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Reaction of copper(I) thio­cyanate and tri­phenyl­phosphane with the bidentate Schiff base N,N′-bis­(trans-2-nitro­cinnamaldehyde)­ethyl­enedi­amine {Nca2en, (1); systematic name (1E,1′E,2E,2′E)-N,N′-(ethane-1,2-di­yl)bis­[3-(2-nitro­phen­yl)prop-2-en-1-imine]}, C20H18N4O4, in a 1:1:1 molar ratio in aceto­nitrile resulted in the formation of the complex {(1E,1′E,2E,2′E)-N,N′-(ethane-1,2-di­yl)bis­[3-(2-nitro­phen­yl)prop-2-en-1-imine]-κ2N,N′}(thio­cyanato-κN)(tri­phenyl­phosphane-κP)copper(I)], [Cu(NCS)(C20H18N4O4)(C18H15P)] or [Cu(NCS)(Nca2en)(PPh3)], (2). The Schiff base and copper(I) complex have been characterized by elemental analyses, IR, electronic and 1H NMR spectroscopy, and X-ray crystallography [from synchrotron data for (1)]. The mol­ecule of (1) lies on a crystallographic inversion centre, with a trans conformation for the ethyl­enedi­amine unit, and displays significant twists from coplanarity of its nitro group, aromatic ring, conjugated chain and especially ethyl­enedi­amine segments. It acts as a bidentate ligand coordinating via the imine N atoms to the CuI atom in complex (2), in which the ethyl­enedi­amine unit necessarily adopts a somewhat flattened gauche conformation, resulting in a rather bowed shape overall for the ligand. The NCS ligand is coordinated through its N atom. The geometry around the CuI atom is distorted tetra­hedral, with a small N—Cu—N bite angle of 81.56 (12)° and an enlarged opposite angle of 117.29 (9)° for SCN—Cu—P. Comparisons are made with the analogous Schiff base having no nitro substituents and with metal complexes of both ligands.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229615010815/lg3171sup1.cif
Contains datablocks global, 1, 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615010815/lg31711sup2.hkl
Contains datablock 1

mol

MDL mol file https://doi.org/10.1107/S2053229615010815/lg31711sup4.mol
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615010815/lg31712sup3.hkl
Contains datablock 2

mol

MDL mol file https://doi.org/10.1107/S2053229615010815/lg31712sup5.mol
Supplementary material

CCDC references: 999034; 999033

Computing details top

Data collection: APEX2 (Bruker, 2006) for (1); SMART (Bruker, 2006) for (2). Cell refinement: APEX2 (Bruker, 2006) for (1); SAINT (Bruker, 2006) for (2). Data reduction: APEX2 (Bruker, 2006) for (1); SAINT (Bruker, 2006) for (2). For both compounds, program(s) used to solve structure: SHELXTL (Sheldrick, 2008b); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: DIAMOND (Brandenburg, 2012). Software used to prepare material for publication: SHELXL2014/7 (Sheldrick, 2015) and local programs for (1); SHELXL2014 (Sheldrick, 2015) and local programs for (2).

(1) (E,E)-N,N'-Bis[(E)-3-(2-nitrophenyl)prop-2-en-1-ylidene]ethane-1,2-diamine top
Crystal data top
C20H18N4O4F(000) = 396
Mr = 378.38Dx = 1.425 Mg m3
Monoclinic, P21/nSynchrotron radiation, λ = 0.6727 Å
a = 11.441 (7) ÅCell parameters from 667 reflections
b = 3.781 (2) Åθ = 3.8–24.9°
c = 20.553 (12) ŵ = 0.10 mm1
β = 97.444 (10)°T = 120 K
V = 881.6 (9) Å3Plate, colourless
Z = 20.10 × 0.08 × 0.01 mm
Data collection top
Bruker APEXII CCD
diffractometer
2804 reflections with I > 2σ(I)
Radiation source: Daresbury SRS station 9.8Rint = 0.042
thin–slice ω scansθmax = 24.9°, θmin = 3.8°
Absorption correction: multi-scan
(TWINABS; Sheldrick, 2008a)
h = 1414
Tmin = 0.90, Tmax = 1.00k = 44
8304 measured reflectionsl = 2525
3085 independent reflections
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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.125H-atom parameters constrained
S = 0.97 w = 1/[σ2(Fo2) + (0.0714P)2]
where P = (Fo2 + 2Fc2)/3
3085 reflections(Δ/σ)max < 0.001
128 parametersΔρmax = 0.19 e Å3
0 restraintsΔρmin = 0.19 e Å3
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. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.9926 (2)0.5701 (7)0.53409 (11)0.0227 (6)
H1A1.01090.38070.56710.027*
H1B1.04790.76860.54560.027*
C20.8147 (2)0.5585 (6)0.57802 (11)0.0216 (5)
H20.85160.38680.60760.026*
C30.6941 (2)0.6670 (6)0.58311 (11)0.0216 (5)
H30.65700.82930.55170.026*
C40.6331 (2)0.5488 (6)0.62995 (11)0.0207 (6)
H40.67040.38400.66080.025*
C50.5119 (2)0.6585 (6)0.63654 (11)0.0205 (6)
C60.4326 (2)0.7507 (6)0.58151 (11)0.0230 (6)
H60.45860.74260.53950.028*
C70.3179 (2)0.8534 (7)0.58595 (12)0.0249 (6)
H70.26720.91970.54760.030*
C80.2772 (2)0.8591 (7)0.64661 (11)0.0248 (6)
H80.19850.93020.64990.030*
C90.3508 (2)0.7616 (7)0.70205 (12)0.0241 (6)
H90.32290.76010.74360.029*
C100.4660 (2)0.6657 (6)0.69655 (11)0.0209 (6)
N10.87125 (19)0.6910 (6)0.53446 (9)0.0219 (5)
N20.5416 (2)0.5838 (6)0.75785 (10)0.0263 (5)
O10.49714 (18)0.4252 (6)0.80087 (8)0.0371 (5)
O20.64449 (17)0.6823 (6)0.76401 (8)0.0362 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0171 (13)0.0241 (13)0.0275 (13)0.0013 (11)0.0055 (11)0.0015 (10)
C20.0213 (13)0.0208 (13)0.0223 (12)0.0015 (11)0.0017 (11)0.0025 (10)
C30.0207 (14)0.0212 (13)0.0228 (11)0.0016 (11)0.0027 (10)0.0005 (10)
C40.0186 (14)0.0210 (13)0.0218 (12)0.0007 (11)0.0006 (10)0.0017 (10)
C50.0209 (14)0.0168 (13)0.0244 (12)0.0023 (11)0.0054 (11)0.0011 (9)
C60.0232 (14)0.0232 (14)0.0233 (12)0.0018 (11)0.0053 (12)0.0005 (10)
C70.0205 (14)0.0270 (14)0.0267 (12)0.0007 (13)0.0016 (11)0.0021 (11)
C80.0156 (13)0.0262 (15)0.0332 (13)0.0016 (11)0.0054 (11)0.0003 (11)
C90.0203 (14)0.0288 (14)0.0245 (12)0.0045 (12)0.0084 (11)0.0008 (11)
C100.0203 (14)0.0206 (14)0.0213 (11)0.0027 (11)0.0010 (11)0.0006 (10)
N10.0176 (11)0.0247 (11)0.0241 (10)0.0012 (9)0.0053 (9)0.0012 (9)
N20.0209 (12)0.0350 (13)0.0238 (11)0.0026 (10)0.0061 (10)0.0022 (9)
O10.0322 (12)0.0533 (13)0.0270 (9)0.0045 (11)0.0087 (9)0.0126 (9)
O20.0169 (10)0.0620 (14)0.0295 (9)0.0023 (10)0.0018 (8)0.0076 (9)
Geometric parameters (Å, º) top
C1—C1i1.528 (5)C5—C101.402 (3)
C1—H1A0.990C6—H60.950
C1—H1B0.990C6—C71.383 (4)
C1—N11.463 (3)C7—H70.950
C2—H20.950C7—C81.386 (3)
C2—C31.456 (4)C8—H80.950
C2—N11.273 (3)C8—C91.376 (4)
C3—H30.950C9—H90.950
C3—C41.337 (3)C9—C101.386 (4)
C4—H40.950C10—N21.466 (3)
C4—C51.471 (3)N2—O11.232 (3)
C5—C61.399 (3)N2—O21.225 (3)
C1i—C1—H1A109.8C5—C6—C7122.5 (2)
C1i—C1—H1B109.8H6—C6—C7118.7
C1i—C1—N1109.3 (2)C6—C7—H7120.1
H1A—C1—H1B108.3C6—C7—C8119.7 (2)
H1A—C1—N1109.8H7—C7—C8120.1
H1B—C1—N1109.8C7—C8—H8120.0
H2—C2—C3119.6C7—C8—C9120.0 (3)
H2—C2—N1119.6H8—C8—C9120.0
C3—C2—N1120.8 (2)C8—C9—H9120.4
C2—C3—H3118.5C8—C9—C10119.3 (2)
C2—C3—C4123.0 (2)H9—C9—C10120.4
H3—C3—C4118.5C5—C10—C9123.0 (2)
C3—C4—H4118.0C5—C10—N2120.4 (2)
C3—C4—C5123.9 (2)C9—C10—N2116.5 (2)
H4—C4—C5118.0C1—N1—C2116.7 (2)
C4—C5—C6121.1 (2)C10—N2—O1117.8 (2)
C4—C5—C10123.5 (2)C10—N2—O2118.5 (2)
C6—C5—C10115.4 (2)O1—N2—O2123.7 (2)
C5—C6—H6118.7
N1—C2—C3—C4176.6 (2)C4—C5—C10—C9178.4 (2)
C2—C3—C4—C5179.1 (2)C4—C5—C10—N24.1 (4)
C3—C4—C5—C630.9 (4)C6—C5—C10—C90.9 (4)
C3—C4—C5—C10151.6 (2)C6—C5—C10—N2178.3 (2)
C4—C5—C6—C7179.7 (2)C3—C2—N1—C1178.9 (2)
C10—C5—C6—C72.0 (4)C1i—C1—N1—C2125.2 (3)
C5—C6—C7—C81.5 (4)C5—C10—N2—O1144.7 (2)
C6—C7—C8—C90.2 (4)C5—C10—N2—O236.7 (3)
C7—C8—C9—C101.4 (4)C9—C10—N2—O137.7 (3)
C8—C9—C10—C50.8 (4)C9—C10—N2—O2140.9 (2)
C8—C9—C10—N2176.7 (2)N1i—C1i—C1—N1180
Symmetry code: (i) x+2, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4···O20.952.452.788 (3)101
C4—H4···O2ii0.952.573.422 (3)149
C7—H7···N1iii0.952.613.519 (4)160
C8—H8···O1iv0.952.573.458 (4)155
C9—H9···O10.952.522.769 (3)95
Symmetry codes: (ii) x+3/2, y1/2, z+3/2; (iii) x+1, y+2, z+1; (iv) x+1/2, y+1/2, z+3/2.
(2) {(1E,1'E,2E,2'E)-N,N'-(Ethane-1,2-diyl)bis[3-(2-nitrophenyl)prop-2-en-1-imine]-κ2N,N'}(thiocyanato-κN)(triphenylphosphane-κP)copper(I)] top
Crystal data top
[Cu(NCS)(C20H18N4O4)(C18H15P)]Z = 2
Mr = 762.27F(000) = 788
Triclinic, P1Dx = 1.399 Mg m3
a = 9.1038 (8) ÅMo Kα radiation, λ = 0.71073 Å
b = 13.8186 (12) ÅCell parameters from 5264 reflections
c = 15.2972 (14) Åθ = 2.3–26.3°
α = 104.7831 (14)°µ = 0.75 mm1
β = 102.6778 (14)°T = 150 K
γ = 91.3000 (14)°Block, orange
V = 1809.0 (3) Å30.34 × 0.30 × 0.30 mm
Data collection top
Bruker SMART 1K CCD
diffractometer
6786 reflections with I > 2σ(I)
Radiation source: sealed tubeRint = 0.025
thin–slice ω scansθmax = 26.4°, θmin = 1.5°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2008a)
h = 1111
Tmin = 0.75, Tmax = 0.81k = 1717
14710 measured reflectionsl = 1919
7308 independent reflections
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)] = 0.069Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.130H-atom parameters constrained
S = 1.35 w = 1/[σ2(Fo2) + (0.0213P)2 + 4.1072P]
where P = (Fo2 + 2Fc2)/3
7308 reflections(Δ/σ)max < 0.001
460 parametersΔρmax = 0.76 e Å3
0 restraintsΔρmin = 0.65 e Å3
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
Cu10.43497 (5)0.33281 (3)0.31978 (3)0.01539 (12)
N11.1164 (4)0.1899 (3)0.6447 (3)0.0363 (9)
O11.0179 (4)0.2216 (3)0.6828 (2)0.0429 (8)
O21.2495 (5)0.1992 (4)0.6860 (3)0.0940 (19)
N20.4633 (4)0.3011 (2)0.4500 (2)0.0206 (7)
O30.2966 (4)0.8025 (2)0.2733 (2)0.0371 (7)
O40.1522 (4)0.8761 (2)0.1817 (3)0.0429 (8)
N30.3104 (3)0.4428 (2)0.3803 (2)0.0177 (6)
N40.2166 (4)0.8030 (3)0.1977 (3)0.0306 (8)
C11.0814 (5)0.1430 (3)0.5439 (3)0.0248 (8)
C21.1994 (5)0.0993 (3)0.5090 (3)0.0311 (9)
H21.29560.10160.54950.037*
C31.1776 (5)0.0526 (3)0.4158 (3)0.0342 (10)
H31.25760.02150.39160.041*
C41.0375 (5)0.0515 (3)0.3578 (3)0.0351 (10)
H41.02100.01950.29320.042*
C50.9209 (5)0.0968 (3)0.3930 (3)0.0290 (9)
H50.82600.09580.35160.035*
C60.9384 (4)0.1440 (3)0.4876 (3)0.0241 (8)
C70.8048 (4)0.1859 (3)0.5189 (3)0.0241 (8)
H70.79160.18060.57740.029*
C80.7016 (4)0.2309 (3)0.4697 (3)0.0234 (8)
H80.71720.24100.41320.028*
C90.5667 (4)0.2648 (3)0.4997 (3)0.0230 (8)
H90.55500.25970.55860.028*
C100.3289 (4)0.3330 (3)0.4839 (3)0.0250 (8)
H10A0.34430.33280.55000.030*
H10B0.24020.28580.44750.030*
C110.3008 (5)0.4383 (3)0.4740 (3)0.0244 (8)
H11A0.19950.45500.48390.029*
H11B0.37710.48780.52130.029*
C120.2507 (4)0.5137 (3)0.3497 (3)0.0211 (8)
H120.19760.55930.38670.025*
C130.2612 (4)0.5268 (3)0.2607 (3)0.0224 (8)
H130.31270.48040.22330.027*
C140.2011 (4)0.6016 (3)0.2294 (3)0.0228 (8)
H140.15450.64870.26950.027*
C150.2005 (4)0.6177 (3)0.1380 (3)0.0227 (8)
C160.1887 (4)0.5350 (3)0.0609 (3)0.0275 (9)
H160.19070.46940.06980.033*
C170.1742 (5)0.5464 (3)0.0282 (3)0.0303 (9)
H170.16720.48910.07920.036*
C180.1698 (5)0.6411 (4)0.0425 (3)0.0338 (10)
H180.15830.64860.10360.041*
C190.1820 (5)0.7246 (3)0.0312 (3)0.0325 (10)
H190.17980.78990.02160.039*
C200.1974 (4)0.7119 (3)0.1196 (3)0.0254 (8)
P10.31569 (10)0.21748 (6)0.19398 (6)0.01374 (19)
C210.3989 (4)0.0974 (3)0.1825 (2)0.0152 (7)
C220.4603 (4)0.0721 (3)0.2646 (3)0.0204 (8)
H220.45880.11770.32250.025*
C230.5239 (4)0.0185 (3)0.2633 (3)0.0268 (9)
H230.56510.03480.31990.032*
C240.5267 (4)0.0849 (3)0.1791 (3)0.0281 (9)
H240.57080.14670.17790.034*
C250.4658 (4)0.0616 (3)0.0971 (3)0.0249 (8)
H250.46680.10780.03940.030*
C260.4026 (4)0.0294 (3)0.0985 (3)0.0193 (7)
H260.36170.04520.04160.023*
C270.3137 (4)0.2494 (3)0.0845 (2)0.0165 (7)
C280.4350 (4)0.3106 (3)0.0812 (3)0.0224 (8)
H280.51700.33200.13410.027*
C290.4374 (4)0.3407 (3)0.0016 (3)0.0259 (8)
H290.52040.38310.00060.031*
C300.3196 (4)0.3093 (3)0.0762 (3)0.0254 (8)
H300.32130.33000.13070.030*
C310.1996 (4)0.2479 (3)0.0743 (3)0.0256 (8)
H310.11930.22510.12800.031*
C320.1955 (4)0.2192 (3)0.0058 (3)0.0213 (8)
H320.11090.17840.00690.026*
C330.1166 (4)0.1808 (3)0.1830 (2)0.0155 (7)
C340.0477 (4)0.0854 (3)0.1332 (3)0.0203 (8)
H340.10520.03610.10390.024*
C350.1039 (4)0.0623 (3)0.1264 (3)0.0261 (9)
H350.14980.00290.09290.031*
C360.1894 (5)0.1347 (3)0.1684 (3)0.0303 (9)
H360.29410.11960.16220.036*
C370.1212 (4)0.2277 (3)0.2188 (3)0.0255 (8)
H370.17850.27630.24910.031*
C380.0300 (4)0.2514 (3)0.2260 (3)0.0199 (8)
H380.07540.31650.26060.024*
N50.6208 (4)0.4041 (2)0.3132 (2)0.0232 (7)
C390.7137 (4)0.4576 (3)0.3062 (3)0.0245 (8)
S10.84730 (16)0.53232 (11)0.29704 (10)0.0519 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0173 (2)0.0141 (2)0.0127 (2)0.00109 (16)0.00241 (16)0.00084 (16)
N10.039 (2)0.036 (2)0.0279 (19)0.0180 (17)0.0045 (17)0.0070 (16)
O10.0356 (18)0.061 (2)0.0277 (17)0.0044 (16)0.0083 (14)0.0030 (15)
O20.062 (3)0.140 (5)0.047 (2)0.061 (3)0.017 (2)0.013 (3)
N20.0249 (16)0.0189 (15)0.0177 (15)0.0019 (13)0.0046 (13)0.0047 (12)
O30.0451 (19)0.0303 (16)0.0408 (19)0.0021 (14)0.0158 (16)0.0134 (14)
O40.0435 (19)0.0250 (16)0.071 (2)0.0142 (14)0.0235 (17)0.0219 (16)
N30.0194 (15)0.0146 (14)0.0187 (15)0.0028 (12)0.0056 (12)0.0025 (12)
N40.0294 (19)0.0238 (18)0.049 (2)0.0043 (15)0.0212 (18)0.0174 (16)
C10.029 (2)0.0224 (19)0.026 (2)0.0082 (16)0.0051 (17)0.0117 (16)
C20.030 (2)0.031 (2)0.038 (2)0.0086 (18)0.0086 (19)0.0176 (19)
C30.041 (3)0.035 (2)0.041 (3)0.017 (2)0.025 (2)0.020 (2)
C40.052 (3)0.039 (2)0.022 (2)0.014 (2)0.019 (2)0.0135 (19)
C50.033 (2)0.037 (2)0.022 (2)0.0062 (18)0.0069 (17)0.0161 (18)
C60.030 (2)0.0219 (19)0.025 (2)0.0037 (16)0.0072 (17)0.0139 (16)
C70.028 (2)0.026 (2)0.0189 (19)0.0023 (16)0.0053 (16)0.0071 (16)
C80.025 (2)0.026 (2)0.0177 (18)0.0013 (16)0.0007 (15)0.0067 (15)
C90.030 (2)0.0215 (19)0.0175 (18)0.0010 (16)0.0047 (16)0.0067 (15)
C100.028 (2)0.031 (2)0.0198 (19)0.0021 (17)0.0085 (16)0.0106 (16)
C110.028 (2)0.028 (2)0.0181 (19)0.0069 (17)0.0101 (16)0.0036 (16)
C120.0225 (19)0.0156 (17)0.0227 (19)0.0000 (15)0.0071 (15)0.0010 (14)
C130.0226 (19)0.0203 (19)0.027 (2)0.0065 (15)0.0094 (16)0.0069 (15)
C140.0203 (19)0.0177 (18)0.032 (2)0.0037 (15)0.0094 (16)0.0068 (16)
C150.0173 (18)0.025 (2)0.030 (2)0.0062 (15)0.0073 (16)0.0128 (16)
C160.023 (2)0.026 (2)0.037 (2)0.0080 (16)0.0078 (18)0.0148 (18)
C170.026 (2)0.036 (2)0.030 (2)0.0058 (18)0.0046 (18)0.0122 (19)
C180.027 (2)0.050 (3)0.034 (2)0.012 (2)0.0094 (19)0.024 (2)
C190.026 (2)0.035 (2)0.049 (3)0.0113 (18)0.013 (2)0.027 (2)
C200.0186 (19)0.024 (2)0.039 (2)0.0076 (16)0.0103 (17)0.0142 (17)
P10.0133 (4)0.0131 (4)0.0143 (4)0.0019 (3)0.0034 (3)0.0025 (3)
C210.0091 (15)0.0145 (16)0.0218 (18)0.0012 (13)0.0048 (14)0.0034 (14)
C220.0216 (18)0.0207 (18)0.0185 (18)0.0034 (15)0.0047 (15)0.0041 (15)
C230.027 (2)0.026 (2)0.029 (2)0.0074 (17)0.0001 (17)0.0146 (17)
C240.026 (2)0.0162 (18)0.044 (3)0.0082 (16)0.0129 (19)0.0075 (17)
C250.028 (2)0.0206 (19)0.027 (2)0.0019 (16)0.0169 (17)0.0016 (16)
C260.0183 (18)0.0206 (18)0.0191 (18)0.0035 (14)0.0062 (15)0.0036 (14)
C270.0178 (17)0.0181 (17)0.0138 (17)0.0051 (14)0.0049 (14)0.0031 (14)
C280.0219 (19)0.026 (2)0.0174 (18)0.0015 (16)0.0031 (15)0.0046 (15)
C290.024 (2)0.028 (2)0.030 (2)0.0008 (16)0.0127 (17)0.0101 (17)
C300.030 (2)0.030 (2)0.0212 (19)0.0132 (17)0.0126 (17)0.0109 (16)
C310.023 (2)0.035 (2)0.0173 (19)0.0056 (17)0.0020 (16)0.0065 (16)
C320.0185 (18)0.0231 (19)0.0218 (19)0.0020 (15)0.0036 (15)0.0060 (15)
C330.0140 (16)0.0172 (17)0.0166 (17)0.0007 (14)0.0028 (14)0.0076 (14)
C340.0181 (18)0.0226 (19)0.0211 (19)0.0032 (15)0.0058 (15)0.0059 (15)
C350.023 (2)0.028 (2)0.023 (2)0.0063 (16)0.0011 (16)0.0062 (16)
C360.0188 (19)0.037 (2)0.041 (3)0.0043 (17)0.0090 (18)0.019 (2)
C370.0221 (19)0.029 (2)0.029 (2)0.0092 (16)0.0111 (17)0.0095 (17)
C380.0185 (18)0.0181 (18)0.0250 (19)0.0040 (14)0.0078 (15)0.0067 (15)
N50.0208 (16)0.0238 (17)0.0216 (17)0.0042 (14)0.0055 (13)0.0001 (13)
C390.024 (2)0.028 (2)0.0189 (19)0.0036 (17)0.0079 (16)0.0015 (16)
S10.0490 (8)0.0519 (8)0.0543 (8)0.0218 (6)0.0266 (7)0.0030 (6)
Geometric parameters (Å, º) top
Cu1—N22.109 (3)C17—H170.950
Cu1—N32.067 (3)C17—C181.380 (6)
Cu1—P12.2049 (10)C18—H180.950
Cu1—N51.973 (3)C18—C191.374 (6)
N1—O11.205 (5)C19—H190.950
N1—O21.225 (5)C19—C201.386 (6)
N1—C11.471 (5)P1—C211.824 (3)
N2—C91.272 (5)P1—C271.834 (4)
N2—C101.465 (5)P1—C331.831 (3)
O3—N41.225 (5)C21—C221.391 (5)
O4—N41.230 (4)C21—C261.393 (5)
N3—C111.471 (5)C22—H220.950
N3—C121.273 (5)C22—C231.389 (5)
N4—C201.474 (5)C23—H230.950
C1—C21.386 (6)C23—C241.383 (6)
C1—C61.398 (5)C24—H240.950
C2—H20.950C24—C251.376 (6)
C2—C31.374 (6)C25—H250.950
C3—H30.950C25—C261.391 (5)
C3—C41.383 (6)C26—H260.950
C4—H40.950C27—C281.393 (5)
C4—C51.385 (6)C27—C321.391 (5)
C5—H50.950C28—H280.950
C5—C61.399 (6)C28—C291.389 (5)
C6—C71.479 (5)C29—H290.950
C7—H70.950C29—C301.383 (6)
C7—C81.338 (5)C30—H300.950
C8—H80.950C30—C311.378 (6)
C8—C91.449 (5)C31—H310.950
C9—H90.950C31—C321.388 (5)
C10—H10A0.990C32—H320.950
C10—H10B0.990C33—C341.397 (5)
C10—C111.522 (5)C33—C381.393 (5)
C11—H11A0.990C34—H340.950
C11—H11B0.990C34—C351.385 (5)
C12—H120.950C35—H350.950
C12—C131.442 (5)C35—C361.395 (6)
C13—H130.950C36—H360.950
C13—C141.326 (5)C36—C371.371 (6)
C14—H140.950C37—H370.950
C14—C151.470 (5)C37—C381.382 (5)
C15—C161.400 (6)C38—H380.950
C15—C201.399 (5)N5—C391.151 (5)
C16—H160.950C39—S11.629 (4)
C16—C171.390 (6)
N2—Cu1—N381.56 (12)C16—C17—C18120.0 (4)
N2—Cu1—P1118.76 (9)H17—C17—C18120.0
N2—Cu1—N5110.10 (13)C17—C18—H18119.8
N3—Cu1—P1117.58 (9)C17—C18—C19120.4 (4)
N3—Cu1—N5105.80 (12)H18—C18—C19119.8
P1—Cu1—N5117.29 (9)C18—C19—H19120.6
O1—N1—O2122.5 (4)C18—C19—C20118.8 (4)
O1—N1—C1120.5 (4)H19—C19—C20120.6
O2—N1—C1116.9 (4)N4—C20—C15119.2 (4)
Cu1—N2—C9134.3 (3)N4—C20—C19117.6 (4)
Cu1—N2—C10106.0 (2)C15—C20—C19123.2 (4)
C9—N2—C10119.7 (3)Cu1—P1—C21112.49 (11)
Cu1—N3—C11112.5 (2)Cu1—P1—C27114.52 (12)
Cu1—N3—C12129.1 (3)Cu1—P1—C33118.05 (12)
C11—N3—C12118.2 (3)C21—P1—C27105.11 (16)
O3—N4—O4124.0 (4)C21—P1—C33102.08 (15)
O3—N4—C20118.9 (3)C27—P1—C33103.01 (16)
O4—N4—C20117.1 (4)P1—C21—C22116.6 (3)
N1—C1—C2115.7 (4)P1—C21—C26125.0 (3)
N1—C1—C6121.6 (4)C22—C21—C26118.3 (3)
C2—C1—C6122.6 (4)C21—C22—H22119.4
C1—C2—H2119.9C21—C22—C23121.1 (3)
C1—C2—C3120.2 (4)H22—C22—C23119.4
H2—C2—C3119.9C22—C23—H23120.2
C2—C3—H3120.5C22—C23—C24119.6 (4)
C2—C3—C4119.0 (4)H23—C23—C24120.2
H3—C3—C4120.5C23—C24—H24119.9
C3—C4—H4119.7C23—C24—C25120.2 (3)
C3—C4—C5120.5 (4)H24—C24—C25119.9
H4—C4—C5119.7C24—C25—H25119.9
C4—C5—H5118.9C24—C25—C26120.1 (3)
C4—C5—C6122.1 (4)H25—C25—C26119.9
H5—C5—C6118.9C21—C26—C25120.6 (3)
C1—C6—C5115.6 (4)C21—C26—H26119.7
C1—C6—C7126.5 (4)C25—C26—H26119.7
C5—C6—C7117.9 (4)P1—C27—C28118.0 (3)
C6—C7—H7118.0P1—C27—C32123.8 (3)
C6—C7—C8124.0 (4)C28—C27—C32118.2 (3)
H7—C7—C8118.0C27—C28—H28119.6
C7—C8—H8118.8C27—C28—C29120.8 (3)
C7—C8—C9122.4 (4)H28—C28—C29119.6
H8—C8—C9118.8C28—C29—H29119.9
N2—C9—C8122.4 (3)C28—C29—C30120.2 (4)
N2—C9—H9118.8H29—C29—C30119.9
C8—C9—H9118.8C29—C30—H30120.2
N2—C10—H10A109.9C29—C30—C31119.6 (4)
N2—C10—H10B109.9H30—C30—C31120.2
N2—C10—C11109.1 (3)C30—C31—H31119.9
H10A—C10—H10B108.3C30—C31—C32120.3 (4)
H10A—C10—C11109.9H31—C31—C32119.9
H10B—C10—C11109.9C27—C32—C31120.9 (4)
N3—C11—C10109.3 (3)C27—C32—H32119.6
N3—C11—H11A109.8C31—C32—H32119.6
N3—C11—H11B109.8P1—C33—C34122.9 (3)
C10—C11—H11A109.8P1—C33—C38118.4 (3)
C10—C11—H11B109.8C34—C33—C38118.7 (3)
H11A—C11—H11B108.3C33—C34—H34119.8
N3—C12—H12119.0C33—C34—C35120.3 (3)
N3—C12—C13122.0 (3)H34—C34—C35119.8
H12—C12—C13119.0C34—C35—H35119.9
C12—C13—H13119.0C34—C35—C36120.1 (4)
C12—C13—C14122.0 (4)H35—C35—C36119.9
H13—C13—C14119.0C35—C36—H36120.2
C13—C14—H14117.2C35—C36—C37119.5 (4)
C13—C14—C15125.5 (4)H36—C36—C37120.2
H14—C14—C15117.2C36—C37—H37119.6
C14—C15—C16119.7 (3)C36—C37—C38120.8 (4)
C14—C15—C20124.2 (4)H37—C37—C38119.6
C16—C15—C20115.9 (4)C33—C38—C37120.5 (3)
C15—C16—H16119.2C33—C38—H38119.7
C15—C16—C17121.7 (4)C37—C38—H38119.7
H16—C16—C17119.2Cu1—N5—C39168.7 (3)
C16—C17—H17120.0N5—C39—S1179.0 (4)
O1—N1—C1—C2173.1 (4)O4—N4—C20—C15149.4 (4)
O1—N1—C1—C67.7 (6)O4—N4—C20—C1932.7 (5)
O2—N1—C1—C210.3 (6)Cu1—P1—C21—C2233.7 (3)
O2—N1—C1—C6168.9 (5)Cu1—P1—C21—C26147.6 (3)
N1—C1—C2—C3179.3 (4)C27—P1—C21—C22158.9 (3)
C6—C1—C2—C31.5 (6)C27—P1—C21—C2622.4 (3)
C1—C2—C3—C41.1 (6)C33—P1—C21—C2293.8 (3)
C2—C3—C4—C50.0 (7)C33—P1—C21—C2684.9 (3)
C3—C4—C5—C60.8 (7)P1—C21—C22—C23178.8 (3)
C4—C5—C6—C10.4 (6)C26—C21—C22—C230.0 (5)
C4—C5—C6—C7177.1 (4)C21—C22—C23—C240.2 (6)
N1—C1—C6—C5179.9 (4)C22—C23—C24—C250.6 (6)
N1—C1—C6—C72.8 (6)C23—C24—C25—C260.8 (6)
C2—C1—C6—C50.7 (6)P1—C21—C26—C25178.4 (3)
C2—C1—C6—C7178.0 (4)C22—C21—C26—C250.2 (5)
C1—C6—C7—C8145.3 (4)C24—C25—C26—C210.6 (6)
C5—C6—C7—C837.4 (6)Cu1—P1—C27—C2829.9 (3)
C6—C7—C8—C9175.6 (4)Cu1—P1—C27—C32147.6 (3)
Cu1—N2—C9—C82.2 (6)C21—P1—C27—C2894.0 (3)
C10—N2—C9—C8179.4 (3)C21—P1—C27—C3288.5 (3)
C7—C8—C9—N2174.9 (4)C33—P1—C27—C28159.4 (3)
Cu1—N2—C10—C1148.3 (3)C33—P1—C27—C3218.1 (3)
C9—N2—C10—C11130.6 (4)P1—C27—C28—C29177.5 (3)
Cu1—N3—C11—C1022.5 (4)C32—C27—C28—C290.2 (5)
C12—N3—C11—C10161.0 (3)C27—C28—C29—C300.7 (6)
N2—C10—C11—N347.6 (4)C28—C29—C30—C310.0 (6)
Cu1—N3—C12—C131.0 (5)C29—C30—C31—C321.2 (6)
C11—N3—C12—C13176.9 (3)C30—C31—C32—C271.8 (6)
N3—C12—C13—C14178.9 (4)P1—C27—C32—C31178.5 (3)
C12—C13—C14—C15177.0 (4)C28—C27—C32—C311.0 (5)
C13—C14—C15—C1634.2 (6)Cu1—P1—C33—C34151.3 (3)
C13—C14—C15—C20151.9 (4)Cu1—P1—C33—C3828.9 (3)
C14—C15—C16—C17174.2 (4)C21—P1—C33—C3427.4 (3)
C20—C15—C16—C170.3 (6)C21—P1—C33—C38152.8 (3)
C15—C16—C17—C180.5 (6)C27—P1—C33—C3481.4 (3)
C16—C17—C18—C190.9 (6)C27—P1—C33—C3898.4 (3)
C17—C18—C19—C200.5 (6)P1—C33—C34—C35179.2 (3)
C18—C19—C20—N4177.5 (4)C38—C33—C34—C350.6 (5)
C18—C19—C20—C150.4 (6)C33—C34—C35—C360.7 (6)
C14—C15—C20—N48.7 (6)C34—C35—C36—C371.9 (6)
C14—C15—C20—C19173.4 (4)C35—C36—C37—C381.9 (6)
C16—C15—C20—N4177.1 (3)C36—C37—C38—C330.7 (6)
C16—C15—C20—C190.7 (6)P1—C33—C38—C37179.2 (3)
O3—N4—C20—C1531.9 (5)C34—C33—C38—C370.5 (5)
O3—N4—C20—C19146.1 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2···O20.952.312.640 (6)100
C7—H7···O10.952.282.735 (5)109
C7—H7···O3i0.952.543.468 (5)165
C11—H11B···N5i0.992.593.339 (5)133
C14—H14···O30.952.442.757 (5)99
C14—H14···O1i0.952.483.387 (5)159
C19—H19···O40.952.512.757 (6)95
C24—H24···O2ii0.952.623.297 (6)129
C28—H28···N50.952.613.471 (5)151
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+2, y, z+1.
 

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