.9600
C1—N11.330 (3)C14—H14C0.9600
C1—C21.564 (3)C15—C161.512 (3)
C2—O31.224 (2)C15—N21.517 (2)
C2—O21.300 (2)C15—H15A0.9700
C3—C41.388 (3)C15—H15B0.9700
C3—N11.396 (2)C16—C171.519 (3)
C3—C3i1.433 (4)C16—H16A0.9700
C4—C51.389 (3)C16—H16B0.9700
C4—H40.9300C17—C181.516 (3)
C5—C5i1.383 (5)C17—H17A0.9700
C5—H50.9300C17—H17B0.9700
C7—C81.512 (3)C18—H18A0.9600
C7—N21.523 (2)C18—H18B0.9600
C7—H7A0.9700C18—H18C0.9600
C7—H7B0.9700C19—C201.511 (3)
C8—C91.523 (3)C19—N21.519 (2)
C8—H8A0.9700C19—H19A0.9700
C8—H8B0.9700C19—H19B0.9700
C9—C101.517 (3)C20—C211.520 (3)
C9—H9A0.9700C20—H20A0.9700
C9—H9B0.9700C20—H20B0.9700
C10—H10A0.9600C21—C221.519 (3)
C10—H10B0.9600C21—H21A0.9700
C10—H10C0.9600C21—H21B0.9700
C11—C121.519 (3)C22—H22A0.9600
C11—N21.527 (2)C22—H22B0.9600
C11—H11A0.9700C22—H22C0.9600
C11—H11B0.9700N1—Ni11.9047 (16)
C12—C131.529 (3)O2—Ni11.9407 (13)
C12—H12A0.9700C6—F11.333 (5)
C12—H12B0.9700C6—F31.335 (5)
C13—C141.519 (3)C6—F21.361 (6)
C13—H13A0.9700F3—F3i1.308 (5)
C13—H13B0.9700Ni1—N1i1.9047 (16)
C14—H14A0.9600Ni1—O2i1.9408 (13)
O1—C1—N1128.92 (18)C16—C15—H15B108.2
O1—C1—C2121.17 (17)N2—C15—H15B108.2
N1—C1—C2109.91 (16)H15A—C15—H15B107.3
O3—C2—O2124.63 (18)C15—C16—C17109.73 (16)
O3—C2—C1119.25 (18)C15—C16—H16A109.7
O2—C2—C1116.12 (16)C17—C16—H16A109.7
C4—C3—N1127.00 (19)C15—C16—H16B109.7
C4—C3—C3i119.50 (12)C17—C16—H16B109.7
N1—C3—C3i113.51 (11)H16A—C16—H16B108.2
C3—C4—C5119.7 (2)C18—C17—C16113.12 (18)
C3—C4—H4120.1C18—C17—H17A109.0
C5—C4—H4120.1C16—C17—H17A109.0
C5i—C5—C4120.69 (13)C18—C17—H17B109.0
C5i—C5—H5119.7C16—C17—H17B109.0
C4—C5—H5119.7H17A—C17—H17B107.8
C8—C7—N2116.96 (15)C17—C18—H18A109.5
C8—C7—H7A108.1C17—C18—H18B109.5
N2—C7—H7A108.1H18A—C18—H18B109.5
C8—C7—H7B108.1C17—C18—H18C109.5
N2—C7—H7B108.1H18A—C18—H18C109.5
H7A—C7—H7B107.3H18B—C18—H18C109.5
C7—C8—C9109.72 (16)C20—C19—N2114.92 (16)
C7—C8—H8A109.7C20—C19—H19A108.5
C9—C8—H8A109.7N2—C19—H19A108.5
C7—C8—H8B109.7C20—C19—H19B108.5
C9—C8—H8B109.7N2—C19—H19B108.5
H8A—C8—H8B108.2H19A—C19—H19B107.5
C10—C9—C8113.21 (18)C19—C20—C21110.68 (17)
C10—C9—H9A108.9C19—C20—H20A109.5
C8—C9—H9A108.9C21—C20—H20A109.5
C10—C9—H9B108.9C19—C20—H20B109.5
C8—C9—H9B108.9C21—C20—H20B109.5
H9A—C9—H9B107.8H20A—C20—H20B108.1
C9—C10—H10A109.5C22—C21—C20111.33 (18)
C9—C10—H10B109.5C22—C21—H21A109.4
H10A—C10—H10B109.5C20—C21—H21A109.4
C9—C10—H10C109.5C22—C21—H21B109.4
H10A—C10—H10C109.5C20—C21—H21B109.4
H10B—C10—H10C109.5H21A—C21—H21B108.0
C12—C11—N2116.55 (16)C21—C22—H22A109.5
C12—C11—H11A108.2C21—C22—H22B109.5
N2—C11—H11A108.2H22A—C22—H22B109.5
C12—C11—H11B108.2C21—C22—H22C109.5
N2—C11—H11B108.2H22A—C22—H22C109.5
H11A—C11—H11B107.3H22B—C22—H22C109.5
C11—C12—C13108.66 (17)C1—N1—C3129.06 (17)
C11—C12—H12A110.0C1—N1—Ni1116.48 (13)
C13—C12—H12A110.0C3—N1—Ni1114.46 (13)
C11—C12—H12B110.0C15—N2—C19111.27 (14)
C13—C12—H12B110.0C15—N2—C7105.92 (14)
H12A—C12—H12B108.3C19—N2—C7111.10 (14)
C14—C13—C12112.47 (19)C15—N2—C11111.66 (14)
C14—C13—H13A109.1C19—N2—C11105.63 (14)
C12—C13—H13A109.1C7—N2—C11111.37 (14)
C14—C13—H13B109.1C2—O2—Ni1112.72 (12)
C12—C13—H13B109.1F1—C6—F3106.8 (4)
H13A—C13—H13B107.8F1—C6—F2105.4 (4)
C13—C14—H14A109.5F3—C6—F2105.0 (4)
C13—C14—H14B109.5F3i—F3—C6124.5 (2)
H14A—C14—H14B109.5N1i—Ni1—N183.96 (9)
C13—C14—H14C109.5N1i—Ni1—O2168.49 (6)
H14A—C14—H14C109.5N1—Ni1—O284.71 (6)
H14B—C14—H14C109.5N1i—Ni1—O2i84.72 (6)
C16—C15—N2116.49 (15)N1—Ni1—O2i168.49 (6)
C16—C15—H15A108.2O2—Ni1—O2i106.67 (8)
N2—C15—H15A108.2
O1—C1—C2—O3−1.0 (3)C3i—C3—N1—C1−176.8 (2)
N1—C1—C2—O3178.08 (18)C4—C3—N1—Ni1−176.64 (18)
O1—C1—C2—O2178.84 (17)C3i—C3—N1—Ni13.0 (3)
N1—C1—C2—O2−2.0 (2)C16—C15—N2—C19−58.4 (2)
N1—C3—C4—C5−177.5 (2)C16—C15—N2—C7−179.28 (16)
C3i—C3—C4—C52.9 (4)C16—C15—N2—C1159.3 (2)
C3—C4—C5—C5i0.3 (5)C20—C19—N2—C15−62.1 (2)
N2—C7—C8—C9−174.95 (15)C20—C19—N2—C755.7 (2)
C7—C8—C9—C10−177.74 (18)C20—C19—N2—C11176.60 (16)
N2—C11—C12—C13177.74 (17)C8—C7—N2—C15174.15 (16)
C11—C12—C13—C14−174.2 (2)C8—C7—N2—C1953.2 (2)
N2—C15—C16—C17−171.21 (16)C8—C7—N2—C11−64.3 (2)
C15—C16—C17—C18−169.98 (18)C12—C11—N2—C1550.4 (2)
N2—C19—C20—C21−175.07 (17)C12—C11—N2—C19171.52 (17)
C19—C20—C21—C22179.53 (19)C12—C11—N2—C7−67.8 (2)
O1—C1—N1—C3−0.8 (3)O3—C2—O2—Ni1−177.48 (16)
C2—C1—N1—C3−179.87 (18)C1—C2—O2—Ni12.7 (2)
O1—C1—N1—Ni1179.39 (16)F1—C6—F3—F3i−131.6 (5)
C2—C1—N1—Ni10.4 (2)F2—C6—F3—F3i116.8 (5)
C4—C3—N1—C13.6 (3)
D—H···AD—HH···AD···AD—H···A
C11—H11A···O10.972.423.347 (2)160
C11—H11B···O1ii0.972.403.368 (2)172
C15—H15A···O2iii0.972.563.529 (2)174
C17—H17A···O2iv0.972.413.333 (3)159
C19—H19A···O3ii0.972.553.441 (2)152
C21—H21B···F10.972.293.208 (4)156
  15 in total

1.  New Metal Oxamates as Precursors of Low-Dimensional Heterobimetallics.

Authors:  Mohammed Fettouhi; Lahcène Ouahab; Ali Boukhari; Olivier Cador; Corine Mathonière; Olivier Kahn
Journal:  Inorg Chem       Date:  1996-08-14       Impact factor: 5.165

2.  Transition metal induced derivatisations resulting in novel coordination behaviour of bis(oxamato) ligands.

Authors:  Tobias Rüffer; Björn Bräuer; François Eya'ane Meva; Bernhard Walfort
Journal:  Dalton Trans       Date:  2008-08-27       Impact factor: 4.390

3.  Magnetic and optical properties of Cu(II)-bis(oxamato) complexes: combined quantum chemical density functional theory and vibrational spectroscopy studies.

Authors:  Björn Bräuer; Florian Weigend; Federico Totti; Dietrich R T Zahn; Tobias Rüffer; Georgeta Salvan
Journal:  J Phys Chem B       Date:  2008-04-15       Impact factor: 2.991

4.  The formation of overlooked compounds in the reaction of methyl amine with the diethyl ester of o-phenylenebis(oxamic acid) in MeOH.

Authors:  Mohammad A Abdulmalic; Azar Aliabadi; Andreas Petr; Vladislav Kataev; Tobias Rüffer
Journal:  Dalton Trans       Date:  2012-11-20       Impact factor: 4.390

5.  Synthesis, structure, spectroscopy and redox chemistry of square-planar nickel(II) complexes with tetradentate o-phenylenedioxamidates and related ligands.

Authors:  Xavier Ottenwaelder; Ally Aukauloo; Yves Journaux; Rosa Carrasco; Joan Cano; Beatriz Cervera; Isabel Castro; Simona Curreli; M Carmen Muñoz; Antonio L Roselló; Bernardino Soto; Rafael Ruiz-García
Journal:  Dalton Trans       Date:  2005-05-25       Impact factor: 4.390

Review 6.  Ligand design for multidimensional magnetic materials: a metallosupramolecular perspective.

Authors:  Emilio Pardo; Rafael Ruiz-García; Joan Cano; Xavier Ottenwaelder; Rodrigue Lescouëzec; Yves Journaux; Francesc Lloret; Miguel Julve
Journal:  Dalton Trans       Date:  2008-04-10       Impact factor: 4.390

7.  SHELXT - integrated space-group and crystal-structure determination.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A Found Adv       Date:  2015-01-01       Impact factor: 2.290

8.  Crystal structure refinement with SHELXL.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr C Struct Chem       Date:  2015-01-01       Impact factor: 1.172

9.  1,4-Dihydro-benzo[g]quinoxaline-2,3-dione.

Authors:  François Eya'ane Meva; Dieter Schaarschmidt; Mohammad A Abdulmalic; Tobias Rüffer
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2012-11-28

10.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20
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