2-[(5-Chloro-2-hy­droxy­benzyl­idene)amino]-3′,6′-bis­(diethyl­amino)­spiro­[isoindoline-1,9′-xanthen]-3-one

Xu, Z.; Guo, W.; Su, B.; Shen, X.-K.; Yang, F.

doi:10.1107/S1600536810019549

organic compounds

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ISSN: 2056-9890

Volume 66| Part 6| June 2010| Page o1500

https://doi.org/10.1107/S1600536810019549

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2-[(5-Chloro-2-hydroxybenzylidene)amino]-3′,6′-bis(diethylamino)spiro[isoindoline-1,9′-xanthen]-3-one

Zhi-hong Xu,^a ^* Wei-yun Guo,^a Bo-wei Su,^a Xu-Ke Shen ^a and Feng-ling Yang ^a

^aCollege of Chemistry and Chemical Engineering, Xuchang University, Xuchang, Henan Province 461000, People's Republic of China
^*Correspondence e-mail: xuzhihong1980@yahoo.cn

(Received 20 April 2010; accepted 25 May 2010; online 29 May 2010)

The title compound, C₃₅H₃₅ClN₄O₃, resulted from a spirolactam ring closure of rhodamine B dye. The xanthene ring system is approximately planar [r.m.s. deviation = 0.050 (9) Å for the xanthene ring]. The dihedral angles formed by the spirolactam and 5-chloro-2-hydroxybenzene rings with the xanthene ring system are 87.9 (7) and 79.1 (7)°, respectively.

Related literature

For rhodamine derivatives bearing a lactam unit, see: Deng et al. (2009 ); Kwon et al., 2005 ; Tian & Peng (2008 ); Wu et al. (2007 ); Xu et al. (2009 ); Zhang et al. (2008 ).

Experimental

Crystal data

C₃₅H₃₅ClN₄O₃
M_r = 595.12
Orthorhombic, P c a 2₁
a = 21.609 (9) Å
b = 11.892 (5) Å
c = 12.355 (5) Å
V = 3175 (2) Å³
Z = 4
Mo Kα radiation
μ = 0.16 mm⁻¹
T = 296 K
0.35 × 0.32 × 0.29 mm

Data collection

Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2005 ) T_min = 0.946, T_max = 0.955
16073 measured reflections
5528 independent reflections
2820 reflections with I > 2σ(I)
R_int = 0.079

Refinement

R[F² > 2σ(F²)] = 0.049
wR(F²) = 0.088
S = 1.02
5528 reflections
394 parameters
1 restraint
H-atom parameters constrained
Δρ_max = 0.20 e Å⁻³
Δρ_min = −0.25 e Å⁻³
Absolute structure: Flack (1983 ), 2521 Friedel pairs
Flack parameter: −0.05 (8)

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supporting information

Crystal structure: contains datablocks I, global. DOI: https://doi.org/10.1107/S1600536810019549/cs2127sup1.cif

Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810019549/cs2127Isup2.hkl

checkCIF report

Comment top

Among many fluorescent compounds, rhodamine dyes are known to have excellent photophysical properties, and they are one of the most widely used fluorophores for labeling and sensing biomolecules. There are a few single-crystal reports on rhodamine derivatives bearing a lactam moiety (Xu et al., 2009; Kwon et al., 2005; Wu et al., 2007; Zhang et al., 2008; Tian et al., 2008; Deng et al., 2009). Detailed information on their molecular and crystal structures is necessary to understand their photophysical and photochemical properties.

In agreement with other reported models, (Xu et al., 2009; Wu et al., 2007; Zhang et al., 2008; Tian et al., 2008) the main skeleton of the molecule is formed by the xanthene ring and the spirolactam-ring. As shown in Figure 1, the atoms of the xanthene ring or the spirolactam-ring are both nearly planar and are almost perpendicular to each other. The dihedral angle between the xanthene and the spirolactam ring fragment mean planes is 87.9 (7)°. The dihedral angle between the xanthene mean plane and the 2-hydroxy-5-cholorobenzene ring is 79.1 (7)°.

Related literature top

For rhodamine derivatives bearing a lactam unit, see: Deng et al. (2009); Kwon et al., 2005; Tian & Peng (2008); Wu et al. (2007); Xu et al. (2009); Zhang et al. (2008).

Experimental top

A portion of rhodamine B hydrazide (0.46 g, 1 mmol) and 2-hydroxy-5-chlorobenzaldehyde (0.17 g, 1.1 mmol) were mixed in 20 ml ethanol to which three drops acetic acid was added. The reaction solution was refluxed for 3 hours under N₂ atmosphere, the precipatate was separated and washed by ethanol to give 0.30 g of the title compound in 50% yield. Single crystals suitable for X-ray measurements were obtained from the mother liquid by slow solvent evaporation at room temperatures.

Structure description top

For rhodamine derivatives bearing a lactam unit, see: Deng et al. (2009); Kwon et al., 2005; Tian & Peng (2008); Wu et al. (2007); Xu et al. (2009); Zhang et al. (2008).

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT (Bruker, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top

Fig. 1. The molecular structure of the title compound, with H atoms omitted and with displacement ellipsoids drawn at 50% probability level

2-[(5-Chloro-2-hydroxybenzylidene)amino]-3',6'- bis(diethylamino)spiro[isoindoline-1,9'-xanthen]-3-one top

Crystal data top

C₃₅H₃₅ClN₄O₃	F(000) = 1256
M_r = 595.12	D_x = 1.245 Mg m⁻³
Orthorhombic, Pca2₁	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2ac	Cell parameters from 1377 reflections
a = 21.609 (9) Å	θ = 2.5–17.6°
b = 11.892 (5) Å	µ = 0.16 mm⁻¹
c = 12.355 (5) Å	T = 296 K
V = 3175 (2) Å³	Block, red
Z = 4	0.35 × 0.32 × 0.29 mm

Data collection top

Bruker APEXII CCD diffractometer	5528 independent reflections
Radiation source: fine-focus sealed tube	2820 reflections with I > 2σ(I)
Graphite monochromator	R_int = 0.079
φ and ω scans	θ_max = 25.2°, θ_min = 1.7°
Absorption correction: multi-scan (SADABS; Bruker, 2005)	h = −21→25
T_min = 0.946, T_max = 0.955	k = −14→14
16073 measured reflections	l = −14→14

Refinement top

Refinement on F²	Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full	H-atom parameters constrained
R[F² > 2σ(F²)] = 0.049	w = 1/[σ²(F_o²) + (0.020P)² + 0.0114P] where P = (F_o² + 2F_c²)/3
wR(F²) = 0.088	(Δ/σ)_max = 0.001
S = 1.02	Δρ_max = 0.20 e Å⁻³
5528 reflections	Δρ_min = −0.25 e Å⁻³
394 parameters	Extinction correction: SHELXL97 (Sheldrick, 2008), Fc^*=kFc[1+0.001xFc²λ³/sin(2θ)]^-1/4
1 restraint	Extinction coefficient: 0.0018 (2)
Primary atom site location: structure-invariant direct methods	Absolute structure: Flack (1983), 2521 Friedel pairs
Secondary atom site location: difference Fourier map	Absolute structure parameter: −0.05 (8)

Crystal data top

C₃₅H₃₅ClN₄O₃	V = 3175 (2) Å³
M_r = 595.12	Z = 4
Orthorhombic, Pca2₁	Mo Kα radiation
a = 21.609 (9) Å	µ = 0.16 mm⁻¹
b = 11.892 (5) Å	T = 296 K
c = 12.355 (5) Å	0.35 × 0.32 × 0.29 mm

Data collection top

Bruker APEXII CCD diffractometer	5528 independent reflections
Absorption correction: multi-scan (SADABS; Bruker, 2005)	2820 reflections with I > 2σ(I)
T_min = 0.946, T_max = 0.955	R_int = 0.079
16073 measured reflections

Refinement top

R[F² > 2σ(F²)] = 0.049	H-atom parameters constrained
wR(F²) = 0.088	Δρ_max = 0.20 e Å⁻³
S = 1.02	Δρ_min = −0.25 e Å⁻³
5528 reflections	Absolute structure: Flack (1983), 2521 Friedel pairs
394 parameters	Absolute structure parameter: −0.05 (8)
1 restraint

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.

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

	x	y	z	U_iso*/U_eq
C1	0.91042 (15)	0.2527 (3)	0.2707 (3)	0.0444 (10)
C2	0.92493 (16)	0.3631 (3)	0.2392 (3)	0.0556 (11)
H2	0.9307	0.4173	0.2926	0.067*
C3	0.93088 (18)	0.3942 (3)	0.1323 (3)	0.0610 (12)
H3	0.9403	0.4684	0.1151	0.073*
C4	0.92276 (16)	0.3146 (3)	0.0482 (3)	0.0514 (10)
C5	0.90881 (15)	0.2049 (3)	0.0793 (3)	0.0498 (10)
H5	0.9034	0.1499	0.0265	0.060*
C6	0.90281 (15)	0.1763 (3)	0.1872 (3)	0.0480 (10)
C7	0.88582 (16)	0.0256 (3)	0.3112 (3)	0.0487 (10)
C8	0.87418 (16)	−0.0896 (3)	0.3190 (3)	0.0504 (11)
H8	0.8687	−0.1325	0.2568	0.060*
C9	0.87086 (18)	−0.1398 (3)	0.4202 (3)	0.0581 (11)
C10	0.88058 (19)	−0.0710 (3)	0.5111 (3)	0.0709 (13)
H10	0.8796	−0.1027	0.5799	0.085*
C11	0.89161 (17)	0.0435 (3)	0.4998 (3)	0.0627 (12)
H11	0.8975	0.0870	0.5615	0.075*
C12	0.89403 (16)	0.0949 (3)	0.3985 (3)	0.0435 (9)
C13	0.90153 (15)	0.2201 (3)	0.3879 (3)	0.0433 (9)
C14	0.84695 (17)	0.2814 (3)	0.4418 (3)	0.0469 (10)
C15	0.78553 (18)	0.2786 (3)	0.4104 (4)	0.0660 (12)
H15	0.7734	0.2405	0.3482	0.079*
C16	0.7425 (2)	0.3343 (4)	0.4747 (4)	0.0814 (15)
H16	0.7009	0.3328	0.4556	0.098*
C17	0.7606 (2)	0.3919 (4)	0.5666 (4)	0.0858 (15)
H17	0.7311	0.4284	0.6085	0.103*
C18	0.8217 (2)	0.3960 (3)	0.5970 (4)	0.0689 (12)
H18	0.8340	0.4341	0.6591	0.083*
C19	0.86485 (18)	0.3410 (3)	0.5316 (3)	0.0489 (10)
C20	0.93194 (19)	0.3317 (3)	0.5431 (3)	0.0514 (10)
C21	1.03453 (16)	0.1615 (3)	0.3910 (3)	0.0563 (11)
H21	1.0103	0.1392	0.3326	0.068*
C22	1.09773 (17)	0.1217 (3)	0.4016 (3)	0.0524 (10)
C23	1.12309 (18)	0.0528 (3)	0.3199 (3)	0.0580 (11)
H23	1.0995	0.0352	0.2593	0.070*
C24	1.1822 (2)	0.0114 (3)	0.3287 (4)	0.0641 (12)
C25	1.21808 (19)	0.0326 (4)	0.4194 (4)	0.0769 (13)
H25	1.2574	0.0015	0.4259	0.092*
C26	1.1946 (2)	0.1004 (4)	0.4997 (4)	0.0796 (15)
H26	1.2186	0.1161	0.5604	0.096*
C27	1.1352 (2)	0.1458 (4)	0.4911 (3)	0.0609 (12)
C28	0.9453 (2)	0.4583 (4)	−0.0927 (4)	0.0861 (15)
H28A	0.9664	0.4545	−0.1619	0.103*
H28B	0.9740	0.4894	−0.0403	0.103*
C29	0.8901 (3)	0.5355 (4)	−0.1026 (4)	0.1127 (19)
H29A	0.8574	0.4974	−0.1404	0.169*
H29B	0.9018	0.6018	−0.1419	0.169*
H29C	0.8760	0.5563	−0.0317	0.169*
C30	0.91860 (19)	0.2621 (4)	−0.1446 (3)	0.0635 (12)
H30A	0.9042	0.3014	−0.2086	0.076*
H30B	0.8863	0.2103	−0.1227	0.076*
C31	0.9757 (2)	0.1955 (4)	−0.1738 (4)	0.1004 (17)
H31A	1.0088	0.2461	−0.1914	0.151*
H31B	0.9669	0.1484	−0.2350	0.151*
H31C	0.9877	0.1495	−0.1134	0.151*
C32	0.8484 (3)	−0.3280 (4)	0.3399 (4)	0.109 (2)
H32A	0.8608	−0.4034	0.3605	0.131*
H32B	0.8748	−0.3041	0.2807	0.131*
C33	0.7837 (3)	−0.3307 (5)	0.3019 (5)	0.177 (3)
H33A	0.7571	−0.3534	0.3603	0.266*
H33B	0.7799	−0.3834	0.2434	0.266*
H33C	0.7718	−0.2572	0.2774	0.266*
C34	0.8455 (3)	−0.3014 (4)	0.5475 (6)	0.125 (2)
H34A	0.8259	−0.2458	0.5935	0.150*
H34B	0.8193	−0.3676	0.5438	0.150*
C35	0.9045 (3)	−0.3290 (5)	0.5864 (6)	0.150 (3)
H35A	0.9210	−0.3904	0.5450	0.225*
H35B	0.9017	−0.3505	0.6611	0.225*
H35C	0.9313	−0.2650	0.5797	0.225*
Cl1	1.21296 (5)	−0.07129 (11)	0.22454 (12)	0.0958 (4)
N1	0.95241 (13)	0.2637 (2)	0.4589 (3)	0.0472 (8)
N2	1.01262 (14)	0.2276 (2)	0.4631 (3)	0.0489 (8)
N3	0.92790 (14)	0.3435 (3)	−0.0588 (3)	0.0665 (10)
N4	0.85785 (18)	−0.2527 (3)	0.4319 (3)	0.0830 (12)
O1	0.88834 (11)	0.0645 (2)	0.2056 (2)	0.0611 (7)
O2	0.96649 (13)	0.3715 (2)	0.6133 (2)	0.0667 (8)
O3	1.11542 (13)	0.2139 (3)	0.5725 (2)	0.0799 (9)
H3A	1.0809	0.2383	0.5579	0.120*

Atomic displacement parameters (Å²) top

	U¹¹	U²²	U³³	U¹²	U¹³	U²³
C1	0.046 (2)	0.046 (2)	0.040 (3)	−0.0038 (18)	−0.0038 (18)	0.000 (2)
C2	0.067 (3)	0.050 (3)	0.049 (3)	−0.015 (2)	−0.005 (2)	−0.009 (2)
C3	0.075 (3)	0.053 (3)	0.055 (3)	−0.022 (2)	−0.003 (2)	0.013 (2)
C4	0.058 (3)	0.057 (3)	0.040 (3)	−0.011 (2)	−0.006 (2)	0.003 (2)
C5	0.067 (3)	0.052 (3)	0.030 (2)	−0.008 (2)	−0.001 (2)	0.004 (2)
C6	0.052 (2)	0.046 (3)	0.046 (3)	−0.0112 (19)	−0.004 (2)	0.008 (2)
C7	0.049 (2)	0.049 (3)	0.048 (3)	0.000 (2)	0.002 (2)	0.006 (2)
C8	0.063 (3)	0.042 (3)	0.046 (3)	−0.0063 (19)	0.001 (2)	−0.004 (2)
C9	0.087 (3)	0.039 (2)	0.048 (3)	−0.004 (2)	0.002 (2)	0.000 (2)
C10	0.120 (4)	0.052 (3)	0.041 (3)	−0.009 (3)	0.002 (3)	0.009 (2)
C11	0.094 (3)	0.053 (3)	0.041 (3)	−0.003 (2)	0.001 (2)	−0.006 (2)
C12	0.054 (2)	0.046 (2)	0.031 (2)	−0.0047 (19)	0.0000 (19)	−0.001 (2)
C13	0.044 (2)	0.043 (2)	0.043 (2)	−0.0087 (18)	−0.0043 (19)	−0.007 (2)
C14	0.048 (2)	0.042 (2)	0.051 (3)	−0.0081 (19)	0.001 (2)	−0.002 (2)
C15	0.061 (3)	0.065 (3)	0.072 (3)	−0.002 (2)	0.004 (3)	−0.019 (3)
C16	0.054 (3)	0.083 (3)	0.108 (5)	0.009 (3)	0.004 (3)	−0.011 (4)
C17	0.068 (4)	0.080 (4)	0.110 (5)	0.011 (3)	0.027 (3)	−0.015 (3)
C18	0.085 (3)	0.059 (3)	0.063 (3)	0.005 (3)	0.008 (3)	−0.006 (2)
C19	0.051 (3)	0.048 (3)	0.048 (3)	−0.003 (2)	0.006 (2)	0.003 (2)
C20	0.069 (3)	0.045 (3)	0.040 (3)	−0.009 (2)	0.005 (2)	0.007 (2)
C21	0.046 (3)	0.069 (3)	0.053 (3)	−0.008 (2)	−0.007 (2)	0.012 (2)
C22	0.043 (2)	0.059 (3)	0.055 (3)	−0.004 (2)	−0.002 (2)	0.009 (2)
C23	0.048 (3)	0.075 (3)	0.050 (3)	−0.001 (2)	−0.003 (2)	0.021 (2)
C24	0.054 (3)	0.083 (3)	0.055 (3)	0.011 (2)	0.006 (3)	0.017 (2)
C25	0.052 (3)	0.093 (4)	0.086 (4)	0.008 (3)	−0.012 (3)	0.020 (3)
C26	0.052 (3)	0.110 (4)	0.077 (4)	−0.006 (3)	−0.023 (3)	0.003 (3)
C27	0.055 (3)	0.073 (3)	0.055 (3)	−0.005 (2)	−0.006 (3)	0.009 (3)
C28	0.121 (4)	0.087 (4)	0.050 (3)	−0.045 (3)	−0.001 (3)	0.018 (3)
C29	0.185 (6)	0.057 (3)	0.096 (4)	−0.014 (4)	−0.037 (4)	0.013 (3)
C30	0.081 (3)	0.075 (3)	0.034 (2)	0.003 (3)	0.000 (2)	0.011 (2)
C31	0.091 (4)	0.115 (4)	0.096 (4)	0.013 (3)	0.020 (3)	0.013 (3)
C32	0.186 (7)	0.061 (3)	0.081 (4)	−0.019 (4)	0.003 (4)	0.003 (3)
C33	0.195 (8)	0.181 (6)	0.155 (7)	−0.090 (6)	−0.022 (6)	−0.032 (6)
C34	0.137 (5)	0.049 (3)	0.190 (7)	−0.019 (3)	−0.056 (5)	0.022 (4)
C35	0.153 (6)	0.115 (5)	0.184 (8)	−0.001 (4)	0.000 (5)	0.034 (5)
Cl1	0.0795 (8)	0.1268 (10)	0.0810 (9)	0.0372 (7)	0.0101 (8)	0.0157 (9)
N1	0.0449 (19)	0.053 (2)	0.044 (2)	−0.0050 (16)	0.0026 (17)	−0.0028 (17)
N2	0.046 (2)	0.058 (2)	0.043 (2)	−0.0033 (16)	−0.0016 (17)	0.0066 (18)
N3	0.088 (3)	0.063 (2)	0.048 (2)	−0.0181 (19)	−0.001 (2)	0.013 (2)
N4	0.155 (4)	0.044 (2)	0.050 (3)	−0.014 (2)	0.013 (2)	0.006 (2)
O1	0.101 (2)	0.0459 (16)	0.0368 (17)	−0.0196 (15)	−0.0012 (16)	0.0044 (14)
O2	0.084 (2)	0.0645 (19)	0.0511 (19)	−0.0140 (15)	−0.0083 (16)	−0.0106 (16)
O3	0.078 (2)	0.092 (2)	0.069 (2)	−0.0026 (18)	−0.0253 (19)	0.000 (2)

Geometric parameters (Å, º) top

C1—C6	1.384 (4)	C22—C27	1.400 (5)
C1—C2	1.405 (4)	C22—C23	1.411 (5)
C1—C13	1.512 (5)	C23—C24	1.374 (5)
C2—C3	1.377 (5)	C23—H23	0.9300
C2—H2	0.9300	C24—C25	1.386 (5)
C3—C4	1.416 (5)	C24—Cl1	1.751 (4)
C3—H3	0.9300	C25—C26	1.375 (5)
C4—N3	1.372 (5)	C25—H25	0.9300
C4—C5	1.393 (5)	C26—C27	1.398 (5)
C5—C6	1.382 (5)	C26—H26	0.9300
C5—H5	0.9300	C27—O3	1.359 (4)
C6—O1	1.384 (4)	C28—N3	1.477 (5)
C7—C12	1.370 (5)	C28—C29	1.511 (5)
C7—O1	1.385 (4)	C28—H28A	0.9700
C7—C8	1.396 (5)	C28—H28B	0.9700
C8—C9	1.387 (5)	C29—H29A	0.9600
C8—H8	0.9300	C29—H29B	0.9600
C9—N4	1.379 (4)	C29—H29C	0.9600
C9—C10	1.405 (5)	C30—N3	1.448 (5)
C10—C11	1.390 (5)	C30—C31	1.510 (5)
C10—H10	0.9300	C30—H30A	0.9700
C11—C12	1.394 (5)	C30—H30B	0.9700
C11—H11	0.9300	C31—H31A	0.9600
C12—C13	1.503 (4)	C31—H31B	0.9600
C13—N1	1.499 (4)	C31—H31C	0.9600
C13—C14	1.539 (5)	C32—N4	1.461 (5)
C14—C19	1.372 (5)	C32—C33	1.477 (6)
C14—C15	1.383 (4)	C32—H32A	0.9700
C15—C16	1.391 (5)	C32—H32B	0.9700
C15—H15	0.9300	C33—H33A	0.9600
C16—C17	1.383 (6)	C33—H33B	0.9600
C16—H16	0.9300	C33—H33C	0.9600
C17—C18	1.373 (5)	C34—C35	1.402 (6)
C17—H17	0.9300	C34—N4	1.565 (7)
C18—C19	1.396 (5)	C34—H34A	0.9700
C18—H18	0.9300	C34—H34B	0.9700
C19—C20	1.461 (5)	C35—H35A	0.9600
C20—O2	1.239 (4)	C35—H35B	0.9600
C20—N1	1.390 (4)	C35—H35C	0.9600
C21—N2	1.279 (4)	N1—N2	1.371 (4)
C21—C22	1.451 (5)	O3—H3A	0.8200
C21—H21	0.9300

C6—C1—C2	115.7 (3)	C23—C24—C25	121.3 (4)
C6—C1—C13	122.0 (3)	C23—C24—Cl1	119.7 (4)
C2—C1—C13	122.2 (3)	C25—C24—Cl1	119.0 (4)
C3—C2—C1	122.5 (4)	C26—C25—C24	119.0 (4)
C3—C2—H2	118.8	C26—C25—H25	120.5
C1—C2—H2	118.8	C24—C25—H25	120.5
C2—C3—C4	120.8 (3)	C25—C26—C27	120.7 (4)
C2—C3—H3	119.6	C25—C26—H26	119.7
C4—C3—H3	119.6	C27—C26—H26	119.7
N3—C4—C5	121.2 (4)	O3—C27—C26	117.5 (4)
N3—C4—C3	122.0 (4)	O3—C27—C22	121.7 (4)
C5—C4—C3	116.8 (4)	C26—C27—C22	120.8 (4)
C6—C5—C4	121.1 (4)	N3—C28—C29	112.5 (4)
C6—C5—H5	119.5	N3—C28—H28A	109.1
C4—C5—H5	119.5	C29—C28—H28A	109.1
C5—C6—C1	123.1 (3)	N3—C28—H28B	109.1
C5—C6—O1	114.5 (3)	C29—C28—H28B	109.1
C1—C6—O1	122.3 (3)	H28A—C28—H28B	107.8
C12—C7—O1	122.4 (3)	C28—C29—H29A	109.5
C12—C7—C8	124.0 (4)	C28—C29—H29B	109.5
O1—C7—C8	113.7 (3)	H29A—C29—H29B	109.5
C9—C8—C7	119.6 (4)	C28—C29—H29C	109.5
C9—C8—H8	120.2	H29A—C29—H29C	109.5
C7—C8—H8	120.2	H29B—C29—H29C	109.5
N4—C9—C8	121.6 (4)	N3—C30—C31	114.3 (4)
N4—C9—C10	120.9 (4)	N3—C30—H30A	108.7
C8—C9—C10	117.5 (3)	C31—C30—H30A	108.7
C11—C10—C9	121.1 (4)	N3—C30—H30B	108.7
C11—C10—H10	119.5	C31—C30—H30B	108.7
C9—C10—H10	119.5	H30A—C30—H30B	107.6
C10—C11—C12	121.7 (4)	C30—C31—H31A	109.5
C10—C11—H11	119.1	C30—C31—H31B	109.5
C12—C11—H11	119.1	H31A—C31—H31B	109.5
C7—C12—C11	116.0 (3)	C30—C31—H31C	109.5
C7—C12—C13	122.8 (3)	H31A—C31—H31C	109.5
C11—C12—C13	121.1 (3)	H31B—C31—H31C	109.5
N1—C13—C12	111.8 (3)	N4—C32—C33	113.1 (5)
N1—C13—C1	112.2 (3)	N4—C32—H32A	109.0
C12—C13—C1	110.6 (3)	C33—C32—H32A	109.0
N1—C13—C14	98.3 (3)	N4—C32—H32B	109.0
C12—C13—C14	110.4 (3)	C33—C32—H32B	109.0
C1—C13—C14	113.0 (3)	H32A—C32—H32B	107.8
C19—C14—C15	120.7 (4)	C32—C33—H33A	109.5
C19—C14—C13	112.3 (3)	C32—C33—H33B	109.5
C15—C14—C13	127.0 (4)	H33A—C33—H33B	109.5
C14—C15—C16	118.0 (4)	C32—C33—H33C	109.5
C14—C15—H15	121.0	H33A—C33—H33C	109.5
C16—C15—H15	121.0	H33B—C33—H33C	109.5
C17—C16—C15	121.0 (4)	C35—C34—N4	104.2 (5)
C17—C16—H16	119.5	C35—C34—H34A	110.9
C15—C16—H16	119.5	N4—C34—H34A	110.9
C18—C17—C16	121.0 (4)	C35—C34—H34B	110.9
C18—C17—H17	119.5	N4—C34—H34B	110.9
C16—C17—H17	119.5	H34A—C34—H34B	108.9
C17—C18—C19	117.8 (4)	C34—C35—H35A	109.5
C17—C18—H18	121.1	C34—C35—H35B	109.5
C19—C18—H18	121.1	H35A—C35—H35B	109.5
C14—C19—C18	121.5 (4)	C34—C35—H35C	109.5
C14—C19—C20	108.6 (4)	H35A—C35—H35C	109.5
C18—C19—C20	129.9 (4)	H35B—C35—H35C	109.5
O2—C20—N1	123.7 (4)	N2—N1—C20	117.1 (3)
O2—C20—C19	129.6 (4)	N2—N1—C13	127.6 (3)
N1—C20—C19	106.7 (4)	C20—N1—C13	113.9 (3)
N2—C21—C22	119.0 (4)	C21—N2—N1	121.1 (3)
N2—C21—H21	120.5	C4—N3—C30	121.8 (3)
C22—C21—H21	120.5	C4—N3—C28	121.7 (4)
C27—C22—C23	117.4 (4)	C30—N3—C28	116.5 (3)
C27—C22—C21	123.3 (4)	C9—N4—C32	122.9 (4)
C23—C22—C21	119.3 (4)	C9—N4—C34	119.4 (4)
C24—C23—C22	120.8 (4)	C32—N4—C34	117.3 (3)
C24—C23—H23	119.6	C6—O1—C7	119.0 (3)
C22—C23—H23	119.6	C27—O3—H3A	109.5

C6—C1—C2—C3	0.4 (6)	C17—C18—C19—C20	179.6 (4)
C13—C1—C2—C3	−177.6 (4)	C14—C19—C20—O2	−179.1 (4)
C1—C2—C3—C4	−0.3 (6)	C18—C19—C20—O2	−0.7 (7)
C2—C3—C4—N3	179.4 (4)	C14—C19—C20—N1	−1.1 (4)
C2—C3—C4—C5	−0.2 (6)	C18—C19—C20—N1	177.4 (4)
N3—C4—C5—C6	−179.1 (3)	N2—C21—C22—C27	4.5 (5)
C3—C4—C5—C6	0.5 (5)	N2—C21—C22—C23	−177.2 (3)
C4—C5—C6—C1	−0.4 (6)	C27—C22—C23—C24	0.1 (6)
C4—C5—C6—O1	179.5 (3)	C21—C22—C23—C24	−178.3 (3)
C2—C1—C6—C5	0.0 (5)	C22—C23—C24—C25	2.2 (6)
C13—C1—C6—C5	178.0 (3)	C22—C23—C24—Cl1	−178.6 (3)
C2—C1—C6—O1	−179.9 (3)	C23—C24—C25—C26	−2.7 (7)
C13—C1—C6—O1	−1.9 (5)	Cl1—C24—C25—C26	178.1 (3)
C12—C7—C8—C9	−0.5 (6)	C24—C25—C26—C27	1.0 (7)
O1—C7—C8—C9	179.6 (3)	C25—C26—C27—O3	−178.7 (4)
C7—C8—C9—N4	178.3 (4)	C25—C26—C27—C22	1.2 (6)
C7—C8—C9—C10	−1.0 (5)	C23—C22—C27—O3	178.2 (3)
N4—C9—C10—C11	−177.8 (4)	C21—C22—C27—O3	−3.5 (6)
C8—C9—C10—C11	1.5 (6)	C23—C22—C27—C26	−1.7 (6)
C9—C10—C11—C12	−0.5 (6)	C21—C22—C27—C26	176.6 (4)
O1—C7—C12—C11	−178.6 (3)	O2—C20—N1—N2	8.8 (5)
C8—C7—C12—C11	1.5 (5)	C19—C20—N1—N2	−169.4 (3)
O1—C7—C12—C13	4.9 (5)	O2—C20—N1—C13	176.5 (3)
C8—C7—C12—C13	−175.1 (3)	C19—C20—N1—C13	−1.7 (4)
C10—C11—C12—C7	−0.9 (6)	C12—C13—N1—N2	53.6 (4)
C10—C11—C12—C13	175.6 (3)	C1—C13—N1—N2	−71.3 (4)
C7—C12—C13—N1	−136.2 (3)	C14—C13—N1—N2	169.6 (3)
C11—C12—C13—N1	47.5 (5)	C12—C13—N1—C20	−112.6 (3)
C7—C12—C13—C1	−10.4 (5)	C1—C13—N1—C20	122.5 (3)
C11—C12—C13—C1	173.3 (3)	C14—C13—N1—C20	3.4 (3)
C7—C12—C13—C14	115.4 (4)	C22—C21—N2—N1	−177.3 (3)
C11—C12—C13—C14	−60.9 (4)	C20—N1—N2—C21	177.5 (3)
C6—C1—C13—N1	134.4 (3)	C13—N1—N2—C21	11.7 (5)
C2—C1—C13—N1	−47.7 (4)	C5—C4—N3—C30	0.6 (6)
C6—C1—C13—C12	8.9 (4)	C3—C4—N3—C30	−179.0 (4)
C2—C1—C13—C12	−173.2 (3)	C5—C4—N3—C28	−177.3 (4)
C6—C1—C13—C14	−115.5 (4)	C3—C4—N3—C28	3.1 (6)
C2—C1—C13—C14	62.4 (4)	C31—C30—N3—C4	−86.1 (4)
N1—C13—C14—C19	−4.0 (4)	C31—C30—N3—C28	91.8 (4)
C12—C13—C14—C19	113.0 (3)	C29—C28—N3—C4	−87.4 (5)
C1—C13—C14—C19	−122.6 (3)	C29—C28—N3—C30	94.6 (5)
N1—C13—C14—C15	177.8 (4)	C8—C9—N4—C32	1.8 (7)
C12—C13—C14—C15	−65.2 (5)	C10—C9—N4—C32	−178.9 (4)
C1—C13—C14—C15	59.3 (5)	C8—C9—N4—C34	−171.5 (4)
C19—C14—C15—C16	−2.3 (6)	C10—C9—N4—C34	7.8 (6)
C13—C14—C15—C16	175.8 (3)	C33—C32—N4—C9	−87.6 (6)
C14—C15—C16—C17	0.7 (6)	C33—C32—N4—C34	85.8 (6)
C15—C16—C17—C18	0.1 (7)	C35—C34—N4—C9	−87.2 (6)
C16—C17—C18—C19	0.6 (7)	C35—C34—N4—C32	99.2 (5)
C15—C14—C19—C18	3.1 (6)	C5—C6—O1—C7	175.3 (3)
C13—C14—C19—C18	−175.2 (3)	C1—C6—O1—C7	−4.9 (5)
C15—C14—C19—C20	−178.3 (3)	C12—C7—O1—C6	3.4 (5)
C13—C14—C19—C20	3.4 (4)	C8—C7—O1—C6	−176.7 (3)
C17—C18—C19—C14	−2.2 (6)

Experimental details

Crystal data
Chemical formula	C₃₅H₃₅ClN₄O₃
M_r	595.12
Crystal system, space group	Orthorhombic, Pca2₁
Temperature (K)	296
a, b, c (Å)	21.609 (9), 11.892 (5), 12.355 (5)
V (Å³)	3175 (2)
Z	4
Radiation type	Mo Kα
µ (mm⁻¹)	0.16
Crystal size (mm)	0.35 × 0.32 × 0.29

Data collection
Diffractometer	Bruker APEXII CCD
Absorption correction	Multi-scan (SADABS; Bruker, 2005)
T_min, T_max	0.946, 0.955
No. of measured, independent and observed [I > 2σ(I)] reflections	16073, 5528, 2820
R_int	0.079
(sin θ/λ)_max (Å⁻¹)	0.599

Refinement
R[F² > 2σ(F²)], wR(F²), S	0.049, 0.088, 1.02
No. of reflections	5528
No. of parameters	394
No. of restraints	1
H-atom treatment	H-atom parameters constrained
Δρ_max, Δρ_min (e Å⁻³)	0.20, −0.25
Absolute structure	Flack (1983), 2521 Friedel pairs
Absolute structure parameter	−0.05 (8)

Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Acknowledgements

The authors thank the Natural Science Foundation of the Education Department of Henan Province (2010B150029) and the Natural Science Foundation of Henan Province (082300420110) for support.

References

Bruker (2005). SAINT, SADABS and APEX2. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Deng, W.-J., Sun, D., Su, B.-Y., Wang, S.-P. & Zheng, H. (2009). Acta Cryst. E65, o1464. Web of Science CSD CrossRef IUCr Journals Google Scholar
Flack, H. D. (1983). Acta Cryst. A39, 876–881. CrossRef CAS Web of Science IUCr Journals Google Scholar
Kwon, J. Y., Jang, Y. J., Lee, Y. J., Kim, K. M., Seo, M. S., Nam, W. & Yoon, I. (2005). J. Am. Chem. Soc. 127, 10107–10111. Web of Science CSD CrossRef PubMed CAS Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Tian, M.-Z. & Peng, X.-J. (2008). Acta Cryst. E64, o1645. Web of Science CSD CrossRef IUCr Journals Google Scholar
Wu, D., Huang, W., Duan, C.-Y., Lin, Z.-H. & Meng, Q.-J. (2007). Inorg. Chem. 46, 1538–1540. Web of Science CSD CrossRef PubMed CAS Google Scholar
Xu, Z.-H., Wang, H.-S., Tao, L.-T. & Wang, H.-W. (2009). Acta Cryst. E65, o1876. Web of Science CSD CrossRef IUCr Journals Google Scholar
Zhang, L.-Z., Peng, X.-J., Gao, S. & Fan, J.-L. (2008). Acta Cryst. E64, o403. Web of Science CSD CrossRef IUCr Journals Google Scholar

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