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This paper reports 22 examples of space-group changes from low to higher symmetry. The revisions involve 15 crystal structures that were originally described in space group
P2
1, six in
P and one in
P1. The relevance of higher-symmetry elements is discussed in connection with the crystallography, the molecular dimensions and, when possible, the spectroscopic properties.
Supporting information
| Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768102022668/an0613sup1.cif Contains datablocks global, barjaf, claecu, qanxos, sazpak, yakvip, bogpiw, novhub, nohned, nohned01, qelpus, aplsol, doqzak, bamubr, farner, farniv, himfue, horbiz, pejvab, sixfio, bihjux, bihlin, zexbuz01, pyrhsb |
CCDC references: 205138; 205139; 205140; 205141; 205142; 205143; 205144; 205145; 205146; 205147; 205148; 205149; 205150; 205151; 205152; 205153; 205154; 205155; 205156; 205157; 205158; 205159; 206124
For all compounds, program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997).
(barjaf) bis(Nitrato)-((4
S,5S)-2,2-dimethyl-4,5-bis(2-pyridyl)-1,3-dioxolane)-cobalt(ii)
top
Crystal data top
C15H16CoN4O8 | γ = 90° |
Mr = 439.25 | V = 1810.3 (6) Å3 |
C2221 | Z = 4 |
a = 7.625 (2) Å | F(000) = 900 |
b = 19.808 (2) Å | Dx = 1.612 Mg m−3 |
c = 11.986 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 1.00 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.046 |
Graphite monochromator | θmax = 46.0°, θmin = 2.1° |
8912 measured reflections | h = −8→8 |
2688 independent reflections | k = −28→28 |
2560 reflections with I > 2σ(I) | l = −12→12 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.018 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.109 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.58 | (Δ/σ)max = 4.200 |
2688 reflections | Δρmax = 0.52 e Å−3 |
105 parameters | Δρmin = −0.22 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.140 (8) |
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 | x | y | z | Uiso*/Ueq | Occ. (<1) |
Co1 | 0.0000 | 0.022600 (15) | 0.2500 | 0.02000 (9)* | |
O2 | 0.01940 (18) | 0.25290 (6) | 0.15650 (11) | 0.0200 (2)* | |
O3 | −0.17430 (17) | −0.02200 (7) | 0.14290 (11) | 0.0200 (2)* | |
O4 | −0.14130 (17) | −0.10820 (6) | 0.03250 (12) | 0.0200 (2)* | |
O5 | 0.08120 (19) | −0.06770 (7) | 0.12090 (12) | 0.0200 (2)* | |
N1 | 0.18870 (19) | 0.08220 (7) | 0.17230 (14) | 0.0200 (2)* | |
N4 | −0.0758 (2) | −0.06610 (8) | 0.09780 (14) | 0.0200 (3)* | |
C1 | 0.3360 (2) | 0.04790 (9) | 0.14270 (15) | 0.0200 (3)* | |
H1 | 0.343 (4) | 0.0021 (15) | 0.159 (3) | 0.020 (6)* | |
C2 | 0.4745 (2) | 0.07900 (8) | 0.08950 (16) | 0.0200 (2)* | |
H2 | 0.574 (4) | 0.0544 (13) | 0.071 (2) | 0.020 (6)* | |
C3 | 0.4643 (2) | 0.14570 (9) | 0.06430 (16) | 0.0200 (3)* | |
H3 | 0.555 (4) | 0.1672 (12) | 0.027 (3) | 0.020 (6)* | |
C4 | 0.3159 (2) | 0.18090 (8) | 0.09570 (16) | 0.0200 (3)* | |
H4 | 0.307 (4) | 0.2269 (13) | 0.081 (3) | 0.020 (6)* | |
C5 | 0.1802 (2) | 0.14760 (9) | 0.14880 (15) | 0.0200 (3)* | |
C6 | 0.0106 (2) | 0.18400 (8) | 0.18520 (13) | 0.0200 (3)* | |
H18 | −0.083 (4) | 0.1564 (14) | 0.144 (2) | 0.020 (6)* | |
C14? | 0.0622 (5) | 0.29070 (16) | 0.2570 (4) | 0.0200 (5)* | 0.50 |
C15 | 0.0000 | 0.35750 (11) | 0.2500 | 0.0200 (4)* | |
H9 | −0.033 (9) | 0.377 (3) | 0.321 (6) | 0.020 (12)* | 0.50 |
H10 | −0.052 (9) | 0.384 (3) | 0.192 (6) | 0.020 (13)* | 0.50 |
H11 | 0.124 (8) | 0.357 (2) | 0.243 (6) | 0.020 (11)* | 0.50 |
C17? | 0.2612 (5) | 0.29550 (17) | 0.2818 (3) | 0.0200 (6)* | 0.50 |
H15? | 0.321 (8) | 0.312 (3) | 0.217 (5) | 0.020 (13)* | 0.50 |
H16? | 0.305 (8) | 0.252 (3) | 0.301 (5) | 0.020 (12)* | 0.50 |
H17? | 0.280 (8) | 0.326 (3) | 0.343 (5) | 0.020 (12)* | 0.50 |
Geometric parameters (Å, º) top
Co1—O3 | 2.0481 (14) | C1—C2 | 1.379 (2) |
Co1—O3i | 2.0481 (14) | C2—C3 | 1.358 (2) |
Co1—N1i | 2.0812 (15) | C3—C4 | 1.381 (2) |
Co1—N1 | 2.0812 (15) | C4—C5 | 1.382 (3) |
O2—C6 | 1.409 (2) | C5—C6 | 1.544 (2) |
O2—C14?i | 1.422 (4) | C6—C6i | 1.562 (3) |
O2—C14? | 1.455 (5) | C14?—C14?i | 0.963 (8) |
O3—N4 | 1.273 (2) | C14?—C15 | 1.408 (4) |
O4—N4 | 1.248 (2) | C14?—O2i | 1.422 (4) |
O5—N4 | 1.229 (2) | C14?—C17? | 1.549 (5) |
N1—C5 | 1.327 (2) | C15—C14?i | 1.408 (4) |
N1—C1 | 1.360 (2) | | |
| | | |
O3—Co1—O3i | 128.89 (8) | C3—C4—C5 | 119.85 (15) |
O3—Co1—N1i | 94.39 (6) | N1—C5—C4 | 121.80 (16) |
O3i—Co1—N1i | 114.38 (6) | N1—C5—C6 | 115.90 (14) |
O3—Co1—N1 | 114.38 (6) | C4—C5—C6 | 122.30 (15) |
O3i—Co1—N1 | 94.39 (6) | O2—C6—C5 | 110.09 (14) |
N1i—Co1—N1 | 110.88 (8) | O2—C6—C6i | 104.34 (8) |
C6—O2—C14?i | 108.13 (18) | C5—C6—C6i | 111.58 (17) |
C6—O2—C14? | 107.87 (18) | C14?i—C14?—C15 | 70.00 (16) |
C14?i—O2—C14? | 39.1 (3) | C14?i—C14?—O2i | 72.3 (4) |
N4—O3—Co1 | 100.33 (11) | C15—C14?—O2i | 113.0 (3) |
C5—N1—C1 | 118.20 (15) | C14?i—C14?—O2 | 68.6 (4) |
C5—N1—Co1 | 127.94 (12) | C15—C14?—O2 | 111.0 (3) |
C1—N1—Co1 | 113.85 (11) | O2i—C14?—O2 | 103.6 (2) |
O5—N4—O4 | 120.92 (17) | C14?i—C14?—C17? | 176.3 (3) |
O5—N4—O3 | 119.79 (17) | C15—C14?—C17? | 106.5 (2) |
O4—N4—O3 | 119.27 (15) | O2i—C14?—C17? | 108.7 (3) |
N1—C1—C2 | 122.01 (16) | O2—C14?—C17? | 114.2 (3) |
C3—C2—C1 | 119.59 (16) | C14?i—C15—C14? | 40.0 (3) |
C2—C3—C4 | 118.53 (16) | | |
Symmetry code: (i) −x, y, −z+1/2. |
(claecu) bis(Chloroacetato)-(
N,
N,
N',
N'-tetramethylethylenediamine) copper(ii)
top
Crystal data top
C10H20Cl2CuN2O4 | γ = 90° |
Mr = 366.72 | V = 1523.5 (11) Å3 |
C2221 | Z = 4 |
a = 9.002 (3) Å | F(000) = 756 |
b = 11.400 (5) Å | Dx = 1.599 Mg m−3 |
c = 14.846 (7) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 1.79 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.006 |
Graphite monochromator | θmax = 45.6°, θmin = 2.7° |
8366 measured reflections | h = −16→16 |
2103 independent reflections | k = −16→16 |
2095 reflections with I > 2σ(I) | l = −14→14 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.006 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.042 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.25 | (Δ/σ)max = 1.279 |
2103 reflections | Δρmax = 0.10 e Å−3 |
79 parameters | Δρmin = −0.16 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.003 (5) |
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 | x | y | z | Uiso*/Ueq | |
Cu1 | 0.00000 | 0.103000 (12) | 0.25000 | 0.02000 (4)* | |
N1 | −0.14260 (7) | −0.02670 (6) | 0.21200 (5) | 0.02000 (11)* | |
C1 | −0.08360 (8) | −0.13590 (7) | 0.25390 (7) | 0.02000 (12)* | |
H1 | −0.1257 (15) | −0.2107 (12) | 0.2215 (9) | 0.020 (3)* | |
H2 | −0.1210 (14) | −0.1400 (12) | 0.3165 (10) | 0.020 (3)* | |
C3 | −0.15370 (7) | −0.04170 (8) | 0.11320 (6) | 0.02000 (13)* | |
H5 | −0.1915 (15) | 0.0310 (11) | 0.0870 (8) | 0.020 (3)* | |
H6 | −0.2118 (13) | −0.1108 (11) | 0.1010 (9) | 0.020 (3)* | |
H7 | −0.0608 (14) | −0.0527 (11) | 0.0830 (9) | 0.020 (3)* | |
C4 | −0.29120 (8) | 0.00080 (7) | 0.24880 (6) | 0.02000 (13)* | |
H8 | −0.3248 (14) | 0.0767 (12) | 0.2150 (8) | 0.020 (3)* | |
H9 | −0.3630 (14) | −0.0630 (12) | 0.2350 (9) | 0.020 (3)* | |
H10 | −0.2898 (13) | 0.0178 (11) | 0.3085 (9) | 0.020 (3)* | |
O1 | −0.10440 (6) | 0.22160 (5) | 0.17640 (4) | 0.02000 (10)* | |
C7 | −0.02140 (7) | 0.23430 (7) | 0.10700 (6) | 0.02000 (12)* | |
C8 | −0.08500 (8) | 0.32340 (8) | 0.04060 (6) | 0.02000 (12)* | |
H17 | −0.1833 (13) | 0.3037 (12) | 0.0180 (8) | 0.020 (3)* | |
H18 | −0.0920 (12) | 0.3990 (13) | 0.0710 (8) | 0.020 (3)* | |
Cl1 | 0.025500 (18) | 0.341600 (17) | −0.057800 (12) | 0.02000 (4)* | |
O2 | 0.09550 (6) | 0.18120 (6) | 0.09410 (4) | 0.02000 (11)* | |
Geometric parameters (Å, º) top
Cu1—O1i | 1.9761 (8) | N1—C1 | 1.4895 (12) |
Cu1—O1 | 1.9762 (8) | C1—C1i | 1.5096 (15) |
Cu1—N1 | 2.0377 (9) | O1—C7 | 1.2809 (10) |
Cu1—N1i | 2.0377 (9) | C7—O2 | 1.2290 (9) |
N1—C4 | 1.4786 (11) | C7—C8 | 1.5268 (12) |
N1—C3 | 1.4801 (14) | C8—Cl1 | 1.7795 (11) |
| | | |
O1i—Cu1—O1 | 93.66 (5) | C4—N1—Cu1 | 108.29 (6) |
O1i—Cu1—N1 | 161.64 (3) | C3—N1—Cu1 | 113.62 (5) |
O1—Cu1—N1 | 92.51 (4) | C1—N1—Cu1 | 105.44 (6) |
O1i—Cu1—N1i | 92.51 (4) | N1—C1—C1i | 108.87 (6) |
O1—Cu1—N1i | 161.64 (3) | C7—O1—Cu1 | 104.16 (5) |
N1—Cu1—N1i | 86.96 (5) | O2—C7—O1 | 124.69 (8) |
C4—N1—C3 | 109.24 (6) | O2—C7—C8 | 123.24 (8) |
C4—N1—C1 | 110.21 (7) | O1—C7—C8 | 112.07 (6) |
C3—N1—C1 | 109.96 (7) | C7—C8—Cl1 | 113.45 (6) |
Symmetry code: (i) −x, y, −z+1/2. |
(qanxos) (
syn-rac)-
trans-Dichloro-(5,7,7,12,14,14-hexamethyl-1,4,8,11-tetraazacyclo- tetradeca-4,11-diene)-cobalt(iii) perchlorate
top
Crystal data top
C16Cl3CoN4O4 | γ = 90° |
Mr = 477.48 | V = 2188.1 (6) Å3 |
C2221 | Z = 4 |
a = 10.621 (2) Å | F(000) = 936 |
b = 11.624 (2) Å | Dx = 1.449 Mg m−3 |
c = 17.723 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 1.18 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.015 |
Graphite monochromator | θmax = 38.6°, θmin = 2.3° |
9520 measured reflections | h = −16→16 |
2392 independent reflections | k = −16→16 |
2382 reflections with I > 2σ(I) | l = −16→16 |
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)] = 0.002 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.015 | (Δ/σ)max = 2.138 |
S = 0.09 | Δρmax = 0.06 e Å−3 |
2392 reflections | Δρmin = −0.08 e Å−3 |
65 parameters | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
0 restraints | Absolute structure parameter: −0.001 (2) |
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 | x | y | z | Uiso*/Ueq | Occ. (<1) |
Co1 | 0.321200 (4) | 0.0000 | 0.0000 | 0.02000 (2)* | |
Cl1 | 0.533000 (7) | 0.0000 | 0.0000 | 0.02000 (2)* | |
Cl2 | 0.109300 (7) | 0.0000 | 0.0000 | 0.02000 (2)* | |
N1 | 0.31570 (2) | 0.068800 (18) | 0.102200 (14) | 0.02000 (4)* | |
N2 | 0.32330 (2) | −0.144600 (19) | 0.053100 (15) | 0.02000 (4)* | |
C1 | 0.38630 (2) | −0.01010 (2) | 0.152600 (17) | 0.02000 (5)* | |
C2 | 0.34350 (2) | −0.13130 (2) | 0.135500 (16) | 0.02000 (5)* | |
C3 | 0.30130 (2) | −0.244700 (19) | 0.025700 (17) | 0.02000 (5)* | |
C4 | 0.26390 (2) | −0.25960 (2) | −0.054800 (17) | 0.02000 (5)* | |
C5 | 0.33980 (2) | −0.19680 (2) | −0.113500 (17) | 0.02000 (5)* | |
C11 | 0.30920 (2) | −0.35280 (2) | 0.072500 (17) | 0.02000 (4)* | |
C12 | 0.29180 (2) | −0.23070 (2) | −0.192300 (16) | 0.02000 (4)* | |
C13 | 0.47870 (2) | −0.22710 (2) | −0.107700 (17) | 0.02000 (4)* | |
Cl3 | 0.0000 | 0.038400 (6) | 0.2500 | 0.02000 (2)* | |
O1 | 0.00450 (4) | 0.15920 (3) | 0.268200 (18) | 0.02000 (8)* | 0.50 |
O2 | −0.10430 (3) | −0.01440 (3) | 0.27610 (3) | 0.02000 (7)* | 0.50 |
O3 | 0.04160 (3) | 0.01610 (3) | 0.17900 (2) | 0.02000 (6)* | 0.50 |
O4 | 0.11040 (3) | −0.00660 (3) | 0.30160 (2) | 0.02000 (7)* | 0.50 |
Geometric parameters (Å, º) top
Co1—N2 | 1.9265 (3) | C5—C12 | 1.5381 (4) |
Co1—N2i | 1.9265 (3) | Cl3—O2 | 1.3483 (4) |
Co1—N1 | 1.9808 (3) | Cl3—O2ii | 1.3483 (4) |
Co1—N1i | 1.9808 (3) | Cl3—O3ii | 1.3586 (4) |
Co1—Cl1 | 2.2495 (4) | Cl3—O3 | 1.3586 (4) |
Co1—Cl2 | 2.2506 (4) | Cl3—O1 | 1.4415 (4) |
N1—C1 | 1.4837 (4) | Cl3—O1ii | 1.4415 (4) |
N1—C5i | 1.5230 (4) | Cl3—O4 | 1.5763 (4) |
N2—C3 | 1.2823 (4) | Cl3—O4ii | 1.5763 (4) |
N2—C2 | 1.4841 (4) | O1—O1ii | 0.6522 (6) |
C1—C2 | 1.5111 (4) | O2—O3ii | 1.0965 (6) |
C3—C4 | 1.4911 (4) | O2—O4ii | 1.3816 (7) |
C3—C11 | 1.5080 (4) | O3—O2ii | 1.0965 (6) |
C4—C5 | 1.5050 (4) | O3—O4ii | 1.6716 (6) |
C5—C13 | 1.5202 (4) | O4—O2ii | 1.3816 (7) |
C5—N1i | 1.5230 (4) | O4—O3ii | 1.6716 (6) |
| | | |
N2—Co1—N2i | 178.673 (13) | O2—Cl3—O3 | 119.88 (2) |
N2—Co1—N1 | 84.601 (14) | O2ii—Cl3—O3 | 47.79 (2) |
N2i—Co1—N1 | 95.439 (13) | O3ii—Cl3—O3 | 158.00 (3) |
N2—Co1—N1i | 95.439 (13) | O2—Cl3—O1 | 113.20 (2) |
N2i—Co1—N1i | 84.601 (14) | O2ii—Cl3—O1 | 119.53 (2) |
N1—Co1—N1i | 176.620 (13) | O3ii—Cl3—O1 | 89.39 (2) |
N2—Co1—Cl1 | 89.337 (7) | O3—Cl3—O1 | 112.48 (2) |
N2i—Co1—Cl1 | 89.337 (7) | O2—Cl3—O1ii | 119.53 (2) |
N1—Co1—Cl1 | 91.690 (6) | O2ii—Cl3—O1ii | 113.20 (2) |
N1i—Co1—Cl1 | 91.690 (6) | O3ii—Cl3—O1ii | 112.48 (2) |
N2—Co1—Cl2 | 90.663 (7) | O3—Cl3—O1ii | 89.39 (2) |
N2i—Co1—Cl2 | 90.663 (7) | O1—Cl3—O1ii | 26.15 (3) |
N1—Co1—Cl2 | 88.310 (6) | O2—Cl3—O4 | 105.13 (2) |
N1i—Co1—Cl2 | 88.310 (6) | O2ii—Cl3—O4 | 55.72 (3) |
Cl1—Co1—Cl2 | 180.0 | O3ii—Cl3—O4 | 68.98 (2) |
C1—N1—C5i | 116.09 (2) | O3—Cl3—O4 | 103.42 (2) |
C1—N1—Co1 | 106.621 (18) | O1—Cl3—O4 | 99.72 (2) |
C5i—N1—Co1 | 120.645 (19) | O1ii—Cl3—O4 | 118.536 (19) |
C3—N2—C2 | 119.57 (2) | O2—Cl3—O4ii | 55.72 (3) |
C3—N2—Co1 | 127.20 (2) | O2ii—Cl3—O4ii | 105.13 (2) |
C2—N2—Co1 | 113.046 (17) | O3ii—Cl3—O4ii | 103.42 (2) |
N1—C1—C2 | 107.67 (2) | O3—Cl3—O4ii | 68.98 (2) |
N2—C2—C1 | 109.75 (2) | O1—Cl3—O4ii | 118.536 (19) |
N2—C3—C4 | 121.08 (2) | O1ii—Cl3—O4ii | 99.72 (2) |
N2—C3—C11 | 122.53 (3) | O4—Cl3—O4ii | 141.24 (3) |
C4—C3—C11 | 116.38 (2) | O1ii—O1—Cl3 | 76.926 (13) |
C3—C4—C5 | 117.54 (2) | O3ii—O2—Cl3 | 66.60 (3) |
C4—C5—C13 | 111.14 (2) | O3ii—O2—O4ii | 136.94 (5) |
C4—C5—N1i | 107.03 (2) | Cl3—O2—O4ii | 70.53 (3) |
C13—C5—N1i | 112.37 (2) | O2ii—O3—Cl3 | 65.61 (3) |
C4—C5—C12 | 109.02 (2) | O2ii—O3—O4ii | 112.72 (4) |
C13—C5—C12 | 108.89 (2) | Cl3—O3—O4ii | 61.67 (2) |
N1i—C5—C12 | 108.30 (2) | O2ii—O4—Cl3 | 53.75 (2) |
O2—Cl3—O2ii | 125.84 (3) | O2ii—O4—O3ii | 99.79 (3) |
O2—Cl3—O3ii | 47.79 (2) | Cl3—O4—O3ii | 49.348 (19) |
O2ii—Cl3—O3ii | 119.88 (2) | | |
Symmetry codes: (i) x, −y, −z; (ii) −x, y, −z+1/2. |
(sazpak) Diaqua-(ethylenediamine-
N,
N')-bis(guanosine
5'-monophosphate-N$7!)-nickel ethylenediamine hydrate
top
Crystal data top
C24N14NiO24.50P2 | γ = 90° |
Mr = 997.01 | V = 8603.1 (15) Å3 |
C2221 | Z = 8 |
a = 17.462 (2) Å | F(000) = 3968 |
b = 17.337 (2) Å | Dx = 1.540 Mg m−3 |
c = 28.417 (2) Å | Mo Kα radiation, λ = 0.71073 Å |
α = 90° | µ = 0.63 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.042 |
Graphite monochromator | θmax = 27.1°, θmin = 1.4° |
14536 measured reflections | h = −20→20 |
3648 independent reflections | k = −20→20 |
3605 reflections with I > 2σ(I) | l = −16→16 |
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)] = 0.006 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.039 | (Δ/σ)max = 0.880 |
S = 0.30 | Δρmax = 0.16 e Å−3 |
3648 reflections | Δρmin = −0.21 e Å−3 |
267 parameters | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
0 restraints | Absolute structure parameter: 0.010 (5) |
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 | x | y | z | Uiso*/Ueq | Occ. (<1) |
Ni1 | 0.298650 (15) | 0.0000 | 0.0000 | 0.02000 (8)* | |
P1 | 0.23220 (2) | 0.29400 (2) | 0.00420 (2) | 0.02000 (10)* | |
O1 | 0.30327 (5) | 0.10173 (5) | −0.04095 (5) | 0.0200 (2)* | |
O3 | 0.45785 (6) | −0.12660 (6) | 0.03725 (5) | 0.0200 (2)* | |
O4 | 0.42922 (6) | 0.25003 (6) | 0.10735 (5) | 0.0200 (3)* | |
O5 | 0.50230 (6) | 0.36440 (5) | 0.01020 (4) | 0.0200 (2)* | |
O6 | 0.59385 (6) | 0.29415 (6) | 0.07580 (5) | 0.0200 (2)* | |
O7 | 0.30607 (5) | 0.27387 (6) | 0.03695 (5) | 0.0200 (2)* | |
O8 | 0.16992 (5) | 0.31813 (6) | 0.03810 (5) | 0.0200 (2)* | |
O9 | 0.21407 (6) | 0.21787 (5) | −0.01960 (4) | 0.0200 (2)* | |
O10 | 0.25460 (6) | 0.35565 (5) | −0.02945 (5) | 0.0200 (2)* | |
N1 | 0.20748 (7) | 0.04338 (7) | 0.04070 (6) | 0.0200 (3)* | |
N3 | 0.38678 (7) | 0.03948 (7) | 0.04695 (6) | 0.0200 (3)* | |
N4 | 0.56972 (7) | −0.06397 (7) | 0.05040 (6) | 0.0200 (3)* | |
N5 | 0.68965 (7) | −0.01035 (7) | 0.06060 (6) | 0.0200 (3)* | |
N6 | 0.58475 (7) | 0.06510 (7) | 0.07595 (6) | 0.0200 (3)* | |
N7 | 0.46355 (7) | 0.13165 (7) | 0.07635 (6) | 0.0200 (3)* | |
C1 | 0.13870 (8) | 0.00740 (8) | 0.02415 (6) | 0.0200 (4)* | |
C3 | 0.45938 (9) | 0.00928 (9) | 0.05435 (7) | 0.0200 (4)* | |
C4 | 0.48853 (9) | −0.06447 (8) | 0.04705 (7) | 0.0200 (4)* | |
C5 | 0.61263 (8) | −0.00117 (9) | 0.06260 (7) | 0.0200 (3)* | |
C6 | 0.50773 (9) | 0.06693 (8) | 0.07015 (7) | 0.0200 (4)* | |
C7 | 0.39065 (9) | 0.11185 (8) | 0.06105 (7) | 0.0200 (4)* | |
C8 | 0.49200 (9) | 0.20405 (8) | 0.09200 (7) | 0.0200 (3)* | |
C9 | 0.42228 (8) | 0.31842 (8) | 0.07590 (7) | 0.0200 (3)* | |
C10 | 0.46997 (8) | 0.29792 (8) | 0.03315 (7) | 0.0200 (4)* | |
C11 | 0.53510 (8) | 0.24885 (8) | 0.05325 (7) | 0.0200 (3)* | |
C12 | 0.33885 (9) | 0.33100 (8) | 0.06725 (7) | 0.0200 (4)* | |
Ni2 | 0.5000 | 0.225350 (14) | 0.2500 | 0.02000 (8)* | |
P3 | 0.22225 (2) | 0.30960 (2) | 0.22155 (2) | 0.02000 (10)* | |
O19 | 0.60582 (5) | 0.22517 (5) | 0.21415 (5) | 0.0200 (2)* | |
O21 | 0.63575 (6) | 0.07470 (6) | 0.20845 (5) | 0.0200 (2)* | |
O22 | 0.25920 (6) | 0.08675 (5) | 0.14255 (4) | 0.0200 (2)* | |
O23 | 0.14867 (5) | 0.03987 (5) | 0.24615 (5) | 0.0200 (2)* | |
O24 | 0.21070 (6) | −0.07095 (5) | 0.18450 (5) | 0.0200 (2)* | |
O25 | 0.23750 (6) | 0.22365 (6) | 0.20230 (5) | 0.0200 (2)* | |
O26 | 0.29385 (5) | 0.32420 (5) | 0.24900 (5) | 0.0200 (2)* | |
O27 | 0.15137 (5) | 0.30417 (5) | 0.25170 (5) | 0.0200 (2)* | |
O28 | 0.21267 (6) | 0.36298 (5) | 0.18020 (5) | 0.0200 (2)* | |
N17 | 0.53875 (7) | 0.31540 (7) | 0.29335 (6) | 0.0200 (3)* | |
N19 | 0.46782 (7) | 0.13418 (7) | 0.20245 (6) | 0.0200 (3)* | |
N20 | 0.58525 (7) | −0.03820 (7) | 0.18255 (6) | 0.0200 (3)* | |
N21 | 0.54817 (7) | −0.15517 (7) | 0.14905 (6) | 0.0200 (3)* | |
N22 | 0.45540 (7) | −0.06000 (7) | 0.16135 (6) | 0.0200 (3)* | |
N23 | 0.37800 (7) | 0.05455 (7) | 0.17325 (6) | 0.0200 (3)* | |
C27 | 0.51533 (8) | 0.38872 (8) | 0.27005 (6) | 0.0200 (4)* | |
C29 | 0.49773 (9) | 0.06528 (9) | 0.19280 (6) | 0.0200 (4)* | |
C30 | 0.57735 (9) | 0.03755 (9) | 0.19640 (7) | 0.0200 (4)* | |
C31 | 0.52692 (8) | −0.08353 (8) | 0.16340 (7) | 0.0200 (4)* | |
C32 | 0.44627 (9) | 0.01367 (8) | 0.17370 (7) | 0.0200 (4)* | |
C33 | 0.39300 (8) | 0.12660 (9) | 0.19060 (7) | 0.0200 (4)* | |
C34 | 0.30295 (9) | 0.02320 (8) | 0.15980 (7) | 0.0200 (3)* | |
C35 | 0.19307 (9) | 0.09912 (8) | 0.17240 (7) | 0.0200 (4)* | |
C36 | 0.21265 (8) | 0.06035 (8) | 0.21845 (7) | 0.0200 (3)* | |
C37 | 0.26145 (8) | −0.01035 (8) | 0.20205 (7) | 0.0200 (4)* | |
C38 | 0.17805 (8) | 0.18565 (9) | 0.17510 (7) | 0.0200 (3)* | |
N13 | 0.14797 (7) | 0.29833 (7) | 0.34425 (6) | 0.0200 (3)* | |
N14 | 0.28272 (7) | 0.15217 (7) | 0.37800 (6) | 0.0200 (3)* | |
C23 | 0.21842 (9) | 0.26832 (8) | 0.36460 (7) | 0.0200 (4)* | |
C24 | 0.22548 (8) | 0.18463 (8) | 0.34900 (7) | 0.0200 (3)* | |
O48 | 0.02962 (11) | 0.18173 (11) | 0.36345 (9) | 0.0200 (5)* | 0.50 |
O49 | 0.05827 (11) | 0.23722 (11) | 0.40845 (10) | 0.0200 (5)* | 0.50 |
O37 | 0.38802 (6) | 0.55832 (6) | 0.03400 (5) | 0.0200 (2)* | |
O39 | 0.30772 (5) | 0.48513 (5) | 0.16625 (4) | 0.0200 (2)* | |
O41 | 0.08448 (6) | 0.19537 (5) | 0.06830 (5) | 0.0200 (2)* | |
O42 | 0.05268 (5) | 0.01863 (5) | 0.37895 (4) | 0.0200 (2)* | |
O45 | 0.0000 | 0.25415 (8) | 0.2500 | 0.0200 (3)* | |
O46 | 0.57687 (5) | 0.42682 (5) | 0.12830 (5) | 0.0200 (2)* | |
Geometric parameters (Å, º) top
Ni1—N1i | 2.1066 (14) | Ni2—O19ii | 2.1100 (11) |
Ni1—N1 | 2.1066 (14) | Ni2—O19 | 2.1100 (11) |
Ni1—O1i | 2.1146 (11) | Ni2—N19 | 2.1541 (14) |
Ni1—O1 | 2.1146 (11) | Ni2—N19ii | 2.1541 (14) |
Ni1—N3 | 2.1487 (14) | P3—O26 | 1.4952 (11) |
Ni1—N3i | 2.1487 (14) | P3—O28 | 1.5051 (12) |
P1—O10 | 1.4865 (12) | P3—O27 | 1.5083 (12) |
P1—O8 | 1.5119 (13) | P3—O25 | 1.6096 (11) |
P1—O9 | 1.5165 (10) | O21—C30 | 1.2538 (19) |
P1—O7 | 1.6284 (12) | O22—C34 | 1.4275 (19) |
O3—C4 | 1.2349 (19) | O22—C35 | 1.449 (2) |
O4—C8 | 1.424 (2) | O23—C36 | 1.412 (2) |
O4—C9 | 1.4897 (19) | O24—C37 | 1.462 (2) |
O5—C10 | 1.4396 (19) | O25—C38 | 1.452 (2) |
O6—C11 | 1.442 (2) | N17—C27 | 1.4905 (19) |
O7—C12 | 1.432 (2) | N19—C29 | 1.332 (2) |
N1—C1 | 1.433 (2) | N19—C33 | 1.356 (2) |
N3—C7 | 1.3189 (19) | N20—C30 | 1.3779 (19) |
N3—C3 | 1.388 (2) | N20—C31 | 1.397 (2) |
N4—C5 | 1.366 (2) | N21—C31 | 1.359 (2) |
N4—C4 | 1.4210 (19) | N22—C31 | 1.315 (2) |
N5—C5 | 1.3555 (19) | N22—C32 | 1.334 (2) |
N6—C5 | 1.304 (2) | N23—C33 | 1.368 (2) |
N6—C6 | 1.355 (2) | N23—C32 | 1.387 (2) |
N7—C6 | 1.373 (2) | N23—C34 | 1.469 (2) |
N7—C7 | 1.388 (2) | C27—C27ii | 1.259 (3) |
N7—C8 | 1.4213 (19) | C29—C32 | 1.379 (3) |
C1—C1i | 1.396 (3) | C29—C30 | 1.475 (2) |
C3—C6 | 1.383 (2) | C34—C37 | 1.518 (3) |
C3—C4 | 1.392 (2) | C35—C36 | 1.510 (3) |
C8—C11 | 1.543 (3) | C35—C38 | 1.5249 (19) |
C9—C12 | 1.493 (2) | C36—C37 | 1.564 (2) |
C9—C10 | 1.515 (3) | N13—C23 | 1.456 (2) |
C10—C11 | 1.531 (2) | N14—C24 | 1.412 (2) |
Ni2—N17 | 2.1007 (14) | C23—C24 | 1.522 (2) |
Ni2—N17ii | 2.1007 (14) | O48—O49 | 1.677 (3) |
| | | |
N1i—Ni1—N1 | 81.82 (8) | N17—Ni2—O19ii | 90.00 (5) |
N1i—Ni1—O1i | 91.90 (5) | N17ii—Ni2—O19ii | 90.12 (5) |
N1—Ni1—O1i | 91.40 (5) | N17—Ni2—O19 | 90.12 (5) |
N1i—Ni1—O1 | 91.40 (5) | N17ii—Ni2—O19 | 90.00 (5) |
N1—Ni1—O1 | 91.90 (5) | O19ii—Ni2—O19 | 179.83 (6) |
O1i—Ni1—O1 | 175.63 (5) | N17—Ni2—N19 | 175.75 (5) |
N1i—Ni1—N3 | 174.81 (6) | N17ii—Ni2—N19 | 95.36 (5) |
N1—Ni1—N3 | 94.97 (5) | O19ii—Ni2—N19 | 94.21 (5) |
O1i—Ni1—N3 | 84.07 (5) | O19—Ni2—N19 | 85.67 (5) |
O1—Ni1—N3 | 92.79 (5) | N17—Ni2—N19ii | 95.36 (5) |
N1i—Ni1—N3i | 94.97 (5) | N17ii—Ni2—N19ii | 175.75 (5) |
N1—Ni1—N3i | 174.81 (6) | O19ii—Ni2—N19ii | 85.67 (5) |
O1i—Ni1—N3i | 92.79 (5) | O19—Ni2—N19ii | 94.21 (5) |
O1—Ni1—N3i | 84.07 (5) | N19—Ni2—N19ii | 85.59 (8) |
N3—Ni1—N3i | 88.51 (8) | O26—P3—O28 | 113.34 (6) |
O10—P1—O8 | 113.59 (6) | O26—P3—O27 | 113.60 (8) |
O10—P1—O9 | 113.19 (7) | O28—P3—O27 | 113.00 (6) |
O8—P1—O9 | 112.01 (6) | O26—P3—O25 | 101.29 (6) |
O10—P1—O7 | 108.26 (6) | O28—P3—O25 | 108.80 (7) |
O8—P1—O7 | 105.36 (7) | O27—P3—O25 | 105.73 (6) |
O9—P1—O7 | 103.52 (6) | C34—O22—C35 | 109.86 (12) |
C8—O4—C9 | 108.93 (13) | C38—O25—P3 | 118.86 (9) |
C12—O7—P1 | 120.80 (9) | C27—N17—Ni2 | 106.56 (10) |
C1—N1—Ni1 | 107.33 (10) | C29—N19—C33 | 103.87 (13) |
C7—N3—C3 | 105.43 (13) | C29—N19—Ni2 | 133.22 (12) |
C7—N3—Ni1 | 121.90 (11) | C33—N19—Ni2 | 118.58 (11) |
C3—N3—Ni1 | 128.92 (11) | C30—N20—C31 | 125.07 (13) |
C5—N4—C4 | 124.68 (14) | C31—N22—C32 | 113.50 (13) |
C5—N6—C6 | 110.83 (14) | C33—N23—C32 | 107.38 (13) |
C6—N7—C7 | 105.84 (12) | C33—N23—C34 | 127.03 (12) |
C6—N7—C8 | 124.44 (12) | C32—N23—C34 | 125.45 (12) |
C7—N7—C8 | 129.56 (12) | C27ii—C27—N17 | 121.25 (9) |
C1i—C1—N1 | 113.75 (11) | N19—C29—C32 | 114.03 (14) |
C6—C3—N3 | 109.52 (13) | N19—C29—C30 | 130.36 (14) |
C6—C3—C4 | 119.27 (14) | C32—C29—C30 | 115.47 (14) |
N3—C3—C4 | 131.16 (14) | O21—C30—N20 | 119.09 (14) |
O3—C4—C3 | 132.56 (13) | O21—C30—C29 | 128.19 (13) |
O3—C4—N4 | 116.95 (14) | N20—C30—C29 | 112.66 (14) |
C3—C4—N4 | 110.45 (13) | N22—C31—N21 | 121.97 (14) |
N6—C5—N5 | 119.08 (15) | N22—C31—N20 | 122.36 (14) |
N6—C5—N4 | 124.82 (13) | N21—C31—N20 | 115.60 (13) |
N5—C5—N4 | 116.10 (15) | N22—C32—C29 | 130.29 (15) |
N6—C6—N7 | 124.13 (14) | N22—C32—N23 | 126.12 (15) |
N6—C6—C3 | 128.92 (16) | C29—C32—N23 | 103.42 (13) |
N7—C6—C3 | 106.81 (13) | N19—C33—N23 | 111.26 (13) |
N3—C7—N7 | 112.17 (13) | O22—C34—N23 | 106.33 (11) |
N7—C8—O4 | 108.73 (11) | O22—C34—C37 | 108.17 (12) |
N7—C8—C11 | 113.06 (16) | N23—C34—C37 | 111.21 (15) |
O4—C8—C11 | 108.19 (12) | O22—C35—C36 | 105.13 (12) |
O4—C9—C12 | 107.12 (12) | O22—C35—C38 | 108.19 (13) |
O4—C9—C10 | 104.45 (12) | C36—C35—C38 | 115.67 (16) |
C12—C9—C10 | 116.00 (16) | O23—C36—C35 | 114.57 (13) |
O5—C10—C9 | 113.01 (12) | O23—C36—C37 | 113.59 (12) |
O5—C10—C11 | 108.82 (11) | C35—C36—C37 | 102.36 (15) |
C9—C10—C11 | 103.86 (15) | O24—C37—C34 | 107.15 (15) |
O6—C11—C10 | 113.06 (12) | O24—C37—C36 | 109.55 (11) |
O6—C11—C8 | 107.69 (15) | C34—C37—C36 | 101.27 (13) |
C10—C11—C8 | 100.58 (13) | O25—C38—C35 | 110.50 (13) |
O7—C12—C9 | 112.83 (13) | N13—C23—C24 | 107.07 (14) |
N17—Ni2—N17ii | 83.99 (8) | N14—C24—C23 | 105.50 (15) |
Symmetry codes: (i) x, −y, −z; (ii) −x+1, y, −z+1/2. |
(yakvip)
catena-(mu!2$-Aqua)bis(diaqua-(mu!3$-beta-
N-oxalyl-
L-alpha,beta-diaminopropionic acid)-sodium) trihydrate
top
Crystal data top
C5H15N2NaO9 | γ = 90° |
Mr = 270.18 | V = 2268.9 (6) Å3 |
C2221 | Z = 8 |
a = 9.453 (2) Å | F(000) = 1136 |
b = 17.812 (2) Å | Dx = 1.582 Mg m−3 |
c = 13.475 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.18 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.013 |
Graphite monochromator | θmax = 67.7°, θmin = 2.3° |
18110 measured reflections | h = −12→12 |
5671 independent reflections | k = −36→36 |
4802 reflections with I > 2σ(I) | l = −14→14 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.009 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.057 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.25 | (Δ/σ)max = 3.198 |
5671 reflections | Δρmax = 0.08 e Å−3 |
113 parameters | Δρmin = −0.21 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.06 (8) |
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 | x | y | z | Uiso*/Ueq | Occ. (<1) |
Na1 | 0.46230 (2) | −0.130200 (8) | −0.088100 (15) | 0.02000 (3)* | |
N1 | 0.53650 (4) | −0.379200 (17) | 0.11550 (3) | 0.02000 (5)* | |
H13 | 0.6197 (9) | −0.3554 (5) | 0.1107 (7) | 0.0200 (16)* | |
N2 | 0.45060 (4) | −0.338300 (16) | −0.07680 (3) | 0.02000 (5)* | |
H1 | 0.5118 (9) | −0.2966 (5) | −0.0634 (6) | 0.0200 (16)* | |
H2 | 0.4028 (9) | −0.3303 (4) | −0.1389 (6) | 0.0200 (17)* | |
H3 | 0.5056 (9) | −0.3835 (4) | −0.0806 (6) | 0.0200 (16)* | |
O1 | 0.78280 (3) | −0.449700 (15) | 0.14750 (3) | 0.02000 (4)* | |
O2 | 0.68190 (3) | −0.559500 (15) | 0.11080 (3) | 0.02000 (4)* | |
O3 | 0.42420 (3) | −0.491600 (15) | 0.12270 (3) | 0.02000 (5)* | |
O4 | 0.12600 (3) | −0.279900 (15) | 0.03880 (3) | 0.02000 (4)* | |
O5 | 0.27360 (3) | −0.220900 (14) | −0.06470 (3) | 0.02000 (4)* | |
C1 | 0.67960 (4) | −0.490300 (18) | 0.12760 (4) | 0.02000 (5)* | |
C2 | 0.53260 (4) | −0.453400 (19) | 0.12160 (3) | 0.02000 (5)* | |
C3 | 0.41030 (5) | −0.333100 (19) | 0.10470 (4) | 0.02000 (5)* | |
H7 | 0.4419 (8) | −0.2783 (5) | 0.1174 (7) | 0.0200 (17)* | |
H8 | 0.3425 (9) | −0.3473 (5) | 0.1533 (6) | 0.0200 (17)* | |
C4 | 0.34080 (4) | −0.339700 (19) | 0.00240 (4) | 0.02000 (6)* | |
H9 | 0.2876 (8) | −0.3890 (4) | −0.0064 (6) | 0.0200 (17)* | |
C5 | 0.23740 (4) | −0.27410 (2) | −0.01060 (4) | 0.02000 (5)* | |
O11 | 0.80390 (3) | −0.181500 (15) | 0.25850 (3) | 0.02000 (5)* | |
O12 | 0.46930 (3) | −0.088300 (15) | 0.08200 (3) | 0.02000 (5)* | |
H16 | 0.3743 (9) | −0.0718 (4) | 0.0807 (6) | 0.0200 (17)* | |
H17 | 0.5124 (9) | −0.0450 (4) | 0.0945 (6) | 0.0200 (16)* | |
O14 | 0.0000 | −0.31080 (2) | 0.2500 | 0.02000 (6)* | |
O15 | 0.63510 (3) | −0.033400 (16) | −0.14920 (3) | 0.02000 (4)* | |
H20 | 0.7289 (16) | −0.0273 (9) | −0.1345 (12) | 0.020 (3)* | 0.50 |
H21 | 0.6519 (17) | −0.0227 (9) | −0.2164 (13) | 0.020 (3)* | 0.50 |
O18 | −0.5000 | −0.17990 (2) | 0.2500 | 0.02000 (6)* | |
Geometric parameters (Å, º) top
Na1—O4i | 2.3238 (4) | O2—C1 | 1.2534 (4) |
Na1—O1ii | 2.3548 (4) | O3—C2 | 1.2301 (5) |
Na1—O12 | 2.4114 (5) | O4—C5 | 1.2501 (5) |
Na1—O5 | 2.4272 (4) | O4—Na1ii | 2.3238 (4) |
Na1—O14i | 2.4476 (4) | O5—C5 | 1.2436 (5) |
Na1—O15 | 2.5138 (4) | C1—C2 | 1.5393 (6) |
N1—C2 | 1.3247 (5) | C3—C4 | 1.5316 (7) |
N1—C3 | 1.4555 (6) | C4—C5 | 1.5334 (5) |
N2—C4 | 1.4889 (7) | O14—Na1ii | 2.4476 (4) |
O1—C1 | 1.2436 (5) | O14—Na1iii | 2.4476 (4) |
O1—Na1i | 2.3548 (4) | | |
| | | |
O4i—Na1—O1ii | 173.443 (13) | C5—O4—Na1ii | 140.37 (3) |
O4i—Na1—O12 | 85.599 (14) | C5—O5—Na1 | 141.77 (3) |
O1ii—Na1—O12 | 98.964 (14) | O1—C1—O2 | 126.67 (4) |
O4i—Na1—O5 | 89.633 (17) | O1—C1—C2 | 118.11 (3) |
O1ii—Na1—O5 | 85.231 (17) | O2—C1—C2 | 115.22 (3) |
O12—Na1—O5 | 95.894 (13) | O3—C2—N1 | 125.15 (4) |
O4i—Na1—O14i | 82.067 (13) | O3—C2—C1 | 121.01 (3) |
O1ii—Na1—O14i | 93.523 (14) | N1—C2—C1 | 113.84 (3) |
O12—Na1—O14i | 167.446 (12) | N1—C3—C4 | 113.47 (3) |
O5—Na1—O14i | 86.389 (13) | N2—C4—C3 | 110.17 (4) |
O4i—Na1—O15 | 97.675 (18) | N2—C4—C5 | 110.47 (4) |
O1ii—Na1—O15 | 86.696 (17) | C3—C4—C5 | 108.53 (3) |
O12—Na1—O15 | 94.658 (14) | O5—C5—O4 | 127.37 (4) |
O5—Na1—O15 | 167.593 (15) | O5—C5—C4 | 118.18 (4) |
O14i—Na1—O15 | 84.719 (13) | O4—C5—C4 | 114.40 (4) |
C2—N1—C3 | 123.11 (3) | Na1ii—O14—Na1iii | 129.146 (19) |
C1—O1—Na1i | 147.50 (3) | | |
Symmetry codes: (i) x+1/2, −y−1/2, −z; (ii) x−1/2, −y−1/2, −z; (iii) −x+1/2, −y−1/2, z+1/2. |
(bogpiw) Dicarbonyl-(eta$5!-cyclopentadienyl)-(sulfur dioxide)-iron(iii)
hexafluoroarsenate
top
Crystal data top
C7H5AsF6FeO4S | γ = 90° |
Mr = 429.94 | V = 1265.9 (5) Å3 |
Cmc21 | Z = 4 |
a = 8.068 (2) Å | F(000) = 832 |
b = 13.904 (4) Å | Dx = 2.256 Mg m−3 |
c = 11.285 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 4.03 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.023 |
Graphite monochromator | θmax = 53.1°, θmin = 2.9° |
7020 measured reflections | h = −16→16 |
1916 independent reflections | k = −16→16 |
1903 reflections with I > 2σ(I) | l = −12→12 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.005 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.024 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.15 | (Δ/σ)max = 2.807 |
1916 reflections | Δρmax = 0.19 e Å−3 |
60 parameters | Δρmin = −0.27 e Å−3 |
1 restraint | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.0108 (18) |
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 | x | y | z | Uiso*/Ueq | |
Fe1 | 0.0000 | 0.184900 (11) | 0.257400 (13) | 0.02000 (3)* | |
As1 | 0.5000 | 0.072700 (7) | 0.063800 (9) | 0.02000 (2)* | |
F1 | 0.5000 | 0.05280 (5) | −0.08470 (5) | 0.02000 (10)* | |
F2 | 0.35070 (4) | 0.16060 (3) | 0.04350 (4) | 0.02000 (7)* | |
F3 | 0.34890 (4) | −0.01220 (3) | 0.08470 (4) | 0.02000 (7)* | |
F5 | 0.5000 | 0.09780 (5) | 0.21090 (5) | 0.02000 (9)* | |
S1 | 0.0000 | 0.172300 (17) | 0.07120 (2) | 0.02000 (4)* | |
O1 | 0.0000 | 0.08190 (5) | 0.01370 (7) | 0.02000 (10)* | |
O2 | 0.0000 | 0.25750 (5) | 0.00080 (7) | 0.02000 (10)* | |
C1 | 0.13670 (7) | 0.10800 (6) | 0.38110 (6) | 0.02000 (9)* | |
C2 | 0.0000 | 0.14200 (7) | 0.43320 (9) | 0.02000 (14)* | |
C5 | 0.08820 (6) | 0.04820 (6) | 0.29260 (6) | 0.02000 (9)* | |
C6 | 0.16640 (6) | 0.27390 (5) | 0.25760 (7) | 0.02000 (9)* | |
O3 | 0.27090 (5) | 0.32580 (3) | 0.26000 (5) | 0.02000 (8)* | |
H1 | 0.2489 (12) | 0.1230 (5) | 0.4023 (9) | 0.020 (3)* | |
H2 | 0.0000 | 0.1852 (9) | 0.4994 (14) | 0.020 (4)* | |
H5 | 0.1592 (12) | 0.0127 (7) | 0.2401 (8) | 0.020 (2)* | |
Geometric parameters (Å, º) top
Fe1—C6 | 1.8258 (7) | As1—F3ii | 1.7133 (5) |
Fe1—C6i | 1.8258 (7) | As1—F2ii | 1.7312 (5) |
Fe1—C5 | 2.0680 (10) | As1—F2 | 1.7312 (5) |
Fe1—C5i | 2.0680 (10) | S1—O1 | 1.4145 (9) |
Fe1—C2 | 2.0716 (11) | S1—O2 | 1.4264 (9) |
Fe1—C1 | 2.0756 (8) | C1—C2 | 1.3362 (9) |
Fe1—C1i | 2.0756 (8) | C1—C5 | 1.3572 (10) |
Fe1—S1 | 2.1086 (5) | C2—C1i | 1.3362 (9) |
As1—F5 | 1.6963 (7) | C5—C5i | 1.4232 (11) |
As1—F1 | 1.6985 (7) | C6—O3 | 1.1101 (8) |
As1—F3 | 1.7133 (5) | | |
| | | |
C6—Fe1—C6i | 94.66 (4) | F5—As1—F1 | 177.50 (3) |
C6—Fe1—C5 | 111.69 (3) | F5—As1—F3 | 90.40 (2) |
C6i—Fe1—C5 | 151.13 (3) | F1—As1—F3 | 91.35 (2) |
C6—Fe1—C5i | 151.13 (3) | F5—As1—F3ii | 90.40 (2) |
C6i—Fe1—C5i | 111.69 (3) | F1—As1—F3ii | 91.35 (2) |
C5—Fe1—C5i | 40.25 (3) | F3—As1—F3ii | 90.72 (3) |
C6—Fe1—C2 | 101.18 (3) | F5—As1—F2ii | 89.10 (2) |
C6i—Fe1—C2 | 101.18 (3) | F1—As1—F2ii | 89.11 (2) |
C5—Fe1—C2 | 63.35 (3) | F3—As1—F2ii | 178.639 (18) |
C5i—Fe1—C2 | 63.35 (3) | F3ii—As1—F2ii | 90.55 (3) |
C6—Fe1—C1 | 87.57 (3) | F5—As1—F2 | 89.10 (2) |
C6i—Fe1—C1 | 137.65 (3) | F1—As1—F2 | 89.11 (2) |
C5—Fe1—C1 | 38.24 (3) | F3—As1—F2 | 90.55 (3) |
C5i—Fe1—C1 | 65.18 (3) | F3ii—As1—F2 | 178.639 (18) |
C2—Fe1—C1 | 37.59 (2) | F2ii—As1—F2 | 88.18 (3) |
C6—Fe1—C1i | 137.65 (3) | O1—S1—O2 | 118.85 (5) |
C6i—Fe1—C1i | 87.57 (3) | O1—S1—Fe1 | 122.07 (4) |
C5—Fe1—C1i | 65.18 (3) | O2—S1—Fe1 | 119.08 (4) |
C5i—Fe1—C1i | 38.24 (3) | C2—C1—C5 | 107.61 (6) |
C2—Fe1—C1i | 37.59 (2) | C2—C1—Fe1 | 71.04 (5) |
C1—Fe1—C1i | 64.19 (4) | C5—C1—Fe1 | 70.58 (5) |
C6—Fe1—S1 | 93.30 (2) | C1i—C2—C1 | 111.25 (9) |
C6i—Fe1—S1 | 93.30 (2) | C1i—C2—Fe1 | 71.37 (5) |
C5—Fe1—S1 | 96.61 (2) | C1—C2—Fe1 | 71.37 (5) |
C5i—Fe1—S1 | 96.61 (2) | C1—C5—C5i | 106.76 (3) |
C2—Fe1—S1 | 158.50 (3) | C1—C5—Fe1 | 71.19 (5) |
C1—Fe1—S1 | 128.86 (2) | C5i—C5—Fe1 | 69.874 (17) |
C1i—Fe1—S1 | 128.86 (2) | O3—C6—Fe1 | 177.51 (6) |
Symmetry codes: (i) −x, y, z; (ii) −x+1, y, z. |
(novhub) bis(mu!2$-bis(Diphenylphosphino)methane)-(mu!2$-nitrato)-dipyridyl-di-copper(i)
nitrate methanol solvate
top
Crystal data top
C61H58Cu2N4O7P4 | γ = 90° |
Mr = 1210.07 | V = 5738.7 (11) Å3 |
Cmc21 | Z = 4 |
a = 21.719 (2) Å | F(000) = 2504 |
b = 16.545 (2) Å | Dx = 1.401 Mg m−3 |
c = 15.970 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.91 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.030 |
Graphite monochromator | θmax = 30.4°, θmin = 1.6° |
10772 measured reflections | h = −20→20 |
2892 independent reflections | k = −20→20 |
2853 reflections with I > 2σ(I) | l = −12→12 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.011 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.046 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.34 | (Δ/σ)max = 1.469 |
2892 reflections | Δρmax = 0.52 e Å−3 |
275 parameters | Δρmin = −0.21 e Å−3 |
1 restraint | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.007 (5) |
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 | x | y | z | Uiso*/Ueq | |
Cu1 | 0.084100 (12) | 0.681600 (11) | 0.070900 (15) | 0.02000 (8)* | |
X1 | 0.53100 (8) | 0.60450 (6) | 0.10790 (9) | 0.0200 (3)* | |
P1 | 0.07030 (3) | 0.81640 (2) | 0.06450 (4) | 0.02000 (13)* | |
P2 | 0.07070 (2) | 0.60340 (2) | 0.18580 (3) | 0.02000 (12)* | |
O3 | 0.0000 | 0.80850 (9) | 0.33590 (12) | 0.0200 (4)* | |
O4 | 0.04960 (7) | 0.62480 (7) | −0.04300 (8) | 0.0200 (3)* | |
O5 | 0.04850 (7) | 0.82290 (6) | 0.45130 (8) | 0.0200 (3)* | |
O6 | 0.0000 | 0.52200 (8) | −0.08560 (10) | 0.0200 (4)* | |
N1 | 0.0000 | 0.59110 (11) | −0.05750 (13) | 0.0200 (5)* | |
N2 | 0.0000 | 0.81740 (10) | 0.41360 (15) | 0.0200 (5)* | |
N4 | 0.17600 (8) | 0.65570 (8) | 0.03470 (9) | 0.0200 (3)* | |
C2 | 0.0000 | 0.61560 (14) | 0.24780 (17) | 0.0200 (5)* | |
C3 | 0.0000 | 0.86000 (13) | 0.11030 (18) | 0.0200 (6)* | |
C4 | 0.22180 (10) | 0.68860 (9) | 0.07670 (13) | 0.0200 (4)* | |
C5 | 0.07830 (9) | 0.86620 (11) | −0.03580 (13) | 0.0200 (4)* | |
C6 | 0.28260 (10) | 0.66730 (10) | 0.06600 (13) | 0.0200 (4)* | |
C7 | 0.07600 (9) | 0.95010 (11) | −0.04500 (13) | 0.0200 (4)* | |
C8 | 0.29610 (12) | 0.60910 (10) | 0.00880 (11) | 0.0200 (4)* | |
C9 | 0.08310 (9) | 0.98530 (11) | −0.12300 (13) | 0.0200 (4)* | |
C10 | 0.25020 (9) | 0.57390 (9) | −0.03560 (12) | 0.0200 (4)* | |
C11 | 0.09290 (10) | 0.93850 (10) | −0.19140 (13) | 0.0200 (4)* | |
C12 | 0.19020 (10) | 0.59870 (9) | −0.02220 (13) | 0.0200 (4)* | |
C13 | 0.09540 (10) | 0.85610 (10) | −0.18420 (13) | 0.0200 (4)* | |
C14 | 0.08790 (10) | 0.81970 (9) | −0.10600 (16) | 0.0200 (5)* | |
C15 | 0.13220 (10) | 0.86050 (9) | 0.12740 (12) | 0.0200 (4)* | |
C16 | 0.18450 (9) | 0.89290 (9) | 0.09120 (13) | 0.0200 (4)* | |
C17 | 0.23560 (11) | 0.91110 (11) | 0.13990 (12) | 0.0200 (4)* | |
C18 | 0.23490 (11) | 0.89860 (9) | 0.22370 (12) | 0.0200 (4)* | |
C19 | 0.18310 (10) | 0.86830 (9) | 0.26150 (13) | 0.0200 (4)* | |
C20 | 0.13180 (11) | 0.84930 (10) | 0.21410 (12) | 0.0200 (4)* | |
C21 | 0.07850 (9) | 0.49490 (10) | 0.17160 (12) | 0.0200 (4)* | |
C22 | 0.07980 (10) | 0.46300 (10) | 0.09130 (13) | 0.0200 (4)* | |
C23 | 0.08290 (9) | 0.37960 (10) | 0.08130 (15) | 0.0200 (4)* | |
C24 | 0.08610 (10) | 0.33050 (11) | 0.14740 (14) | 0.0200 (5)* | |
C25 | 0.08680 (10) | 0.36090 (11) | 0.22710 (13) | 0.0200 (4)* | |
C26 | 0.08260 (9) | 0.44350 (11) | 0.23900 (15) | 0.0200 (4)* | |
C27 | 0.13110 (10) | 0.62360 (10) | 0.26460 (11) | 0.0200 (4)* | |
C28 | 0.18930 (9) | 0.59360 (9) | 0.24910 (12) | 0.0200 (4)* | |
C29 | 0.23720 (10) | 0.61230 (9) | 0.30290 (11) | 0.0200 (4)* | |
C30 | 0.22740 (11) | 0.66010 (10) | 0.37120 (12) | 0.0200 (4)* | |
C31 | 0.16970 (11) | 0.68970 (9) | 0.38750 (12) | 0.0200 (4)* | |
C32 | 0.12170 (12) | 0.67090 (9) | 0.33390 (12) | 0.0200 (4)* | |
H1 | 0.0693 (10) | 0.9834 (11) | 0.0047 (14) | 0.020 (5)* | |
H2 | 0.0812 (9) | 1.0451 (12) | −0.1264 (15) | 0.020 (5)* | |
H3 | 0.0960 (10) | 0.9649 (10) | −0.2458 (14) | 0.020 (6)* | |
H4 | 0.1042 (11) | 0.8227 (10) | −0.2330 (14) | 0.020 (6)* | |
H5 | 0.0905 (9) | 0.7605 (10) | −0.1002 (13) | 0.020 (5)* | |
H6 | 0.1848 (9) | 0.9048 (10) | 0.0313 (14) | 0.020 (5)* | |
H7 | 0.2717 (10) | 0.9339 (10) | 0.1132 (12) | 0.020 (5)* | |
H8 | 0.2719 (10) | 0.9074 (10) | 0.2567 (13) | 0.020 (5)* | |
H9 | 0.1816 (9) | 0.8616 (10) | 0.3229 (13) | 0.020 (5)* | |
H10 | 0.0953 (11) | 0.8273 (10) | 0.2412 (16) | 0.020 (6)* | |
H11 | 0.0781 (8) | 0.4988 (12) | 0.0431 (13) | 0.020 (5)* | |
H12 | 0.0844 (9) | 0.3558 (11) | 0.0272 (15) | 0.020 (5)* | |
H13 | 0.0857 (9) | 0.2731 (13) | 0.1378 (12) | 0.020 (5)* | |
H14 | 0.0912 (10) | 0.3229 (10) | 0.2753 (15) | 0.020 (6)* | |
H15 | 0.0823 (9) | 0.4666 (11) | 0.2962 (14) | 0.020 (6)* | |
H16 | 0.1957 (9) | 0.5610 (10) | 0.1994 (12) | 0.020 (5)* | |
H17 | 0.2781 (10) | 0.5877 (10) | 0.2905 (11) | 0.020 (5)* | |
H18 | 0.2628 (10) | 0.6710 (11) | 0.4067 (13) | 0.020 (5)* | |
H19 | 0.1630 (9) | 0.7245 (10) | 0.4371 (11) | 0.020 (4)* | |
H20 | 0.0795 (10) | 0.6917 (12) | 0.3464 (15) | 0.020 (6)* | |
H46 | 0.2118 (10) | 0.7316 (10) | 0.1169 (12) | 0.020 (5)* | |
H47 | 0.3149 (9) | 0.6926 (10) | 0.1019 (12) | 0.020 (5)* | |
H48 | 0.3387 (11) | 0.5934 (10) | 0.0027 (11) | 0.020 (5)* | |
H49 | 0.2597 (9) | 0.5316 (10) | −0.0777 (12) | 0.020 (5)* | |
H50 | 0.1567 (10) | 0.5731 (9) | −0.0546 (11) | 0.020 (5)* | |
H51 | 0.0000 | 0.5760 (14) | 0.2929 (17) | 0.020 (6)* | |
H52 | 0.0000 | 0.6680 (14) | 0.2738 (16) | 0.020 (7)* | |
H53 | 0.0000 | 0.8514 (14) | 0.1698 (19) | 0.020 (7)* | |
H54 | 0.0000 | 0.9180 (14) | 0.1013 (16) | 0.020 (7)* | |
Geometric parameters (Å, º) top
Cu1—N4 | 2.1217 (17) | C7—C9 | 1.384 (3) |
Cu1—O4 | 2.1802 (13) | C8—C10 | 1.355 (3) |
Cu1—P1 | 2.2526 (5) | C9—C11 | 1.356 (3) |
Cu1—P2 | 2.2640 (6) | C10—C12 | 1.383 (3) |
X1—X1i | 1.347 (3) | C11—C13 | 1.369 (2) |
P1—C5 | 1.810 (2) | C13—C14 | 1.396 (3) |
P1—C15 | 1.830 (2) | C15—C16 | 1.383 (3) |
P1—C3 | 1.8403 (15) | C15—C20 | 1.397 (3) |
P2—C21 | 1.8173 (18) | C16—C17 | 1.388 (3) |
P2—C2 | 1.8382 (15) | C17—C18 | 1.354 (3) |
P2—C27 | 1.848 (2) | C18—C19 | 1.372 (3) |
O3—N2 | 1.250 (3) | C19—C20 | 1.383 (3) |
O4—N1 | 1.2349 (16) | C21—C26 | 1.375 (3) |
O5—N2 | 1.2167 (18) | C21—C22 | 1.387 (3) |
O6—N1 | 1.228 (2) | C22—C23 | 1.391 (2) |
N1—O4ii | 1.2349 (16) | C23—C24 | 1.334 (3) |
N2—O5ii | 1.2167 (18) | C24—C25 | 1.369 (3) |
N4—C4 | 1.317 (3) | C25—C26 | 1.383 (2) |
N4—C12 | 1.345 (2) | C27—C32 | 1.371 (3) |
C2—P2ii | 1.8382 (15) | C27—C28 | 1.380 (3) |
C3—P1ii | 1.8403 (15) | C28—C29 | 1.384 (3) |
C4—C6 | 1.377 (3) | C29—C30 | 1.364 (3) |
C5—C14 | 1.376 (3) | C30—C31 | 1.370 (3) |
C5—C7 | 1.397 (2) | C31—C32 | 1.384 (3) |
C6—C8 | 1.359 (3) | | |
| | | |
N4—Cu1—O4 | 90.51 (6) | C8—C6—C4 | 118.1 (2) |
N4—Cu1—P1 | 108.23 (4) | C9—C7—C5 | 120.60 (18) |
O4—Cu1—P1 | 110.07 (3) | C10—C8—C6 | 119.8 (2) |
N4—Cu1—P2 | 103.08 (4) | C11—C9—C7 | 120.16 (16) |
O4—Cu1—P2 | 112.69 (3) | C8—C10—C12 | 119.00 (17) |
P1—Cu1—P2 | 125.84 (2) | C9—C11—C13 | 120.5 (2) |
C5—P1—C15 | 103.52 (9) | N4—C12—C10 | 121.90 (19) |
C5—P1—C3 | 104.65 (11) | C11—C13—C14 | 120.00 (18) |
C15—P1—C3 | 103.60 (10) | C5—C14—C13 | 120.36 (15) |
C5—P1—Cu1 | 118.57 (6) | C16—C15—C20 | 118.1 (2) |
C15—P1—Cu1 | 105.79 (6) | C16—C15—P1 | 121.91 (15) |
C3—P1—Cu1 | 118.72 (7) | C20—C15—P1 | 119.12 (17) |
C21—P2—C2 | 104.69 (10) | C15—C16—C17 | 120.4 (2) |
C21—P2—C27 | 101.39 (8) | C18—C17—C16 | 120.8 (2) |
C2—P2—C27 | 101.90 (9) | C17—C18—C19 | 120.0 (2) |
C21—P2—Cu1 | 116.83 (7) | C18—C19—C20 | 120.19 (19) |
C2—P2—Cu1 | 118.76 (8) | C19—C20—C15 | 120.5 (2) |
C27—P2—Cu1 | 110.93 (6) | C26—C21—C22 | 119.16 (16) |
N1—O4—Cu1 | 130.61 (12) | C26—C21—P2 | 121.29 (14) |
O6—N1—O4 | 119.26 (9) | C22—C21—P2 | 119.55 (13) |
O6—N1—O4ii | 119.26 (9) | C21—C22—C23 | 118.99 (18) |
O4—N1—O4ii | 121.46 (18) | C24—C23—C22 | 121.1 (2) |
O5—N2—O5ii | 119.9 (2) | C23—C24—C25 | 120.85 (18) |
O5—N2—O3 | 120.01 (12) | C24—C25—C26 | 119.36 (18) |
O5ii—N2—O3 | 120.01 (12) | C21—C26—C25 | 120.53 (19) |
C4—N4—C12 | 117.41 (18) | C32—C27—C28 | 119.11 (18) |
C4—N4—Cu1 | 119.22 (13) | C32—C27—P2 | 123.18 (17) |
C12—N4—Cu1 | 122.77 (13) | C28—C27—P2 | 117.57 (13) |
P2ii—C2—P2 | 113.30 (14) | C27—C28—C29 | 119.77 (17) |
P1—C3—P1ii | 112.13 (13) | C30—C29—C28 | 120.6 (2) |
N4—C4—C6 | 123.71 (17) | C29—C30—C31 | 120.12 (19) |
C14—C5—C7 | 118.39 (19) | C30—C31—C32 | 119.40 (18) |
C14—C5—P1 | 118.77 (14) | C27—C32—C31 | 121.0 (2) |
C7—C5—P1 | 122.83 (15) | | |
Symmetry codes: (i) −x+1, y, z; (ii) −x, y, z. |
(nohned) 1,1'-Dihydroxy-2,2'-(1,4,7,10-tetraoxadeca-1,10-diyl)-6,6'-(2,5-diazahexa-1,5-
-diene-1,6-diyl)dibenzene
top
Crystal data top
C22N2O6 | γ = 90° |
Mr = 388.24 | V = 2174.1 (7) Å3 |
P212121 | Z = 4 |
a = 12.148 (2) Å | F(000) = 776 |
b = 8.251 (2) Å | Dx = 1.186 Mg m−3 |
c = 21.690 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.09 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.021 |
Graphite monochromator | θmax = 32.9°, θmin = 1.9° |
12290 measured reflections | h = −12→12 |
3081 independent reflections | k = −8→8 |
3050 reflections with I > 2σ(I) | l = −14→14 |
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)] = 0.019 | w = 1/[σ2(Fo2) + (0.P)2 + 0.0178P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.077 | (Δ/σ)max = 0.745 |
S = 0.63 | Δρmax = 0.59 e Å−3 |
3081 reflections | Δρmin = −0.58 e Å−3 |
121 parameters | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
0 restraints | Absolute structure parameter: 0.1 (6) |
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 | x | y | z | Uiso*/Ueq | |
O1 | 0.48470 (7) | 0.01990 (11) | 0.07400 (5) | 0.0200 (2)* | |
O2 | 0.49230 (7) | −0.11310 (11) | −0.09220 (5) | 0.0200 (2)* | |
O3 | 0.64660 (7) | 0.02390 (11) | −0.16910 (5) | 0.0200 (2)* | |
O4 | 0.81390 (7) | 0.02970 (11) | −0.07060 (5) | 0.0200 (2)* | |
O5 | 0.85960 (7) | 0.04990 (11) | 0.06020 (5) | 0.0200 (2)* | |
O6 | 0.67100 (7) | 0.04800 (11) | 0.13490 (5) | 0.0200 (2)* | |
C1 | 0.60760 (11) | −0.14270 (15) | 0.21420 (8) | 0.0200 (3)* | |
C2 | 0.52320 (10) | −0.24260 (15) | 0.23560 (8) | 0.0200 (3)* | |
C3 | 0.42490 (11) | −0.25420 (16) | 0.20260 (7) | 0.0200 (3)* | |
C4 | 0.41100 (10) | −0.16610 (16) | 0.14840 (8) | 0.0200 (3)* | |
C5 | 0.49550 (11) | −0.06610 (15) | 0.12700 (8) | 0.0200 (3)* | |
C6 | 0.59380 (10) | −0.05450 (15) | 0.15990 (8) | 0.0200 (3)* | |
C7 | 0.31010 (10) | −0.18380 (16) | 0.11490 (8) | 0.0200 (3)* | |
N1 | 0.29180 (9) | −0.10300 (13) | 0.06330 (6) | 0.0200 (2)* | |
C8 | 0.18870 (10) | −0.12040 (15) | 0.02970 (8) | 0.0200 (3)* | |
C9 | 0.19740 (10) | −0.22580 (15) | −0.02480 (8) | 0.0200 (3)* | |
N2 | 0.28900 (9) | −0.16300 (13) | −0.06720 (7) | 0.0200 (2)* | |
C10 | 0.26260 (11) | −0.10710 (15) | −0.11970 (8) | 0.0200 (3)* | |
C11 | 0.31460 (10) | 0.01900 (15) | −0.21840 (8) | 0.0200 (3)* | |
C12 | 0.39290 (11) | 0.08680 (15) | −0.25770 (8) | 0.0200 (3)* | |
C13 | 0.50370 (11) | 0.08770 (15) | −0.24090 (8) | 0.0200 (3)* | |
C14 | 0.53630 (10) | 0.02060 (15) | −0.18470 (8) | 0.0200 (3)* | |
C15 | 0.45790 (10) | −0.04730 (16) | −0.14540 (8) | 0.0200 (3)* | |
C16 | 0.34710 (10) | −0.04800 (16) | −0.16230 (8) | 0.0200 (3)* | |
C17 | 0.66970 (11) | 0.15400 (15) | −0.12900 (8) | 0.0200 (3)* | |
C18 | 0.79130 (11) | 0.16050 (15) | −0.11140 (8) | 0.0200 (3)* | |
C19 | 0.92230 (10) | 0.03700 (16) | −0.04360 (8) | 0.0200 (3)* | |
C20 | 0.92130 (11) | 0.14000 (15) | 0.01580 (8) | 0.0200 (3)* | |
C21 | 0.85090 (10) | 0.13690 (15) | 0.11630 (8) | 0.0200 (3)* | |
C22 | 0.78000 (10) | 0.04060 (16) | 0.15820 (8) | 0.0200 (3)* | |
Geometric parameters (Å, º) top
O1—C5 | 1.3573 (18) | C5—C6 | 1.3944 (19) |
O2—C15 | 1.3420 (17) | C7—N1 | 1.322 (2) |
O3—C14 | 1.3823 (16) | N1—C8 | 1.4562 (18) |
O3—C17 | 1.4098 (18) | C8—C9 | 1.471 (2) |
O4—C18 | 1.4224 (18) | C9—N2 | 1.5338 (18) |
O4—C19 | 1.4425 (16) | N2—C10 | 1.270 (2) |
O5—C21 | 1.4167 (19) | C10—C16 | 1.465 (2) |
O5—C20 | 1.4290 (17) | C11—C16 | 1.394 (2) |
O6—C6 | 1.3743 (16) | C11—C12 | 1.394 (2) |
O6—C22 | 1.4186 (16) | C12—C13 | 1.3945 (19) |
C1—C6 | 1.395 (2) | C13—C14 | 1.396 (2) |
C1—C2 | 1.3950 (18) | C14—C15 | 1.396 (2) |
C2—C3 | 1.396 (2) | C15—C16 | 1.3950 (19) |
C3—C4 | 1.392 (2) | C17—C18 | 1.5267 (19) |
C4—C5 | 1.3964 (18) | C19—C20 | 1.543 (2) |
C4—C7 | 1.4324 (18) | C21—C22 | 1.483 (2) |
| | | |
C14—O3—C17 | 111.04 (11) | C10—N2—C9 | 118.50 (11) |
C18—O4—C19 | 113.40 (10) | N2—C10—C16 | 120.64 (12) |
C21—O5—C20 | 110.75 (10) | C16—C11—C12 | 119.98 (12) |
C6—O6—C22 | 118.03 (11) | C11—C12—C13 | 120.06 (15) |
C6—C1—C2 | 120.07 (13) | C12—C13—C14 | 119.99 (14) |
C1—C2—C3 | 119.92 (15) | O3—C14—C15 | 121.33 (13) |
C4—C3—C2 | 120.07 (12) | O3—C14—C13 | 118.74 (13) |
C3—C4—C5 | 120.00 (13) | C15—C14—C13 | 119.93 (12) |
C3—C4—C7 | 118.61 (12) | O2—C15—C16 | 121.65 (13) |
C5—C4—C7 | 121.38 (15) | O2—C15—C14 | 118.37 (12) |
O1—C5—C6 | 118.71 (12) | C16—C15—C14 | 119.98 (14) |
O1—C5—C4 | 121.29 (12) | C11—C16—C15 | 120.07 (14) |
C6—C5—C4 | 120.00 (15) | C11—C16—C10 | 118.97 (12) |
O6—C6—C5 | 115.13 (14) | C15—C16—C10 | 120.79 (15) |
O6—C6—C1 | 124.91 (12) | O3—C17—C18 | 111.94 (11) |
C5—C6—C1 | 119.96 (12) | O4—C18—C17 | 108.40 (11) |
N1—C7—C4 | 121.47 (12) | O4—C19—C20 | 110.78 (10) |
C7—N1—C8 | 121.25 (11) | O5—C20—C19 | 106.27 (10) |
N1—C8—C9 | 113.49 (11) | O5—C21—C22 | 107.35 (11) |
C8—C9—N2 | 109.52 (10) | O6—C22—C21 | 107.50 (12) |
(nohned01) (1$2!,8$2!-Dihydroxy-1,8(1,3)-dibenzena-1,6-diaza-9,12,15,18-tetraoxacyclooctade
caphane-2,6-diene)
top
Crystal data top
C22H26N2O6 | γ = 90° |
Mr = 414.45 | V = 2174.1 (7) Å3 |
P212121 | Z = 4 |
a = 12.148 (2) Å | F(000) = 880 |
b = 8.251 (2) Å | Dx = 1.266 Mg m−3 |
c = 21.690 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.09 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.022 |
Graphite monochromator | θmax = 30.5°, θmin = 1.9° |
10320 measured reflections | h = −10→10 |
2588 independent reflections | k = −8→8 |
2565 reflections with I > 2σ(I) | l = −14→14 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.019 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.081 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.51 | (Δ/σ)max = 9.439 |
2588 reflections | Δρmax = 0.07 e Å−3 |
217 parameters | Δρmin = −0.29 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.0 (7) |
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 | x | y | z | Uiso*/Ueq | |
O1 | 0.48390 (8) | 0.01970 (12) | 0.07450 (6) | 0.0200 (2)* | |
O2 | 0.49260 (9) | −0.11210 (11) | −0.09210 (6) | 0.0200 (2)* | |
O3 | 0.64640 (9) | 0.02470 (11) | −0.16880 (6) | 0.0200 (2)* | |
O4 | 0.81450 (9) | 0.02870 (12) | −0.07080 (6) | 0.0200 (2)* | |
O5 | 0.86010 (9) | 0.05030 (12) | 0.06020 (6) | 0.0200 (2)* | |
O6 | 0.67050 (9) | 0.04680 (12) | 0.13530 (6) | 0.0200 (3)* | |
C1 | 0.60720 (15) | −0.14240 (16) | 0.21400 (9) | 0.0200 (3)* | |
H1 | 0.6733 (16) | −0.135 (2) | 0.2359 (9) | 0.020 (5)* | |
C2 | 0.52340 (13) | −0.24270 (17) | 0.23510 (10) | 0.0200 (3)* | |
H2 | 0.5334 (15) | −0.302 (2) | 0.2712 (9) | 0.020 (4)* | |
C3 | 0.42550 (14) | −0.25450 (17) | 0.20230 (9) | 0.0200 (3)* | |
H3 | 0.3697 (14) | −0.322 (2) | 0.2164 (8) | 0.020 (4)* | |
C4 | 0.41140 (12) | −0.16610 (17) | 0.14830 (9) | 0.0200 (3)* | |
C5 | 0.49520 (13) | −0.06580 (17) | 0.12720 (9) | 0.0200 (3)* | |
C6 | 0.59320 (13) | −0.05400 (17) | 0.16000 (9) | 0.0200 (3)* | |
C7 | 0.30960 (13) | −0.18270 (18) | 0.11430 (9) | 0.0200 (3)* | |
H4 | 0.2553 (15) | −0.2519 (19) | 0.1292 (9) | 0.020 (4)* | |
N1 | 0.29210 (11) | −0.10370 (14) | 0.06340 (7) | 0.0200 (3)* | |
C8 | 0.18920 (14) | −0.12110 (17) | 0.02990 (9) | 0.0200 (3)* | |
H5 | 0.1639 (13) | −0.014 (2) | 0.0176 (9) | 0.020 (4)* | |
H6 | 0.1343 (14) | −0.167 (2) | 0.0573 (9) | 0.020 (4)* | |
C9 | 0.19760 (14) | −0.22340 (17) | −0.02510 (9) | 0.0200 (3)* | |
H7 | 0.1279 (14) | −0.223 (2) | −0.0469 (9) | 0.020 (4)* | |
H8 | 0.2134 (14) | −0.334 (2) | −0.0129 (9) | 0.020 (4)* | |
N2 | 0.28830 (11) | −0.16210 (14) | −0.06770 (7) | 0.0200 (3)* | |
C10 | 0.26340 (15) | −0.10710 (16) | −0.11960 (9) | 0.0200 (3)* | |
H9 | 0.1897 (15) | −0.103 (2) | −0.1313 (8) | 0.020 (4)* | |
C11 | 0.31490 (14) | 0.01820 (16) | −0.21840 (8) | 0.0200 (3)* | |
H10 | 0.2411 (15) | 0.017 (2) | −0.2296 (8) | 0.020 (4)* | |
C12 | 0.39270 (14) | 0.08580 (17) | −0.25770 (10) | 0.0200 (3)* | |
H11 | 0.3709 (14) | 0.130 (2) | −0.2951 (9) | 0.020 (5)* | |
C13 | 0.50330 (14) | 0.08720 (16) | −0.24110 (10) | 0.0200 (3)* | |
H12 | 0.5553 (15) | 0.1324 (19) | −0.2673 (9) | 0.020 (4)* | |
C14 | 0.53590 (13) | 0.02070 (17) | −0.18500 (9) | 0.0200 (3)* | |
C15 | 0.45810 (12) | −0.04700 (17) | −0.14580 (9) | 0.0200 (3)* | |
C16 | 0.34760 (13) | −0.04830 (16) | −0.16250 (9) | 0.0200 (3)* | |
C17 | 0.67020 (14) | 0.15330 (16) | −0.12810 (10) | 0.0200 (3)* | |
H13 | 0.6266 (15) | 0.141 (2) | −0.0909 (9) | 0.020 (5)* | |
H14 | 0.6502 (14) | 0.255 (2) | −0.1473 (9) | 0.020 (5)* | |
C18 | 0.79020 (14) | 0.15600 (17) | −0.11150 (10) | 0.0200 (4)* | |
H15 | 0.8343 (15) | 0.1452 (19) | −0.1486 (9) | 0.020 (4)* | |
H16 | 0.8083 (14) | 0.259 (2) | −0.0923 (9) | 0.020 (4)* | |
C19 | 0.92040 (13) | 0.03910 (18) | −0.04390 (9) | 0.0200 (3)* | |
H17 | 0.9703 (14) | 0.090 (2) | −0.0731 (9) | 0.020 (4)* | |
H18 | 0.9473 (13) | −0.070 (2) | −0.0358 (9) | 0.020 (4)* | |
C20 | 0.92250 (14) | 0.13510 (17) | 0.01590 (9) | 0.0200 (3)* | |
H19 | 0.9976 (16) | 0.1479 (19) | 0.0301 (9) | 0.020 (4)* | |
H20 | 0.8913 (14) | 0.242 (2) | 0.0093 (9) | 0.020 (4)* | |
C21 | 0.85170 (14) | 0.13710 (17) | 0.11730 (9) | 0.0200 (3)* | |
H21 | 0.8200 (14) | 0.244 (2) | 0.1105 (9) | 0.020 (4)* | |
H22 | 0.9240 (15) | 0.1507 (19) | 0.1357 (8) | 0.020 (5)* | |
C22 | 0.78060 (13) | 0.04180 (17) | 0.15860 (10) | 0.0200 (3)* | |
H23 | 0.8062 (14) | −0.070 (2) | 0.1602 (9) | 0.020 (4)* | |
H24 | 0.7828 (14) | 0.086 (2) | 0.1999 (9) | 0.020 (4)* | |
Geometric parameters (Å, º) top
O1—C5 | 1.350 (2) | C5—C6 | 1.390 (2) |
O2—C15 | 1.349 (2) | C7—N1 | 1.300 (2) |
O3—C14 | 1.388 (2) | N1—C8 | 1.453 (2) |
O3—C17 | 1.4102 (19) | C8—C9 | 1.465 (2) |
O4—C18 | 1.403 (2) | C9—N2 | 1.524 (2) |
O4—C19 | 1.415 (2) | N2—C10 | 1.251 (2) |
O5—C20 | 1.410 (2) | C10—C16 | 1.465 (2) |
O5—C21 | 1.434 (2) | C11—C16 | 1.389 (3) |
O6—C6 | 1.3640 (18) | C11—C12 | 1.390 (2) |
O6—C22 | 1.430 (2) | C12—C13 | 1.391 (3) |
C1—C2 | 1.389 (2) | C13—C14 | 1.392 (3) |
C1—C6 | 1.390 (2) | C14—C15 | 1.389 (2) |
C2—C3 | 1.389 (3) | C15—C16 | 1.390 (2) |
C3—C4 | 1.390 (2) | C17—C18 | 1.502 (3) |
C4—C5 | 1.389 (2) | C19—C20 | 1.520 (3) |
C4—C7 | 1.446 (2) | C21—C22 | 1.472 (2) |
| | | |
C14—O3—C17 | 112.00 (12) | C10—N2—C9 | 119.41 (14) |
C18—O4—C19 | 113.90 (12) | N2—C10—C16 | 121.52 (16) |
C20—O5—C21 | 112.27 (12) | C16—C11—C12 | 119.97 (17) |
C6—O6—C22 | 119.17 (13) | C11—C12—C13 | 120.1 (2) |
C2—C1—C6 | 120.02 (17) | C12—C13—C14 | 119.85 (18) |
C3—C2—C1 | 120.02 (18) | O3—C14—C15 | 120.85 (16) |
C2—C3—C4 | 120.01 (15) | O3—C14—C13 | 119.14 (15) |
C5—C4—C3 | 119.98 (16) | C15—C14—C13 | 120.00 (16) |
C5—C4—C7 | 120.99 (16) | O2—C15—C14 | 118.51 (15) |
C3—C4—C7 | 119.02 (14) | O2—C15—C16 | 121.44 (15) |
O1—C5—C4 | 121.03 (15) | C14—C15—C16 | 120.05 (17) |
O1—C5—C6 | 118.93 (14) | C11—C16—C15 | 120.03 (15) |
C4—C5—C6 | 120.04 (17) | C11—C16—C10 | 119.04 (15) |
O6—C6—C1 | 124.51 (16) | C15—C16—C10 | 120.73 (17) |
O6—C6—C5 | 115.55 (16) | O3—C17—C18 | 111.12 (14) |
C1—C6—C5 | 119.94 (15) | O4—C18—C17 | 110.11 (14) |
N1—C7—C4 | 121.70 (14) | O4—C19—C20 | 113.49 (13) |
C7—N1—C8 | 121.06 (13) | O5—C20—C19 | 108.30 (13) |
N1—C8—C9 | 113.84 (13) | O5—C21—C22 | 107.49 (13) |
C8—C9—N2 | 110.66 (13) | O6—C22—C21 | 108.56 (14) |
(qelpus) (
S!
C$)-
trans-bis(mu!2$-Chloro)-bis(
N,
N-dimethyl-1-(2-naphthyl)ethylamine-C,
N)- -dipalladium(ii) monohydrate
top
Crystal data top
C28H32Cl2N2Pd2·H2O | γ = 90° |
Mr = 698.27 | V = 3040.2 (7) Å3 |
P212121 | Z = 4 |
a = 6.6179 (7) Å | F(000) = 1400 |
b = 12.924 (2) Å | Dx = 1.526 Mg m−3 |
c = 35.545 (5) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 1.38 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.028 |
Graphite monochromator | θmax = 26.9°, θmin = 1.2° |
8976 measured reflections | h = −6→6 |
2252 independent reflections | k = −10→10 |
2240 reflections with I > 2σ(I) | l = −16→16 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.007 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.042 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.36 | (Δ/σ)max = 3.897 |
2252 reflections | Δρmax = 0.16 e Å−3 |
269 parameters | Δρmin = −0.22 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.015 (19) |
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 | x | y | z | Uiso*/Ueq | |
Pd1 | 0.29800 (3) | 0.327500 (18) | 0.203400 (10) | 0.02000 (8)* | |
Pd2 | 0.62320 (3) | 0.435800 (18) | 0.137300 (11) | 0.02000 (8)* | |
Cl1 | 0.53520 (9) | 0.46130 (6) | 0.20440 (4) | 0.02000 (18)* | |
Cl2 | 0.44690 (9) | 0.27970 (6) | 0.14200 (4) | 0.02000 (17)* | |
O1 | 0.6635 (3) | 0.25870 (16) | 0.46260 (9) | 0.0200 (5)* | |
N1 | 0.0719 (3) | 0.2168 (2) | 0.20540 (12) | 0.0200 (6)* | |
N2 | 0.7921 (4) | 0.56950 (19) | 0.13160 (10) | 0.0200 (6)* | |
C1 | 0.1918 (4) | 0.3544 (2) | 0.25390 (13) | 0.0200 (7)* | |
C2 | 0.3020 (4) | 0.3999 (2) | 0.28330 (13) | 0.0200 (6)* | |
C3 | 0.2210 (4) | 0.4127 (2) | 0.31880 (13) | 0.0200 (7)* | |
C4 | 0.3265 (4) | 0.4588 (2) | 0.35060 (14) | 0.0200 (7)* | |
C5 | 0.2514 (4) | 0.4669 (2) | 0.38340 (15) | 0.0200 (8)* | |
C6 | 0.0561 (4) | 0.4322 (2) | 0.38980 (17) | 0.0200 (7)* | |
C7 | −0.0630 (4) | 0.3890 (2) | 0.36320 (15) | 0.0200 (7)* | |
C8 | 0.0157 (4) | 0.3745 (2) | 0.32560 (16) | 0.0200 (7)* | |
C9 | −0.0837 (4) | 0.3272 (2) | 0.29590 (14) | 0.0200 (7)* | |
C10 | 0.0042 (4) | 0.3142 (2) | 0.26140 (14) | 0.0200 (7)* | |
C11 | −0.0981 (4) | 0.2609 (2) | 0.22890 (14) | 0.0200 (7)* | |
C12 | −0.2628 (4) | 0.1856 (3) | 0.23910 (17) | 0.0200 (7)* | |
C13 | 0.1561 (4) | 0.1202 (3) | 0.22180 (16) | 0.0200 (7)* | |
C14 | −0.0049 (4) | 0.1912 (3) | 0.16700 (15) | 0.0200 (8)* | |
C15 | 0.6715 (4) | 0.4245 (2) | 0.08220 (14) | 0.0200 (7)* | |
C16 | 0.5654 (4) | 0.3708 (2) | 0.05660 (16) | 0.0200 (7)* | |
C17 | 0.6130 (4) | 0.3772 (2) | 0.01770 (15) | 0.0200 (7)* | |
C18 | 0.5025 (4) | 0.3228 (2) | −0.00960 (16) | 0.0200 (7)* | |
C19 | 0.5571 (4) | 0.3209 (2) | −0.04580 (17) | 0.0200 (7)* | |
C20 | 0.7217 (4) | 0.3776 (2) | −0.05780 (16) | 0.0200 (7)* | |
C21 | 0.8260 (4) | 0.4355 (2) | −0.03310 (15) | 0.0200 (7)* | |
C22 | 0.7743 (4) | 0.4390 (2) | 0.00630 (15) | 0.0200 (7)* | |
C23 | 0.8734 (4) | 0.4975 (2) | 0.03260 (16) | 0.0200 (7)* | |
C24 | 0.8293 (4) | 0.4925 (2) | 0.07010 (16) | 0.0200 (7)* | |
C25 | 0.9425 (4) | 0.5525 (3) | 0.10030 (15) | 0.0200 (7)* | |
C26 | 1.1223 (5) | 0.4905 (3) | 0.11230 (16) | 0.0200 (7)* | |
C27 | 0.6534 (4) | 0.6546 (3) | 0.11920 (16) | 0.0200 (8)* | |
C28 | 0.8932 (5) | 0.6028 (2) | 0.16710 (14) | 0.0200 (7)* | |
H1 | 0.433 (4) | 0.422 (2) | 0.2787 (11) | 0.020 (9)* | |
H2 | 0.457 (5) | 0.484 (2) | 0.3467 (11) | 0.020 (9)* | |
H3 | 0.327 (5) | 0.496 (2) | 0.4029 (12) | 0.020 (9)* | |
H4 | 0.004 (5) | 0.440 (2) | 0.4139 (12) | 0.020 (9)* | |
H5 | −0.194 (5) | 0.369 (2) | 0.3690 (11) | 0.020 (8)* | |
H6 | −0.215 (4) | 0.303 (2) | 0.2995 (11) | 0.020 (8)* | |
H7 | −0.161 (4) | 0.315 (2) | 0.2138 (11) | 0.020 (9)* | |
H8 | −0.318 (5) | 0.156 (2) | 0.2166 (12) | 0.020 (9)* | |
H9 | −0.368 (5) | 0.221 (2) | 0.2525 (11) | 0.020 (8)* | |
H10 | −0.208 (4) | 0.132 (2) | 0.2547 (11) | 0.020 (8)* | |
H11 | 0.262 (5) | 0.095 (2) | 0.2061 (12) | 0.020 (9)* | |
H12 | 0.051 (4) | 0.069 (2) | 0.2236 (11) | 0.020 (9)* | |
H13 | 0.209 (5) | 0.134 (2) | 0.2465 (13) | 0.020 (9)* | |
H14 | −0.060 (4) | 0.252 (3) | 0.1556 (12) | 0.020 (9)* | |
H15 | −0.108 (5) | 0.139 (2) | 0.1688 (11) | 0.020 (8)* | |
H16 | 0.104 (4) | 0.166 (2) | 0.1518 (12) | 0.020 (8)* | |
H17 | 0.459 (4) | 0.329 (2) | 0.0644 (11) | 0.020 (9)* | |
H18 | 0.387 (4) | 0.287 (2) | −0.0022 (12) | 0.020 (8)* | |
H19 | 0.484 (4) | 0.281 (2) | −0.0629 (11) | 0.020 (9)* | |
H20 | 0.760 (5) | 0.376 (2) | −0.0829 (12) | 0.020 (10)* | |
H21 | 0.935 (4) | 0.475 (2) | −0.0417 (12) | 0.020 (9)* | |
H22 | 0.975 (4) | 0.542 (2) | 0.0247 (11) | 0.020 (9)* | |
H23 | 0.987 (4) | 0.619 (3) | 0.0902 (12) | 0.020 (9)* | |
H24 | 1.195 (5) | 0.528 (2) | 0.1313 (11) | 0.020 (8)* | |
H25 | 1.209 (5) | 0.479 (2) | 0.0911 (12) | 0.020 (9)* | |
H26 | 1.078 (4) | 0.425 (2) | 0.1222 (11) | 0.020 (8)* | |
H27 | 0.556 (5) | 0.668 (2) | 0.1385 (13) | 0.020 (8)* | |
H28 | 0.585 (5) | 0.634 (2) | 0.0965 (14) | 0.020 (9)* | |
H29 | 0.730 (4) | 0.716 (2) | 0.1146 (11) | 0.020 (9)* | |
H30 | 0.793 (5) | 0.616 (2) | 0.1860 (12) | 0.020 (9)* | |
H31 | 0.968 (4) | 0.665 (2) | 0.1626 (11) | 0.020 (9)* | |
H32 | 0.983 (4) | 0.549 (2) | 0.1755 (12) | 0.020 (9)* | |
Geometric parameters (Å, º) top
Pd1—C1 | 1.959 (4) | C12—H10 | 0.96 (3) |
Pd1—N1 | 2.071 (2) | C13—H11 | 0.96 (3) |
Pd1—Cl1 | 2.3357 (7) | C13—H12 | 0.96 (3) |
Pd1—Cl2 | 2.4730 (12) | C13—H13 | 0.96 (4) |
Pd2—C15 | 1.990 (5) | C14—H14 | 0.96 (3) |
Pd2—N2 | 2.068 (2) | C14—H15 | 0.96 (3) |
Pd2—Cl2 | 2.3365 (8) | C14—H16 | 0.96 (3) |
Pd2—Cl1 | 2.4772 (13) | C15—C16 | 1.343 (6) |
N1—C13 | 1.486 (5) | C15—C24 | 1.431 (4) |
N1—C14 | 1.494 (6) | C16—C17 | 1.421 (6) |
N1—C11 | 1.513 (4) | C16—H17 | 0.93 (3) |
N2—C28 | 1.492 (5) | C17—C22 | 1.393 (4) |
N2—C27 | 1.499 (4) | C17—C18 | 1.404 (6) |
N2—C25 | 1.509 (5) | C18—C19 | 1.337 (6) |
C1—C10 | 1.372 (4) | C18—H18 | 0.93 (3) |
C1—C2 | 1.403 (6) | C19—C20 | 1.380 (5) |
C2—C3 | 1.381 (6) | C19—H19 | 0.93 (3) |
C2—H1 | 0.93 (3) | C20—C21 | 1.344 (6) |
C3—C4 | 1.456 (6) | C20—H20 | 0.93 (4) |
C3—C8 | 1.466 (4) | C21—C22 | 1.442 (5) |
C4—C5 | 1.272 (6) | C21—H21 | 0.93 (3) |
C4—H2 | 0.93 (3) | C22—C23 | 1.370 (6) |
C5—C6 | 1.387 (4) | C23—C24 | 1.366 (6) |
C5—H3 | 0.93 (4) | C23—H22 | 0.93 (3) |
C6—C7 | 1.352 (6) | C24—C25 | 1.521 (6) |
C6—H4 | 0.93 (4) | C25—C26 | 1.497 (4) |
C7—C8 | 1.447 (7) | C25—H23 | 0.98 (3) |
C7—H5 | 0.93 (3) | C26—H24 | 0.96 (4) |
C8—C9 | 1.386 (6) | C26—H25 | 0.96 (4) |
C9—C10 | 1.368 (6) | C26—H26 | 0.96 (3) |
C9—H6 | 0.93 (3) | C27—H27 | 0.96 (4) |
C10—C11 | 1.506 (6) | C27—H28 | 0.96 (4) |
C11—C12 | 1.506 (4) | C27—H29 | 0.96 (3) |
C11—H7 | 0.98 (3) | C28—H30 | 0.96 (4) |
C12—H8 | 0.96 (4) | C28—H31 | 0.96 (3) |
C12—H9 | 0.96 (3) | C28—H32 | 0.96 (3) |
| | | |
C1—Pd1—N1 | 80.33 (14) | H9—C12—H10 | 110 (3) |
C1—Pd1—Cl1 | 95.50 (9) | N1—C13—H11 | 110 (2) |
N1—Pd1—Cl1 | 175.05 (9) | N1—C13—H12 | 109.4 (19) |
C1—Pd1—Cl2 | 174.89 (10) | H11—C13—H12 | 110 (3) |
N1—Pd1—Cl2 | 98.37 (11) | N1—C13—H13 | 109.4 (19) |
Cl1—Pd1—Cl2 | 86.02 (3) | H11—C13—H13 | 109 (3) |
C15—Pd2—N2 | 83.00 (13) | H12—C13—H13 | 109 (3) |
C15—Pd2—Cl2 | 95.00 (9) | N1—C14—H14 | 109 (2) |
N2—Pd2—Cl2 | 176.77 (8) | N1—C14—H15 | 110 (2) |
C15—Pd2—Cl1 | 174.40 (9) | H14—C14—H15 | 109 (3) |
N2—Pd2—Cl1 | 96.33 (10) | N1—C14—H16 | 109 (2) |
Cl2—Pd2—Cl1 | 85.91 (3) | H14—C14—H16 | 109 (3) |
Pd1—Cl1—Pd2 | 92.57 (4) | H15—C14—H16 | 109 (3) |
Pd2—Cl2—Pd1 | 92.66 (4) | C16—C15—C24 | 119.7 (5) |
C13—N1—C14 | 107.5 (3) | C16—C15—Pd2 | 128.4 (3) |
C13—N1—C11 | 112.3 (3) | C24—C15—Pd2 | 111.6 (3) |
C14—N1—C11 | 109.6 (2) | C15—C16—C17 | 120.9 (4) |
C13—N1—Pd1 | 108.83 (17) | C15—C16—H17 | 120 (3) |
C14—N1—Pd1 | 111.6 (2) | C17—C16—H17 | 119 (3) |
C11—N1—Pd1 | 107.21 (18) | C22—C17—C18 | 119.0 (5) |
C28—N2—C27 | 108.2 (3) | C22—C17—C16 | 119.1 (4) |
C28—N2—C25 | 111.7 (2) | C18—C17—C16 | 121.9 (3) |
C27—N2—C25 | 107.1 (3) | C19—C18—C17 | 122.3 (4) |
C28—N2—Pd2 | 113.6 (2) | C19—C18—H18 | 119 (3) |
C27—N2—Pd2 | 108.12 (18) | C17—C18—H18 | 119 (3) |
C25—N2—Pd2 | 107.89 (19) | C18—C19—C20 | 120.1 (4) |
C10—C1—C2 | 119.0 (4) | C18—C19—H19 | 120 (2) |
C10—C1—Pd1 | 115.8 (3) | C20—C19—H19 | 120 (2) |
C2—C1—Pd1 | 124.8 (2) | C21—C20—C19 | 119.9 (5) |
C3—C2—C1 | 121.9 (3) | C21—C20—H20 | 119.9 (18) |
C3—C2—H1 | 119 (2) | C19—C20—H20 | 120.1 (19) |
C1—C2—H1 | 119 (2) | C20—C21—C22 | 122.0 (4) |
C2—C3—C4 | 124.9 (3) | C20—C21—H21 | 119 (3) |
C2—C3—C8 | 118.0 (4) | C22—C21—H21 | 119 (2) |
C4—C3—C8 | 117.0 (4) | C23—C22—C17 | 119.0 (5) |
C5—C4—C3 | 123.9 (3) | C23—C22—C21 | 124.5 (3) |
C5—C4—H2 | 118 (3) | C17—C22—C21 | 116.5 (4) |
C3—C4—H2 | 118 (3) | C24—C23—C22 | 122.5 (3) |
C4—C5—C6 | 119.2 (5) | C24—C23—H22 | 119 (2) |
C4—C5—H3 | 120 (2) | C22—C23—H22 | 119 (2) |
C6—C5—H3 | 120 (2) | C23—C24—C15 | 118.6 (4) |
C7—C6—C5 | 124.2 (5) | C23—C24—C25 | 124.0 (3) |
C7—C6—H4 | 118.0 (19) | C15—C24—C25 | 117.4 (5) |
C5—C6—H4 | 118 (2) | C26—C25—N2 | 113.1 (4) |
C6—C7—C8 | 119.3 (3) | C26—C25—C24 | 108.6 (3) |
C6—C7—H5 | 120 (3) | N2—C25—C24 | 105.6 (2) |
C8—C7—H5 | 120 (2) | C26—C25—H23 | 109.8 (17) |
C9—C8—C7 | 126.2 (3) | N2—C25—H23 | 110 (2) |
C9—C8—C3 | 117.6 (5) | C24—C25—H23 | 110 (2) |
C7—C8—C3 | 116.3 (4) | C25—C26—H24 | 109.4 (18) |
C10—C9—C8 | 122.4 (3) | C25—C26—H25 | 110 (2) |
C10—C9—H6 | 119 (2) | H24—C26—H25 | 109 (3) |
C8—C9—H6 | 119 (2) | C25—C26—H26 | 109.6 (17) |
C9—C10—C1 | 120.8 (4) | H24—C26—H26 | 110 (3) |
C9—C10—C11 | 123.6 (3) | H25—C26—H26 | 109 (2) |
C1—C10—C11 | 115.5 (4) | N2—C27—H27 | 109 (2) |
C12—C11—C10 | 115.9 (4) | N2—C27—H28 | 109.6 (18) |
C12—C11—N1 | 115.3 (3) | H27—C27—H28 | 109 (3) |
C10—C11—N1 | 105.2 (2) | N2—C27—H29 | 109.4 (17) |
C12—C11—H7 | 106.6 (17) | H27—C27—H29 | 109 (3) |
C10—C11—H7 | 107 (2) | H28—C27—H29 | 109 (3) |
N1—C11—H7 | 107 (2) | N2—C28—H30 | 109 (2) |
C11—C12—H8 | 110 (2) | N2—C28—H31 | 109 (2) |
C11—C12—H9 | 109.5 (18) | H30—C28—H31 | 109 (3) |
H8—C12—H9 | 109 (3) | N2—C28—H32 | 110 (2) |
C11—C12—H10 | 109.5 (18) | H30—C28—H32 | 110 (3) |
H8—C12—H10 | 109 (3) | H31—C28—H32 | 109 (2) |
Crystal data top
C15BrO2 | γ = 90° |
Mr = 292.06 | V = 1383.7 (10) Å3 |
P43 | Z = 4 |
a = 13.750 (5) Å | F(000) = 564 |
b = 13.750 (5) Å | Dx = 1.402 Mg m−3 |
c = 7.319 (4) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 2.96 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.053 |
Graphite monochromator | θmax = 47.1°, θmin = 1.5° |
20164 measured reflections | h = −15→15 |
5044 independent reflections | k = −15→15 |
4914 reflections with I > 2σ(I) | l = −10→10 |
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)] = 0.009 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.050 | (Δ/σ)max = 0.261 |
S = 0.31 | Δρmax = 0.41 e Å−3 |
5044 reflections | Δρmin = −0.41 e Å−3 |
73 parameters | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
1 restraint | Absolute structure parameter: 0.015 (2) |
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 | x | y | z | Uiso*/Ueq | |
Br1 | 0.889000 (6) | 0.835000 (6) | 0.499500 (15) | 0.02000 (2)* | |
O4 | 0.78510 (5) | 0.53550 (5) | −0.05260 (9) | 0.02000 (10)* | |
O11 | 0.59220 (5) | 0.45900 (5) | 0.01880 (9) | 0.02000 (10)* | |
C1 | 0.87600 (6) | 0.41500 (7) | 0.32000 (11) | 0.02000 (12)* | |
C2 | 0.93450 (7) | 0.39800 (7) | 0.14500 (11) | 0.02000 (12)* | |
C3 | 0.85700 (6) | 0.37750 (6) | 0.00900 (12) | 0.02000 (12)* | |
C13 | 0.77000 (7) | 0.44650 (7) | 0.04250 (10) | 0.02000 (13)* | |
C4 | 0.81100 (7) | 0.60800 (7) | 0.05750 (11) | 0.02000 (12)* | |
C5 | 0.83300 (6) | 0.70200 (6) | 0.00850 (12) | 0.02000 (12)* | |
C6 | 0.85750 (7) | 0.77150 (7) | 0.13450 (11) | 0.02000 (12)* | |
C7 | 0.85500 (7) | 0.74450 (6) | 0.31800 (11) | 0.02000 (12)* | |
C8 | 0.83200 (7) | 0.64800 (7) | 0.37700 (11) | 0.02000 (12)* | |
C18 | 0.80750 (6) | 0.58100 (6) | 0.25200 (12) | 0.02000 (11)* | |
C28 | 0.78500 (6) | 0.47400 (6) | 0.26400 (11) | 0.02000 (12)* | |
C9 | 0.89200 (7) | 0.38000 (7) | −0.19600 (11) | 0.02000 (12)* | |
C10 | 0.67600 (6) | 0.40250 (7) | −0.00650 (12) | 0.02000 (12)* | |
C12 | 0.87550 (7) | 0.87700 (7) | 0.08550 (11) | 0.02000 (12)* | |
C31 | 0.70000 (7) | 0.45700 (7) | 0.38600 (11) | 0.02000 (13)* | |
Geometric parameters (Å, º) top
Br1—C7 | 1.8793 (11) | C13—C28 | 1.6774 (14) |
O4—C4 | 1.3304 (12) | C4—C5 | 1.3750 (13) |
O4—C13 | 1.4231 (12) | C4—C18 | 1.4719 (14) |
O11—C10 | 1.4020 (11) | C5—C6 | 1.3701 (13) |
C1—C2 | 1.5304 (13) | C6—C7 | 1.3938 (14) |
C1—C28 | 1.5465 (13) | C6—C12 | 1.5147 (13) |
C2—C3 | 1.4852 (13) | C7—C8 | 1.4308 (13) |
C3—C13 | 1.5464 (14) | C8—C18 | 1.3413 (13) |
C3—C9 | 1.5761 (14) | C18—C28 | 1.5060 (13) |
C13—C10 | 1.4715 (14) | C28—C31 | 1.4893 (13) |
| | | |
C4—O4—C13 | 112.78 (8) | C5—C6—C12 | 123.29 (8) |
C2—C1—C28 | 106.47 (7) | C7—C6—C12 | 119.16 (8) |
C3—C2—C1 | 102.29 (8) | C6—C7—C8 | 122.91 (8) |
C2—C3—C13 | 109.41 (7) | C6—C7—Br1 | 119.91 (7) |
C2—C3—C9 | 114.51 (8) | C8—C7—Br1 | 117.11 (7) |
C13—C3—C9 | 111.95 (7) | C18—C8—C7 | 119.12 (8) |
O4—C13—C10 | 111.25 (7) | C8—C18—C4 | 118.57 (8) |
O4—C13—C3 | 109.71 (7) | C8—C18—C28 | 133.06 (8) |
C10—C13—C3 | 112.87 (7) | C4—C18—C28 | 108.03 (7) |
O4—C13—C28 | 105.12 (7) | C31—C28—C18 | 110.46 (7) |
C10—C13—C28 | 115.86 (7) | C31—C28—C1 | 113.19 (7) |
C3—C13—C28 | 101.33 (7) | C18—C28—C1 | 111.21 (7) |
O4—C4—C5 | 127.25 (8) | C31—C28—C13 | 116.59 (8) |
O4—C4—C18 | 112.83 (8) | C18—C28—C13 | 100.90 (7) |
C5—C4—C18 | 119.77 (8) | C1—C28—C13 | 103.73 (7) |
C6—C5—C4 | 122.29 (8) | O11—C10—C13 | 117.51 (8) |
C5—C6—C7 | 117.18 (9) | | |
(doqzak) (2-Hydroxyethanolato)-oxo-(
N-(1-oxy-2-methylprop-2-yl)-2-oxy-1-naphthaldimato)- -vanadium(v)
top
Crystal data top
C17H20NO5V | γ = 90° |
Mr = 369.28 | V = 1720 (2) Å3 |
P43 | Z = 4 |
a = 9.717 (8) Å | F(000) = 768 |
b = 9.717 (8) Å | Dx = 1.426 Mg m−3 |
c = 18.217 (9) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.60 mm−1 |
β = 90° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.014 |
Graphite monochromator | θmax = 45.5°, θmin = 2.1° |
23096 measured reflections | h = −12→12 |
5780 independent reflections | k = −12→12 |
5762 reflections with I > 2σ(I) | l = −18→18 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.008 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.031 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.18 | (Δ/σ)max = 1.238 |
5780 reflections | Δρmax = 0.07 e Å−3 |
177 parameters | Δρmin = −0.17 e Å−3 |
1 restraint | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.009 (2) |
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 | x | y | z | Uiso*/Ueq | |
V1 | 0.069400 (6) | 0.780500 (6) | 0.904700 (4) | 0.02000 (2)* | |
O1 | −0.01470 (3) | 0.66230 (3) | 0.944000 (18) | 0.02000 (4)* | |
O2 | 0.24500 (3) | 0.72300 (3) | 0.919600 (17) | 0.02000 (4)* | |
O3 | −0.07580 (3) | 0.85510 (3) | 0.848100 (18) | 0.02000 (4)* | |
O4 | 0.18240 (3) | 0.97420 (3) | 0.855800 (19) | 0.02000 (4)* | |
H36 | 0.1440 (7) | 0.9987 (7) | 0.8064 (4) | 0.0200 (14)* | |
O5 | 0.06890 (3) | 0.90760 (3) | 0.979400 (18) | 0.02000 (5)* | |
N1 | 0.11340 (3) | 0.67980 (3) | 0.80530 (2) | 0.02000 (5)* | |
C1 | 0.33160 (4) | 0.69930 (4) | 0.85840 (2) | 0.02000 (5)* | |
H1 | 0.4213 (7) | 0.6660 (7) | 0.8702 (4) | 0.0200 (14)* | |
H2 | 0.3473 (7) | 0.7872 (7) | 0.8361 (4) | 0.0200 (14)* | |
C2 | 0.25340 (4) | 0.61560 (3) | 0.80370 (2) | 0.02000 (5)* | |
C3 | 0.03330 (3) | 0.65850 (3) | 0.75130 (2) | 0.02000 (5)* | |
H37 | 0.0625 (7) | 0.5958 (7) | 0.7088 (4) | 0.0200 (15)* | |
C4 | −0.10290 (4) | 0.71460 (3) | 0.74200 (2) | 0.02000 (5)* | |
C5 | −0.14500 (3) | 0.81670 (3) | 0.79040 (2) | 0.02000 (5)* | |
C6 | −0.27200 (4) | 0.88860 (3) | 0.77550 (2) | 0.02000 (5)* | |
H3 | −0.3037 (7) | 0.9552 (7) | 0.8081 (4) | 0.0200 (14)* | |
C7 | −0.34410 (3) | 0.85950 (3) | 0.71490 (2) | 0.02000 (5)* | |
H4 | −0.4225 (7) | 0.9111 (7) | 0.7050 (4) | 0.0200 (15)* | |
C8 | −0.38570 (3) | 0.72790 (3) | 0.60060 (2) | 0.02000 (5)* | |
H5 | −0.4632 (7) | 0.7805 (7) | 0.5901 (4) | 0.0200 (14)* | |
C9 | −0.34860 (4) | 0.63010 (3) | 0.55650 (2) | 0.02000 (5)* | |
H6 | −0.4015 (7) | 0.6141 (7) | 0.5148 (4) | 0.0200 (14)* | |
C10 | −0.23600 (3) | 0.54940 (4) | 0.56820 (3) | 0.02000 (5)* | |
H7 | −0.2131 (7) | 0.4802 (7) | 0.5351 (4) | 0.0200 (14)* | |
C11 | −0.15530 (3) | 0.57210 (3) | 0.63060 (2) | 0.02000 (5)* | |
H8 | −0.0800 (6) | 0.5156 (7) | 0.6399 (4) | 0.0200 (15)* | |
C12 | −0.18600 (3) | 0.67770 (4) | 0.67910 (2) | 0.02000 (6)* | |
C13 | −0.30710 (3) | 0.75510 (4) | 0.66590 (2) | 0.02000 (5)* | |
C14 | 0.23600 (3) | 0.46700 (4) | 0.82990 (2) | 0.02000 (5)* | |
H9 | 0.1855 (7) | 0.4156 (7) | 0.7939 (4) | 0.0200 (14)* | |
H10 | 0.1866 (7) | 0.4662 (7) | 0.8756 (4) | 0.0200 (14)* | |
H11 | 0.3249 (7) | 0.4259 (7) | 0.8369 (4) | 0.0200 (14)* | |
C15 | 0.32350 (3) | 0.62830 (3) | 0.72900 (2) | 0.02000 (5)* | |
H12 | 0.2740 (7) | 0.5748 (7) | 0.6935 (4) | 0.0200 (14)* | |
H13 | 0.4163 (7) | 0.5950 (7) | 0.7325 (4) | 0.0200 (14)* | |
H14 | 0.3244 (7) | 0.7230 (7) | 0.7141 (4) | 0.0200 (14)* | |
C16 | 0.15860 (3) | 1.08410 (3) | 0.90740 (2) | 0.02000 (5)* | |
H15 | 0.2260 (7) | 1.1574 (7) | 0.9042 (4) | 0.0200 (14)* | |
H16 | 0.0696 (7) | 1.1241 (7) | 0.8981 (4) | 0.0200 (14)* | |
C17 | 0.15710 (3) | 1.02080 (4) | 0.97930 (2) | 0.02000 (6)* | |
H17 | 0.2494 (7) | 0.9914 (7) | 0.9923 (4) | 0.0200 (14)* | |
H18 | 0.1267 (7) | 1.0872 (7) | 1.0156 (4) | 0.0200 (14)* | |
Geometric parameters (Å, º) top
V1—O1 | 1.5810 (11) | C6—H3 | 0.931 (7) |
V1—O2 | 1.8159 (15) | C7—C13 | 1.3983 (9) |
V1—O5 | 1.8377 (9) | C7—H4 | 0.930 (7) |
V1—O3 | 1.8919 (12) | C8—C9 | 1.2956 (9) |
V1—N1 | 2.1022 (10) | C8—C13 | 1.4381 (8) |
V1—O4 | 2.3541 (17) | C8—H5 | 0.930 (7) |
O2—C1 | 1.4157 (8) | C9—C10 | 1.3629 (12) |
O3—C5 | 1.3024 (7) | C9—H6 | 0.930 (7) |
O4—C16 | 1.4413 (9) | C10—C11 | 1.3985 (8) |
O4—H36 | 1.003 (8) | C10—H7 | 0.930 (7) |
O5—C17 | 1.3944 (12) | C11—C12 | 1.3866 (9) |
N1—C3 | 1.2714 (8) | C11—H8 | 0.930 (6) |
N1—C2 | 1.4969 (13) | C12—C13 | 1.4171 (12) |
C1—C2 | 1.4939 (9) | C14—H9 | 0.959 (7) |
C1—H1 | 0.954 (7) | C14—H10 | 0.961 (7) |
C1—H2 | 0.958 (7) | C14—H11 | 0.960 (7) |
C2—C15 | 1.5268 (9) | C15—H12 | 0.959 (7) |
C2—C14 | 1.5302 (12) | C15—H13 | 0.960 (7) |
C3—C4 | 1.4413 (13) | C15—H14 | 0.959 (7) |
C3—H37 | 1.025 (7) | C16—C17 | 1.4471 (9) |
C4—C5 | 1.3889 (9) | C16—H15 | 0.969 (6) |
C4—C12 | 1.4469 (9) | C16—H16 | 0.963 (7) |
C5—C6 | 1.4438 (12) | C17—H17 | 0.971 (7) |
C6—C7 | 1.3377 (8) | C17—H18 | 0.970 (7) |
| | | |
O1—V1—O2 | 101.215 (17) | C5—C6—H3 | 120.0 (4) |
O1—V1—O5 | 98.72 (5) | C6—C7—C13 | 123.06 (4) |
O2—V1—O5 | 95.66 (2) | C6—C7—H4 | 118.4 (5) |
O1—V1—O3 | 98.03 (3) | C13—C7—H4 | 118.6 (5) |
O2—V1—O3 | 154.18 (2) | C9—C8—C13 | 120.00 (5) |
O5—V1—O3 | 98.29 (4) | C9—C8—H5 | 120.1 (5) |
O1—V1—N1 | 99.03 (4) | C13—C8—H5 | 119.9 (5) |
O2—V1—N1 | 78.14 (3) | C8—C9—C10 | 123.26 (5) |
O5—V1—N1 | 162.028 (15) | C8—C9—H6 | 118.4 (4) |
O3—V1—N1 | 81.99 (5) | C10—C9—H6 | 118.4 (4) |
O1—V1—O4 | 173.358 (14) | C9—C10—C11 | 119.11 (4) |
O2—V1—O4 | 82.200 (14) | C9—C10—H7 | 120.4 (4) |
O5—V1—O4 | 75.17 (4) | C11—C10—H7 | 120.5 (4) |
O3—V1—O4 | 80.52 (2) | C12—C11—C10 | 120.93 (4) |
N1—V1—O4 | 87.21 (4) | C12—C11—H8 | 119.3 (4) |
C1—O2—V1 | 119.40 (4) | C10—C11—H8 | 119.7 (4) |
C5—O3—V1 | 135.65 (3) | C11—C12—C13 | 117.60 (4) |
C16—O4—V1 | 105.71 (4) | C11—C12—C4 | 124.61 (4) |
C16—O4—H36 | 110.5 (4) | C13—C12—C4 | 117.79 (3) |
V1—O4—H36 | 110.8 (4) | C7—C13—C12 | 119.36 (4) |
C17—O5—V1 | 121.84 (3) | C7—C13—C8 | 121.66 (4) |
C3—N1—C2 | 118.26 (4) | C12—C13—C8 | 118.93 (3) |
C3—N1—V1 | 128.15 (4) | C2—C14—H9 | 109.5 (4) |
C2—N1—V1 | 113.30 (3) | C2—C14—H10 | 109.5 (4) |
O2—C1—C2 | 108.15 (5) | H9—C14—H10 | 109.4 (6) |
O2—C1—H1 | 114.9 (5) | C2—C14—H11 | 109.5 (4) |
C2—C1—H1 | 115.5 (4) | H9—C14—H11 | 109.5 (6) |
O2—C1—H2 | 106.5 (4) | H10—C14—H11 | 109.3 (6) |
C2—C1—H2 | 106.5 (4) | C2—C15—H12 | 109.5 (4) |
H1—C1—H2 | 104.6 (6) | C2—C15—H13 | 109.4 (5) |
C1—C2—N1 | 102.85 (3) | H12—C15—H13 | 109.5 (6) |
C1—C2—C15 | 108.88 (5) | C2—C15—H14 | 109.5 (4) |
N1—C2—C15 | 112.90 (4) | H12—C15—H14 | 109.5 (6) |
C1—C2—C14 | 111.22 (5) | H13—C15—H14 | 109.5 (6) |
N1—C2—C14 | 106.67 (3) | O4—C16—C17 | 106.08 (6) |
C15—C2—C14 | 113.80 (3) | O4—C16—H15 | 113.4 (4) |
N1—C3—C4 | 126.27 (4) | C17—C16—H15 | 111.9 (5) |
N1—C3—H37 | 120.8 (4) | O4—C16—H16 | 109.2 (4) |
C4—C3—H37 | 113.0 (4) | C17—C16—H16 | 108.8 (5) |
C5—C4—C3 | 117.77 (4) | H15—C16—H16 | 107.4 (5) |
C5—C4—C12 | 121.02 (4) | O5—C17—C16 | 110.04 (4) |
C3—C4—C12 | 120.78 (4) | O5—C17—H17 | 109.6 (4) |
O3—C5—C4 | 124.40 (4) | C16—C17—H17 | 109.7 (5) |
O3—C5—C6 | 117.02 (3) | O5—C17—H18 | 109.7 (4) |
C4—C5—C6 | 118.56 (5) | C16—C17—H18 | 109.7 (4) |
C7—C6—C5 | 120.03 (4) | H17—C17—H18 | 108.1 (6) |
C7—C6—H3 | 120.0 (4) | | |
(bamubr) bis(Tetra-n-butylammonium) tetrabromo-uranyl
top
Crystal data top
C16Br2NOU0.50 | γ = 90° |
Mr = 501.01 | V = 4298 (8) Å3 |
C2/c | Z = 8 |
a = 17.731 (15) Å | F(000) = 1816 |
b = 14.681 (15) Å | Dx = 1.549 Mg m−3 |
c = 17.08 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 7.52 mm−1 |
β = 104.80 (8)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.020 |
Graphite monochromator | θmax = 60.3°, θmin = 1.8° |
22662 measured reflections | h = −24→24 |
7087 independent reflections | k = −24→24 |
6880 reflections with I > 2σ(I) | l = −30→30 |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Primary atom site location: structure-invariant direct methods |
R[F2 > 2σ(F2)] = 0.010 | Secondary atom site location: difference Fourier map |
wR(F2) = 0.086 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.57 | (Δ/σ)max = 3.860 |
7087 reflections | Δρmax = 1.42 e Å−3 |
83 parameters | Δρmin = −0.75 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. |
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 | Uiso*/Ueq | |
U1 | 0.0000 | 0.131200 (4) | 0.7500 | 0.02000 (3)* | |
Br1 | 0.162100 (11) | 0.127300 (9) | 0.820300 (9) | 0.02000 (4)* | |
Br3 | 0.0000 | −0.060300 (14) | 0.7500 | 0.02000 (5)* | |
Br4 | 0.0000 | 0.322300 (14) | 0.7500 | 0.02000 (5)* | |
O1 | 0.01450 (9) | 0.13100 (5) | 0.65450 (8) | 0.0200 (2)* | |
N1 | 0.21180 (8) | 0.08170 (8) | 0.13450 (7) | 0.02000 (18)* | |
C1 | 0.20170 (9) | 0.16820 (8) | 0.08500 (7) | 0.02000 (19)* | |
C2 | 0.12650 (9) | 0.21600 (8) | 0.07950 (7) | 0.02000 (19)* | |
C3 | 0.12330 (9) | 0.29930 (9) | 0.01800 (8) | 0.0200 (2)* | |
C4 | 0.05070 (10) | 0.35670 (9) | 0.01250 (8) | 0.0200 (2)* | |
C5 | 0.20750 (10) | 0.09500 (8) | 0.21900 (8) | 0.02000 (19)* | |
C6 | 0.26380 (9) | 0.16780 (8) | 0.26700 (7) | 0.02000 (19)* | |
C7 | 0.26900 (9) | 0.15900 (9) | 0.35800 (8) | 0.0200 (2)* | |
C8 | 0.31980 (9) | 0.08130 (9) | 0.39450 (7) | 0.02000 (19)* | |
C9 | 0.29300 (8) | 0.04500 (9) | 0.12750 (7) | 0.02000 (18)* | |
C10 | 0.31080 (8) | −0.04530 (9) | 0.17250 (7) | 0.02000 (19)* | |
C11 | 0.39100 (9) | −0.07500 (9) | 0.15550 (7) | 0.02000 (18)* | |
C12 | 0.41000 (9) | −0.17550 (8) | 0.19150 (7) | 0.0200 (2)* | |
C13 | 0.14750 (9) | 0.01150 (9) | 0.09800 (7) | 0.02000 (19)* | |
C14 | 0.14120 (9) | −0.00780 (8) | 0.01000 (7) | 0.0200 (2)* | |
C15 | 0.08050 (10) | −0.09300 (9) | −0.01600 (8) | 0.02000 (19)* | |
C16 | 0.11620 (9) | −0.17480 (8) | 0.00800 (8) | 0.02000 (19)* | |
Geometric parameters (Å, º) top
U1—O1 | 1.715 (2) | C2—C3 | 1.604 (2) |
U1—O1i | 1.715 (2) | C3—C4 | 1.521 (2) |
U1—Br4 | 2.806 (3) | C5—C6 | 1.547 (2) |
U1—Br3 | 2.811 (3) | C6—C7 | 1.538 (3) |
U1—Br1 | 2.818 (3) | C7—C8 | 1.488 (2) |
U1—Br1i | 2.818 (3) | C9—C10 | 1.524 (2) |
N1—C5 | 1.477 (2) | C10—C11 | 1.583 (2) |
N1—C1 | 1.511 (2) | C11—C12 | 1.601 (2) |
N1—C13 | 1.545 (2) | C13—C14 | 1.505 (2) |
N1—C9 | 1.570 (2) | C14—C15 | 1.636 (2) |
C1—C2 | 1.488 (2) | C15—C16 | 1.371 (2) |
| | | |
O1—U1—O1i | 179.80 (5) | C1—N1—C13 | 111.42 (13) |
O1—U1—Br4 | 90.10 (3) | C5—N1—C9 | 113.38 (13) |
O1i—U1—Br4 | 90.10 (3) | C1—N1—C9 | 103.05 (11) |
O1—U1—Br3 | 89.90 (3) | C13—N1—C9 | 109.69 (12) |
O1i—U1—Br3 | 89.90 (3) | C2—C1—N1 | 114.07 (12) |
Br4—U1—Br3 | 180.0 | C1—C2—C3 | 106.39 (12) |
O1—U1—Br1 | 91.19 (10) | C4—C3—C2 | 110.53 (13) |
O1i—U1—Br1 | 88.81 (10) | N1—C5—C6 | 114.94 (12) |
Br4—U1—Br1 | 91.164 (3) | C7—C6—C5 | 109.96 (12) |
Br3—U1—Br1 | 88.836 (3) | C8—C7—C6 | 111.17 (12) |
O1—U1—Br1i | 88.81 (10) | C10—C9—N1 | 109.62 (11) |
O1i—U1—Br1i | 91.19 (10) | C9—C10—C11 | 103.12 (11) |
Br4—U1—Br1i | 91.164 (3) | C10—C11—C12 | 107.11 (11) |
Br3—U1—Br1i | 88.836 (3) | C14—C13—N1 | 112.78 (12) |
Br1—U1—Br1i | 177.672 (6) | C13—C14—C15 | 106.91 (12) |
C5—N1—C1 | 114.03 (11) | C16—C15—C14 | 111.55 (15) |
C5—N1—C13 | 105.39 (12) | | |
Symmetry code: (i) −x, y, −z+3/2. |
(farner) Tetrachloro-bis(
N,
N,
N,
N'-tetramethylurea)-uranium(iv)
top
Crystal data top
C10Cl4N4O2U | γ = 90° |
Mr = 587.97 | V = 2019.2 (4) Å3 |
C2/c | Z = 4 |
a = 16.429 (2) Å | F(000) = 1056 |
b = 8.514 (1) Å | Dx = 1.934 Mg m−3 |
c = 16.418 (2) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 8.57 mm−1 |
β = 118.45 (2)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.004 |
Graphite monochromator | θmax = 52.7°, θmin = 2.8° |
9718 measured reflections | h = −26→26 |
3303 independent reflections | k = −8→8 |
3049 reflections with I > 2σ(I) | l = −24→24 |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Primary atom site location: structure-invariant direct methods |
R[F2 > 2σ(F2)] = 0.004 | Secondary atom site location: difference Fourier map |
wR(F2) = 0.046 | w = 1/[σ2(Fo2) + (0.P)2 + 0.0533P] where P = (Fo2 + 2Fc2)/3 |
S = 0.49 | (Δ/σ)max = 2.086 |
3303 reflections | Δρmax = 0.41 e Å−3 |
42 parameters | Δρmin = −0.25 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. |
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 | Uiso*/Ueq | |
U1 | 0.250000 | 0.250000 | 0.00000 | 0.02000 (3)* | |
Cl1 | 0.393300 (13) | 0.061300 (17) | 0.071700 (14) | 0.02000 (5)* | |
Cl2 | 0.359100 (13) | 0.496100 (18) | 0.056600 (14) | 0.02000 (5)* | |
N1 | 0.34620 (12) | 0.24600 (6) | −0.20230 (13) | 0.0200 (3)* | |
N2 | 0.18350 (6) | 0.23820 (10) | −0.28790 (7) | 0.0200 (2)* | |
O1 | 0.25710 (11) | 0.24990 (4) | −0.13170 (12) | 0.0200 (3)* | |
C1 | 0.26210 (12) | 0.24460 (8) | −0.20710 (13) | 0.0200 (3)* | |
C2 | 0.42870 (4) | 0.28520 (16) | −0.11240 (5) | 0.02000 (9)* | |
C3 | 0.36330 (5) | 0.16840 (10) | −0.27530 (5) | 0.02000 (12)* | |
C4 | 0.09560 (5) | 0.19710 (9) | −0.28570 (5) | 0.02000 (14)* | |
C5 | 0.17310 (6) | 0.31540 (7) | −0.37460 (7) | 0.02000 (14)* | |
Geometric parameters (Å, º) top
U1—O1i | 2.2202 (17) | N1—C2 | 1.490 (2) |
U1—O1 | 2.2202 (17) | N1—C3 | 1.5075 (18) |
U1—Cl1i | 2.6209 (4) | N2—C1 | 1.341 (2) |
U1—Cl1 | 2.6209 (4) | N2—C5 | 1.5019 (13) |
U1—Cl2i | 2.6229 (3) | N2—C4 | 1.5030 (12) |
U1—Cl2 | 2.6229 (3) | O1—C1 | 1.280 (2) |
N1—C1 | 1.346 (2) | | |
| | | |
O1i—U1—O1 | 180.000 (19) | Cl1—U1—Cl2 | 90.833 (15) |
O1i—U1—Cl1i | 89.11 (4) | Cl2i—U1—Cl2 | 180.000 (10) |
O1—U1—Cl1i | 90.89 (4) | C1—N1—C2 | 118.94 (14) |
O1i—U1—Cl1 | 90.89 (4) | C1—N1—C3 | 121.63 (13) |
O1—U1—Cl1 | 89.11 (4) | C2—N1—C3 | 117.36 (11) |
Cl1i—U1—Cl1 | 180.0 | C1—N2—C5 | 122.75 (10) |
O1i—U1—Cl2i | 90.07 (3) | C1—N2—C4 | 117.98 (11) |
O1—U1—Cl2i | 89.93 (3) | C5—N2—C4 | 116.61 (8) |
Cl1i—U1—Cl2i | 90.833 (15) | C1—O1—U1 | 177.92 (6) |
Cl1—U1—Cl2i | 89.167 (15) | O1—C1—N2 | 118.88 (16) |
O1i—U1—Cl2 | 89.93 (3) | O1—C1—N1 | 118.69 (17) |
O1—U1—Cl2 | 90.07 (3) | N2—C1—N1 | 122.42 (17) |
Cl1i—U1—Cl2 | 89.167 (15) | | |
Symmetry code: (i) −x+1/2, −y+1/2, −z. |
(farniv) Tetrabromo-bis(
N,
N,
N',
N'-tetramethylurea)-uranium(iv)
top
Crystal data top
C10Br4N4O2U | γ = 90° |
Mr = 765.81 | V = 2156.7 (12) Å3 |
C2/c | Z = 4 |
a = 16.764 (5) Å | F(000) = 1344 |
b = 8.710 (4) Å | Dx = 2.359 Mg m−3 |
c = 16.655 (3) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 14.94 mm−1 |
β = 117.52 (2)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.008 |
Graphite monochromator | θmax = 50.6°, θmin = 2.7° |
9718 measured reflections | h = −26→26 |
3303 independent reflections | k = −8→8 |
3198 reflections with I > 2σ(I) | l = −24→24 |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Primary atom site location: structure-invariant direct methods |
R[F2 > 2σ(F2)] = 0.004 | Secondary atom site location: difference Fourier map |
wR(F2) = 0.033 | w = 1/[σ2(Fo2) + (0.P)2 + 0.0089P] where P = (Fo2 + 2Fc2)/3 |
S = 0.39 | (Δ/σ)max = 1.266 |
3303 reflections | Δρmax = 0.37 e Å−3 |
42 parameters | Δρmin = −0.36 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. |
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 | Uiso*/Ueq | |
U1 | 0.250000 | 0.250000 | 0.000000 | 0.02000 (3)* | |
Br1 | 0.397900 (6) | 0.054000 (13) | 0.071300 (7) | 0.02000 (3)* | |
Br2 | 0.361200 (7) | 0.506600 (12) | 0.055100 (7) | 0.02000 (3)* | |
N1 | 0.34020 (9) | 0.24560 (9) | −0.20330 (9) | 0.0200 (2)* | |
N2 | 0.18210 (7) | 0.23880 (11) | −0.28320 (8) | 0.0200 (2)* | |
O1 | 0.25540 (8) | 0.24970 (6) | −0.13030 (8) | 0.0200 (2)* | |
C1 | 0.25870 (10) | 0.24560 (10) | −0.20600 (11) | 0.0200 (3)* | |
C2 | 0.42070 (5) | 0.28650 (17) | −0.11930 (6) | 0.02000 (12)* | |
C3 | 0.35600 (6) | 0.16900 (12) | −0.27430 (7) | 0.02000 (16)* | |
C4 | 0.09800 (6) | 0.19720 (13) | −0.28080 (7) | 0.02000 (18)* | |
C5 | 0.17170 (7) | 0.31710 (10) | −0.36600 (8) | 0.02000 (18)* | |
Geometric parameters (Å, º) top
U1—O1 | 2.2134 (13) | N1—C2 | 1.4699 (17) |
U1—O1i | 2.2134 (13) | N1—C3 | 1.4843 (17) |
U1—Br2 | 2.7806 (9) | N2—C1 | 1.334 (2) |
U1—Br2i | 2.7806 (9) | N2—C4 | 1.4740 (15) |
U1—Br1i | 2.7841 (8) | N2—C5 | 1.4748 (17) |
U1—Br1 | 2.7841 (8) | O1—C1 | 1.288 (2) |
N1—C1 | 1.346 (2) | | |
| | | |
O1—U1—O1i | 180.00 (6) | Br2i—U1—Br1 | 88.68 (3) |
O1—U1—Br2 | 89.98 (3) | Br1i—U1—Br1 | 180.000 (5) |
O1i—U1—Br2 | 90.02 (3) | C1—N1—C2 | 120.21 (12) |
O1—U1—Br2i | 90.02 (3) | C1—N1—C3 | 121.69 (12) |
O1i—U1—Br2i | 89.98 (3) | C2—N1—C3 | 116.35 (10) |
Br2—U1—Br2i | 180.0 | C1—N2—C4 | 119.44 (11) |
O1—U1—Br1i | 90.82 (3) | C1—N2—C5 | 121.73 (10) |
O1i—U1—Br1i | 89.18 (3) | C4—N2—C5 | 115.96 (10) |
Br2—U1—Br1i | 88.68 (3) | C1—O1—U1 | 178.47 (6) |
Br2i—U1—Br1i | 91.32 (3) | O1—C1—N2 | 119.15 (13) |
O1—U1—Br1 | 89.18 (3) | O1—C1—N1 | 117.99 (14) |
O1i—U1—Br1 | 90.82 (3) | N2—C1—N1 | 122.84 (14) |
Br2—U1—Br1 | 91.32 (3) | | |
Symmetry code: (i) −x+1/2, −y+1/2, −z. |
(himfue) (2,6-bis((Di-t-butylphosphino)methyl)phenoxy)-trifluoroacetato-palladium(ii)
top
Crystal data top
C26H43F3O3P2Pd | γ = 90° |
Mr = 628.94 | V = 5761.9 (19) Å3 |
I2/a | Z = 8 |
a = 20.244 (4) Å | F(000) = 2608 |
b = 10.714 (2) Å | Dx = 1.450 Mg m−3 |
c = 27.238 (5) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.80 mm−1 |
β = 102.76 (3)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.016 |
Graphite monochromator | θmax = 47.4°, θmin = 1.5° |
26382 measured reflections | h = −35→35 |
8546 independent reflections | k = −10→10 |
8103 reflections with I > 2σ(I) | l = −45→45 |
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)] = 0.014 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.065 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.64 | w = 1/[σ2(Fo2) + (0.P)2 + 0.0757P] where P = (Fo2 + 2Fc2)/3 |
8546 reflections | (Δ/σ)max = 4.722 |
313 parameters | Δρmax = 0.62 e Å−3 |
0 restraints | Δρmin = −0.31 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. |
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 | Uiso*/Ueq | |
Pd1 | 0.166400 (3) | 0.310100 (6) | 0.358900 (2) | 0.02000 (3)* | |
P1 | 0.262600 (10) | 0.42870 (2) | 0.353400 (8) | 0.02000 (4)* | |
P2 | 0.103200 (10) | 0.12920 (2) | 0.365800 (8) | 0.02000 (5)* | |
O1 | 0.20160 (3) | 0.19960 (5) | 0.31210 (3) | 0.02000 (12)* | |
O2 | 0.12750 (3) | 0.43130 (6) | 0.40390 (2) | 0.02000 (10)* | |
C1 | 0.08110 (4) | 0.49590 (8) | 0.38160 (3) | 0.02000 (13)* | |
O3 | 0.04970 (3) | 0.49200 (6) | 0.33760 (2) | 0.02000 (10)* | |
C2 | 0.05660 (4) | 0.59310 (8) | 0.41490 (3) | 0.02000 (12)* | |
F1 | 0.00680 (2) | 0.66760 (5) | 0.391300 (18) | 0.02000 (8)* | |
F2 | 0.10670 (2) | 0.66660 (5) | 0.437300 (18) | 0.02000 (8)* | |
F3 | 0.03350 (2) | 0.53820 (5) | 0.452100 (19) | 0.02000 (8)* | |
C3 | 0.25040 (4) | 0.13560 (8) | 0.34420 (3) | 0.02000 (13)* | |
C4 | 0.31530 (4) | 0.18580 (7) | 0.35650 (4) | 0.02000 (15)* | |
C5 | 0.36600 (4) | 0.11650 (8) | 0.38750 (3) | 0.02000 (12)* | |
C6 | 0.35020 (4) | 0.00390 (8) | 0.40620 (3) | 0.02000 (13)* | |
C7 | 0.28490 (4) | −0.04050 (8) | 0.39720 (3) | 0.02000 (12)* | |
C8 | 0.23240 (4) | 0.02780 (8) | 0.36640 (3) | 0.02000 (12)* | |
C9 | 0.32280 (4) | 0.31410 (7) | 0.33650 (3) | 0.02000 (15)* | |
C10 | 0.15790 (4) | −0.00260 (8) | 0.35510 (3) | 0.02000 (12)* | |
C11 | 0.31060 (3) | 0.50120 (8) | 0.41260 (3) | 0.02000 (13)* | |
C12 | 0.24400 (3) | 0.54040 (8) | 0.29880 (3) | 0.02000 (12)* | |
C13 | 0.33460 (4) | 0.39900 (9) | 0.44900 (3) | 0.02000 (12)* | |
C14 | 0.37210 (4) | 0.58130 (8) | 0.40370 (3) | 0.02000 (13)* | |
C15 | 0.26600 (4) | 0.58920 (8) | 0.43510 (3) | 0.02000 (13)* | |
C16 | 0.19420 (4) | 0.46850 (8) | 0.25690 (3) | 0.02000 (13)* | |
C17 | 0.30470 (4) | 0.57050 (8) | 0.27770 (3) | 0.02000 (13)* | |
C18 | 0.20690 (4) | 0.65410 (9) | 0.31240 (3) | 0.02000 (12)* | |
C19 | 0.02510 (4) | 0.10780 (8) | 0.31550 (3) | 0.02000 (12)* | |
C20 | 0.09060 (4) | 0.10040 (9) | 0.43090 (3) | 0.02000 (12)* | |
C21 | 0.05650 (4) | −0.02340 (8) | 0.43750 (3) | 0.02000 (12)* | |
C22 | −0.03300 (4) | 0.18590 (7) | 0.32590 (3) | 0.02000 (15)* | |
C23 | 0.00200 (4) | −0.02740 (8) | 0.30630 (3) | 0.02000 (13)* | |
C24 | 0.05000 (4) | 0.20590 (8) | 0.44820 (3) | 0.02000 (14)* | |
C25 | 0.16170 (4) | 0.10310 (9) | 0.46460 (3) | 0.02000 (12)* | |
C26 | 0.04280 (4) | 0.15510 (9) | 0.26740 (3) | 0.02000 (12)* | |
H1 | 0.4103 (6) | 0.1461 (12) | 0.3955 (5) | 0.020 (3)* | |
H2 | 0.3848 (6) | −0.0437 (12) | 0.4255 (5) | 0.020 (3)* | |
H3 | 0.2754 (6) | −0.1155 (12) | 0.4116 (5) | 0.020 (3)* | |
H4 | 0.3157 (7) | 0.3100 (10) | 0.3001 (5) | 0.020 (3)* | |
H5 | 0.3688 (6) | 0.3430 (13) | 0.3496 (5) | 0.020 (3)* | |
H6 | 0.1507 (6) | −0.0722 (11) | 0.3761 (5) | 0.020 (3)* | |
H7 | 0.1441 (6) | −0.0290 (12) | 0.3203 (5) | 0.020 (3)* | |
H8 | 0.3662 (6) | 0.3476 (12) | 0.4366 (5) | 0.020 (3)* | |
H9 | 0.2968 (6) | 0.3493 (12) | 0.4531 (5) | 0.020 (3)* | |
H10 | 0.3566 (6) | 0.4341 (12) | 0.4809 (5) | 0.020 (3)* | |
H11 | 0.3556 (6) | 0.6492 (12) | 0.3816 (5) | 0.020 (3)* | |
H12 | 0.4011 (6) | 0.5301 (12) | 0.3888 (5) | 0.020 (3)* | |
H13 | 0.3970 (6) | 0.6133 (12) | 0.4351 (5) | 0.020 (3)* | |
H14 | 0.2511 (6) | 0.6567 (13) | 0.4122 (5) | 0.020 (3)* | |
H15 | 0.2914 (6) | 0.6219 (11) | 0.4665 (5) | 0.020 (3)* | |
H16 | 0.2273 (6) | 0.5444 (12) | 0.4409 (5) | 0.020 (3)* | |
H17 | 0.1523 (6) | 0.4553 (12) | 0.2670 (5) | 0.020 (3)* | |
H18 | 0.2135 (6) | 0.3894 (11) | 0.2514 (5) | 0.020 (3)* | |
H19 | 0.1860 (6) | 0.5162 (12) | 0.2264 (5) | 0.020 (3)* | |
H20 | 0.3268 (6) | 0.4945 (12) | 0.2718 (5) | 0.020 (3)* | |
H21 | 0.3356 (6) | 0.6212 (11) | 0.3012 (5) | 0.020 (3)* | |
H22 | 0.2905 (6) | 0.6150 (12) | 0.2466 (5) | 0.020 (3)* | |
H23 | 0.1747 (6) | 0.6284 (11) | 0.3315 (5) | 0.020 (3)* | |
H24 | 0.1836 (7) | 0.6952 (10) | 0.2822 (5) | 0.020 (3)* | |
H25 | 0.2389 (6) | 0.7107 (12) | 0.3321 (5) | 0.020 (3)* | |
H26 | 0.0108 (6) | −0.0224 (12) | 0.4182 (5) | 0.020 (3)* | |
H27 | 0.0564 (6) | −0.0353 (12) | 0.4724 (5) | 0.020 (3)* | |
H28 | 0.0809 (6) | −0.0904 (12) | 0.4262 (5) | 0.020 (3)* | |
H29 | −0.0482 (6) | 0.1515 (13) | 0.3540 (5) | 0.020 (3)* | |
H30 | −0.0697 (7) | 0.1855 (10) | 0.2968 (5) | 0.020 (3)* | |
H31 | −0.0180 (6) | 0.2700 (13) | 0.3334 (5) | 0.020 (3)* | |
H32 | −0.0112 (6) | −0.0594 (11) | 0.3356 (5) | 0.020 (3)* | |
H33 | 0.0384 (6) | −0.0768 (11) | 0.2994 (5) | 0.020 (3)* | |
H34 | −0.0359 (6) | −0.0312 (12) | 0.2780 (5) | 0.020 (3)* | |
H35 | 0.0052 (7) | 0.2076 (12) | 0.4273 (5) | 0.020 (3)* | |
H36 | 0.0720 (6) | 0.2841 (13) | 0.4456 (5) | 0.020 (3)* | |
H37 | 0.0475 (7) | 0.1919 (10) | 0.4825 (5) | 0.020 (3)* | |
H38 | 0.1883 (6) | 0.0372 (12) | 0.4550 (5) | 0.020 (3)* | |
H39 | 0.1589 (6) | 0.0918 (12) | 0.4990 (5) | 0.020 (3)* | |
H40 | 0.1826 (7) | 0.1818 (11) | 0.4610 (5) | 0.020 (3)* | |
H41 | 0.0794 (6) | 0.1069 (11) | 0.2603 (5) | 0.020 (3)* | |
H42 | 0.0559 (6) | 0.2410 (12) | 0.2714 (5) | 0.020 (3)* | |
H43 | 0.0040 (6) | 0.1471 (12) | 0.2400 (5) | 0.020 (3)* | |
Geometric parameters (Å, º) top
Pd1—O1 | 1.9838 (7) | C13—H10 | 0.961 (13) |
Pd1—O2 | 2.0579 (7) | C14—H11 | 0.956 (13) |
Pd1—P2 | 2.3526 (4) | C14—H12 | 0.957 (13) |
Pd1—P1 | 2.3577 (4) | C14—H13 | 0.955 (12) |
Pd1—C3 | 2.6169 (9) | C15—H14 | 0.959 (13) |
P1—C9 | 1.8581 (9) | C15—H15 | 0.961 (13) |
P1—C11 | 1.8589 (9) | C15—H16 | 0.961 (12) |
P1—C12 | 1.8811 (9) | C16—H17 | 0.958 (12) |
P2—C10 | 1.8568 (9) | C16—H18 | 0.959 (12) |
P2—C19 | 1.8635 (10) | C16—H19 | 0.958 (13) |
P2—C20 | 1.8720 (9) | C17—H20 | 0.960 (12) |
O1—C3 | 1.3524 (11) | C17—H21 | 0.959 (12) |
O2—C1 | 1.2158 (10) | C17—H22 | 0.959 (13) |
C1—O3 | 1.2270 (10) | C18—H23 | 0.960 (13) |
C1—C2 | 1.5336 (12) | C18—H24 | 0.960 (14) |
C2—F2 | 1.3220 (10) | C18—H25 | 0.960 (13) |
C2—F1 | 1.3343 (9) | C19—C26 | 1.5196 (12) |
C2—F3 | 1.3419 (11) | C19—C22 | 1.5202 (12) |
C3—C8 | 1.3891 (12) | C19—C23 | 1.5258 (12) |
C3—C4 | 1.3904 (12) | C20—C21 | 1.5241 (12) |
C4—C5 | 1.3910 (12) | C20—C25 | 1.5269 (11) |
C4—C9 | 1.4986 (12) | C20—C24 | 1.5318 (13) |
C5—C6 | 1.3744 (12) | C21—H26 | 0.958 (12) |
C5—H1 | 0.931 (12) | C21—H27 | 0.960 (12) |
C6—C7 | 1.3750 (11) | C21—H28 | 0.960 (12) |
C6—H2 | 0.930 (13) | C22—H29 | 0.959 (13) |
C7—C8 | 1.4053 (12) | C22—H30 | 0.959 (14) |
C7—H3 | 0.933 (12) | C22—H31 | 0.958 (13) |
C8—C10 | 1.5068 (11) | C23—H32 | 0.959 (12) |
C9—H4 | 0.971 (14) | C23—H33 | 0.959 (12) |
C9—H5 | 0.971 (12) | C23—H34 | 0.961 (12) |
C10—H6 | 0.970 (12) | C24—H35 | 0.959 (13) |
C10—H7 | 0.969 (12) | C24—H36 | 0.959 (13) |
C11—C13 | 1.4850 (12) | C24—H37 | 0.959 (14) |
C11—C15 | 1.5245 (12) | C25—H38 | 0.959 (12) |
C11—C14 | 1.5744 (11) | C25—H39 | 0.959 (13) |
C12—C17 | 1.5021 (12) | C25—H40 | 0.958 (12) |
C12—C18 | 1.5193 (12) | C26—H41 | 0.957 (12) |
C12—C16 | 1.5505 (12) | C26—H42 | 0.957 (13) |
C13—H8 | 0.960 (13) | C26—H43 | 0.960 (12) |
C13—H9 | 0.959 (13) | | |
| | | |
O1—Pd1—O2 | 176.64 (3) | C11—C13—H10 | 109.5 (8) |
O1—Pd1—P2 | 80.71 (3) | H8—C13—H10 | 109.3 (10) |
O2—Pd1—P2 | 100.71 (2) | H9—C13—H10 | 109.5 (10) |
O1—Pd1—P1 | 82.06 (3) | C11—C14—H11 | 109.5 (7) |
O2—Pd1—P1 | 97.35 (2) | C11—C14—H12 | 109.4 (8) |
P2—Pd1—P1 | 156.998 (8) | H11—C14—H12 | 109.3 (10) |
O1—Pd1—C3 | 30.41 (3) | C11—C14—H13 | 109.7 (8) |
O2—Pd1—C3 | 152.75 (3) | H11—C14—H13 | 109.4 (11) |
P2—Pd1—C3 | 78.87 (2) | H12—C14—H13 | 109.5 (10) |
P1—Pd1—C3 | 78.55 (2) | C11—C15—H14 | 109.5 (8) |
C9—P1—C11 | 104.20 (4) | C11—C15—H15 | 109.6 (7) |
C9—P1—C12 | 104.61 (4) | H14—C15—H15 | 109.5 (11) |
C11—P1—C12 | 113.26 (4) | C11—C15—H16 | 109.5 (8) |
C9—P1—Pd1 | 104.82 (3) | H14—C15—H16 | 109.4 (10) |
C11—P1—Pd1 | 116.81 (3) | H15—C15—H16 | 109.3 (11) |
C12—P1—Pd1 | 111.67 (3) | C12—C16—H17 | 109.6 (7) |
C10—P2—C19 | 103.27 (4) | C12—C16—H18 | 109.5 (7) |
C10—P2—C20 | 103.54 (4) | H17—C16—H18 | 109.4 (10) |
C19—P2—C20 | 113.90 (4) | C12—C16—H19 | 109.5 (7) |
C10—P2—Pd1 | 105.09 (3) | H17—C16—H19 | 109.4 (10) |
C19—P2—Pd1 | 115.51 (3) | H18—C16—H19 | 109.5 (11) |
C20—P2—Pd1 | 113.69 (3) | C12—C17—H20 | 109.4 (7) |
C3—O1—Pd1 | 101.65 (6) | C12—C17—H21 | 109.5 (8) |
C1—O2—Pd1 | 114.63 (6) | H20—C17—H21 | 109.5 (10) |
O2—C1—O3 | 130.16 (8) | C12—C17—H22 | 109.5 (7) |
O2—C1—C2 | 113.96 (7) | H20—C17—H22 | 109.5 (10) |
O3—C1—C2 | 115.81 (7) | H21—C17—H22 | 109.4 (11) |
F2—C2—F1 | 106.68 (7) | C12—C18—H23 | 109.5 (7) |
F2—C2—F3 | 105.81 (7) | C12—C18—H24 | 109.6 (8) |
F1—C2—F3 | 105.89 (6) | H23—C18—H24 | 109.4 (11) |
F2—C2—C1 | 111.23 (6) | C12—C18—H25 | 109.5 (8) |
F1—C2—C1 | 115.46 (7) | H23—C18—H25 | 109.5 (11) |
F3—C2—C1 | 111.17 (7) | H24—C18—H25 | 109.4 (10) |
O1—C3—C8 | 118.59 (7) | C26—C19—C22 | 108.46 (7) |
O1—C3—C4 | 118.43 (8) | C26—C19—C23 | 107.28 (7) |
C8—C3—C4 | 122.78 (7) | C22—C19—C23 | 109.36 (6) |
O1—C3—Pd1 | 47.94 (4) | C26—C19—P2 | 105.64 (5) |
C8—C3—Pd1 | 106.59 (6) | C22—C19—P2 | 111.16 (6) |
C4—C3—Pd1 | 107.35 (6) | C23—C19—P2 | 114.65 (6) |
C3—C4—C5 | 118.10 (8) | C21—C20—C25 | 109.69 (7) |
C3—C4—C9 | 115.69 (7) | C21—C20—C24 | 108.55 (7) |
C5—C4—C9 | 126.15 (8) | C25—C20—C24 | 107.44 (7) |
C6—C5—C4 | 119.51 (7) | C21—C20—P2 | 114.53 (6) |
C6—C5—H1 | 120.2 (8) | C25—C20—P2 | 105.00 (6) |
C4—C5—H1 | 120.3 (8) | C24—C20—P2 | 111.37 (6) |
C5—C6—C7 | 122.06 (7) | C20—C21—H26 | 109.5 (8) |
C5—C6—H2 | 118.9 (8) | C20—C21—H27 | 109.4 (8) |
C7—C6—H2 | 119.1 (8) | H26—C21—H27 | 109.4 (10) |
C6—C7—C8 | 119.79 (8) | C20—C21—H28 | 109.5 (8) |
C6—C7—H3 | 120.2 (7) | H26—C21—H28 | 109.6 (10) |
C8—C7—H3 | 120.0 (8) | H27—C21—H28 | 109.4 (11) |
C3—C8—C7 | 117.15 (7) | C19—C22—H29 | 109.6 (8) |
C3—C8—C10 | 115.96 (7) | C19—C22—H30 | 109.5 (8) |
C7—C8—C10 | 126.89 (8) | H29—C22—H30 | 109.3 (11) |
C4—C9—P1 | 113.04 (7) | C19—C22—H31 | 109.6 (7) |
C4—C9—H4 | 109.0 (7) | H29—C22—H31 | 109.5 (11) |
P1—C9—H4 | 109.0 (7) | H30—C22—H31 | 109.4 (10) |
C4—C9—H5 | 108.9 (8) | C19—C23—H32 | 109.5 (7) |
P1—C9—H5 | 109.0 (8) | C19—C23—H33 | 109.6 (7) |
H4—C9—H5 | 107.7 (11) | H32—C23—H33 | 109.5 (10) |
C8—C10—P2 | 114.10 (6) | C19—C23—H34 | 109.5 (8) |
C8—C10—H6 | 108.6 (7) | H32—C23—H34 | 109.4 (10) |
P2—C10—H6 | 108.6 (7) | H33—C23—H34 | 109.4 (11) |
C8—C10—H7 | 108.8 (7) | C20—C24—H35 | 109.4 (8) |
P2—C10—H7 | 108.8 (7) | C20—C24—H36 | 109.4 (8) |
H6—C10—H7 | 107.7 (10) | H35—C24—H36 | 109.5 (11) |
C13—C11—C15 | 108.85 (7) | C20—C24—H37 | 109.4 (7) |
C13—C11—C14 | 110.58 (6) | H35—C24—H37 | 109.6 (11) |
C15—C11—C14 | 106.47 (7) | H36—C24—H37 | 109.5 (10) |
C13—C11—P1 | 107.60 (6) | C20—C25—H38 | 109.5 (7) |
C15—C11—P1 | 111.38 (5) | C20—C25—H39 | 109.5 (7) |
C14—C11—P1 | 111.95 (6) | H38—C25—H39 | 109.4 (10) |
C17—C12—C18 | 114.29 (7) | C20—C25—H40 | 109.5 (8) |
C17—C12—C16 | 106.20 (7) | H38—C25—H40 | 109.4 (11) |
C18—C12—C16 | 107.56 (6) | H39—C25—H40 | 109.5 (11) |
C17—C12—P1 | 113.66 (6) | C19—C26—H41 | 109.6 (8) |
C18—C12—P1 | 109.92 (6) | C19—C26—H42 | 109.6 (7) |
C16—C12—P1 | 104.47 (6) | H41—C26—H42 | 109.5 (10) |
C11—C13—H8 | 109.5 (8) | C19—C26—H43 | 109.4 (8) |
C11—C13—H9 | 109.6 (7) | H41—C26—H43 | 109.4 (11) |
H8—C13—H9 | 109.5 (11) | H42—C26—H43 | 109.4 (11) |
(horbiz)
trans-2-(alpha-Cumyl)cyclohexyl
2-(1,2-bis(benzyloxy)ethyl)-5-(tri-isopropylsily
l)-2,3-dihydro-4
H-4-pyridone-1-carboxylate
top
Crystal data top
C47H63NO6Si | γ = 90° |
Mr = 766.07 | V = 8664 (2) Å3 |
I2/a | Z = 8 |
a = 33.990 (4) Å | F(000) = 3312 |
b = 9.5179 (13) Å | Dx = 1.175 Mg m−3 |
c = 29.467 (4) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.10 mm−1 |
β = 114.65 (3)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.020 |
Graphite monochromator | θmax = 45.1°, θmin = 1.3° |
41716 measured reflections | h = −55→55 |
13023 independent reflections | k = −10→10 |
11934 reflections with I > 2σ(I) | l = −45→45 |
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)] = 0.032 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.208 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.13 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
13023 reflections | (Δ/σ)max = 13.453 |
473 parameters | Δρmax = 1.14 e Å−3 |
0 restraints | Δρmin = −0.24 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. |
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 | Uiso*/Ueq | |
Si1 | 0.347800 (7) | 0.47870 (2) | −0.189600 (8) | 0.02000 (8)* | |
N1 | 0.36520 (2) | 0.36990 (7) | −0.04530 (2) | 0.02000 (13)* | |
O1 | 0.440800 (18) | 0.54280 (6) | −0.106700 (19) | 0.02000 (11)* | |
O2 | 0.394500 (19) | 0.10660 (6) | −0.03280 (2) | 0.02000 (11)* | |
O3 | 0.501900 (19) | 0.21040 (6) | −0.00240 (2) | 0.02000 (11)* | |
O4 | 0.517900 (19) | 0.05550 (6) | 0.07780 (2) | 0.02000 (11)* | |
O5 | 0.297600 (19) | 0.31790 (6) | −0.05030 (2) | 0.02000 (12)* | |
O6 | 0.357300 (19) | 0.29070 (6) | 0.02210 (2) | 0.02000 (11)* | |
C1 | 0.36400 (2) | 0.65510 (8) | −0.20590 (3) | 0.02000 (13)* | |
H1 | 0.3962 (5) | 0.6508 (13) | −0.1936 (5) | 0.020 (3)* | |
C2 | 0.35530 (2) | 0.77820 (8) | −0.17790 (2) | 0.02000 (13)* | |
H2 | 0.3648 (4) | 0.8659 (14) | −0.1877 (5) | 0.020 (3)* | |
H3 | 0.3714 (4) | 0.7640 (14) | −0.1419 (5) | 0.020 (3)* | |
H4 | 0.3243 (4) | 0.7835 (14) | −0.1863 (5) | 0.020 (3)* | |
C3 | 0.34710 (3) | 0.68620 (8) | −0.26120 (3) | 0.02000 (14)* | |
H5 | 0.3573 (4) | 0.7789 (14) | −0.2660 (5) | 0.020 (3)* | |
H6 | 0.3154 (4) | 0.6854 (14) | −0.2762 (5) | 0.020 (3)* | |
H7 | 0.3576 (4) | 0.6145 (14) | −0.2774 (5) | 0.020 (3)* | |
C4 | 0.28780 (2) | 0.45310 (8) | −0.21340 (3) | 0.02000 (13)* | |
H8 | 0.2835 (4) | 0.3619 (14) | −0.1991 (5) | 0.020 (3)* | |
C5 | 0.26370 (3) | 0.56530 (8) | −0.19690 (3) | 0.02000 (13)* | |
H9 | 0.2328 (4) | 0.5425 (15) | −0.2107 (5) | 0.020 (3)* | |
H10 | 0.2677 (4) | 0.6576 (14) | −0.2090 (5) | 0.020 (3)* | |
H11 | 0.2753 (4) | 0.5669 (14) | −0.1603 (5) | 0.020 (3)* | |
C6 | 0.26460 (2) | 0.43770 (8) | −0.27050 (3) | 0.02000 (12)* | |
H12 | 0.2336 (4) | 0.4236 (14) | −0.2804 (5) | 0.020 (3)* | |
H13 | 0.2765 (4) | 0.3567 (14) | −0.2811 (5) | 0.020 (3)* | |
H14 | 0.2691 (4) | 0.5231 (14) | −0.2864 (5) | 0.020 (3)* | |
C7 | 0.36920 (3) | 0.33680 (8) | −0.21800 (3) | 0.02000 (13)* | |
H15 | 0.3547 (4) | 0.3502 (14) | −0.2550 (5) | 0.020 (3)* | |
C8 | 0.41710 (2) | 0.34390 (8) | −0.20350 (3) | 0.02000 (13)* | |
H16 | 0.4256 (4) | 0.2677 (14) | −0.2200 (5) | 0.020 (3)* | |
H17 | 0.4327 (5) | 0.3340 (14) | −0.1672 (5) | 0.020 (3)* | |
H18 | 0.4243 (4) | 0.4345 (14) | −0.2139 (5) | 0.020 (3)* | |
C9 | 0.35740 (3) | 0.18820 (8) | −0.20750 (3) | 0.02000 (13)* | |
H19 | 0.3690 (4) | 0.1189 (14) | −0.2233 (5) | 0.020 (3)* | |
H20 | 0.3258 (5) | 0.1791 (14) | −0.2210 (5) | 0.020 (3)* | |
H21 | 0.3698 (4) | 0.1720 (14) | −0.1713 (5) | 0.020 (3)* | |
C10 | 0.37220 (2) | 0.45430 (8) | −0.11990 (3) | 0.02000 (13)* | |
C11 | 0.41720 (3) | 0.49120 (8) | −0.08880 (3) | 0.02000 (13)* | |
C12 | 0.43450 (3) | 0.47060 (8) | −0.03320 (3) | 0.02000 (14)* | |
H22 | 0.4308 (4) | 0.5591 (14) | −0.0177 (5) | 0.020 (3)* | |
H23 | 0.4658 (4) | 0.4500 (15) | −0.0198 (5) | 0.020 (3)* | |
C13 | 0.41190 (2) | 0.35250 (8) | −0.01880 (2) | 0.02000 (13)* | |
H24 | 0.4204 (4) | 0.3558 (14) | 0.0180 (5) | 0.020 (3)* | |
C14 | 0.34870 (2) | 0.40330 (8) | −0.09560 (3) | 0.02000 (14)* | |
H25 | 0.3186 (4) | 0.3896 (14) | −0.1148 (5) | 0.020 (3)* | |
C15 | 0.42540 (2) | 0.20720 (8) | −0.03280 (3) | 0.02000 (13)* | |
H26 | 0.4243 (4) | 0.2132 (14) | −0.0671 (5) | 0.020 (3)* | |
C16 | 0.47090 (3) | 0.17010 (8) | 0.00370 (3) | 0.02000 (13)* | |
C17 | 0.47420 (2) | 0.07980 (8) | 0.04740 (3) | 0.02000 (13)* | |
H27 | 0.4603 (4) | 0.1281 (14) | 0.0667 (5) | 0.020 (3)* | |
H28 | 0.4591 (4) | −0.0107 (14) | 0.0351 (5) | 0.020 (3)* | |
C18 | 0.52350 (3) | −0.03270 (8) | 0.11590 (3) | 0.02000 (13)* | |
H29 | 0.5535 (4) | −0.0687 (14) | 0.1297 (5) | 0.020 (3)* | |
H30 | 0.5038 (4) | −0.1139 (15) | 0.1027 (5) | 0.020 (3)* | |
C19 | 0.51480 (3) | 0.03570 (8) | 0.15870 (3) | 0.02000 (14)* | |
C20 | 0.53490 (3) | 0.13810 (7) | 0.18620 (3) | 0.02000 (13)* | |
H31 | 0.5552 (4) | 0.1880 (14) | 0.1778 (5) | 0.020 (3)* | |
C21 | 0.52900 (3) | 0.18000 (8) | 0.22620 (3) | 0.02000 (13)* | |
H32 | 0.5469 (4) | 0.2530 (15) | 0.2462 (5) | 0.020 (3)* | |
C22 | 0.50200 (3) | 0.12920 (8) | 0.23850 (3) | 0.02000 (13)* | |
H33 | 0.4972 (5) | 0.1678 (14) | 0.2654 (5) | 0.020 (3)* | |
C23 | 0.47900 (3) | 0.01670 (8) | 0.21290 (3) | 0.02000 (14)* | |
H34 | 0.4590 (5) | −0.0304 (14) | 0.2224 (5) | 0.020 (3)* | |
C24 | 0.48660 (3) | −0.02760 (7) | 0.17050 (3) | 0.02000 (13)* | |
H35 | 0.4707 (5) | −0.1047 (14) | 0.1509 (5) | 0.020 (3)* | |
C25 | 0.38910 (3) | −0.01040 (8) | −0.06610 (3) | 0.02000 (13)* | |
H36 | 0.4147 (4) | −0.0724 (14) | −0.0525 (5) | 0.020 (3)* | |
H37 | 0.3855 (4) | 0.0240 (13) | −0.0993 (5) | 0.020 (3)* | |
C26 | 0.35010 (3) | −0.08800 (8) | −0.07050 (3) | 0.02000 (13)* | |
C27 | 0.35380 (2) | −0.21340 (8) | −0.04670 (3) | 0.02000 (13)* | |
H38 | 0.3812 (4) | −0.2541 (14) | −0.0268 (5) | 0.020 (3)* | |
C28 | 0.31080 (2) | −0.28480 (8) | −0.05380 (3) | 0.02000 (13)* | |
H39 | 0.3086 (4) | −0.3714 (14) | −0.0392 (5) | 0.020 (3)* | |
C29 | 0.27370 (2) | −0.19830 (8) | −0.08690 (3) | 0.02000 (13)* | |
H40 | 0.2457 (4) | −0.2359 (14) | −0.0948 (5) | 0.020 (3)* | |
C30 | 0.27500 (3) | −0.08010 (8) | −0.10590 (3) | 0.02000 (13)* | |
H41 | 0.2492 (4) | −0.0303 (13) | −0.1253 (5) | 0.020 (3)* | |
C31 | 0.31090 (3) | −0.03180 (8) | −0.09860 (3) | 0.02000 (14)* | |
H42 | 0.3110 (4) | 0.0550 (15) | −0.1145 (5) | 0.020 (3)* | |
C32 | 0.33590 (3) | 0.32310 (8) | −0.02630 (3) | 0.02000 (14)* | |
C33 | 0.33260 (3) | 0.21700 (8) | 0.04540 (3) | 0.02000 (13)* | |
H43 | 0.3025 (4) | 0.2553 (14) | 0.0323 (5) | 0.020 (3)* | |
C34 | 0.33130 (2) | 0.06420 (8) | 0.03210 (3) | 0.02000 (13)* | |
H44 | 0.3613 (5) | 0.0297 (14) | 0.0421 (5) | 0.020 (3)* | |
H45 | 0.3157 (4) | 0.0532 (15) | −0.0046 (5) | 0.020 (3)* | |
C35 | 0.30900 (3) | −0.02490 (8) | 0.05770 (3) | 0.02000 (14)* | |
H46 | 0.2787 (4) | 0.0064 (14) | 0.0470 (5) | 0.020 (3)* | |
H47 | 0.3088 (4) | −0.1248 (14) | 0.0481 (5) | 0.020 (3)* | |
C36 | 0.33260 (2) | −0.00970 (8) | 0.11200 (3) | 0.02000 (13)* | |
H48 | 0.3628 (4) | −0.0428 (14) | 0.1226 (5) | 0.020 (3)* | |
H49 | 0.3187 (4) | −0.0679 (15) | 0.1290 (5) | 0.020 (3)* | |
C37 | 0.33260 (3) | 0.14280 (8) | 0.12650 (3) | 0.02000 (13)* | |
H50 | 0.3478 (5) | 0.1514 (14) | 0.1633 (5) | 0.020 (3)* | |
H51 | 0.3024 (5) | 0.1744 (14) | 0.1163 (5) | 0.020 (3)* | |
C38 | 0.35550 (3) | 0.24180 (8) | 0.10160 (3) | 0.02000 (13)* | |
H52 | 0.3855 (4) | 0.2041 (14) | 0.1122 (5) | 0.020 (3)* | |
C39 | 0.36080 (2) | 0.39670 (8) | 0.11800 (3) | 0.02000 (13)* | |
C40 | 0.31780 (3) | 0.47410 (7) | 0.09080 (3) | 0.02000 (14)* | |
H53 | 0.3095 (4) | 0.4706 (14) | 0.0547 (5) | 0.020 (3)* | |
H54 | 0.3212 (4) | 0.5724 (14) | 0.1018 (5) | 0.020 (3)* | |
H55 | 0.2954 (4) | 0.4292 (14) | 0.0985 (5) | 0.020 (3)* | |
C41 | 0.37470 (2) | 0.40660 (8) | 0.17560 (3) | 0.02000 (13)* | |
H56 | 0.3774 (5) | 0.5056 (14) | 0.1857 (5) | 0.020 (3)* | |
H57 | 0.4025 (4) | 0.3591 (14) | 0.1931 (5) | 0.020 (3)* | |
H58 | 0.3528 (5) | 0.3612 (14) | 0.1841 (5) | 0.020 (3)* | |
C42 | 0.39730 (3) | 0.46480 (8) | 0.10870 (3) | 0.02000 (14)* | |
C43 | 0.39200 (2) | 0.59350 (8) | 0.08540 (3) | 0.02000 (13)* | |
H59 | 0.3648 (4) | 0.6403 (14) | 0.0737 (5) | 0.020 (3)* | |
C44 | 0.42890 (2) | 0.65870 (8) | 0.07870 (3) | 0.02000 (13)* | |
H60 | 0.4257 (4) | 0.7465 (15) | 0.0622 (5) | 0.020 (3)* | |
C45 | 0.46690 (2) | 0.59010 (8) | 0.09670 (3) | 0.02000 (13)* | |
H61 | 0.4909 (4) | 0.6305 (14) | 0.0930 (5) | 0.020 (3)* | |
C46 | 0.47160 (3) | 0.46680 (8) | 0.11950 (3) | 0.02000 (14)* | |
H62 | 0.4985 (4) | 0.4190 (14) | 0.1313 (5) | 0.020 (3)* | |
C47 | 0.43780 (3) | 0.41010 (8) | 0.12580 (3) | 0.02000 (13)* | |
H63 | 0.4429 (5) | 0.3244 (14) | 0.1439 (5) | 0.020 (3)* | |
Geometric parameters (Å, º) top
Si1—C4 | 1.8754 (9) | C19—C24 | 1.2964 (11) |
Si1—C10 | 1.8813 (9) | C20—C21 | 1.3363 (11) |
Si1—C7 | 1.8871 (8) | C20—H31 | 0.952 (13) |
Si1—C1 | 1.8903 (8) | C21—C22 | 1.2185 (12) |
N1—C14 | 1.3853 (10) | C21—H32 | 0.949 (14) |
N1—C32 | 1.4031 (10) | C22—C23 | 1.3546 (11) |
N1—C13 | 1.4570 (10) | C22—H33 | 0.948 (13) |
O1—C11 | 1.2312 (10) | C23—C24 | 1.4404 (11) |
O2—C15 | 1.4212 (10) | C23—H34 | 0.949 (14) |
O2—C25 | 1.4444 (10) | C24—H35 | 0.951 (14) |
O3—C16 | 1.2032 (10) | C25—C26 | 1.4752 (11) |
O4—C18 | 1.3502 (9) | C25—H36 | 0.987 (14) |
O4—C17 | 1.3973 (10) | C25—H37 | 0.990 (13) |
O5—C32 | 1.1956 (11) | C26—C31 | 1.3516 (11) |
O6—C32 | 1.3390 (10) | C26—C27 | 1.3633 (11) |
O6—C33 | 1.4660 (10) | C27—C28 | 1.5449 (11) |
C1—C3 | 1.5140 (11) | C27—H38 | 0.952 (13) |
C1—C2 | 1.5312 (11) | C28—C29 | 1.4810 (11) |
C1—H1 | 1.000 (14) | C28—H39 | 0.947 (13) |
C2—H2 | 0.981 (14) | C29—C30 | 1.2656 (10) |
C2—H3 | 0.979 (13) | C29—H40 | 0.950 (14) |
C2—H4 | 0.978 (13) | C30—C31 | 1.2360 (11) |
C3—H5 | 0.980 (13) | C30—H41 | 0.950 (14) |
C3—H6 | 0.979 (13) | C31—H42 | 0.950 (13) |
C3—H7 | 0.981 (14) | C33—C34 | 1.5021 (11) |
C4—C6 | 1.5387 (11) | C33—C38 | 1.5260 (11) |
C4—C5 | 1.5427 (11) | C33—H43 | 1.000 (13) |
C4—H8 | 1.002 (13) | C34—C35 | 1.5296 (11) |
C5—H9 | 0.979 (13) | C34—H44 | 0.992 (14) |
C5—H10 | 0.979 (13) | C34—H45 | 0.992 (13) |
C5—H11 | 0.982 (13) | C35—C36 | 1.4676 (11) |
C6—H12 | 0.978 (13) | C35—H46 | 0.989 (13) |
C6—H13 | 0.980 (13) | C35—H47 | 0.991 (14) |
C6—H14 | 0.982 (13) | C36—C37 | 1.5131 (10) |
C7—C8 | 1.5025 (11) | C36—H48 | 0.991 (13) |
C7—C9 | 1.5364 (11) | C36—H49 | 0.989 (13) |
C7—H15 | 1.000 (14) | C37—C38 | 1.5838 (11) |
C8—H16 | 0.981 (13) | C37—H50 | 0.991 (13) |
C8—H17 | 0.980 (14) | C37—H51 | 0.988 (14) |
C8—H18 | 0.980 (13) | C38—C39 | 1.5385 (11) |
C9—H19 | 0.980 (13) | C38—H52 | 1.000 (13) |
C9—H20 | 0.981 (14) | C39—C42 | 1.5225 (11) |
C9—H21 | 0.982 (13) | C39—C40 | 1.5310 (12) |
C10—C14 | 1.3651 (11) | C39—C41 | 1.5633 (11) |
C10—C11 | 1.4606 (11) | C40—H53 | 0.981 (13) |
C11—C12 | 1.5049 (10) | C40—H54 | 0.981 (13) |
C12—C13 | 1.5184 (11) | C40—H55 | 0.979 (13) |
C12—H22 | 0.991 (13) | C41—H56 | 0.981 (13) |
C12—H23 | 0.988 (13) | C41—H57 | 0.978 (14) |
C13—C15 | 1.5656 (11) | C41—H58 | 0.979 (13) |
C13—H24 | 1.000 (13) | C42—C47 | 1.3570 (11) |
C14—H25 | 0.949 (14) | C42—C43 | 1.3788 (11) |
C15—C16 | 1.5119 (12) | C43—C44 | 1.4845 (11) |
C15—H26 | 0.997 (13) | C43—H59 | 0.952 (14) |
C16—C17 | 1.5129 (10) | C44—C45 | 1.3433 (11) |
C17—H27 | 0.991 (13) | C44—H60 | 0.950 (14) |
C17—H28 | 0.991 (13) | C45—C46 | 1.3284 (10) |
C18—C19 | 1.5534 (11) | C45—H61 | 0.948 (13) |
C18—H29 | 0.988 (13) | C46—C47 | 1.3504 (12) |
C18—H30 | 0.990 (14) | C46—H62 | 0.948 (13) |
C19—C20 | 1.2695 (10) | C47—H63 | 0.950 (13) |
| | | |
C4—Si1—C10 | 107.92 (4) | C21—C20—H31 | 118.2 (8) |
C4—Si1—C7 | 107.54 (4) | C22—C21—C20 | 123.55 (7) |
C10—Si1—C7 | 108.65 (4) | C22—C21—H32 | 118.2 (8) |
C4—Si1—C1 | 114.01 (4) | C20—C21—H32 | 118.2 (8) |
C10—Si1—C1 | 110.15 (4) | C21—C22—C23 | 118.64 (7) |
C7—Si1—C1 | 108.42 (4) | C21—C22—H33 | 120.6 (8) |
C14—N1—C32 | 117.50 (7) | C23—C22—H33 | 120.8 (8) |
C14—N1—C13 | 117.64 (6) | C22—C23—C24 | 116.35 (7) |
C32—N1—C13 | 123.09 (6) | C22—C23—H34 | 121.8 (8) |
C15—O2—C25 | 113.82 (6) | C24—C23—H34 | 121.8 (8) |
C18—O4—C17 | 112.30 (6) | C19—C24—C23 | 121.11 (7) |
C32—O6—C33 | 116.50 (6) | C19—C24—H35 | 119.5 (8) |
C3—C1—C2 | 111.01 (6) | C23—C24—H35 | 119.4 (8) |
C3—C1—Si1 | 115.29 (5) | O2—C25—C26 | 107.50 (6) |
C2—C1—Si1 | 113.61 (5) | O2—C25—H36 | 110.1 (8) |
C3—C1—H1 | 105.3 (7) | C26—C25—H36 | 110.1 (8) |
C2—C1—H1 | 105.3 (7) | O2—C25—H37 | 110.2 (8) |
Si1—C1—H1 | 105.2 (7) | C26—C25—H37 | 110.0 (8) |
C1—C2—H2 | 109.3 (8) | H36—C25—H37 | 108.9 (11) |
C1—C2—H3 | 109.4 (8) | C31—C26—C27 | 121.16 (7) |
H2—C2—H3 | 109.4 (11) | C31—C26—C25 | 118.41 (7) |
C1—C2—H4 | 109.4 (8) | C27—C26—C25 | 120.42 (7) |
H2—C2—H4 | 109.5 (11) | C26—C27—C28 | 115.87 (7) |
H3—C2—H4 | 109.7 (10) | C26—C27—H38 | 122.0 (8) |
C1—C3—H5 | 109.5 (8) | C28—C27—H38 | 122.1 (8) |
C1—C3—H6 | 109.7 (8) | C29—C28—C27 | 110.01 (7) |
H5—C3—H6 | 109.3 (11) | C29—C28—H39 | 125.2 (8) |
C1—C3—H7 | 109.6 (8) | C27—C28—H39 | 124.8 (8) |
H5—C3—H7 | 109.5 (11) | C30—C29—C28 | 127.46 (7) |
H6—C3—H7 | 109.3 (11) | C30—C29—H40 | 116.3 (8) |
C6—C4—C5 | 108.25 (6) | C28—C29—H40 | 116.3 (8) |
C6—C4—Si1 | 113.75 (6) | C31—C30—C29 | 117.89 (8) |
C5—C4—Si1 | 115.45 (5) | C31—C30—H41 | 121.0 (8) |
C6—C4—H8 | 106.2 (8) | C29—C30—H41 | 121.1 (8) |
C5—C4—H8 | 106.1 (7) | C30—C31—C26 | 127.51 (8) |
Si1—C4—H8 | 106.4 (8) | C30—C31—H42 | 116.3 (8) |
C4—C5—H9 | 109.5 (8) | C26—C31—H42 | 116.1 (8) |
C4—C5—H10 | 109.5 (8) | O5—C32—O6 | 126.46 (8) |
H9—C5—H10 | 109.6 (11) | O5—C32—N1 | 123.78 (7) |
C4—C5—H11 | 109.5 (8) | O6—C32—N1 | 109.72 (7) |
H9—C5—H11 | 109.2 (10) | O6—C33—C34 | 107.54 (6) |
H10—C5—H11 | 109.5 (11) | O6—C33—C38 | 107.56 (6) |
C4—C6—H12 | 109.6 (8) | C34—C33—C38 | 112.28 (6) |
C4—C6—H13 | 109.4 (8) | O6—C33—H43 | 109.8 (7) |
H12—C6—H13 | 109.5 (12) | C34—C33—H43 | 109.8 (8) |
C4—C6—H14 | 109.4 (8) | C38—C33—H43 | 109.8 (8) |
H12—C6—H14 | 109.5 (11) | C33—C34—C35 | 112.01 (6) |
H13—C6—H14 | 109.4 (11) | C33—C34—H44 | 109.2 (8) |
C8—C7—C9 | 109.09 (6) | C35—C34—H44 | 109.2 (8) |
C8—C7—Si1 | 114.46 (5) | C33—C34—H45 | 109.3 (8) |
C9—C7—Si1 | 112.85 (6) | C35—C34—H45 | 109.3 (8) |
C8—C7—H15 | 106.7 (8) | H44—C34—H45 | 107.8 (10) |
C9—C7—H15 | 106.6 (8) | C36—C35—C34 | 108.97 (7) |
Si1—C7—H15 | 106.6 (8) | C36—C35—H46 | 109.9 (7) |
C7—C8—H16 | 109.5 (8) | C34—C35—H46 | 109.9 (8) |
C7—C8—H17 | 109.6 (8) | C36—C35—H47 | 110.0 (8) |
H16—C8—H17 | 109.4 (11) | C34—C35—H47 | 109.7 (8) |
C7—C8—H18 | 109.5 (8) | H46—C35—H47 | 108.4 (11) |
H16—C8—H18 | 109.4 (11) | C35—C36—C37 | 109.76 (6) |
H17—C8—H18 | 109.5 (11) | C35—C36—H48 | 109.6 (8) |
C7—C9—H19 | 109.5 (8) | C37—C36—H48 | 109.7 (8) |
C7—C9—H20 | 109.5 (7) | C35—C36—H49 | 109.7 (8) |
H19—C9—H20 | 109.7 (11) | C37—C36—H49 | 109.8 (8) |
C7—C9—H21 | 109.5 (8) | H48—C36—H49 | 108.2 (11) |
H19—C9—H21 | 109.6 (11) | C36—C37—C38 | 112.46 (6) |
H20—C9—H21 | 109.1 (10) | C36—C37—H50 | 109.1 (8) |
C14—C10—C11 | 116.43 (6) | C38—C37—H50 | 109.0 (8) |
C14—C10—Si1 | 121.91 (6) | C36—C37—H51 | 109.2 (8) |
C11—C10—Si1 | 121.65 (6) | C38—C37—H51 | 109.1 (8) |
O1—C11—C10 | 121.74 (7) | H50—C37—H51 | 108.0 (11) |
O1—C11—C12 | 119.33 (7) | C33—C38—C39 | 115.40 (6) |
C10—C11—C12 | 118.89 (7) | C33—C38—C37 | 106.49 (6) |
C11—C12—C13 | 112.78 (6) | C39—C38—C37 | 116.13 (6) |
C11—C12—H22 | 108.9 (8) | C33—C38—H52 | 106.0 (8) |
C13—C12—H22 | 108.9 (8) | C39—C38—H52 | 106.0 (8) |
C11—C12—H23 | 109.1 (8) | C37—C38—H52 | 106.0 (8) |
C13—C12—H23 | 109.1 (8) | C42—C39—C40 | 111.87 (6) |
H22—C12—H23 | 107.9 (11) | C42—C39—C38 | 110.42 (6) |
N1—C13—C12 | 109.34 (6) | C40—C39—C38 | 109.60 (6) |
N1—C13—C15 | 109.43 (6) | C42—C39—C41 | 105.65 (6) |
C12—C13—C15 | 110.01 (6) | C40—C39—C41 | 109.24 (6) |
N1—C13—H24 | 109.6 (8) | C38—C39—C41 | 109.97 (6) |
C12—C13—H24 | 109.2 (7) | C39—C40—H53 | 109.4 (8) |
C15—C13—H24 | 109.3 (8) | C39—C40—H54 | 109.3 (8) |
C10—C14—N1 | 125.34 (7) | H53—C40—H54 | 109.4 (11) |
C10—C14—H25 | 117.2 (8) | C39—C40—H55 | 109.5 (8) |
N1—C14—H25 | 117.4 (8) | H53—C40—H55 | 109.7 (11) |
O2—C15—C16 | 112.29 (6) | H54—C40—H55 | 109.6 (11) |
O2—C15—C13 | 107.30 (6) | C39—C41—H56 | 109.6 (8) |
C16—C15—C13 | 110.13 (6) | C39—C41—H57 | 109.4 (8) |
O2—C15—H26 | 108.9 (8) | H56—C41—H57 | 109.7 (11) |
C16—C15—H26 | 109.2 (8) | C39—C41—H58 | 109.5 (8) |
C13—C15—H26 | 109.0 (8) | H56—C41—H58 | 109.3 (11) |
O3—C16—C15 | 121.26 (7) | H57—C41—H58 | 109.4 (12) |
O3—C16—C17 | 123.34 (7) | C47—C42—C43 | 115.30 (8) |
C15—C16—C17 | 115.40 (6) | C47—C42—C39 | 123.12 (7) |
O4—C17—C16 | 108.74 (6) | C43—C42—C39 | 121.39 (7) |
O4—C17—H27 | 110.0 (8) | C42—C43—C44 | 119.70 (7) |
C16—C17—H27 | 109.9 (8) | C42—C43—H59 | 120.1 (8) |
O4—C17—H28 | 109.9 (8) | C44—C43—H59 | 120.2 (8) |
C16—C17—H28 | 109.8 (8) | C45—C44—C43 | 118.09 (7) |
H27—C17—H28 | 108.4 (11) | C45—C44—H60 | 121.0 (8) |
O4—C18—C19 | 113.95 (6) | C43—C44—H60 | 120.9 (7) |
O4—C18—H29 | 108.7 (8) | C46—C45—C44 | 121.47 (8) |
C19—C18—H29 | 108.9 (8) | C46—C45—H61 | 119.2 (8) |
O4—C18—H30 | 108.7 (7) | C44—C45—H61 | 119.3 (8) |
C19—C18—H30 | 108.6 (8) | C45—C46—C47 | 119.53 (8) |
H29—C18—H30 | 107.7 (11) | C45—C46—H62 | 120.2 (8) |
C20—C19—C24 | 116.54 (7) | C47—C46—H62 | 120.2 (8) |
C20—C19—C18 | 127.30 (7) | C46—C47—C42 | 125.81 (7) |
C24—C19—C18 | 115.81 (7) | C46—C47—H63 | 117.0 (8) |
C19—C20—C21 | 123.60 (8) | C42—C47—H63 | 117.2 (8) |
C19—C20—H31 | 118.2 (8) | | |
(pejvab) bis(mu!2$-Ethane-1,2-dithiolato-
S,
S,
S',
S')-bis(ethene-1,2-dithiolato)- -technetium(iv)
top
Crystal data top
C8H12S8Tc2 | γ = 90° |
Mr = 560.66 | V = 844.2 (8) Å3 |
I2/m | Z = 2 |
a = 11.361 (6) Å | F(000) = 548 |
b = 8.303 (5) Å | Dx = 2.206 Mg m−3 |
c = 8.987 (5) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 2.61 mm−1 |
β = 95.25 (5)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.016 |
Graphite monochromator | θmax = 68.7°, θmin = 2.8° |
6858 measured reflections | h = −27→27 |
2519 independent reflections | k = −9→9 |
2178 reflections with I > 2σ(I) | l = −18→18 |
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)] = 0.010 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.065 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.42 | w = 1/[σ2(Fo2) + (0.P)2 + 0.0178P] where P = (Fo2 + 2Fc2)/3 |
2519 reflections | (Δ/σ)max = 2.510 |
38 parameters | Δρmax = 0.87 e Å−3 |
0 restraints | Δρmin = −1.25 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. |
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 | Uiso*/Ueq | |
Tc1 | 0.401300 (6) | 0.0000 | 0.063600 (7) | 0.02000 (4)* | |
S1 | 0.436700 (15) | 0.17480 (3) | −0.138900 (19) | 0.02000 (4)* | |
S3 | 0.20160 (2) | 0.0000 | −0.00570 (3) | 0.02000 (5)* | |
S4 | 0.34530 (2) | 0.0000 | 0.30230 (3) | 0.02000 (5)* | |
C1 | 0.36160 (7) | 0.08990 (10) | −0.31090 (8) | 0.02000 (10)* | |
C3 | 0.12240 (9) | 0.0000 | 0.16090 (10) | 0.02000 (12)* | |
C4 | 0.18580 (9) | 0.0000 | 0.30030 (11) | 0.02000 (12)* | |
H1 | 0.4060 (14) | 0.131 (2) | −0.4050 (19) | 0.020 (3)* | |
H2 | 0.2713 (13) | 0.132 (2) | −0.3223 (17) | 0.020 (3)* | |
H5 | 0.0275 (19) | 0.0000 | 0.152 (3) | 0.020 (5)* | |
H6 | 0.142 (2) | 0.0000 | 0.400 (3) | 0.020 (5)* | |
Geometric parameters (Å, º) top
Tc1—S4 | 2.2927 (13) | S3—C3 | 1.8160 (14) |
Tc1—S3 | 2.2971 (13) | S4—C4 | 1.8105 (14) |
Tc1—S1i | 2.3904 (10) | C1—C1i | 1.4929 (19) |
Tc1—S1 | 2.3904 (10) | C1—H1 | 1.080 (16) |
Tc1—S1ii | 2.3925 (10) | C1—H2 | 1.079 (15) |
Tc1—S1iii | 2.3925 (10) | C3—C4 | 1.3868 (17) |
Tc1—Tc1iii | 2.6087 (14) | C3—H5 | 1.07 (2) |
S1—C1 | 1.8366 (12) | C4—H6 | 1.06 (2) |
S1—Tc1iii | 2.3925 (10) | | |
| | | |
S4—Tc1—S3 | 84.37 (5) | S1ii—Tc1—Tc1iii | 56.91 (3) |
S4—Tc1—S1i | 142.44 (2) | S1iii—Tc1—Tc1iii | 56.91 (3) |
S3—Tc1—S1i | 91.40 (4) | C1—S1—Tc1 | 108.07 (5) |
S4—Tc1—S1 | 142.44 (2) | C1—S1—Tc1iii | 106.94 (5) |
S3—Tc1—S1 | 91.40 (4) | Tc1—S1—Tc1iii | 66.11 (4) |
S1i—Tc1—S1 | 74.77 (5) | C3—S3—Tc1 | 109.15 (6) |
S4—Tc1—S1ii | 90.43 (4) | C4—S4—Tc1 | 110.73 (6) |
S3—Tc1—S1ii | 142.36 (2) | C1i—C1—S1 | 112.57 (3) |
S1i—Tc1—S1ii | 113.89 (4) | C1i—C1—H1 | 108.6 (9) |
S1—Tc1—S1ii | 70.63 (4) | S1—C1—H1 | 108.8 (9) |
S4—Tc1—S1iii | 90.43 (4) | C1i—C1—H2 | 108.8 (9) |
S3—Tc1—S1iii | 142.36 (2) | S1—C1—H2 | 108.7 (8) |
S1i—Tc1—S1iii | 70.63 (4) | H1—C1—H2 | 109.3 (12) |
S1—Tc1—S1iii | 113.89 (4) | C4—C3—S3 | 119.29 (9) |
S1ii—Tc1—S1iii | 74.69 (5) | C4—C3—H5 | 120.4 (12) |
S4—Tc1—Tc1iii | 137.16 (3) | S3—C3—H5 | 120.3 (12) |
S3—Tc1—Tc1iii | 138.46 (3) | C3—C4—S4 | 116.46 (9) |
S1i—Tc1—Tc1iii | 56.98 (3) | C3—C4—H6 | 121.5 (12) |
S1—Tc1—Tc1iii | 56.98 (3) | S4—C4—H6 | 122.1 (12) |
Symmetry codes: (i) x, −y, z; (ii) −x+1, y, −z; (iii) −x+1, −y, −z. |
(sixfio) (eta$3!-Allyl)-(
N,
N'-dimethyl-2-(diphenylphosphanyl)aniline-N,
P)-palladium(ii) hexafluorophosphate
top
Crystal data top
C23H25F6NP2Pd | γ = 90° |
Mr = 597.78 | V = 2425.1 (17) Å3 |
Ia | Z = 4 |
a = 15.197 (6) Å | F(000) = 1200 |
b = 9.042 (3) Å | Dx = 1.637 Mg m−3 |
c = 18.559 (9) Å | Mo Kα radiation, λ = 0.71070 Å |
α = 90° | µ = 0.96 mm−1 |
β = 108.02 (4)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.013 |
Graphite monochromator | θmax = 44.9°, θmin = 2.3° |
9712 measured reflections | h = −22→22 |
6772 independent reflections | k = −9→9 |
6443 reflections with I > 2σ(I) | l = −31→31 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.009 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.032 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.16 | (Δ/σ)max = 0.783 |
6772 reflections | Δρmax = 0.18 e Å−3 |
233 parameters | Δρmin = −0.19 e Å−3 |
2 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.004 (6) |
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 | x | y | z | Uiso*/Ueq | |
Pd1 | 0.136600 (4) | 0.277800 (6) | 0.071000 (4) | 0.02000 (2)* | |
P1 | 0.286000 (16) | 0.33420 (2) | 0.131900 (14) | 0.02000 (4)* | |
N1 | 0.13570 (5) | 0.18680 (10) | 0.17890 (4) | 0.02000 (11)* | |
C1 | 0.30530 (7) | 0.22880 (9) | 0.22060 (6) | 0.02000 (17)* | |
C2 | 0.39300 (7) | 0.20910 (9) | 0.27130 (6) | 0.02000 (16)* | |
H1 | 0.4442 (11) | 0.2513 (16) | 0.2619 (9) | 0.020 (3)* | |
C3 | 0.40390 (6) | 0.12530 (10) | 0.33660 (5) | 0.02000 (13)* | |
H2 | 0.4625 (9) | 0.1100 (15) | 0.3708 (7) | 0.020 (3)* | |
C4 | 0.32860 (6) | 0.06680 (10) | 0.34950 (5) | 0.02000 (13)* | |
H3 | 0.3360 (9) | 0.0136 (15) | 0.3939 (7) | 0.020 (3)* | |
C5 | 0.24160 (6) | 0.08290 (10) | 0.29960 (5) | 0.02000 (13)* | |
H4 | 0.1908 (9) | 0.0399 (15) | 0.3094 (8) | 0.020 (3)* | |
C6 | 0.23010 (6) | 0.16590 (9) | 0.23270 (5) | 0.02000 (15)* | |
C7 | 0.08630 (6) | 0.04110 (9) | 0.16260 (5) | 0.02000 (14)* | |
H5 | 0.0254 (9) | 0.0556 (15) | 0.1278 (8) | 0.020 (3)* | |
H6 | 0.0816 (9) | −0.0003 (16) | 0.2090 (8) | 0.020 (3)* | |
H7 | 0.1202 (9) | −0.0253 (15) | 0.1407 (7) | 0.020 (3)* | |
C8 | 0.08270 (7) | 0.29020 (9) | 0.21360 (6) | 0.02000 (16)* | |
H8 | 0.0216 (10) | 0.3045 (16) | 0.1791 (8) | 0.020 (3)* | |
H9 | 0.1142 (9) | 0.3835 (16) | 0.2239 (8) | 0.020 (3)* | |
H10 | 0.0786 (11) | 0.2485 (16) | 0.2600 (9) | 0.020 (3)* | |
C9 | −0.01070 (7) | 0.27000 (9) | −0.00150 (6) | 0.02000 (17)* | |
H11 | −0.0438 (10) | 0.1782 (16) | −0.0015 (8) | 0.020 (3)* | |
H12 | −0.0477 (10) | 0.3578 (16) | −0.0023 (8) | 0.020 (3)* | |
C10 | 0.04710 (7) | 0.27330 (8) | −0.04370 (6) | 0.02000 (17)* | |
H13 | 0.0358 (11) | 0.2043 (16) | −0.0827 (9) | 0.020 (3)* | |
C11 | 0.11920 (6) | 0.36460 (11) | −0.03620 (5) | 0.02000 (13)* | |
H14 | 0.1047 (9) | 0.4692 (15) | −0.0424 (7) | 0.020 (3)* | |
H15 | 0.1639 (10) | 0.3335 (15) | −0.0607 (8) | 0.020 (3)* | |
C12 | 0.37580 (7) | 0.28290 (8) | 0.09130 (6) | 0.02000 (17)* | |
C13 | 0.35470 (6) | 0.18820 (12) | 0.02930 (5) | 0.02000 (12)* | |
H31 | 0.2942 (10) | 0.1451 (15) | 0.0104 (8) | 0.020 (3)* | |
C14 | 0.42180 (6) | 0.15360 (9) | −0.00470 (5) | 0.02000 (15)* | |
H32 | 0.4076 (9) | 0.0873 (16) | −0.0472 (8) | 0.020 (3)* | |
C15 | 0.51000 (7) | 0.21400 (9) | 0.02340 (6) | 0.02000 (17)* | |
H33 | 0.5563 (10) | 0.1906 (17) | −0.0003 (8) | 0.020 (3)* | |
C16 | 0.53110 (6) | 0.30870 (11) | 0.08530 (5) | 0.02000 (12)* | |
H34 | 0.5917 (9) | 0.3517 (15) | 0.1041 (8) | 0.020 (3)* | |
C17 | 0.46400 (6) | 0.34320 (9) | 0.11930 (5) | 0.02000 (15)* | |
H35 | 0.4783 (9) | 0.4095 (15) | 0.1617 (8) | 0.020 (3)* | |
C18 | 0.30760 (6) | 0.52580 (10) | 0.15740 (5) | 0.02000 (13)* | |
C19 | 0.29680 (6) | 0.62700 (10) | 0.09890 (5) | 0.02000 (13)* | |
H36 | 0.2787 (9) | 0.5931 (16) | 0.0474 (8) | 0.020 (3)* | |
C20 | 0.31250 (7) | 0.77660 (9) | 0.11520 (6) | 0.02000 (17)* | |
H37 | 0.3056 (9) | 0.8460 (15) | 0.0747 (8) | 0.020 (3)* | |
C21 | 0.33920 (6) | 0.82500 (10) | 0.18990 (5) | 0.02000 (14)* | |
H38 | 0.3505 (9) | 0.9282 (16) | 0.2010 (8) | 0.020 (3)* | |
C22 | 0.35010 (7) | 0.72370 (8) | 0.24840 (6) | 0.02000 (18)* | |
H39 | 0.3685 (11) | 0.7576 (16) | 0.3000 (9) | 0.020 (3)* | |
C23 | 0.33440 (6) | 0.57430 (10) | 0.23220 (5) | 0.02000 (13)* | |
H40 | 0.3416 (9) | 0.5048 (15) | 0.2728 (7) | 0.020 (3)* | |
P2 | 0.170000 (15) | 0.63070 (3) | 0.375400 (13) | 0.02000 (4)* | |
F1 | 0.15630 (3) | 0.68450 (7) | 0.29300 (3) | 0.02000 (8)* | |
F2 | 0.18200 (3) | 0.57270 (6) | 0.45920 (3) | 0.02000 (9)* | |
F3 | 0.27140 (4) | 0.69320 (7) | 0.40210 (3) | 0.02000 (9)* | |
F4 | 0.13170 (4) | 0.78090 (5) | 0.39450 (4) | 0.02000 (12)* | |
F5 | 0.20920 (3) | 0.47680 (6) | 0.35770 (3) | 0.02000 (9)* | |
F6 | 0.06910 (4) | 0.56400 (6) | 0.34930 (3) | 0.02000 (9)* | |
Geometric parameters (Å, º) top
Pd1—C11 | 2.0781 (13) | C10—H13 | 0.930 (15) |
Pd1—C10 | 2.1428 (16) | C11—H14 | 0.970 (14) |
Pd1—N1 | 2.1689 (12) | C11—H15 | 0.969 (14) |
Pd1—C9 | 2.2278 (15) | C12—C13 | 1.3899 (15) |
Pd1—P1 | 2.2594 (11) | C12—C17 | 1.3903 (14) |
P1—C18 | 1.7992 (11) | C13—C14 | 1.3907 (15) |
P1—C12 | 1.8115 (13) | C13—H31 | 0.960 (14) |
P1—C1 | 1.8454 (12) | C14—C15 | 1.3908 (14) |
N1—C6 | 1.4848 (13) | C14—H32 | 0.961 (14) |
N1—C7 | 1.5001 (13) | C15—C16 | 1.3885 (14) |
N1—C8 | 1.5028 (13) | C15—H33 | 0.962 (15) |
C1—C6 | 1.3560 (14) | C16—C17 | 1.3905 (15) |
C1—C2 | 1.3847 (15) | C16—H34 | 0.960 (14) |
C2—C3 | 1.3950 (14) | C17—H35 | 0.959 (13) |
C2—H1 | 0.930 (16) | C18—C19 | 1.3902 (13) |
C3—C4 | 1.3476 (13) | C18—C23 | 1.3912 (14) |
C3—H2 | 0.930 (12) | C19—C20 | 1.3905 (13) |
C4—C5 | 1.3672 (13) | C19—H36 | 0.959 (14) |
C4—H3 | 0.930 (13) | C20—C21 | 1.3893 (15) |
C5—C6 | 1.4146 (14) | C20—H37 | 0.960 (14) |
C5—H4 | 0.931 (13) | C21—C22 | 1.3906 (14) |
C7—H5 | 0.960 (13) | C21—H38 | 0.960 (14) |
C7—H6 | 0.962 (14) | C22—C23 | 1.3885 (13) |
C7—H7 | 0.959 (13) | C22—H39 | 0.961 (16) |
C8—H8 | 0.960 (14) | C23—H40 | 0.961 (13) |
C8—H9 | 0.960 (14) | P2—F1 | 1.5562 (9) |
C8—H10 | 0.960 (16) | P2—F4 | 1.5609 (7) |
C9—C10 | 1.3459 (17) | P2—F3 | 1.5707 (8) |
C9—H11 | 0.971 (15) | P2—F6 | 1.5780 (8) |
C9—H12 | 0.970 (14) | P2—F5 | 1.5876 (7) |
C10—C11 | 1.3443 (14) | P2—F2 | 1.5974 (9) |
| | | |
C11—Pd1—C10 | 37.10 (4) | C11—C10—H13 | 116.1 (10) |
C11—Pd1—N1 | 172.71 (3) | C9—C10—H13 | 116.2 (10) |
C10—Pd1—N1 | 136.61 (4) | Pd1—C10—H13 | 133.9 (9) |
C11—Pd1—C9 | 68.11 (5) | C10—C11—Pd1 | 74.06 (7) |
C10—Pd1—C9 | 35.80 (5) | C10—C11—H14 | 116.0 (8) |
N1—Pd1—C9 | 104.68 (5) | Pd1—C11—H14 | 116.0 (8) |
C11—Pd1—P1 | 101.79 (4) | C10—C11—H15 | 116.1 (8) |
C10—Pd1—P1 | 137.06 (4) | Pd1—C11—H15 | 116.1 (8) |
N1—Pd1—P1 | 85.19 (4) | H14—C11—H15 | 113.2 (11) |
C9—Pd1—P1 | 167.37 (3) | C13—C12—C17 | 119.99 (10) |
C18—P1—C12 | 104.85 (4) | C13—C12—P1 | 119.44 (8) |
C18—P1—C1 | 107.27 (5) | C17—C12—P1 | 120.49 (8) |
C12—P1—C1 | 107.85 (5) | C12—C13—C14 | 120.03 (9) |
C18—P1—Pd1 | 114.98 (3) | C12—C13—H31 | 120.2 (9) |
C12—P1—Pd1 | 120.26 (4) | C14—C13—H31 | 119.8 (9) |
C1—P1—Pd1 | 100.81 (5) | C13—C14—C15 | 119.89 (9) |
C6—N1—C7 | 110.06 (7) | C13—C14—H32 | 120.2 (8) |
C6—N1—C8 | 108.99 (8) | C15—C14—H32 | 119.9 (8) |
C7—N1—C8 | 109.37 (7) | C16—C15—C14 | 120.10 (10) |
C6—N1—Pd1 | 112.86 (7) | C16—C15—H33 | 120.0 (9) |
C7—N1—Pd1 | 107.02 (6) | C14—C15—H33 | 119.9 (9) |
C8—N1—Pd1 | 108.48 (6) | C15—C16—C17 | 119.98 (9) |
C6—C1—C2 | 121.12 (10) | C15—C16—H34 | 120.0 (8) |
C6—C1—P1 | 117.05 (8) | C17—C16—H34 | 120.0 (8) |
C2—C1—P1 | 121.77 (8) | C12—C17—C16 | 120.00 (9) |
C1—C2—C3 | 119.40 (10) | C12—C17—H35 | 120.0 (8) |
C1—C2—H1 | 120.3 (10) | C16—C17—H35 | 120.0 (8) |
C3—C2—H1 | 120.3 (10) | C19—C18—C23 | 119.95 (9) |
C4—C3—C2 | 119.23 (9) | C19—C18—P1 | 117.42 (7) |
C4—C3—H2 | 120.4 (8) | C23—C18—P1 | 122.63 (7) |
C2—C3—H2 | 120.3 (8) | C18—C19—C20 | 119.97 (9) |
C3—C4—C5 | 122.29 (9) | C18—C19—H36 | 119.7 (8) |
C3—C4—H3 | 118.9 (8) | C20—C19—H36 | 120.3 (8) |
C5—C4—H3 | 118.8 (8) | C21—C20—C19 | 120.07 (9) |
C4—C5—C6 | 118.82 (9) | C21—C20—H37 | 120.2 (8) |
C4—C5—H4 | 120.6 (8) | C19—C20—H37 | 119.7 (8) |
C6—C5—H4 | 120.5 (8) | C20—C21—C22 | 119.94 (9) |
C1—C6—C5 | 119.09 (9) | C20—C21—H38 | 119.9 (8) |
C1—C6—N1 | 121.58 (9) | C22—C21—H38 | 120.2 (8) |
C5—C6—N1 | 119.28 (8) | C23—C22—C21 | 120.05 (10) |
N1—C7—H5 | 109.5 (8) | C23—C22—H39 | 120.2 (9) |
N1—C7—H6 | 109.4 (8) | C21—C22—H39 | 119.7 (9) |
H5—C7—H6 | 109.4 (11) | C22—C23—C18 | 120.03 (9) |
N1—C7—H7 | 109.5 (8) | C22—C23—H40 | 119.7 (8) |
H5—C7—H7 | 109.4 (11) | C18—C23—H40 | 120.2 (8) |
H6—C7—H7 | 109.5 (12) | F1—P2—F4 | 90.30 (4) |
N1—C8—H8 | 109.5 (9) | F1—P2—F3 | 91.00 (5) |
N1—C8—H9 | 109.4 (8) | F4—P2—F3 | 90.78 (4) |
H8—C8—H9 | 109.5 (12) | F1—P2—F6 | 89.77 (5) |
N1—C8—H10 | 109.4 (9) | F4—P2—F6 | 90.40 (4) |
H8—C8—H10 | 109.5 (13) | F3—P2—F6 | 178.58 (3) |
H9—C8—H10 | 109.5 (12) | F1—P2—F5 | 90.88 (4) |
C10—C9—Pd1 | 68.66 (7) | F4—P2—F5 | 178.82 (4) |
C10—C9—H11 | 116.8 (9) | F3—P2—F5 | 89.22 (4) |
Pd1—C9—H11 | 116.8 (9) | F6—P2—F5 | 89.58 (4) |
C10—C9—H12 | 116.9 (8) | F1—P2—F2 | 178.59 (3) |
Pd1—C9—H12 | 116.9 (8) | F4—P2—F2 | 90.16 (4) |
H11—C9—H12 | 113.7 (13) | F3—P2—F2 | 90.32 (5) |
C11—C10—C9 | 127.67 (9) | F6—P2—F2 | 88.90 (5) |
C11—C10—Pd1 | 68.83 (6) | F5—P2—F2 | 88.66 (4) |
C9—C10—Pd1 | 75.54 (7) | | |
(bihjux) Tetra-aqua-(14-methyl-2,5,8-trioxa-11,14,17-triaza-1$2!,9$2!-dihydroxy-
-1,9(1,3)-dibenzenacyclo-octadecaphane-10,17-diene)-cerium(iii) trichloride
monohydrate
top
Crystal data top
C46H78Ce2Cl6N6O20 | γ = 90° |
Mr = 1528.08 | V = 1670.7 (12) Å3 |
P21/m | Z = 1 |
a = 10.983 (5) Å | F(000) = 774 |
b = 16.960 (6) Å | Dx = 1.519 Mg m−3 |
c = 9.058 (4) Å | Mo Kα radiation, λ = 0.71073 Å |
α = 90° | µ = 1.65 mm−1 |
β = 98.03 (7)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.014 |
Graphite monochromator | θmax = 43.2°, θmin = 1.9° |
17852 measured reflections | h = −11→11 |
4588 independent reflections | k = −18→18 |
4555 reflections with I > 2σ(I) | l = −10→10 |
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)] = 0.065 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.163 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.17 | w = 1/[σ2(Fo2) + (0.P)2 + 11.9541P] where P = (Fo2 + 2Fc2)/3 |
4588 reflections | (Δ/σ)max = 165.835 |
93 parameters | Δρmax = 1.97 e Å−3 |
0 restraints | Δρmin = −3.41 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. |
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 | Uiso*/Ueq | Occ. (<1) |
Ce1 | 0.15730 (3) | 0.2500 | 0.66210 (4) | 0.02000 (12)* | |
Cl1 | 0.16990 (15) | 0.2500 | 0.15380 (16) | 0.0200 (3)* | |
Cl2 | 0.42720 (14) | 0.89250 (9) | 0.31880 (15) | 0.0200 (3)* | 0.75 |
Cl3 | 0.3277 (4) | 0.4726 (3) | 0.5107 (5) | 0.0200 (7)* | 0.25 |
O1 | 0.2309 (3) | 0.3593 (2) | 0.8124 (4) | 0.0200 (6)* | |
O3 | 0.0247 (3) | 0.1139 (2) | 0.6306 (4) | 0.0200 (6)* | |
O4 | −0.0668 (5) | 0.2500 | 0.5286 (5) | 0.0200 (9)* | |
O6 | 0.3912 (5) | 0.2500 | 0.7006 (5) | 0.0200 (9)* | |
O7 | 0.0117 (5) | 0.2500 | 0.8672 (5) | 0.0200 (9)* | |
O8 | 0.2016 (3) | 0.1629 (2) | 0.4463 (4) | 0.0200 (6)* | |
O10 | −0.2437 (5) | 0.2500 | 0.7946 (5) | 0.0200 (9)* | |
N1 | 0.3911 (4) | 0.4032 (2) | 1.0422 (4) | 0.0200 (7)* | |
N2 | 0.5127 (5) | 0.2500 | 1.1447 (6) | 0.0200 (10)* | |
C1 | −0.0030 (4) | 0.5107 (3) | 0.7561 (5) | 0.0200 (8)* | |
C2 | 0.0441 (4) | 0.5651 (3) | 0.8644 (5) | 0.0200 (8)* | |
C3 | 0.1544 (4) | 0.5495 (3) | 0.9557 (5) | 0.0200 (8)* | |
C4 | 0.2174 (4) | 0.4797 (3) | 0.9388 (5) | 0.0200 (8)* | |
C5 | 0.1703 (5) | 0.4254 (3) | 0.8304 (5) | 0.0200 (8)* | |
C6 | 0.0601 (4) | 0.4409 (3) | 0.7391 (5) | 0.0200 (8)* | |
C7 | 0.3252 (4) | 0.4660 (3) | 1.0417 (5) | 0.0200 (8)* | |
C8 | 0.4964 (4) | 0.3916 (3) | 1.1504 (5) | 0.0200 (8)* | |
C9 | 0.5090 (4) | 0.3187 (3) | 1.2346 (5) | 0.0200 (8)* | |
C10 | 0.6113 (6) | 0.2500 | 1.0641 (7) | 0.0200 (11)* | |
C20 | −0.0967 (4) | 0.1128 (3) | 0.5570 (5) | 0.0200 (8)* | |
C21 | −0.1093 (4) | 0.1780 (3) | 0.4492 (5) | 0.0200 (8)* | |
Geometric parameters (Å, º) top
Ce1—O1 | 2.374 (4) | N1—C8 | 1.421 (6) |
Ce1—O1i | 2.374 (4) | N2—C10 | 1.388 (9) |
Ce1—O6 | 2.544 (5) | N2—C9 | 1.425 (6) |
Ce1—O8i | 2.551 (4) | N2—C9i | 1.425 (6) |
Ce1—O8 | 2.551 (4) | C1—C6 | 1.391 (7) |
Ce1—O4 | 2.586 (5) | C1—C2 | 1.393 (6) |
Ce1—O7 | 2.615 (5) | C2—C3 | 1.393 (7) |
Ce1—O3 | 2.723 (4) | C3—C4 | 1.390 (7) |
Ce1—O3i | 2.723 (4) | C4—C5 | 1.392 (7) |
O1—C5 | 1.325 (6) | C4—C7 | 1.420 (7) |
O3—C6i | 1.369 (6) | C5—C6 | 1.392 (7) |
O3—C20 | 1.405 (6) | C6—O3i | 1.369 (6) |
O4—C21 | 1.460 (5) | C8—C9 | 1.449 (7) |
O4—C21i | 1.460 (5) | C20—C21 | 1.469 (7) |
N1—C7 | 1.287 (6) | | |
| | | |
O1—Ce1—O1i | 102.68 (17) | O8—Ce1—O3i | 124.55 (11) |
O1—Ce1—O6 | 70.42 (11) | O4—Ce1—O3i | 59.39 (8) |
O1i—Ce1—O6 | 70.42 (11) | O7—Ce1—O3i | 72.74 (9) |
O1—Ce1—O8i | 84.33 (12) | O3—Ce1—O3i | 115.93 (15) |
O1i—Ce1—O8i | 143.67 (12) | C5—O1—Ce1 | 126.5 (3) |
O6—Ce1—O8i | 78.93 (13) | C6i—O3—C20 | 119.2 (4) |
O1—Ce1—O8 | 143.67 (12) | C6i—O3—Ce1 | 114.0 (3) |
O1i—Ce1—O8 | 84.33 (12) | C20—O3—Ce1 | 121.3 (3) |
O6—Ce1—O8 | 78.93 (13) | C21—O4—C21i | 113.5 (5) |
O8i—Ce1—O8 | 70.78 (16) | C21—O4—Ce1 | 116.6 (3) |
O1—Ce1—O4 | 119.58 (10) | C21i—O4—Ce1 | 116.6 (3) |
O1i—Ce1—O4 | 119.58 (10) | C7—N1—C8 | 121.3 (4) |
O6—Ce1—O4 | 160.22 (16) | C10—N2—C9 | 112.8 (4) |
O8i—Ce1—O4 | 84.99 (13) | C10—N2—C9i | 112.8 (4) |
O8—Ce1—O4 | 84.99 (13) | C9—N2—C9i | 109.7 (5) |
O1—Ce1—O7 | 77.62 (11) | C6—C1—C2 | 120.0 (4) |
O1i—Ce1—O7 | 77.62 (11) | C1—C2—C3 | 119.9 (4) |
O6—Ce1—O7 | 127.49 (16) | C4—C3—C2 | 120.1 (4) |
O8i—Ce1—O7 | 138.20 (10) | C3—C4—C5 | 120.0 (4) |
O8—Ce1—O7 | 138.20 (10) | C3—C4—C7 | 116.7 (4) |
O4—Ce1—O7 | 72.28 (16) | C5—C4—C7 | 123.3 (5) |
O1—Ce1—O3 | 148.91 (11) | O1—C5—C4 | 120.2 (4) |
O1i—Ce1—O3 | 62.12 (12) | O1—C5—C6 | 119.8 (4) |
O6—Ce1—O3 | 121.97 (8) | C4—C5—C6 | 120.0 (4) |
O8i—Ce1—O3 | 124.55 (11) | O3i—C6—C1 | 124.1 (4) |
O8—Ce1—O3 | 65.49 (11) | O3i—C6—C5 | 115.7 (4) |
O4—Ce1—O3 | 59.39 (8) | C1—C6—C5 | 120.0 (4) |
O7—Ce1—O3 | 72.74 (9) | N1—C7—C4 | 123.7 (4) |
O1—Ce1—O3i | 62.12 (12) | N1—C8—C9 | 119.3 (4) |
O1i—Ce1—O3i | 148.91 (11) | N2—C9—C8 | 113.9 (4) |
O6—Ce1—O3i | 121.97 (8) | O3—C20—C21 | 107.5 (4) |
O8i—Ce1—O3i | 65.49 (11) | O4—C21—C20 | 107.9 (4) |
Symmetry code: (i) x, −y+1/2, z. |
(bihlin) Tetra-aqua-(14-methyl-2,5,8-trioxa-11,14,17-triaza-1$2!,9$2!-dihydroxy-
-1,9(1,3)-dibenzenacyclo-octadecaphane-10,17-diene)-dysprosium(iii)
trichloride monohydrate
top
Crystal data top
C46H78Cl6Dy2N6O20 | γ = 90° |
Mr = 1572.84 | V = 1634.8 (12) Å3 |
P21/m | Z = 1 |
a = 10.870 (5) Å | F(000) = 790 |
b = 16.785 (6) Å | Dx = 1.598 Mg m−3 |
c = 9.046 (4) Å | Mo Kα radiation, λ = 0.71073 Å |
α = 90° | µ = 2.58 mm−1 |
β = 97.91 (8)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.018 |
Graphite monochromator | θmax = 43.5°, θmin = 1.9° |
17852 measured reflections | h = −11→11 |
4588 independent reflections | k = −18→18 |
4539 reflections with I > 2σ(I) | l = −10→10 |
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)] = 0.046 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.129 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.20 | w = 1/[σ2(Fo2) + (0.P)2 + 5.4182P] where P = (Fo2 + 2Fc2)/3 |
4588 reflections | (Δ/σ)max = 61.082 |
93 parameters | Δρmax = 2.33 e Å−3 |
0 restraints | Δρmin = −2.63 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. |
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 | Uiso*/Ueq | Occ. (<1) |
Dy1 | 0.15690 (2) | 0.2500 | 0.66630 (3) | 0.02000 (9)* | |
Cl1 | 0.16210 (12) | 0.2500 | 0.16360 (14) | 0.0200 (3)* | |
Cl2 | 0.42750 (12) | 0.89130 (8) | 0.31740 (14) | 0.0200 (2)* | 0.75 |
Cl3 | 0.3243 (4) | 0.4745 (2) | 0.5197 (4) | 0.0200 (6)* | 0.25 |
O1 | 0.2307 (3) | 0.35530 (18) | 0.8130 (3) | 0.0200 (5)* | |
O3 | 0.0256 (3) | 0.11750 (18) | 0.6345 (3) | 0.0200 (5)* | |
O4 | −0.0559 (4) | 0.2500 | 0.5190 (5) | 0.0200 (8)* | |
O6 | 0.3815 (4) | 0.2500 | 0.6989 (5) | 0.0200 (8)* | |
O7 | 0.0173 (4) | 0.2500 | 0.8499 (5) | 0.0200 (8)* | |
O8 | 0.2001 (3) | 0.16530 (19) | 0.4627 (3) | 0.0200 (5)* | |
O10 | −0.2365 (4) | 0.2500 | 0.7849 (5) | 0.0200 (8)* | |
N1 | 0.3949 (3) | 0.4000 (2) | 1.0434 (4) | 0.0200 (6)* | |
N2 | 0.5169 (5) | 0.2500 | 1.1572 (6) | 0.0200 (9)* | |
C1 | −0.0028 (4) | 0.5095 (2) | 0.7595 (4) | 0.0200 (7)* | |
C2 | 0.0446 (4) | 0.5635 (2) | 0.8698 (4) | 0.0200 (7)* | |
C3 | 0.1553 (4) | 0.5470 (3) | 0.9617 (4) | 0.0200 (7)* | |
C4 | 0.2189 (4) | 0.4765 (3) | 0.9433 (4) | 0.0200 (7)* | |
C5 | 0.1716 (4) | 0.4225 (3) | 0.8329 (4) | 0.0200 (7)* | |
C6 | 0.0608 (4) | 0.4390 (3) | 0.7414 (4) | 0.0200 (7)* | |
C7 | 0.3266 (4) | 0.4629 (2) | 1.0433 (5) | 0.0200 (7)* | |
C8 | 0.5143 (4) | 0.3905 (3) | 1.1475 (4) | 0.0200 (7)* | |
C9 | 0.5143 (4) | 0.3217 (2) | 1.2395 (5) | 0.0200 (7)* | |
C10 | 0.6269 (6) | 0.2500 | 1.0768 (6) | 0.0200 (10)* | |
C20 | −0.0944 (4) | 0.1143 (3) | 0.5526 (4) | 0.0200 (7)* | |
C21 | −0.1028 (4) | 0.1787 (2) | 0.4404 (5) | 0.0200 (7)* | |
Geometric parameters (Å, º) top
Dy1—O1 | 2.288 (3) | N1—C8 | 1.503 (5) |
Dy1—O1i | 2.288 (3) | N2—C9 | 1.417 (5) |
Dy1—O7 | 2.399 (5) | N2—C9i | 1.417 (5) |
Dy1—O6 | 2.419 (5) | N2—C10 | 1.483 (8) |
Dy1—O8 | 2.423 (3) | C1—C6 | 1.391 (6) |
Dy1—O8i | 2.423 (3) | C1—C2 | 1.393 (6) |
Dy1—O4 | 2.506 (5) | C2—C3 | 1.393 (6) |
Dy1—O3 | 2.637 (3) | C3—C4 | 1.392 (6) |
Dy1—O3i | 2.637 (3) | C4—C5 | 1.394 (6) |
O1—C5 | 1.323 (5) | C4—C7 | 1.396 (6) |
O3—C6i | 1.371 (5) | C5—C6 | 1.392 (6) |
O3—C20 | 1.410 (5) | C6—O3i | 1.371 (5) |
O4—C21 | 1.448 (5) | C8—C9 | 1.423 (6) |
O4—C21i | 1.448 (5) | C20—C21 | 1.477 (6) |
N1—C7 | 1.291 (5) | | |
| | | |
O1—Dy1—O1i | 101.15 (16) | O8—Dy1—O3i | 124.79 (10) |
O1—Dy1—O7 | 78.65 (10) | O8i—Dy1—O3i | 65.22 (11) |
O1i—Dy1—O7 | 78.65 (10) | O4—Dy1—O3i | 59.72 (7) |
O1—Dy1—O6 | 70.23 (11) | O3—Dy1—O3i | 115.01 (14) |
O1i—Dy1—O6 | 70.23 (11) | C5—O1—Dy1 | 126.8 (3) |
O7—Dy1—O6 | 129.77 (15) | C6i—O3—C20 | 119.5 (3) |
O1—Dy1—O8 | 143.60 (11) | C6i—O3—Dy1 | 114.3 (2) |
O1i—Dy1—O8 | 84.17 (11) | C20—O3—Dy1 | 122.5 (2) |
O7—Dy1—O8 | 137.17 (9) | C21—O4—C21i | 111.4 (4) |
O6—Dy1—O8 | 78.15 (12) | C21—O4—Dy1 | 119.9 (2) |
O1—Dy1—O8i | 84.17 (11) | C21i—O4—Dy1 | 119.9 (2) |
O1i—Dy1—O8i | 143.60 (11) | C7—N1—C8 | 122.3 (4) |
O7—Dy1—O8i | 137.17 (9) | C9—N2—C9i | 116.2 (5) |
O6—Dy1—O8i | 78.15 (12) | C9—N2—C10 | 109.5 (3) |
O8—Dy1—O8i | 71.85 (15) | C9i—N2—C10 | 109.5 (3) |
O1—Dy1—O4 | 122.19 (9) | C6—C1—C2 | 119.8 (4) |
O1i—Dy1—O4 | 122.19 (9) | C3—C2—C1 | 120.1 (4) |
O7—Dy1—O4 | 75.08 (15) | C4—C3—C2 | 120.0 (4) |
O6—Dy1—O4 | 155.15 (14) | C3—C4—C5 | 119.9 (4) |
O8—Dy1—O4 | 81.78 (12) | C3—C4—C7 | 116.6 (4) |
O8i—Dy1—O4 | 81.78 (12) | C5—C4—C7 | 123.5 (4) |
O1—Dy1—O3 | 148.88 (10) | O1—C5—C6 | 119.0 (4) |
O1i—Dy1—O3 | 63.45 (11) | O1—C5—C4 | 120.9 (4) |
O7—Dy1—O3 | 72.01 (9) | C6—C5—C4 | 120.0 (4) |
O6—Dy1—O3 | 122.37 (7) | O3i—C6—C1 | 125.2 (4) |
O8—Dy1—O3 | 65.22 (11) | O3i—C6—C5 | 114.6 (4) |
O8i—Dy1—O3 | 124.79 (10) | C1—C6—C5 | 120.2 (4) |
O4—Dy1—O3 | 59.72 (7) | N1—C7—C4 | 124.4 (4) |
O1—Dy1—O3i | 63.45 (11) | C9—C8—N1 | 112.5 (4) |
O1i—Dy1—O3i | 148.88 (10) | N2—C9—C8 | 112.3 (4) |
O7—Dy1—O3i | 72.01 (8) | O3—C20—C21 | 107.4 (3) |
O6—Dy1—O3i | 122.37 (7) | O4—C21—C20 | 106.4 (3) |
Symmetry code: (i) x, −y+1/2, z. |
(zexbuz01) Chloro-tris(2,2,6,6-tetramethyl-3,5-heptanedionato)-zirconium(iv)
top
Crystal data top
C33H57ClO6Zr | γ = 90° |
Mr = 676.46 | V = 1895.2 (14) Å3 |
P21/m | Z = 2 |
a = 10.679 (5) Å | F(000) = 720 |
b = 18.263 (7) Å | Dx = 1.185 Mg m−3 |
c = 10.973 (5) Å | Mo Kα radiation, λ = 0.71073 Å |
α = 90° | µ = 0.40 mm−1 |
β = 117.68 (5)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.006 |
Graphite monochromator | θmax = 52.2°, θmin = 2.1° |
20610 measured reflections | h = −11→11 |
5289 independent reflections | k = −19→19 |
5255 reflections with I > 2σ(I) | l = −11→11 |
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)] = 0.221 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.395 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.74 | w = 1/[σ2(Fo2) + (0.P)2 + 181.8093P] where P = (Fo2 + 2Fc2)/3 |
5289 reflections | (Δ/σ)max = 90.043 |
96 parameters | Δρmax = 4.04 e Å−3 |
0 restraints | Δρmin = −7.23 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. |
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 | Uiso*/Ueq | |
Zr1 | 0.84820 (13) | 0.2500 | 0.37470 (13) | 0.0200 (3)* | |
Cl1 | 0.7498 (3) | 0.2500 | 0.1192 (3) | 0.0200 (6)* | |
O1 | 1.0691 (10) | 0.2500 | 0.5131 (9) | 0.0200 (17)* | |
O2 | 0.8539 (10) | 0.2500 | 0.5706 (9) | 0.0200 (17)* | |
O3 | 0.6790 (7) | 0.3235 (4) | 0.3429 (6) | 0.0200 (13)* | |
O4 | 0.9232 (7) | 0.3537 (4) | 0.3519 (6) | 0.0200 (12)* | |
C1 | 1.3069 (13) | 0.2500 | 0.6871 (13) | 0.020 (2)* | |
C2 | 1.3724 (9) | 0.1878 (5) | 0.7679 (9) | 0.0200 (16)* | |
C3 | 1.3349 (13) | 0.2500 | 0.5742 (13) | 0.020 (2)* | |
C5 | 1.1497 (13) | 0.2500 | 0.6406 (13) | 0.020 (2)* | |
C6 | 1.0969 (13) | 0.2500 | 0.7373 (13) | 0.020 (2)* | |
H1 | 1.1711 | 0.2500 | 0.8451 | 0.02 (4)* | |
C7 | 0.9524 (13) | 0.2500 | 0.6988 (13) | 0.020 (2)* | |
C8 | 0.8934 (13) | 0.2500 | 0.8012 (13) | 0.020 (2)* | |
C9 | 0.7997 (9) | 0.1813 (5) | 0.7744 (9) | 0.0200 (17)* | |
C10 | 1.0141 (13) | 0.2500 | 0.9509 (13) | 0.020 (2)* | |
C12 | 0.4996 (9) | 0.4111 (5) | 0.2713 (9) | 0.0200 (16)* | |
C13 | 0.4647 (9) | 0.4923 (5) | 0.2310 (9) | 0.0200 (16)* | |
C14 | 0.4822 (9) | 0.3934 (5) | 0.3975 (9) | 0.0200 (16)* | |
C15 | 0.3901 (9) | 0.3649 (5) | 0.1510 (9) | 0.0200 (16)* | |
C16 | 0.6440 (9) | 0.3873 (5) | 0.2952 (9) | 0.0200 (16)* | |
C17 | 0.7292 (9) | 0.4318 (5) | 0.2643 (9) | 0.0200 (16)* | |
H2 | 0.6861 | 0.4830 | 0.2140 | 0.02 (3)* | |
C18 | 0.8678 (9) | 0.4150 (5) | 0.2938 (9) | 0.0200 (16)* | |
C19 | 0.9565 (9) | 0.4637 (5) | 0.2537 (9) | 0.0200 (16)* | |
C20 | 0.9740 (9) | 0.4238 (5) | 0.1428 (9) | 0.0200 (16)* | |
C21 | 0.9017 (9) | 0.5386 (5) | 0.2176 (9) | 0.0200 (16)* | |
C22 | 1.1040 (9) | 0.4692 (5) | 0.3801 (9) | 0.0200 (16)* | |
Geometric parameters (Å, º) top
Zr1—O4 | 2.116 (7) | C6—H1 | 1.0753 |
Zr1—O4i | 2.116 (7) | C7—C8 | 1.52 (2) |
Zr1—O2 | 2.122 (10) | C8—C9i | 1.545 (12) |
Zr1—O1 | 2.131 (9) | C8—C9 | 1.545 (12) |
Zr1—O3 | 2.145 (7) | C8—C10 | 1.547 (17) |
Zr1—O3i | 2.145 (7) | C12—C16 | 1.503 (13) |
Zr1—Cl1 | 2.495 (4) | C12—C14 | 1.515 (13) |
O1—C5 | 1.257 (15) | C12—C13 | 1.543 (13) |
O2—C7 | 1.308 (15) | C12—C15 | 1.545 (12) |
O3—C16 | 1.261 (12) | C16—C17 | 1.375 (14) |
O4—C18 | 1.288 (11) | C17—C18 | 1.394 (13) |
C1—C3 | 1.40 (2) | C17—H2 | 1.0746 |
C1—C2i | 1.411 (12) | C18—C19 | 1.506 (14) |
C1—C2 | 1.411 (12) | C19—C21 | 1.468 (13) |
C1—C5 | 1.511 (18) | C19—C20 | 1.503 (13) |
C5—C6 | 1.41 (2) | C19—C22 | 1.544 (12) |
C6—C7 | 1.398 (18) | | |
| | | |
O4—Zr1—O4i | 127.0 (4) | C7—C6—C5 | 122.8 (12) |
O4—Zr1—O2 | 106.6 (2) | C7—C6—H1 | 118.6 |
O4i—Zr1—O2 | 106.6 (2) | C5—C6—H1 | 118.6 |
O4—Zr1—O1 | 74.3 (2) | O2—C7—C6 | 123.3 (13) |
O4i—Zr1—O1 | 74.3 (2) | O2—C7—C8 | 113.1 (11) |
O2—Zr1—O1 | 77.1 (4) | C6—C7—C8 | 123.7 (11) |
O4—Zr1—O3 | 75.9 (3) | C7—C8—C9i | 108.2 (7) |
O4i—Zr1—O3 | 151.3 (3) | C7—C8—C9 | 108.2 (7) |
O2—Zr1—O3 | 77.9 (3) | C9i—C8—C9 | 108.5 (10) |
O1—Zr1—O3 | 133.3 (2) | C7—C8—C10 | 110.9 (11) |
O4—Zr1—O3i | 151.3 (3) | C9i—C8—C10 | 110.4 (7) |
O4i—Zr1—O3i | 75.9 (3) | C9—C8—C10 | 110.4 (7) |
O2—Zr1—O3i | 77.9 (3) | C16—C12—C14 | 109.3 (7) |
O1—Zr1—O3i | 133.3 (2) | C16—C12—C13 | 114.8 (8) |
O3—Zr1—O3i | 77.5 (4) | C14—C12—C13 | 110.6 (8) |
O4—Zr1—Cl1 | 81.50 (18) | C16—C12—C15 | 107.4 (8) |
O4i—Zr1—Cl1 | 81.50 (18) | C14—C12—C15 | 107.4 (8) |
O2—Zr1—Cl1 | 159.6 (3) | C13—C12—C15 | 107.1 (7) |
O1—Zr1—Cl1 | 123.3 (3) | O3—C16—C17 | 123.1 (9) |
O3—Zr1—Cl1 | 86.21 (19) | O3—C16—C12 | 115.0 (9) |
O3i—Zr1—Cl1 | 86.21 (19) | C17—C16—C12 | 121.9 (9) |
C5—O1—Zr1 | 138.8 (9) | C16—C17—C18 | 124.4 (9) |
C7—O2—Zr1 | 136.0 (9) | C16—C17—H2 | 117.8 |
C16—O3—Zr1 | 135.3 (7) | C18—C17—H2 | 117.8 |
C18—O4—Zr1 | 136.4 (6) | O4—C18—C17 | 120.0 (9) |
C3—C1—C2i | 107.9 (8) | O4—C18—C19 | 116.8 (8) |
C3—C1—C2 | 107.9 (8) | C17—C18—C19 | 123.1 (8) |
C2i—C1—C2 | 107.3 (11) | C21—C19—C20 | 114.7 (8) |
C3—C1—C5 | 111.2 (11) | C21—C19—C18 | 113.8 (8) |
C2i—C1—C5 | 111.2 (8) | C20—C19—C18 | 106.4 (8) |
C2—C1—C5 | 111.2 (8) | C21—C19—C22 | 107.1 (8) |
O1—C5—C6 | 122.0 (12) | C20—C19—C22 | 107.5 (8) |
O1—C5—C1 | 117.1 (12) | C18—C19—C22 | 107.1 (7) |
C6—C5—C1 | 121.0 (11) | | |
Symmetry code: (i) x, −y+1/2, z. |
(pyrhsb) Pyridinium hexachloro-antimony(v)
top
Crystal data top
C5H6N+·Cl6Sb− | γ = 90° |
Mr = 414.56 | V = 1286 (4) Å3 |
P21/a | Z = 4 |
a = 15.42 (3) Å | F(000) = 784 |
b = 11.66 (2) Å | Dx = 2.142 Mg m−3 |
c = 7.21 (1) Å | Mo Kα radiation, λ = 0.71073 Å |
α = 90° | µ = 3.35 mm−1 |
β = 97.31 (4)° | T = 293 K |
Data collection top
Radiation source: fine-focus sealed tube | Rint = 0.007 |
Graphite monochromator | θmax = 42.0°, θmin = 2.2° |
12890 measured reflections | h = −15→15 |
3289 independent reflections | k = −12→12 |
3277 reflections with I > 2σ(I) | l = −8→8 |
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)] = 0.061 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.167 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.35 | w = 1/[σ2(Fo2) + (0.P)2 + 16.8959P] where P = (Fo2 + 2Fc2)/3 |
3289 reflections | (Δ/σ)max = 2.226 |
77 parameters | Δρmax = 2.17 e Å−3 |
0 restraints | Δρmin = −3.22 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. |
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 | Uiso*/Ueq | Occ. (<1) |
Sb1 | 0.33750 (4) | 0.32820 (4) | 0.25310 (7) | 0.02000 (15)* | |
Cl1 | 0.36500 (13) | 0.45900 (16) | 0.0180 (2) | 0.0200 (3)* | |
Cl5 | 0.31000 (13) | 0.19500 (16) | 0.4840 (2) | 0.0200 (3)* | |
Cl6 | 0.30550 (13) | 0.18600 (16) | 0.0295 (2) | 0.0200 (3)* | |
Cl7 | 0.36850 (13) | 0.46850 (16) | 0.4825 (2) | 0.0200 (3)* | |
Cl8 | 0.18950 (13) | 0.38400 (16) | 0.2155 (2) | 0.0200 (3)* | |
Cl9 | 0.48400 (13) | 0.27150 (16) | 0.2860 (2) | 0.0200 (3)* | |
N1 | 0.4420 (12) | 0.7237 (12) | 0.2380 (18) | 0.020 (3)* | 0.50 |
C3 | 0.5080 (12) | 0.7877 (16) | 0.194 (2) | 0.020 (3)* | 0.50 |
C4 | 0.5070 (11) | 0.9037 (14) | 0.240 (2) | 0.020 (3)* | 0.50 |
C5 | 0.4200 (13) | 0.9527 (14) | 0.277 (2) | 0.020 (3)* | 0.50 |
C6 | 0.3600 (11) | 0.8747 (18) | 0.318 (2) | 0.020 (3)* | 0.50 |
C7 | 0.3680 (13) | 0.7717 (17) | 0.290 (2) | 0.020 (3)* | 0.50 |
N2' | 0.3950 (12) | 0.7233 (12) | 0.2510 (18) | 0.020 (3)* | 0.50 |
C10' | 0.4760 (14) | 0.7573 (16) | 0.201 (2) | 0.020 (3)* | 0.50 |
C9' | 0.4980 (11) | 0.8623 (15) | 0.168 (2) | 0.020 (3)* | 0.50 |
C8' | 0.4510 (13) | 0.9483 (14) | 0.239 (2) | 0.020 (3)* | 0.50 |
C2' | 0.3640 (11) | 0.9243 (17) | 0.296 (2) | 0.020 (3)* | 0.50 |
C1' | 0.3420 (13) | 0.8053 (17) | 0.292 (2) | 0.020 (3)* | 0.50 |
Geometric parameters (Å, º) top
Sb1—Cl6 | 2.321 (3) | C5—C8' | 0.58 (2) |
Sb1—Cl7 | 2.332 (3) | C5—C2' | 0.95 (2) |
Sb1—Cl9 | 2.337 (5) | C5—C6 | 1.36 (3) |
Sb1—Cl5 | 2.354 (3) | C5—C9' | 1.85 (3) |
Sb1—Cl8 | 2.355 (5) | C6—C2' | 0.605 (19) |
Sb1—Cl1 | 2.358 (3) | C6—C1' | 0.87 (2) |
N1—C10' | 0.73 (2) | C6—C7 | 1.23 (3) |
N1—N2' | 0.743 (17) | C6—C8' | 1.80 (3) |
N1—C3 | 1.33 (2) | C6—N2' | 1.93 (2) |
N1—C7 | 1.37 (3) | C7—C1' | 0.56 (2) |
N1—C1' | 1.89 (2) | C7—N2' | 0.78 (2) |
N1—C9' | 1.93 (2) | C7—C2' | 1.78 (3) |
C3—C10' | 0.61 (2) | C7—C10' | 1.87 (3) |
C3—C9' | 0.90 (2) | N2'—C1' | 1.32 (2) |
C3—C4 | 1.39 (2) | N2'—C10' | 1.40 (3) |
C4—C9' | 0.710 (19) | C10'—C9' | 1.30 (3) |
C4—C8' | 1.01 (2) | C9'—C8' | 1.37 (2) |
C4—C5 | 1.51 (3) | C8'—C2' | 1.48 (3) |
C4—C10' | 1.79 (3) | C2'—C1' | 1.43 (3) |
| | | |
Cl6—Sb1—Cl7 | 178.76 (7) | N2'—C7—C2' | 139 (2) |
Cl6—Sb1—Cl9 | 89.18 (9) | C6—C7—C2' | 9.4 (10) |
Cl7—Sb1—Cl9 | 91.04 (9) | N1—C7—C2' | 116.7 (15) |
Cl6—Sb1—Cl5 | 88.76 (14) | C1'—C7—C10' | 138 (4) |
Cl7—Sb1—Cl5 | 90.02 (14) | N2'—C7—C10' | 42.8 (18) |
Cl9—Sb1—Cl5 | 90.02 (9) | C6—C7—C10' | 104.9 (16) |
Cl6—Sb1—Cl8 | 90.01 (9) | N1—C7—C10' | 19.2 (8) |
Cl7—Sb1—Cl8 | 89.77 (9) | C2'—C7—C10' | 97.7 (12) |
Cl9—Sb1—Cl8 | 179.14 (7) | N1—N2'—C7 | 128 (3) |
Cl5—Sb1—Cl8 | 90.26 (9) | N1—N2'—C1' | 132 (2) |
Cl6—Sb1—Cl1 | 90.26 (14) | C7—N2'—C1' | 8.7 (15) |
Cl7—Sb1—Cl1 | 90.96 (14) | N1—N2'—C10' | 18.0 (15) |
Cl9—Sb1—Cl1 | 89.77 (9) | C7—N2'—C10' | 115 (2) |
Cl5—Sb1—Cl1 | 179.00 (7) | C1'—N2'—C10' | 116.9 (15) |
Cl8—Sb1—Cl1 | 89.93 (9) | N1—N2'—C6 | 109.6 (18) |
C10'—N1—N2' | 144 (3) | C7—N2'—C6 | 20.1 (18) |
C10'—N1—C3 | 7.5 (16) | C1'—N2'—C6 | 22.4 (10) |
N2'—N1—C3 | 145 (2) | C10'—N2'—C6 | 95.3 (11) |
C10'—N1—C7 | 123 (2) | C3—C10'—N1 | 163 (3) |
N2'—N1—C7 | 26.5 (15) | C3—C10'—C9' | 38 (2) |
C3—N1—C7 | 121.7 (15) | N1—C10'—C9' | 142 (3) |
C10'—N1—C1' | 116 (2) | C3—C10'—N2' | 159 (3) |
N2'—N1—C1' | 31.1 (14) | N1—C10'—N2' | 18.3 (16) |
C3—N1—C1' | 115.7 (13) | C9'—C10'—N2' | 125.1 (17) |
C7—N1—C1' | 6.8 (11) | C3—C10'—C4 | 42 (2) |
C10'—N1—C9' | 24.6 (18) | N1—C10'—C4 | 130 (2) |
N2'—N1—C9' | 121.0 (18) | C9'—C10'—C4 | 19.6 (9) |
C3—N1—C9' | 24.2 (9) | N2'—C10'—C4 | 117.4 (14) |
C7—N1—C9' | 98.4 (12) | C3—C10'—C7 | 137 (3) |
C1'—N1—C9' | 92.1 (10) | N1—C10'—C7 | 37.9 (18) |
C10'—C3—C9' | 117 (4) | C9'—C10'—C7 | 104.1 (15) |
C10'—C3—N1 | 9.0 (18) | N2'—C10'—C7 | 22.1 (8) |
C9'—C3—N1 | 118 (2) | C4—C10'—C7 | 95.3 (12) |
C10'—C3—C4 | 120 (3) | C4—C9'—C3 | 120 (3) |
C9'—C3—C4 | 26.3 (12) | C4—C9'—C10' | 123 (2) |
N1—C3—C4 | 117.1 (15) | C3—C9'—C10' | 24.9 (14) |
C9'—C4—C8' | 105 (2) | C4—C9'—C8' | 45.1 (18) |
C9'—C4—C3 | 34.1 (17) | C3—C9'—C8' | 135 (2) |
C8'—C4—C3 | 122.3 (19) | C10'—C9'—C8' | 117.2 (16) |
C9'—C4—C5 | 107 (2) | C4—C9'—C5 | 51.6 (19) |
C8'—C4—C5 | 13.5 (12) | C3—C9'—C5 | 124.5 (18) |
C3—C4—C5 | 116.5 (15) | C10'—C9'—C5 | 105.1 (14) |
C9'—C4—C10' | 37.9 (18) | C8'—C9'—C5 | 12.2 (9) |
C8'—C4—C10' | 106.3 (17) | C4—C9'—N1 | 116 (2) |
C3—C4—C10' | 17.3 (9) | C3—C9'—N1 | 37.4 (14) |
C5—C4—C10' | 99.4 (13) | C10'—C9'—N1 | 13.5 (10) |
C8'—C5—C2' | 148 (3) | C8'—C9'—N1 | 103.8 (13) |
C8'—C5—C6 | 132 (3) | C5—C9'—N1 | 91.7 (10) |
C2'—C5—C6 | 22.8 (13) | C5—C8'—C4 | 143 (3) |
C8'—C5—C4 | 24 (2) | C5—C8'—C9' | 138 (3) |
C2'—C5—C4 | 137 (2) | C4—C8'—C9' | 29.9 (12) |
C6—C5—C4 | 115.5 (15) | C5—C8'—C2' | 20 (2) |
C8'—C5—C9' | 30 (2) | C4—C8'—C2' | 135.0 (19) |
C2'—C5—C9' | 121.0 (18) | C9'—C8'—C2' | 120.4 (16) |
C6—C5—C9' | 102.1 (13) | C5—C8'—C6 | 34 (2) |
C4—C5—C9' | 21.6 (7) | C4—C8'—C6 | 117.0 (17) |
C2'—C6—C1' | 151 (3) | C9'—C8'—C6 | 103.9 (13) |
C2'—C6—C7 | 151 (3) | C2'—C8'—C6 | 18.1 (8) |
C1'—C6—C7 | 24.2 (16) | C6—C2'—C5 | 120 (3) |
C2'—C6—C5 | 38 (2) | C6—C2'—C1' | 17.1 (19) |
C1'—C6—C5 | 142 (2) | C5—C2'—C1' | 124 (2) |
C7—C6—C5 | 122.3 (18) | C6—C2'—C8' | 112 (3) |
C2'—C6—C8' | 50 (2) | C5—C2'—C8' | 11.9 (13) |
C1'—C6—C8' | 128 (2) | C1'—C2'—C8' | 113.6 (16) |
C7—C6—C8' | 108.4 (15) | C6—C2'—C7 | 19 (2) |
C5—C6—C8' | 14.0 (9) | C5—C2'—C7 | 108.0 (18) |
C2'—C6—N2' | 140 (3) | C1'—C2'—C7 | 15.8 (10) |
C1'—C6—N2' | 35.3 (16) | C8'—C2'—C7 | 98.4 (13) |
C7—C6—N2' | 12.5 (11) | C7—C1'—C6 | 116 (4) |
C5—C6—N2' | 109.8 (14) | C7—C1'—N2' | 12 (2) |
C8'—C6—N2' | 95.9 (11) | C6—C1'—N2' | 122 (2) |
C1'—C7—N2' | 159 (4) | C7—C1'—C2' | 121 (4) |
C1'—C7—C6 | 39 (3) | C6—C1'—C2' | 11.8 (13) |
N2'—C7—C6 | 147 (3) | N2'—C1'—C2' | 123.9 (17) |
C1'—C7—N1 | 156 (4) | C7—C1'—N1 | 17 (3) |
N2'—C7—N1 | 25.3 (15) | C6—C1'—N1 | 105 (2) |
C6—C7—N1 | 123.5 (19) | N2'—C1'—N1 | 17.0 (8) |
C1'—C7—C2' | 44 (3) | C2'—C1'—N1 | 107.1 (14) |
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