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In the title compound, [Hf(C9H6NO)4]·2C7H8, the hafnium metal centre is coordinated by four N,O-donating bidentate quinolin-8-olate ligands arranged to give a square-anti­prismatic coordination polyhedron with a slightly distorted dodeca­hedral geometry. The average Hf—O and Hf—N distances are 2.096 (3) and 2.398 (3) Å, respectively, and the average O—Hf—N bite angle is 70.99 (11)°. The crystal packing is controlled by π–π inter­actions between quinoline ligands of neighbouring mol­ecules and hydrogen-bonding inter­actions. The inter­planar distances vary between 3.138 (1) and 3.208 (2) Å, while the centroid–centroid distances range from 3.576 (1) to 4.074 (1) Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536809043244/bg2301sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536809043244/bg2301Isup2.hkl
Contains datablock I

CCDC reference: 758639

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.033
  • wR factor = 0.100
  • Data-to-parameter ratio = 15.8

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT919_ALERT_3_B Reflection(s) # Likely Affected by the Beamstop 1
Alert level C PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 3.05 PLAT432_ALERT_2_C Short Inter X...Y Contact C41 .. C45 .. 3.16 Ang. PLAT432_ALERT_2_C Short Inter X...Y Contact C43 .. C49 .. 3.18 Ang. PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 22 PLAT912_ALERT_4_C Missing # of FCF Reflections Above STh/L= 0.600 11
Alert level G PLAT960_ALERT_3_G Number of Intensities with I .LT. - 2*sig(I) .. 1 PLAT154_ALERT_1_G The su's on the Cell Angles are Equal (x 10000) 200 Deg.
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 5 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

This study forms part of an ongoing researh project that investigates the chelating behaviour of O,O'- and O,N-bidentate ligands with hafnium(IV) and zirconium(IV) for possible separation of these two metals (Viljoen et al. 2008, 2009). The total separation of zircon ore(ZrSiO4), which contains traces of hafnium, is of most importance for nucleur aplications. A few hafnium complexes containing β-diketonato ligands have been reported by others (Zherikova et al. (2008); Demakopoulos et al. (1995)). An analogous zirconium complex has been reported by Lewis & Fay (1974).

The title compound [Hf(C9H6NO)4].2(C7H8), where C9H6NO ( Ox-) = 8-hydroxyquinoline and C7H8 = toluene, crystallizes in the form of yellow plate-like crystals of in the triclinic system (P1, Z=2) (Figure 1) with two toluene solvent molecules in the asymmetric unit. The HfIV atom is eight coordinated and surrounded by four chelating β-diketonato Ox- ligands to give a square antiprismatic coordination polyhedron with a slight distortion towards a dodecahedral geometry. The Hf—O and Hf—N bond lengths vary from 2.085 (3) Å to 2.103 (3) Å and 2.391 (3) Å to 2.404 (3) Å, respectivily, and the O—Hf—N bite angles vary from 70.73 (11)° to 71.16 (11)° . The dihedral angle between the two phenyl rings in the quinoline ligands are all less than 1°, indicating a negligible distortion due to coordination or packing. The molecular units are connected by π-π interactions between different quinoline ligands of neighbouring molecules to produce a three dimensional network, with interplaner distances varying between 3.138 (1) Å and 3.208 (2) Å and centroid-to-centroid distances from 3.576 (1) Å and 4.074 (1) Å (see Figure 2). Lastly, a strong C—H···O hydrogen bonding interaction is observed between a solvent molecule and one of the oxygen atoms from a neighbouring metallic molecular group (see Table 1).

Related literature top

For a Zr analogue of the title compound, see: Lewis & Fay (1974). For hafnium and zirconium β-diketonato complexes, see: Viljoen et al. (2008, 2009); Demakopoulos et al. (1995), Zherikova et al. (2005, 2006); Steyn et al. (2008); Calderazzo et al. (1998).

For related literature, see: Zherikova et al. (2008).

Experimental top

Chemicals were purchased from Sigma and Aldrich and used as received except for toluene which was dried by passage over alumina. Syntheses were perfomed using modified Schlenk conditions. OxH (0.369 g, 254 mmol) was added to a suspension of HfCl4 (0.201 g, 0.63 mmol) in toluene (10 ml). The dissolution turned into a slightly yellow solution after 10 min, and after refluxing for ca 20 h, the crude product was filtered and washed with toluene. The filtrate was slowly recrystallized at 253 K at near qauntitative yield. Spectroscopy data: 1H NMR (Benzene-d6;):δ = 6.70 (d, 1H, J = 6 Hz), 7.29 (dd, 2H, J = 7.8 Hz, 6 Hz), 7.36 (t, 2H, J = 7.8 Hz), 8.13 (d, 1H, J = 7.2 Hz); IR (ATR): ν(CO) 1659 cm-1.

Refinement top

The aromatic, methine, and methyl H atoms were placed in geometrically idealized positions (C—H = 0.93–0.98) and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C) for aromatic and methine, and Uiso(H) = 1.5Ueq(C) for methyl protons. Torsion angles for methyl protons were refined from electron density. The highest residual electron density was located 2.34 Å from H311 and was essentially meaningless.

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus (Bruker, 2004); program(s) used to solve structure: SIR92 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. Representation of the title compound (I), showing the numbering scheme and displacement ellipsoids (50% probability). H atoms omitted for clarity.
[Figure 2] Fig. 2. Graphical illustration of π-π interaction and stacking between different quinoline ligands of neighbouring molecules to produce a three dimensional network (displacement ellipsoids at the 50% probability level, H atoms omitted for clarity). Symmetry codes: (') 1 - x, -y, 1 - z; (") 1 - x, 1 - y, 1 - z.
Tetrakis(quinolin-8-olato-κ2N,O)hafnium(IV) toluene disolvate top
Crystal data top
[Hf(C9H6NO)4]·2C7H8Z = 2
Mr = 939.35F(000) = 944
Triclinic, P1Dx = 1.602 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 11.3323 (5) ÅCell parameters from 9377 reflections
b = 12.5539 (5) Åθ = 2.6–28.1°
c = 15.7126 (7) ŵ = 2.73 mm1
α = 69.746 (2)°T = 100 K
β = 69.700 (2)°Plate, yellow
γ = 75.787 (2)°0.22 × 0.10 × 0.04 mm
V = 1946.79 (14) Å3
Data collection top
Bruker X8 APEXII 4K Kappa CCD
diffractometer
8458 independent reflections
Radiation source: fine-focus sealed tube7551 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.044
ω and ϕ scansθmax = 27°, θmin = 1.4°
Absorption correction: multi-scan
(SADABS; Bruker, 2004)
h = 1414
Tmin = 0.585, Tmax = 0.899k = 1616
22928 measured reflectionsl = 2020
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0618P)2]
where P = (Fo2 + 2Fc2)/3
8458 reflections(Δ/σ)max = 0.002
534 parametersΔρmax = 1.16 e Å3
0 restraintsΔρmin = 0.81 e Å3
Crystal data top
[Hf(C9H6NO)4]·2C7H8γ = 75.787 (2)°
Mr = 939.35V = 1946.79 (14) Å3
Triclinic, P1Z = 2
a = 11.3323 (5) ÅMo Kα radiation
b = 12.5539 (5) ŵ = 2.73 mm1
c = 15.7126 (7) ÅT = 100 K
α = 69.746 (2)°0.22 × 0.10 × 0.04 mm
β = 69.700 (2)°
Data collection top
Bruker X8 APEXII 4K Kappa CCD
diffractometer
8458 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2004)
7551 reflections with I > 2σ(I)
Tmin = 0.585, Tmax = 0.899Rint = 0.044
22928 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0330 restraints
wR(F2) = 0.100H-atom parameters constrained
S = 1.04Δρmax = 1.16 e Å3
8458 reflectionsΔρmin = 0.81 e Å3
534 parameters
Special details top

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C110.0301 (4)0.2510 (4)0.5067 (3)0.0187 (9)
H110.06710.31580.46650.022*
C120.0455 (4)0.2069 (4)0.4758 (3)0.0221 (10)
H120.0570.24150.41590.026*
C130.1014 (5)0.1134 (4)0.5345 (3)0.0237 (10)
H130.14980.08290.51390.028*
C140.0872 (4)0.0617 (4)0.6263 (3)0.0184 (9)
C150.1430 (5)0.0332 (4)0.6941 (4)0.0244 (10)
H150.1950.06780.68010.029*
C160.1200 (5)0.0747 (4)0.7813 (3)0.0239 (10)
H160.15730.13760.82560.029*
C170.0420 (4)0.0252 (4)0.8055 (3)0.0200 (9)
H170.02930.05490.86520.024*
C180.0159 (4)0.0675 (3)0.7407 (3)0.0151 (8)
C190.0091 (4)0.1124 (3)0.6511 (3)0.0125 (8)
C210.1816 (4)0.2455 (3)0.8712 (3)0.0158 (9)
H210.25330.19010.86580.019*
C220.1269 (5)0.2752 (4)0.9567 (3)0.0202 (9)
H220.16110.23861.00720.024*
C230.0237 (5)0.3580 (4)0.9650 (3)0.0205 (10)
H230.01150.37911.02090.025*
C240.0297 (4)0.4116 (4)0.8891 (3)0.0168 (9)
C250.1373 (5)0.4969 (4)0.8906 (3)0.0219 (10)
H250.17850.52190.94430.026*
C260.1805 (5)0.5423 (4)0.8124 (3)0.0249 (10)
H260.25150.59840.8140.03*
C270.1215 (4)0.5072 (3)0.7294 (3)0.0177 (9)
H270.15340.54030.67760.021*
C280.0158 (4)0.4235 (3)0.7253 (3)0.0151 (9)
C290.0305 (4)0.3765 (3)0.8060 (3)0.0139 (8)
C310.2648 (4)0.5148 (3)0.5866 (3)0.0148 (8)
H310.18850.53790.57120.018*
C320.3397 (5)0.5985 (4)0.5694 (3)0.0191 (9)
H320.31260.67560.54330.023*
C330.4522 (5)0.5659 (4)0.5911 (3)0.0203 (10)
H330.50250.62070.57960.024*
C340.4924 (4)0.4487 (4)0.6312 (3)0.0157 (9)
C350.6077 (4)0.4046 (4)0.6546 (3)0.0205 (9)
H350.66350.4540.64460.025*
C360.6377 (5)0.2882 (4)0.6923 (3)0.0224 (10)
H360.71370.25980.70790.027*
C370.5553 (4)0.2116 (4)0.7076 (3)0.0199 (9)
H370.57730.13360.7340.024*
C380.4435 (4)0.2497 (3)0.6844 (3)0.0147 (8)
C390.4106 (4)0.3707 (3)0.6462 (3)0.0137 (8)
C410.2922 (4)0.0275 (3)0.6404 (3)0.0124 (8)
H410.26270.04790.70620.015*
C420.3422 (4)0.1154 (3)0.5959 (3)0.0165 (9)
H420.34530.19190.63190.02*
C430.3857 (4)0.0878 (3)0.4999 (3)0.0152 (9)
H430.41850.14530.46980.018*
C440.3809 (4)0.0293 (3)0.4459 (3)0.0136 (8)
C450.4271 (4)0.0700 (3)0.3460 (3)0.0158 (9)
H450.46240.01830.31030.019*
C460.4198 (4)0.1852 (4)0.3018 (3)0.0163 (9)
H460.44870.21050.23610.02*
C470.3701 (4)0.2663 (3)0.3526 (3)0.0159 (9)
H470.36740.34410.32020.019*
C480.3249 (4)0.2319 (3)0.4504 (3)0.0121 (8)
C490.3295 (4)0.1114 (3)0.4969 (3)0.0115 (8)
C1010.4169 (5)0.8733 (4)0.9727 (4)0.0242 (10)
C1020.3554 (5)0.8060 (4)1.0597 (3)0.0287 (11)
H1020.40190.76091.10140.034*
C1030.2263 (5)0.8043 (4)1.0863 (4)0.0286 (11)
H1030.18710.75711.14490.034*
C1040.1550 (5)0.8725 (4)1.0261 (3)0.0233 (10)
H1040.06790.87161.04380.028*
C1050.2150 (5)0.9418 (4)0.9396 (3)0.0233 (10)
H1050.16780.98860.89880.028*
C1060.3449 (5)0.9423 (4)0.9129 (3)0.0197 (9)
H1060.38430.98950.85420.024*
C1070.5587 (5)0.8748 (5)0.9431 (4)0.0414 (14)
H10A0.57950.89760.98790.062*
H10B0.58360.92830.88140.062*
H10C0.60290.79960.94110.062*
C2010.2346 (5)0.6255 (4)0.8215 (3)0.0232 (10)
C2020.2835 (4)0.5123 (4)0.8235 (3)0.0206 (9)
H2020.2480.4740.79940.025*
C2030.3829 (5)0.4553 (4)0.8601 (3)0.0281 (11)
H2030.41450.37960.85990.034*
C2040.4356 (6)0.5098 (5)0.8971 (4)0.0394 (14)
H2040.50340.47120.92150.047*
C2050.3890 (7)0.6201 (5)0.8981 (4)0.0459 (17)
H2050.42390.65650.92420.055*
C2060.2888 (6)0.6785 (4)0.8601 (3)0.0389 (15)
H2060.25780.75420.86070.047*
C2070.1292 (5)0.6861 (4)0.7794 (4)0.0353 (13)
H20A0.16270.71320.71170.053*
H20B0.08670.75010.80390.053*
H20C0.06990.63440.79510.053*
N10.0504 (3)0.2037 (3)0.5909 (2)0.0148 (7)
N20.1342 (3)0.2939 (3)0.7981 (2)0.0140 (7)
N30.2993 (3)0.4043 (3)0.6239 (2)0.0141 (7)
N40.2853 (3)0.0823 (3)0.5933 (2)0.0130 (7)
O10.0910 (3)0.1197 (2)0.75695 (19)0.0144 (6)
O20.0440 (3)0.3817 (2)0.6519 (2)0.0141 (6)
O30.3619 (3)0.1828 (2)0.6929 (2)0.0142 (6)
O40.2786 (3)0.3022 (2)0.5050 (2)0.0134 (6)
Hf0.194221 (16)0.246881 (12)0.651652 (11)0.01143 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C110.016 (2)0.022 (2)0.018 (2)0.0016 (18)0.0059 (18)0.0054 (17)
C120.018 (3)0.032 (2)0.017 (2)0.000 (2)0.0085 (19)0.0083 (19)
C130.013 (2)0.031 (2)0.035 (3)0.0034 (19)0.013 (2)0.016 (2)
C140.013 (2)0.019 (2)0.027 (2)0.0022 (17)0.0079 (19)0.0091 (18)
C150.017 (3)0.024 (2)0.038 (3)0.0043 (19)0.010 (2)0.012 (2)
C160.020 (3)0.023 (2)0.028 (3)0.0068 (19)0.005 (2)0.0058 (19)
C170.018 (2)0.022 (2)0.018 (2)0.0031 (18)0.0045 (19)0.0058 (18)
C180.012 (2)0.0166 (19)0.016 (2)0.0025 (17)0.0006 (17)0.0075 (16)
C190.008 (2)0.0133 (18)0.016 (2)0.0005 (16)0.0033 (17)0.0050 (16)
C210.015 (2)0.0147 (19)0.018 (2)0.0002 (16)0.0058 (18)0.0057 (16)
C220.023 (3)0.024 (2)0.015 (2)0.0067 (19)0.0075 (19)0.0038 (18)
C230.021 (3)0.026 (2)0.014 (2)0.0077 (19)0.0015 (19)0.0096 (18)
C240.016 (2)0.020 (2)0.014 (2)0.0086 (18)0.0002 (18)0.0039 (17)
C250.022 (3)0.024 (2)0.019 (2)0.0049 (19)0.0013 (19)0.0109 (18)
C260.019 (3)0.024 (2)0.031 (3)0.0039 (19)0.005 (2)0.013 (2)
C270.013 (2)0.019 (2)0.018 (2)0.0046 (17)0.0010 (18)0.0038 (17)
C280.019 (2)0.0137 (18)0.014 (2)0.0060 (17)0.0025 (18)0.0040 (16)
C290.012 (2)0.0146 (19)0.016 (2)0.0055 (16)0.0013 (17)0.0053 (16)
C310.015 (2)0.0174 (19)0.015 (2)0.0035 (17)0.0039 (17)0.0075 (16)
C320.024 (3)0.016 (2)0.016 (2)0.0032 (18)0.0039 (19)0.0054 (17)
C330.026 (3)0.021 (2)0.017 (2)0.0075 (19)0.0012 (19)0.0105 (18)
C340.015 (2)0.021 (2)0.013 (2)0.0083 (17)0.0011 (17)0.0097 (17)
C350.017 (2)0.029 (2)0.021 (2)0.0114 (19)0.0008 (19)0.0129 (19)
C360.015 (2)0.032 (2)0.029 (3)0.0004 (19)0.008 (2)0.018 (2)
C370.019 (2)0.023 (2)0.022 (2)0.0014 (19)0.0065 (19)0.0122 (18)
C380.017 (2)0.0164 (19)0.015 (2)0.0048 (17)0.0049 (18)0.0077 (16)
C390.011 (2)0.020 (2)0.013 (2)0.0042 (17)0.0010 (17)0.0102 (16)
C410.009 (2)0.0159 (18)0.014 (2)0.0028 (16)0.0040 (16)0.0046 (16)
C420.015 (2)0.0141 (19)0.022 (2)0.0016 (17)0.0059 (18)0.0061 (17)
C430.007 (2)0.0175 (19)0.024 (2)0.0026 (16)0.0027 (17)0.0105 (17)
C440.011 (2)0.0152 (19)0.019 (2)0.0030 (16)0.0063 (17)0.0071 (16)
C450.014 (2)0.020 (2)0.018 (2)0.0010 (17)0.0032 (18)0.0129 (17)
C460.012 (2)0.026 (2)0.014 (2)0.0055 (18)0.0057 (17)0.0061 (17)
C470.016 (2)0.0165 (19)0.017 (2)0.0002 (17)0.0076 (18)0.0048 (16)
C480.008 (2)0.0155 (19)0.016 (2)0.0054 (16)0.0030 (16)0.0052 (16)
C490.013 (2)0.0126 (18)0.0120 (19)0.0058 (16)0.0041 (16)0.0036 (15)
C1010.022 (3)0.024 (2)0.029 (3)0.002 (2)0.008 (2)0.012 (2)
C1020.031 (3)0.028 (2)0.021 (3)0.002 (2)0.012 (2)0.002 (2)
C1030.032 (3)0.027 (2)0.021 (2)0.006 (2)0.005 (2)0.0017 (19)
C1040.016 (2)0.023 (2)0.032 (3)0.0052 (19)0.003 (2)0.012 (2)
C1050.029 (3)0.018 (2)0.029 (3)0.0045 (19)0.018 (2)0.0111 (19)
C1060.023 (3)0.017 (2)0.019 (2)0.0089 (18)0.0017 (19)0.0051 (17)
C1070.024 (3)0.051 (3)0.045 (4)0.005 (3)0.005 (3)0.014 (3)
C2010.027 (3)0.021 (2)0.013 (2)0.012 (2)0.0096 (19)0.0033 (17)
C2020.017 (2)0.027 (2)0.019 (2)0.0059 (19)0.0004 (19)0.0112 (18)
C2030.028 (3)0.036 (3)0.018 (2)0.009 (2)0.003 (2)0.006 (2)
C2040.034 (3)0.069 (4)0.017 (3)0.027 (3)0.004 (2)0.006 (3)
C2050.071 (5)0.063 (4)0.020 (3)0.052 (4)0.005 (3)0.009 (3)
C2060.068 (5)0.025 (2)0.020 (3)0.026 (3)0.008 (3)0.009 (2)
C2070.029 (3)0.027 (3)0.027 (3)0.005 (2)0.003 (2)0.001 (2)
N10.0113 (19)0.0180 (17)0.0155 (18)0.0010 (14)0.0043 (15)0.0068 (14)
N20.0152 (19)0.0123 (15)0.0143 (18)0.0064 (14)0.0028 (15)0.0021 (13)
N30.0129 (19)0.0173 (17)0.0130 (17)0.0036 (14)0.0005 (15)0.0076 (14)
N40.0104 (18)0.0131 (16)0.0185 (18)0.0021 (14)0.0061 (15)0.0061 (14)
O10.0159 (16)0.0165 (13)0.0131 (14)0.0052 (12)0.0043 (12)0.0049 (11)
O20.0149 (16)0.0143 (13)0.0139 (15)0.0001 (12)0.0047 (12)0.0059 (11)
O30.0119 (16)0.0149 (13)0.0177 (15)0.0019 (11)0.0042 (12)0.0071 (11)
O40.0143 (16)0.0118 (13)0.0149 (15)0.0054 (11)0.0014 (12)0.0050 (11)
Hf0.01205 (11)0.01173 (10)0.01191 (10)0.00236 (7)0.00353 (7)0.00454 (7)
Geometric parameters (Å, º) top
C11—N11.325 (5)C41—C421.408 (5)
C11—C121.409 (6)C41—H410.93
C11—H110.93C42—C431.357 (6)
C12—C131.356 (7)C42—H420.93
C12—H120.93C43—C441.419 (5)
C13—C141.411 (6)C43—H430.93
C13—H130.93C44—C491.413 (5)
C14—C151.407 (6)C44—C451.417 (6)
C14—C191.423 (6)C45—C461.366 (6)
C15—C161.380 (7)C45—H450.93
C15—H150.93C46—C471.400 (6)
C16—C171.407 (6)C46—H460.93
C16—H160.93C47—C481.383 (6)
C17—C181.382 (6)C47—H470.93
C17—H170.93C48—O41.332 (5)
C18—O11.326 (5)C48—C491.432 (5)
C18—C191.424 (6)C49—N41.363 (5)
C19—N11.360 (5)C101—C1021.377 (7)
C21—N21.328 (5)C101—C1061.386 (6)
C21—C221.409 (6)C101—C1071.513 (7)
C21—H210.93C102—C1031.378 (7)
C22—C231.362 (6)C102—H1020.93
C22—H220.93C103—C1041.382 (7)
C23—C241.411 (6)C103—H1030.93
C23—H230.93C104—C1051.377 (7)
C24—C251.410 (6)C104—H1040.93
C24—C291.413 (6)C105—C1061.385 (7)
C25—C261.367 (6)C105—H1050.93
C25—H250.93C106—H1060.93
C26—C271.410 (6)C107—H10A0.96
C26—H260.93C107—H10B0.96
C27—C281.385 (6)C107—H10C0.96
C27—H270.93C201—C2021.386 (6)
C28—O21.329 (5)C201—C2061.389 (7)
C28—C291.422 (6)C201—C2071.482 (7)
C29—N21.365 (5)C202—C2031.371 (7)
C31—N31.322 (5)C202—H2020.93
C31—C321.407 (6)C203—C2041.371 (7)
C31—H310.93C203—H2030.93
C32—C331.364 (6)C204—C2051.359 (9)
C32—H320.93C204—H2040.93
C33—C341.414 (6)C205—C2061.393 (9)
C33—H330.93C205—H2050.93
C34—C351.409 (6)C206—H2060.93
C34—C391.418 (6)C207—H20A0.96
C35—C361.377 (6)C207—H20B0.96
C35—H350.93C207—H20C0.96
C36—C371.407 (6)N1—Hf2.395 (3)
C36—H360.93N2—Hf2.400 (3)
C37—C381.367 (6)N3—Hf2.391 (3)
C37—H370.93N4—Hf2.404 (3)
C38—O31.340 (5)O1—Hf2.098 (3)
C38—C391.433 (6)O2—Hf2.085 (3)
C39—N31.353 (5)O3—Hf2.103 (3)
C41—N41.317 (5)O4—Hf2.096 (3)
N1—C11—C12122.4 (4)C48—C47—H47119.7
N1—C11—H11118.8C46—C47—H47119.7
C12—C11—H11118.8O4—C48—C47125.2 (4)
C13—C12—C11119.2 (4)O4—C48—C49117.2 (3)
C13—C12—H12120.4C47—C48—C49117.7 (4)
C11—C12—H12120.4N4—C49—C44123.0 (4)
C12—C13—C14121.0 (4)N4—C49—C48115.2 (3)
C12—C13—H13119.5C44—C49—C48121.8 (4)
C14—C13—H13119.5C102—C101—C106118.2 (5)
C15—C14—C13126.1 (4)C102—C101—C107121.5 (5)
C15—C14—C19118.2 (4)C106—C101—C107120.2 (5)
C13—C14—C19115.7 (4)C101—C102—C103121.4 (5)
C16—C15—C14119.6 (4)C101—C102—H102119.3
C16—C15—H15120.2C103—C102—H102119.3
C14—C15—H15120.2C102—C103—C104120.2 (5)
C15—C16—C17122.2 (4)C102—C103—H103119.9
C15—C16—H16118.9C104—C103—H103119.9
C17—C16—H16118.9C105—C104—C103119.0 (5)
C18—C17—C16120.1 (4)C105—C104—H104120.5
C18—C17—H17119.9C103—C104—H104120.5
C16—C17—H17119.9C104—C105—C106120.6 (4)
O1—C18—C17124.5 (4)C104—C105—H105119.7
O1—C18—C19117.4 (4)C106—C105—H105119.7
C17—C18—C19118.1 (4)C105—C106—C101120.6 (4)
N1—C19—C14123.1 (4)C105—C106—H106119.7
N1—C19—C18115.1 (4)C101—C106—H106119.7
C14—C19—C18121.7 (4)C101—C107—H10A109.5
N2—C21—C22122.1 (4)C101—C107—H10B109.5
N2—C21—H21118.9H10A—C107—H10B109.5
C22—C21—H21118.9C101—C107—H10C109.5
C23—C22—C21119.7 (4)H10A—C107—H10C109.5
C23—C22—H22120.1H10B—C107—H10C109.5
C21—C22—H22120.1C202—C201—C206117.1 (5)
C22—C23—C24120.0 (4)C202—C201—C207120.8 (4)
C22—C23—H23120C206—C201—C207122.1 (5)
C24—C23—H23120C203—C202—C201121.8 (4)
C25—C24—C23124.7 (4)C203—C202—H202119.1
C25—C24—C29118.6 (4)C201—C202—H202119.1
C23—C24—C29116.7 (4)C204—C203—C202120.0 (5)
C26—C25—C24119.3 (4)C204—C203—H203120
C26—C25—H25120.4C202—C203—H203120
C24—C25—H25120.4C205—C204—C203120.1 (6)
C25—C26—C27122.5 (4)C205—C204—H204120
C25—C26—H26118.7C203—C204—H204120
C27—C26—H26118.7C204—C205—C206120.0 (5)
C28—C27—C26119.9 (4)C204—C205—H205120
C28—C27—H27120C206—C205—H205120
C26—C27—H27120C201—C206—C205121.0 (5)
O2—C28—C27124.6 (4)C201—C206—H206119.5
O2—C28—C29117.3 (4)C205—C206—H206119.5
C27—C28—C29118.0 (4)C201—C207—H20A109.5
N2—C29—C24122.8 (4)C201—C207—H20B109.5
N2—C29—C28115.4 (4)H20A—C207—H20B109.5
C24—C29—C28121.7 (4)C201—C207—H20C109.5
N3—C31—C32122.3 (4)H20A—C207—H20C109.5
N3—C31—H31118.9H20B—C207—H20C109.5
C32—C31—H31118.9C11—N1—C19118.5 (4)
C33—C32—C31119.6 (4)C11—N1—Hf128.7 (3)
C33—C32—H32120.2C19—N1—Hf112.7 (3)
C31—C32—H32120.2C21—N2—C29118.5 (4)
C32—C33—C34119.9 (4)C21—N2—Hf129.1 (3)
C32—C33—H33120C29—N2—Hf112.2 (3)
C34—C33—H33120C31—N3—C39118.9 (4)
C35—C34—C33125.0 (4)C31—N3—Hf128.1 (3)
C35—C34—C39118.5 (4)C39—N3—Hf112.9 (2)
C33—C34—C39116.4 (4)C41—N4—C49118.0 (3)
C36—C35—C34119.9 (4)C41—N4—Hf129.4 (3)
C36—C35—H35120C49—N4—Hf112.5 (2)
C34—C35—H35120C18—O1—Hf123.2 (3)
C35—C36—C37121.2 (4)C28—O2—Hf123.8 (3)
C35—C36—H36119.4C38—O3—Hf123.4 (2)
C37—C36—H36119.4C48—O4—Hf123.6 (2)
C38—C37—C36121.3 (4)O2—Hf—O494.50 (11)
C38—C37—H37119.4O2—Hf—O197.00 (11)
C36—C37—H37119.4O4—Hf—O1141.84 (10)
O3—C38—C37125.4 (4)O2—Hf—O3142.31 (11)
O3—C38—C39116.5 (4)O4—Hf—O397.89 (11)
C37—C38—C39118.1 (4)O1—Hf—O394.85 (11)
N3—C39—C34122.9 (4)O2—Hf—N378.53 (12)
N3—C39—C38116.0 (4)O4—Hf—N373.74 (11)
C34—C39—C38121.0 (4)O1—Hf—N3144.27 (11)
N4—C41—C42123.1 (4)O3—Hf—N371.16 (11)
N4—C41—H41118.4O2—Hf—N173.68 (11)
C42—C41—H41118.4O4—Hf—N177.94 (11)
C43—C42—C41119.6 (4)O1—Hf—N170.73 (11)
C43—C42—H42120.2O3—Hf—N1143.78 (11)
C41—C42—H42120.2N3—Hf—N1138.19 (12)
C42—C43—C44119.5 (4)O2—Hf—N271.04 (11)
C42—C43—H43120.2O4—Hf—N2145.17 (11)
C44—C43—H43120.2O1—Hf—N272.67 (11)
C49—C44—C45117.8 (4)O3—Hf—N278.70 (11)
C49—C44—C43116.8 (4)N3—Hf—N272.39 (11)
C45—C44—C43125.4 (4)N1—Hf—N2124.51 (12)
C46—C45—C44120.1 (4)O2—Hf—N4142.23 (11)
C46—C45—H45119.9O4—Hf—N470.84 (11)
C44—C45—H45119.9O1—Hf—N477.98 (11)
C45—C46—C47122.0 (4)O3—Hf—N475.31 (11)
C45—C46—H46119N3—Hf—N4126.37 (12)
C47—C46—H46119N1—Hf—N469.32 (11)
C48—C47—C46120.6 (4)N2—Hf—N4138.57 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C105—H105···O1i0.932.563.467 (5)166
Symmetry code: (i) x, y+1, z.

Experimental details

Crystal data
Chemical formula[Hf(C9H6NO)4]·2C7H8
Mr939.35
Crystal system, space groupTriclinic, P1
Temperature (K)100
a, b, c (Å)11.3323 (5), 12.5539 (5), 15.7126 (7)
α, β, γ (°)69.746 (2), 69.700 (2), 75.787 (2)
V3)1946.79 (14)
Z2
Radiation typeMo Kα
µ (mm1)2.73
Crystal size (mm)0.22 × 0.10 × 0.04
Data collection
DiffractometerBruker X8 APEXII 4K Kappa CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2004)
Tmin, Tmax0.585, 0.899
No. of measured, independent and
observed [I > 2σ(I)] reflections
22928, 8458, 7551
Rint0.044
(sin θ/λ)max1)0.639
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.033, 0.100, 1.04
No. of reflections8458
No. of parameters534
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)1.16, 0.81

Computer programs: APEX2 (Bruker, 2005), SAINT-Plus (Bruker, 2004), SIR92 (Altomare et al., 1999), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg & Putz, 2005), WinGX (Farrugia, 1999).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C105—H105···O1i0.932.563.467 (5)166.1
Symmetry code: (i) x, y+1, z.
 

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