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Metal-organic frameworks (MOFs) have potentially useful applications and an intriguing variety of architectures and topologies. Two homochiral coordination polymers have been synthesized by the hydro­thermal method, namely poly[([mu]-N-benzyl-L-phenyl­alaninato-[kappa]4O,O':O,N)([mu]-formato-[kappa]2O:O')zinc(II)], [Zn(C16H16NO2)(HCOO)]n, (1), and poly[([mu]-N-benzyl-L-leucinato-[kappa]4O,O':O,N)([mu]-formato-[kappa]2O:O')zinc(II)], [Zn(C13H18NO2)(HCOO)]n, (2), and studied by single-crystal X-ray diffraction, elemental analyses, IR spectroscopy and fluorescence spectroscopy. Compounds (1) and (2) each have a two-dimensional layer structure, with the benzyl or isobutyl groups of the ligands directed towards the inter­layer inter­face. Photoluminescence investigations show that both (1) and (2) display a strong emission in the blue region.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229615012115/qs3048sup1.cif
Contains datablocks global, 1, 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615012115/qs30481sup2.hkl
Contains datablock 1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615012115/qs30482sup3.hkl
Contains datablock 2

CCDC references: 1408511; 1408510

Computing details top

For both compounds, data collection: SMART (Bruker, 1999); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus (Bruker, 2001); 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: SHELXL97 (Sheldrick, 2008).

(1) Poly[(µ-N-benzyl-L-phenylalaninato-κ4O,O':O,N)(µ-formato-κ2O:O')zinc(II)], top
Crystal data top
[Zn(C16H16NO2)(HCO2)]Z = 4
Mr = 364.69F(000) = 752
Monoclinic, C2Dx = 1.478 Mg m3
Hall symbol: C 2yMo Kα radiation, λ = 0.71073 Å
a = 33.2283 (19) ŵ = 1.52 mm1
b = 6.6469 (4) ÅT = 293 K
c = 7.4241 (4) ÅNeedle, white
β = 91.299 (5)°0.26 × 0.05 × 0.04 mm
V = 1639.30 (16) Å3
Data collection top
Bruker APEX CCD area-detector
diffractometer
2909 independent reflections
Radiation source: fine-focus sealed tube2563 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.048
ω scansθmax = 26.0°, θmin = 2.5°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 4039
Tmin = 0.694, Tmax = 0.942k = 87
5538 measured reflectionsl = 89
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.078 w = 1/[σ2(Fo2) + (0.0264P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.99(Δ/σ)max = 0.001
2909 reflectionsΔρmax = 0.52 e Å3
208 parametersΔρmin = 0.36 e Å3
1 restraintAbsolute structure: Flack (1983), with 1154 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.009 (17)
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
xyzUiso*/Ueq
Zn10.233914 (10)0.42083 (8)0.73454 (5)0.03079 (13)
N10.17375 (8)0.3623 (4)0.6437 (4)0.0304 (8)
H1B0.15970.47090.63970.036*
O10.24190 (8)0.1911 (5)0.5410 (4)0.0392 (7)
O20.21213 (8)0.0329 (4)0.3117 (4)0.0392 (7)
O30.24662 (8)0.2510 (4)0.9489 (4)0.0394 (7)
O40.29276 (8)0.1716 (4)1.1569 (4)0.0463 (8)
C10.02920 (17)0.1151 (12)0.7521 (10)0.093 (2)
H1A0.00170.08930.74770.111*
C20.05512 (18)0.0259 (11)0.8210 (10)0.101 (3)
H2A0.04520.14620.86590.121*
C30.09645 (16)0.0098 (9)0.8246 (8)0.0717 (17)
H3A0.11410.08790.86900.086*
C40.11124 (12)0.1906 (8)0.7620 (6)0.0442 (11)
C50.08440 (13)0.3284 (8)0.6956 (7)0.0614 (15)
H5A0.09390.45060.65260.074*
C60.04331 (15)0.2908 (10)0.6905 (8)0.0793 (19)
H6A0.02560.38720.64460.095*
C70.15600 (12)0.2295 (8)0.7796 (6)0.0481 (12)
H7A0.16150.28740.89760.058*
H7B0.16980.10100.77570.058*
C80.17382 (11)0.2780 (6)0.4625 (5)0.0281 (9)
H8A0.15060.18870.44620.034*
C90.21230 (12)0.1574 (6)0.4396 (6)0.0330 (9)
C100.17216 (10)0.4422 (9)0.3178 (5)0.0368 (10)
H10A0.19130.54690.35000.044*
H10B0.18010.38490.20390.044*
C110.13122 (12)0.5339 (6)0.2949 (6)0.0385 (10)
C120.12273 (16)0.7232 (8)0.3638 (8)0.0676 (16)
H12A0.14320.79770.41930.081*
C130.08452 (18)0.8022 (9)0.3512 (10)0.090 (2)
H13A0.07940.92930.39760.108*
C140.05434 (18)0.6950 (11)0.2711 (10)0.093 (2)
H14A0.02840.74780.26560.111*
C150.06178 (16)0.5078 (10)0.1977 (8)0.081 (2)
H15A0.04130.43520.14040.097*
C160.10044 (11)0.4307 (12)0.2113 (5)0.0521 (11)
H16A0.10570.30490.16220.063*
C170.27963 (12)0.2741 (6)1.0299 (6)0.0390 (10)
H17A0.29590.37850.99090.047*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.0324 (2)0.0312 (2)0.0285 (2)0.0020 (3)0.00401 (15)0.0016 (3)
N10.0302 (16)0.031 (2)0.0296 (18)0.0029 (13)0.0007 (13)0.0032 (13)
O10.0337 (17)0.0432 (17)0.040 (2)0.0097 (14)0.0080 (14)0.0090 (15)
O20.0373 (16)0.0433 (16)0.0369 (18)0.0064 (13)0.0001 (13)0.0157 (15)
O30.0460 (17)0.0373 (16)0.0344 (18)0.0074 (14)0.0087 (14)0.0120 (13)
O40.0523 (18)0.0430 (17)0.043 (2)0.0019 (15)0.0129 (14)0.0177 (15)
C10.051 (4)0.122 (6)0.106 (6)0.033 (4)0.007 (3)0.003 (5)
C20.069 (4)0.104 (8)0.130 (6)0.038 (4)0.005 (4)0.018 (5)
C30.056 (3)0.070 (4)0.090 (5)0.015 (3)0.003 (3)0.009 (3)
C40.041 (2)0.061 (3)0.031 (3)0.010 (2)0.0051 (19)0.003 (2)
C50.040 (3)0.075 (4)0.070 (4)0.008 (2)0.007 (2)0.005 (3)
C60.038 (3)0.110 (5)0.090 (5)0.006 (3)0.008 (3)0.015 (4)
C70.041 (2)0.072 (3)0.031 (3)0.009 (2)0.0029 (19)0.002 (2)
C80.0262 (19)0.030 (2)0.028 (2)0.0040 (17)0.0010 (16)0.0018 (17)
C90.038 (2)0.030 (2)0.030 (2)0.0020 (18)0.0023 (18)0.0036 (19)
C100.0328 (18)0.047 (3)0.031 (2)0.004 (3)0.0006 (15)0.006 (3)
C110.037 (2)0.040 (2)0.039 (3)0.000 (2)0.0054 (19)0.007 (2)
C120.064 (3)0.040 (3)0.098 (5)0.006 (3)0.013 (3)0.002 (3)
C130.083 (4)0.055 (4)0.132 (7)0.026 (3)0.000 (4)0.003 (4)
C140.056 (4)0.088 (5)0.133 (7)0.033 (4)0.010 (4)0.024 (5)
C150.047 (3)0.113 (6)0.082 (4)0.007 (3)0.021 (3)0.012 (4)
C160.048 (2)0.062 (3)0.046 (2)0.007 (4)0.0087 (18)0.004 (4)
C170.045 (2)0.034 (2)0.037 (3)0.010 (2)0.007 (2)0.006 (2)
Geometric parameters (Å, º) top
Zn1—O2i1.979 (3)C5—C61.388 (6)
Zn1—O31.988 (3)C5—H5A0.9300
Zn1—O4ii2.061 (3)C6—H6A0.9300
Zn1—O12.118 (3)C7—H7A0.9700
Zn1—N12.131 (3)C7—H7B0.9700
N1—C81.457 (5)C8—C91.522 (5)
N1—C71.474 (5)C8—C101.531 (6)
N1—H1B0.8600C8—H8A0.9800
O1—C91.245 (5)C10—C111.497 (5)
O2—C91.259 (5)C10—H10A0.9700
O2—Zn1iii1.979 (3)C10—H10B0.9700
O3—C171.248 (4)C11—C161.368 (6)
O4—C171.235 (5)C11—C121.390 (6)
O4—Zn1iv2.061 (3)C12—C131.375 (7)
C1—C61.343 (9)C12—H12A0.9300
C1—C21.364 (9)C13—C141.356 (8)
C1—H1A0.9300C13—H13A0.9300
C2—C31.393 (7)C14—C151.383 (9)
C2—H2A0.9300C14—H14A0.9300
C3—C41.383 (7)C15—C161.385 (7)
C3—H3A0.9300C15—H15A0.9300
C4—C51.363 (6)C16—H16A0.9300
C4—C71.512 (5)C17—H17A0.9300
O2i—Zn1—O3100.12 (11)C4—C7—H7A108.1
O2i—Zn1—O4ii99.37 (13)N1—C7—H7B108.1
O3—Zn1—O4ii103.38 (12)C4—C7—H7B108.1
O2i—Zn1—O191.49 (12)H7A—C7—H7B107.3
O3—Zn1—O196.08 (12)N1—C8—C9108.9 (3)
O4ii—Zn1—O1155.56 (11)N1—C8—C10111.9 (3)
O2i—Zn1—N1149.45 (12)C9—C8—C10108.3 (3)
O3—Zn1—N1109.27 (12)N1—C8—H8A109.2
O4ii—Zn1—N182.11 (11)C9—C8—H8A109.2
O1—Zn1—N177.57 (11)C10—C8—H8A109.2
C8—N1—C7114.3 (3)O1—C9—O2124.3 (4)
C8—N1—Zn1109.9 (2)O1—C9—C8119.5 (4)
C7—N1—Zn1106.3 (2)O2—C9—C8116.2 (3)
C8—N1—H1B107.6C11—C10—C8112.9 (3)
C7—N1—H1B107.5C11—C10—H10A109.0
Zn1—N1—H1B111.2C8—C10—H10A109.0
C9—O1—Zn1115.5 (3)C11—C10—H10B109.0
C9—O2—Zn1iii112.9 (2)C8—C10—H10B109.0
C17—O3—Zn1119.0 (3)H10A—C10—H10B107.8
C17—O4—Zn1iv126.7 (3)C16—C11—C12117.7 (5)
C6—C1—C2120.2 (6)C16—C11—C10121.0 (4)
C6—C1—H1A119.9C12—C11—C10121.2 (4)
C2—C1—H1A119.9C13—C12—C11121.0 (5)
C1—C2—C3120.2 (6)C13—C12—H12A119.5
C1—C2—H2A119.9C11—C12—H12A119.5
C3—C2—H2A119.9C14—C13—C12120.1 (6)
C4—C3—C2120.0 (6)C14—C13—H13A120.0
C4—C3—H3A120.0C12—C13—H13A120.0
C2—C3—H3A120.0C13—C14—C15120.6 (5)
C5—C4—C3118.1 (4)C13—C14—H14A119.7
C5—C4—C7123.4 (4)C15—C14—H14A119.7
C3—C4—C7118.4 (5)C16—C15—C14118.5 (6)
C4—C5—C6121.6 (5)C16—C15—H15A120.7
C4—C5—H5A119.2C14—C15—H15A120.7
C6—C5—H5A119.2C11—C16—C15122.0 (6)
C1—C6—C5119.9 (6)C11—C16—H16A119.0
C1—C6—H6A120.1C15—C16—H16A119.0
C5—C6—H6A120.1O4—C17—O3126.3 (4)
N1—C7—C4116.8 (4)O4—C17—H17A116.9
N1—C7—H7A108.1O3—C17—H17A116.9
Symmetry codes: (i) x+1/2, y+1/2, z+1; (ii) x+1/2, y+1/2, z+2; (iii) x+1/2, y1/2, z+1; (iv) x+1/2, y1/2, z+2.
(2) Poly[(µ-N-benzyl-L-leucinato-κ4O,O':O,N)(µ-formato-κ2O:O')zinc(II)], top
Crystal data top
[Zn(C13H18NO2)(HCO2)]Z = 4
Mr = 330.67F(000) = 688
Orthorhombic, P212121Dx = 1.438 Mg m3
Hall symbol: P 2ac 2abMo Kα radiation, λ = 0.71073 Å
a = 6.4790 (4) ŵ = 1.62 mm1
b = 7.6577 (4) ÅT = 293 K
c = 30.7746 (19) ÅNeedle, white
V = 1526.86 (16) Å30.24 × 0.07 × 0.06 mm
Data collection top
Bruker APEX CCD area-detector
diffractometer
2886 independent reflections
Radiation source: fine-focus sealed tube2661 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
ω scansθmax = 26.0°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 67
Tmin = 0.697, Tmax = 0.909k = 95
4702 measured reflectionsl = 3727
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.069H-atom parameters constrained
wR(F2) = 0.135 w = 1/[σ2(Fo2) + (0.0155P)2 + 6.1609P]
where P = (Fo2 + 2Fc2)/3
S = 1.17(Δ/σ)max < 0.001
2886 reflectionsΔρmax = 1.31 e Å3
181 parametersΔρmin = 1.19 e Å3
0 restraintsAbsolute structure: Flack (1983), with 1117 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.02 (4)
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
xyzUiso*/Ueq
Zn10.12573 (12)0.48766 (10)0.01666 (2)0.0284 (2)
N10.1917 (9)0.4143 (7)0.08201 (18)0.0297 (13)
H1B0.07980.41890.09700.036*
O10.3434 (7)0.2859 (7)0.00767 (16)0.0348 (12)
O30.1279 (9)0.6024 (7)0.04675 (16)0.0457 (13)
O20.4980 (7)0.0621 (6)0.04052 (16)0.0351 (12)
O40.1931 (7)0.8106 (7)0.00242 (18)0.0384 (14)
C40.3823 (13)0.5194 (11)0.1481 (2)0.0431 (17)
C130.3805 (12)0.1942 (9)0.0403 (2)0.0335 (16)
C70.3372 (12)0.5431 (9)0.1002 (2)0.0390 (19)
H7A0.28110.65920.09580.047*
H7B0.46600.53590.08430.047*
C80.2726 (10)0.2330 (9)0.0829 (2)0.0279 (15)
H8A0.37220.22200.10670.033*
C140.2239 (11)0.7302 (9)0.0325 (2)0.0326 (17)
H14A0.33120.77140.04980.039*
C100.0087 (14)0.0964 (11)0.1362 (3)0.045 (2)
H10A0.03760.21450.14370.054*
C90.0964 (12)0.1030 (9)0.0901 (2)0.0338 (17)
H9A0.14540.01270.08250.041*
H9B0.01490.13190.07020.041*
C120.1687 (14)0.0427 (15)0.1695 (3)0.070 (3)
H12A0.10720.04150.19790.105*
H12B0.28110.12440.16910.105*
H12C0.21940.07180.16260.105*
C110.1795 (13)0.0228 (19)0.1376 (3)0.075 (3)
H11A0.23380.02580.16660.112*
H11B0.14020.13860.12900.112*
H11C0.28300.02080.11810.112*
C10.460 (2)0.458 (2)0.2350 (3)0.088 (4)
H1A0.48560.43430.26420.106*
C50.2290 (15)0.5402 (13)0.1788 (3)0.059 (3)
H5A0.09770.57410.17000.071*
C30.5749 (14)0.4706 (14)0.1623 (3)0.064 (3)
H3A0.68130.45860.14220.077*
C20.6137 (19)0.4389 (17)0.2055 (3)0.087 (4)
H2A0.74470.40470.21450.105*
C60.2675 (17)0.512 (2)0.2223 (3)0.082 (3)
H6A0.16380.52840.24280.098*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.0329 (4)0.0183 (3)0.0340 (4)0.0008 (4)0.0026 (3)0.0053 (4)
N10.031 (3)0.027 (3)0.031 (3)0.000 (2)0.004 (2)0.000 (2)
O10.030 (3)0.038 (3)0.037 (3)0.013 (2)0.003 (2)0.006 (2)
O30.045 (3)0.041 (3)0.051 (3)0.025 (3)0.001 (3)0.018 (2)
O20.038 (3)0.019 (3)0.049 (3)0.021 (2)0.007 (2)0.004 (2)
O40.032 (3)0.031 (3)0.052 (3)0.008 (2)0.003 (2)0.007 (2)
C40.054 (4)0.036 (4)0.039 (4)0.006 (6)0.005 (4)0.008 (3)
C130.037 (4)0.027 (4)0.036 (4)0.018 (4)0.002 (4)0.003 (3)
C70.049 (5)0.024 (4)0.044 (4)0.002 (4)0.002 (4)0.004 (3)
C80.030 (3)0.019 (4)0.034 (4)0.010 (3)0.004 (3)0.002 (3)
C140.029 (4)0.024 (4)0.044 (4)0.002 (3)0.000 (3)0.004 (3)
C100.051 (5)0.043 (5)0.042 (4)0.001 (4)0.012 (4)0.006 (4)
C90.045 (4)0.021 (3)0.036 (4)0.000 (3)0.005 (4)0.006 (3)
C120.075 (6)0.089 (9)0.045 (5)0.017 (6)0.005 (5)0.025 (5)
C110.062 (6)0.107 (10)0.056 (5)0.030 (7)0.008 (4)0.013 (7)
C10.105 (9)0.122 (13)0.037 (5)0.010 (9)0.020 (6)0.001 (6)
C50.069 (6)0.057 (7)0.051 (5)0.009 (5)0.002 (4)0.014 (5)
C30.065 (6)0.070 (7)0.057 (5)0.003 (6)0.008 (4)0.003 (5)
C20.071 (7)0.125 (12)0.066 (6)0.013 (9)0.021 (6)0.002 (6)
C60.093 (7)0.111 (10)0.040 (5)0.002 (9)0.014 (5)0.019 (8)
Geometric parameters (Å, º) top
Zn1—O2i1.982 (5)C14—H14A0.9300
Zn1—O4ii1.989 (5)C10—C121.514 (11)
Zn1—O32.081 (5)C10—C111.524 (12)
Zn1—O12.110 (5)C10—C91.531 (10)
Zn1—N12.132 (6)C10—H10A0.9800
N1—C71.475 (8)C9—H9A0.9700
N1—C81.484 (9)C9—H9B0.9700
N1—H1B0.8599C12—H12A0.9600
O1—C131.248 (8)C12—H12B0.9600
O3—C141.239 (8)C12—H12C0.9600
O2—C131.266 (8)C11—H11A0.9600
O2—Zn1iii1.982 (5)C11—H11B0.9600
O4—C141.255 (8)C11—H11C0.9600
O4—Zn1iv1.989 (5)C1—C21.355 (14)
C4—C51.379 (11)C1—C61.370 (16)
C4—C31.374 (11)C1—H1A0.9300
C4—C71.514 (9)C5—C61.381 (12)
C13—C81.516 (9)C5—H5A0.9300
C7—H7A0.9700C3—C21.376 (12)
C7—H7B0.9700C3—H3A0.9300
C8—C91.531 (10)C2—H2A0.9300
C8—H8A0.9800C6—H6A0.9300
O2i—Zn1—O4ii101.5 (2)O4—C14—H14A116.2
O2i—Zn1—O398.4 (2)C12—C10—C11111.5 (7)
O4ii—Zn1—O3103.6 (2)C12—C10—C9112.5 (7)
O2i—Zn1—O191.3 (2)C11—C10—C9110.0 (7)
O4ii—Zn1—O198.38 (18)C12—C10—H10A107.5
O3—Zn1—O1153.55 (19)C11—C10—H10A107.5
O2i—Zn1—N1150.6 (2)C9—C10—H10A107.5
O4ii—Zn1—N1107.1 (2)C8—C9—C10115.6 (6)
O3—Zn1—N181.4 (2)C8—C9—H9A108.4
O1—Zn1—N178.3 (2)C10—C9—H9A108.4
C7—N1—C8113.1 (5)C8—C9—H9B108.4
C7—N1—Zn1108.1 (4)C10—C9—H9B108.4
C8—N1—Zn1109.5 (4)H9A—C9—H9B107.4
C7—N1—H1B107.9C10—C12—H12A109.5
C8—N1—H1B109.0C10—C12—H12B109.5
Zn1—N1—H1B109.1H12A—C12—H12B109.5
C13—O1—Zn1115.8 (5)C10—C12—H12C109.5
C14—O3—Zn1124.9 (5)H12A—C12—H12C109.5
C13—O2—Zn1iii113.5 (4)H12B—C12—H12C109.5
C14—O4—Zn1iv118.4 (5)C10—C11—H11A109.5
C5—C4—C3117.9 (7)C10—C11—H11B109.5
C5—C4—C7120.9 (7)H11A—C11—H11B109.5
C3—C4—C7121.1 (7)C10—C11—H11C109.5
O1—C13—O2124.8 (7)H11A—C11—H11C109.5
O1—C13—C8119.8 (7)H11B—C11—H11C109.5
O2—C13—C8115.4 (6)C2—C1—C6120.7 (9)
N1—C7—C4114.4 (6)C2—C1—H1A119.7
N1—C7—H7A108.7C6—C1—H1A119.7
C4—C7—H7A108.7C4—C5—C6121.1 (9)
N1—C7—H7B108.7C4—C5—H5A119.5
C4—C7—H7B108.7C6—C5—H5A119.5
H7A—C7—H7B107.6C2—C3—C4121.4 (9)
N1—C8—C9110.3 (5)C2—C3—H3A119.3
N1—C8—C13109.3 (5)C4—C3—H3A119.3
C9—C8—C13110.0 (6)C1—C2—C3119.7 (10)
N1—C8—H8A109.1C1—C2—H2A120.2
C9—C8—H8A109.1C3—C2—H2A120.2
C13—C8—H8A109.1C1—C6—C5119.2 (9)
O3—C14—O4127.6 (7)C1—C6—H6A120.4
O3—C14—H14A116.2C5—C6—H6A120.4
Symmetry codes: (i) x1/2, y+1/2, z; (ii) x+1/2, y+3/2, z; (iii) x+1/2, y+1/2, z; (iv) x1/2, y+3/2, z.
 

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