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The structural changes in a crystal of 9-methylanthracene (1) during the [4 + 4] photodimerization were monitored by means of X-ray diffraction. This is the first example in the literature of such a study of a [4 + 4] photodimerization. The results obtained were compared with data for the [2 + 2] photodimerization. The shape of the product molecules and their preferred packing can explain the crystal disintegration. This was the reason that the reaction was monitored only to 28% completion. As far as could be determined the reaction proceeds with a constant rate. The cell volume increases at the beginning of the transformation and decreases afterwards. The product molecules do not assume a fixed position in the crystal during the photo-reaction, but move in a smooth way that includes a rotational component. The movements of the reactant are much smaller. Movements of molecules characterized by a rotational component were also observed in the case of the [2 + 2] photodimerization of 5-benzylidene-2-benzylcyclopentanone and 5-benzylidene-2-(4-chlorobenzyl)-cyclopentanone. The distance between the reacting atoms of the adjacent monomer molecules of (1) decreases with the degree of reaction completion, but more slowly than in the case of the [2 + 2] photodimerizations cited above. The orientation of the neighbouring monomer molecules changes during the phototransformation so that the monomer pair resembles the dimer product.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768103023255/bk0138sup1.cif
Contains datablocks 0D, 3D, 4D, 6D, 8D, 11D, 15D, 18D, 24D, 26D, 28D, 100D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk01380Dsup2.hkl
Contains datablock 0%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk01383Dsup3.hkl
Contains datablock 3%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk01384Dsup4.hkl
Contains datablock 4%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk01386Dsup5.hkl
Contains datablock 6%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk01388Dsup6.hkl
Contains datablock 8%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk013811Dsup7.hkl
Contains datablock 11%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk013815Dsup8.hkl
Contains datablock 15%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk013818Dsup9.hkl
Contains datablock 18%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk013824Dsup10.hkl
Contains datablock 24%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk013826Dsup11.hkl
Contains datablock 26%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk013828Dsup12.hkl
Contains datablock 28%D

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768103023255/bk0138100Dsup13.hkl
Contains datablock 100%D

CCDC references: 227661; 227662; 227663; 227664; 227665; 227666; 227667; 227668; 227669; 227670; 227671; 227672

Computing details top

For all compounds, data collection: Kuma KM4CCD software 2000; cell refinement: Kuma KM4CCD software 2000; data reduction: Kuma KM4CCD software 2000; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 1997; software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

(0D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.233 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8859 (13) ÅCell parameters from 500 reflections
b = 14.594 (2) Åθ = 4–22°
c = 8.0395 (11) ŵ = 0.07 mm1
β = 96.505 (14)°T = 293 K
V = 1035.9 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1262 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.023
Graphite monochromatorθmax = 26.0°, θmin = 4.3°
ω scansh = 1010
3393 measured reflectionsk = 1816
1938 independent reflectionsl = 95
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.060All H-atom parameters refined
wR(F2) = 0.204Calculated w = 1/[σ2(Fo2) + (0.1171P)2 + 0.0477P]
where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max < 0.001
1938 reflectionsΔρmax = 0.22 e Å3
185 parametersΔρmin = 0.19 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.032 (12)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.1009 (3)0.57943 (14)0.3038 (3)0.0641 (6)
C20.2497 (3)0.59727 (17)0.3397 (3)0.0762 (7)
C30.3316 (3)0.64095 (18)0.2223 (3)0.0761 (7)
C40.2611 (2)0.66448 (15)0.0724 (3)0.0639 (6)
C50.1959 (3)0.68064 (13)0.3295 (3)0.0604 (6)
C60.3457 (3)0.66953 (15)0.3674 (3)0.0714 (7)
C70.4329 (3)0.63021 (16)0.2501 (3)0.0709 (7)
C80.3658 (2)0.60228 (14)0.0992 (3)0.0607 (6)
C90.1350 (2)0.58685 (12)0.1057 (2)0.0486 (5)
C100.0323 (2)0.67012 (12)0.1287 (2)0.0516 (5)
C110.0196 (2)0.60296 (12)0.1462 (2)0.0479 (5)
C120.1050 (2)0.64636 (12)0.0266 (2)0.0500 (5)
C130.1208 (2)0.65419 (11)0.1715 (2)0.0476 (5)
C140.2076 (2)0.61278 (11)0.0516 (2)0.0457 (5)
C150.2250 (3)0.5431 (2)0.2326 (3)0.0729 (7)
H10.039 (2)0.5478 (16)0.400 (3)0.086 (7)*
H20.308 (3)0.5794 (17)0.448 (4)0.095 (8)*
H30.444 (3)0.6548 (15)0.252 (3)0.081 (7)*
H40.314 (3)0.6943 (16)0.018 (3)0.080 (7)*
H50.132 (2)0.7084 (13)0.409 (3)0.060 (5)*
H60.397 (3)0.6884 (16)0.476 (3)0.085 (7)*
H70.556 (3)0.6233 (17)0.281 (3)0.096 (8)*
H80.433 (2)0.5754 (16)0.016 (3)0.076 (6)*
H100.092 (2)0.7007 (13)0.214 (3)0.056 (5)*
H15A0.245 (4)0.582 (3)0.310 (6)0.156 (14)*
H15B0.322 (5)0.516 (3)0.180 (6)0.188 (17)*
H15C0.168 (4)0.493 (2)0.293 (4)0.128 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0766 (15)0.0622 (12)0.0519 (12)0.0040 (10)0.0001 (10)0.0040 (9)
C20.0766 (17)0.0821 (15)0.0647 (15)0.0065 (12)0.0146 (12)0.0004 (12)
C30.0562 (15)0.0836 (16)0.0851 (18)0.0042 (11)0.0065 (12)0.0070 (13)
C40.0529 (13)0.0692 (13)0.0700 (15)0.0008 (9)0.0092 (10)0.0006 (11)
C50.0793 (16)0.0527 (11)0.0485 (12)0.0040 (9)0.0043 (10)0.0042 (9)
C60.0798 (17)0.0681 (13)0.0607 (14)0.0002 (11)0.0155 (12)0.0006 (11)
C70.0612 (15)0.0747 (14)0.0735 (15)0.0053 (10)0.0073 (11)0.0046 (11)
C80.0549 (13)0.0614 (12)0.0655 (14)0.0076 (9)0.0061 (10)0.0051 (10)
C90.0563 (12)0.0451 (9)0.0458 (10)0.0020 (7)0.0122 (8)0.0019 (7)
C100.0571 (13)0.0496 (10)0.0497 (11)0.0025 (8)0.0125 (9)0.0045 (8)
C110.0546 (12)0.0444 (9)0.0447 (10)0.0026 (7)0.0051 (8)0.0035 (7)
C120.0507 (11)0.0481 (10)0.0521 (11)0.0008 (7)0.0092 (8)0.0037 (8)
C130.0575 (12)0.0404 (9)0.0449 (11)0.0004 (7)0.0054 (8)0.0026 (7)
C140.0505 (11)0.0409 (9)0.0463 (11)0.0025 (7)0.0077 (8)0.0048 (7)
C150.0798 (18)0.0811 (16)0.0609 (14)0.0067 (13)0.0217 (12)0.0094 (13)
Geometric parameters (Å, º) top
C1—C21.347 (3)C7—H71.10 (3)
C1—C111.428 (3)C8—C141.422 (3)
C1—H11.10 (2)C8—H81.03 (2)
C2—C31.408 (4)C9—C111.396 (3)
C2—H21.00 (3)C9—C141.405 (3)
C3—C41.338 (3)C9—C151.508 (3)
C3—H31.02 (2)C10—C121.384 (3)
C4—C121.419 (3)C10—C131.385 (3)
C4—H41.00 (2)C10—H101.02 (2)
C5—C61.342 (3)C11—C121.438 (3)
C5—C131.419 (3)C13—C141.435 (2)
C5—H50.99 (2)C15—H15A0.88 (5)
C6—C71.409 (3)C15—H15B0.99 (5)
C6—H60.97 (3)C15—H15C0.99 (4)
C7—C81.353 (3)
C2—C1—C11122.0 (2)C11—C9—C14120.27 (16)
C2—C1—H1119.2 (12)C11—C9—C15119.81 (19)
C11—C1—H1118.8 (13)C14—C9—C15119.91 (19)
C1—C2—C3120.9 (2)C12—C10—C13121.86 (17)
C1—C2—H2122.3 (15)C12—C10—H10119.5 (11)
C3—C2—H2116.8 (15)C13—C10—H10118.7 (11)
C4—C3—C2119.7 (2)C9—C11—C1123.53 (18)
C4—C3—H3120.6 (14)C9—C11—C12119.91 (17)
C2—C3—H3119.8 (14)C1—C11—C12116.55 (19)
C3—C4—C12122.0 (2)C10—C12—C4122.05 (18)
C3—C4—H4123.5 (13)C10—C12—C11119.05 (18)
C12—C4—H4114.5 (13)C4—C12—C11118.89 (19)
C6—C5—C13121.6 (2)C10—C13—C5121.73 (18)
C6—C5—H5122.1 (11)C10—C13—C14119.45 (17)
C13—C5—H5116.2 (12)C5—C13—C14118.78 (18)
C5—C6—C7120.3 (2)C9—C14—C8123.49 (17)
C5—C6—H6121.1 (14)C9—C14—C13119.43 (17)
C7—C6—H6118.7 (14)C8—C14—C13117.06 (17)
C8—C7—C6120.2 (2)C9—C15—H15A112 (2)
C8—C7—H7120.3 (14)C9—C15—H15B112 (3)
C6—C7—H7119.5 (14)H15A—C15—H15B109 (3)
C7—C8—C14122.1 (2)C9—C15—H15C111.5 (18)
C7—C8—H8117.9 (12)H15A—C15—H15C105 (3)
C14—C8—H8119.9 (12)H15B—C15—H15C107 (3)
(3D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.232 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8804 (14) ÅCell parameters from 500 reflections
b = 14.593 (3) Åθ = 4–22°
c = 8.0508 (14) ŵ = 0.07 mm1
β = 96.460 (16)°T = 293 K
V = 1036.7 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1231 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.024
Graphite monochromatorθmax = 26.0°, θmin = 4.6°
ω scansh = 1010
3403 measured reflectionsk = 1816
1938 independent reflectionsl = 95
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.068H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.238Calculated w = 1/[σ2(Fo2) + (0.1495P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max < 0.001
1938 reflectionsΔρmax = 0.31 e Å3
198 parametersΔρmin = 0.21 e Å3
184 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.015 (12)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C1M1.1009 (3)0.42021 (16)0.3037 (3)0.0650 (7)0.971 (3)
H1M1.04930.44850.38400.078*0.971 (3)
C2M1.2503 (3)0.40254 (18)0.3396 (3)0.0758 (7)0.971 (3)
H2M1.29960.41930.44320.091*0.971 (3)
C3M1.3322 (3)0.35933 (19)0.2228 (4)0.0767 (8)0.971 (3)
H3M1.43500.34730.24910.092*0.971 (3)
C4M1.2616 (3)0.33536 (17)0.0724 (4)0.0647 (7)0.971 (3)
H4M1.31660.30600.00370.078*0.971 (3)
C5M0.8047 (3)0.31924 (14)0.3287 (3)0.0594 (6)0.971 (3)
H5M0.86100.29350.40750.071*0.971 (3)
C6M0.6542 (3)0.33036 (16)0.3671 (3)0.0721 (7)0.971 (3)
H6M0.60770.31200.47100.087*0.971 (3)
C7M0.5677 (3)0.36962 (17)0.2502 (3)0.0727 (7)0.971 (3)
H7M0.46360.37650.27640.087*0.971 (3)
C8M0.6347 (3)0.39746 (17)0.1000 (3)0.0608 (6)0.971 (3)
H8M0.57530.42440.02540.073*0.971 (3)
C9M0.8654 (2)0.41317 (13)0.1060 (2)0.0487 (6)0.971 (3)
C10M1.0328 (2)0.33010 (13)0.1277 (2)0.0517 (6)0.971 (3)
H10M1.08850.30270.20540.062*0.971 (3)
C11M1.0199 (2)0.39673 (13)0.1465 (3)0.0479 (6)0.971 (3)
C12M1.1055 (2)0.35368 (13)0.0268 (3)0.0499 (6)0.971 (3)
C13M0.8796 (2)0.34578 (12)0.1711 (2)0.0482 (6)0.971 (3)
C14M0.7923 (2)0.38714 (13)0.0515 (2)0.0457 (5)0.971 (3)
C15M0.7744 (3)0.45683 (16)0.2320 (3)0.0711 (7)0.971 (3)
H15A0.67100.46350.18410.107*0.971 (3)
H15B0.81580.51600.26260.107*0.971 (3)
H15C0.77840.41880.32970.107*0.971 (3)
C1D1.097 (6)0.398 (4)0.366 (4)0.086 (16)*0.029 (3)
C2D1.232 (6)0.353 (5)0.413 (5)0.083 (19)*0.029 (3)
C3D1.323 (6)0.333 (5)0.289 (6)0.09 (2)*0.029 (3)
C4D1.284 (5)0.356 (5)0.122 (6)0.053 (15)*0.029 (3)
C5D0.865 (5)0.357 (4)0.283 (5)0.056 (15)*0.029 (3)
C6D0.710 (6)0.342 (5)0.317 (7)0.10 (3)*0.029 (3)
C7D0.618 (5)0.363 (6)0.196 (7)0.08 (2)*0.029 (3)
C8D0.676 (4)0.401 (5)0.044 (7)0.052 (19)*0.029 (3)
C9D0.903 (3)0.4656 (19)0.146 (4)0.069 (10)*0.029 (3)
C10D1.086 (3)0.4264 (19)0.100 (4)0.061 (15)*0.029 (3)
C11D1.058 (4)0.423 (3)0.199 (4)0.024 (8)*0.029 (3)
C12D1.149 (4)0.403 (3)0.076 (4)0.077 (18)*0.029 (3)
C13D0.922 (4)0.395 (3)0.131 (4)0.065 (16)*0.029 (3)
C14D0.830 (3)0.413 (3)0.002 (4)0.028 (9)*0.029 (3)
C15D0.830 (5)0.466 (3)0.312 (5)0.046 (13)*0.029 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.0792 (16)0.0628 (13)0.0517 (14)0.0032 (11)0.0019 (11)0.0047 (10)
C2M0.0759 (17)0.0808 (16)0.0659 (16)0.0061 (12)0.0133 (12)0.0010 (12)
C3M0.0552 (15)0.0847 (18)0.087 (2)0.0050 (11)0.0069 (13)0.0105 (15)
C4M0.0523 (14)0.0712 (15)0.0713 (16)0.0010 (10)0.0096 (11)0.0004 (12)
C5M0.0786 (16)0.0520 (12)0.0470 (12)0.0027 (10)0.0043 (10)0.0060 (9)
C6M0.0821 (18)0.0679 (14)0.0608 (15)0.0001 (12)0.0166 (12)0.0013 (11)
C7M0.0606 (15)0.0772 (16)0.0763 (17)0.0063 (12)0.0093 (13)0.0052 (13)
C8M0.0550 (14)0.0612 (14)0.0657 (16)0.0072 (10)0.0051 (12)0.0034 (12)
C9M0.0571 (12)0.0446 (10)0.0459 (12)0.0009 (8)0.0123 (8)0.0010 (8)
C10M0.0580 (13)0.0496 (11)0.0491 (12)0.0026 (8)0.0137 (9)0.0041 (8)
C11M0.0545 (13)0.0437 (10)0.0450 (12)0.0045 (8)0.0035 (9)0.0020 (8)
C12M0.0497 (12)0.0468 (10)0.0539 (12)0.0023 (8)0.0093 (9)0.0030 (8)
C13M0.0586 (13)0.0405 (10)0.0458 (12)0.0002 (8)0.0069 (9)0.0025 (8)
C14M0.0520 (12)0.0395 (10)0.0460 (12)0.0016 (8)0.0071 (9)0.0029 (8)
C15M0.0768 (16)0.0802 (15)0.0585 (15)0.0053 (12)0.0175 (12)0.0090 (11)
Geometric parameters (Å, º) top
C1M—C2M1.351 (3)C1D—C11D1.394 (18)
C1M—C11M1.426 (3)C2D—C3D1.384 (19)
C2M—C3M1.402 (4)C3D—C4D1.388 (19)
C3M—C4M1.345 (4)C4D—C12D1.391 (18)
C4M—C12M1.419 (3)C5D—C6D1.388 (19)
C5M—C6M1.347 (3)C5D—C13D1.391 (18)
C5M—C13M1.418 (3)C6D—C7D1.380 (19)
C6M—C7M1.402 (3)C7D—C8D1.382 (19)
C7M—C8M1.349 (4)C8D—C14D1.389 (18)
C8M—C14M1.418 (3)C9D—C14D1.500 (17)
C9M—C11M1.395 (3)C9D—C11D1.525 (17)
C9M—C14M1.410 (3)C9D—C15D1.548 (18)
C9M—C15M1.508 (3)C9D—C10Di1.624 (18)
C10M—C12M1.380 (3)C10D—C12D1.503 (17)
C10M—C13M1.385 (3)C10D—C13D1.517 (17)
C11M—C12M1.437 (3)C10D—C9Di1.624 (18)
C13M—C14M1.435 (3)C11D—C12D1.389 (17)
C1D—C2D1.386 (19)C13D—C14D1.415 (17)
C2M—C1M—C11M122.0 (2)C3D—C4D—C12D120 (2)
C1M—C2M—C3M120.9 (2)C6D—C5D—C13D119 (2)
C4M—C3M—C2M119.7 (2)C7D—C6D—C5D119 (2)
C3M—C4M—C12M121.8 (2)C6D—C7D—C8D121 (2)
C6M—C5M—C13M121.7 (2)C7D—C8D—C14D122 (2)
C5M—C6M—C7M120.0 (2)C14D—C9D—C11D108.0 (19)
C8M—C7M—C6M120.3 (2)C14D—C9D—C15D121 (2)
C7M—C8M—C14M122.5 (2)C11D—C9D—C15D102.1 (19)
C11M—C9M—C14M120.33 (18)C14D—C9D—C10Di110 (2)
C11M—C9M—C15M120.20 (19)C11D—C9D—C10Di112 (2)
C14M—C9M—C15M119.46 (18)C15D—C9D—C10Di103 (2)
C12M—C10M—C13M122.19 (18)C12D—C10D—C13D110 (2)
C9M—C11M—C1M123.43 (19)C12D—C10D—C9Di114 (2)
C9M—C11M—C12M119.95 (19)C13D—C10D—C9Di110 (2)
C1M—C11M—C12M116.62 (19)C12D—C11D—C1D122 (2)
C10M—C12M—C4M122.1 (2)C12D—C11D—C9D118.0 (18)
C10M—C12M—C11M118.98 (19)C1D—C11D—C9D120 (2)
C4M—C12M—C11M119.0 (2)C11D—C12D—C4D118 (2)
C10M—C13M—C5M121.91 (18)C11D—C12D—C10D116.1 (19)
C10M—C13M—C14M119.34 (18)C4D—C12D—C10D126 (2)
C5M—C13M—C14M118.72 (19)C5D—C13D—C14D122 (2)
C9M—C14M—C8M123.99 (18)C5D—C13D—C10D121 (2)
C9M—C14M—C13M119.20 (18)C14D—C13D—C10D116.7 (19)
C8M—C14M—C13M116.80 (19)C8D—C14D—C13D116 (2)
C2D—C1D—C11D120 (2)C8D—C14D—C9D126 (2)
C3D—C2D—C1D117 (2)C13D—C14D—C9D116.5 (18)
C2D—C3D—C4D123 (2)
Symmetry code: (i) x+2, y+1, z.
(4D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.231 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8789 (13) ÅCell parameters from 500 reflections
b = 14.592 (2) Åθ = 4–22°
c = 8.0602 (12) ŵ = 0.07 mm1
β = 96.480 (16)°T = 293 K
V = 1037.6 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1214 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.025
Graphite monochromatorθmax = 26.0°, θmin = 4.6°
ω scansh = 1010
3396 measured reflectionsk = 1816
1937 independent reflectionsl = 95
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.069H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.238Calculated w = 1/[σ2(Fo2) + (0.146P)2 + 0.0231P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
1937 reflectionsΔρmax = 0.31 e Å3
198 parametersΔρmin = 0.18 e Å3
184 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.007 (10)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C1M1.1014 (3)0.42008 (17)0.3037 (3)0.0660 (7)0.956 (3)
H1M1.04980.44830.38390.079*0.956 (3)
C2M1.2509 (3)0.40255 (19)0.3401 (3)0.0770 (8)0.956 (3)
H2M1.30010.41950.44350.092*0.956 (3)
C3M1.3324 (3)0.3590 (2)0.2235 (5)0.0789 (8)0.956 (3)
H3M1.43500.34640.25010.095*0.956 (3)
C4M1.2620 (3)0.33538 (18)0.0731 (4)0.0651 (7)0.956 (3)
H4M1.31720.30630.00310.078*0.956 (3)
C5M0.8056 (3)0.31908 (15)0.3281 (3)0.0600 (7)0.956 (3)
H5M0.86200.29350.40690.072*0.956 (3)
C6M0.6549 (3)0.33015 (17)0.3665 (3)0.0734 (8)0.956 (3)
H6M0.60830.31150.47020.088*0.956 (3)
C7M0.5685 (3)0.36974 (18)0.2500 (3)0.0726 (8)0.956 (3)
H7M0.46450.37690.27660.087*0.956 (3)
C8M0.6349 (3)0.39742 (18)0.1001 (3)0.0609 (7)0.956 (3)
H8M0.57530.42420.02560.073*0.956 (3)
C9M0.8654 (2)0.41280 (13)0.1056 (2)0.0496 (6)0.956 (3)
C10M1.0336 (2)0.33006 (14)0.1274 (3)0.0528 (6)0.956 (3)
H10M1.08960.30300.20510.063*0.956 (3)
C11M1.0198 (2)0.39684 (14)0.1462 (3)0.0484 (6)0.956 (3)
C12M1.1061 (2)0.35357 (14)0.0275 (3)0.0512 (6)0.956 (3)
C13M0.8803 (2)0.34550 (12)0.1705 (2)0.0492 (6)0.956 (3)
C14M0.7926 (2)0.38715 (14)0.0517 (3)0.0465 (6)0.956 (3)
C15M0.7740 (3)0.45678 (18)0.2318 (3)0.0703 (7)0.956 (3)
H15A0.67060.46350.18380.105*0.956 (3)
H15B0.81550.51600.26210.105*0.956 (3)
H15C0.77790.41880.32940.105*0.956 (3)
C1D1.084 (4)0.395 (3)0.366 (4)0.079 (14)*0.044 (3)
C2D1.225 (4)0.358 (3)0.417 (4)0.071 (13)*0.044 (3)
C3D1.324 (4)0.345 (3)0.299 (5)0.09 (2)*0.044 (3)
C4D1.289 (4)0.367 (3)0.131 (5)0.056 (12)*0.044 (3)
C5D0.875 (4)0.358 (3)0.289 (4)0.056 (11)*0.044 (3)
C6D0.724 (4)0.335 (4)0.328 (5)0.10 (2)*0.044 (3)
C7D0.626 (4)0.353 (4)0.210 (6)0.10 (2)*0.044 (3)
C8D0.678 (3)0.392 (4)0.059 (5)0.044 (14)*0.044 (3)
C9D0.896 (3)0.4638 (16)0.140 (3)0.065 (9)*0.044 (3)
C10D1.089 (3)0.4282 (16)0.096 (3)0.049 (10)*0.044 (3)
C11D1.048 (3)0.418 (2)0.198 (3)0.029 (8)*0.044 (3)
C12D1.147 (3)0.404 (3)0.080 (3)0.071 (13)*0.044 (3)
C13D0.925 (3)0.400 (2)0.139 (3)0.059 (11)*0.044 (3)
C14D0.828 (3)0.414 (2)0.013 (3)0.036 (9)*0.044 (3)
C15D0.826 (4)0.466 (3)0.307 (4)0.053 (11)*0.044 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.0810 (18)0.0653 (15)0.0506 (15)0.0024 (12)0.0027 (11)0.0042 (11)
C2M0.0765 (18)0.0810 (17)0.0684 (17)0.0050 (13)0.0138 (13)0.0013 (13)
C3M0.0574 (17)0.0866 (19)0.089 (2)0.0033 (13)0.0059 (14)0.0112 (16)
C4M0.0535 (15)0.0702 (15)0.0717 (16)0.0002 (11)0.0078 (11)0.0021 (13)
C5M0.0799 (18)0.0521 (13)0.0474 (13)0.0037 (11)0.0047 (11)0.0059 (9)
C6M0.0819 (19)0.0671 (15)0.0656 (16)0.0001 (13)0.0156 (13)0.0016 (12)
C7M0.0614 (16)0.0756 (17)0.0772 (17)0.0058 (13)0.0080 (13)0.0051 (13)
C8M0.0566 (15)0.0611 (15)0.0647 (16)0.0089 (12)0.0047 (13)0.0054 (12)
C9M0.0578 (13)0.0459 (11)0.0468 (12)0.0005 (9)0.0135 (9)0.0013 (8)
C10M0.0576 (14)0.0513 (11)0.0516 (13)0.0022 (9)0.0153 (9)0.0047 (9)
C11M0.0564 (14)0.0440 (11)0.0446 (12)0.0026 (9)0.0046 (9)0.0023 (9)
C12M0.0517 (13)0.0473 (11)0.0556 (13)0.0018 (8)0.0103 (9)0.0017 (9)
C13M0.0615 (14)0.0398 (10)0.0471 (13)0.0008 (8)0.0089 (9)0.0030 (8)
C14M0.0514 (13)0.0411 (11)0.0474 (12)0.0021 (9)0.0069 (9)0.0034 (9)
C15M0.0764 (16)0.0787 (16)0.0574 (15)0.0064 (12)0.0146 (12)0.0076 (12)
Geometric parameters (Å, º) top
C1M—C2M1.351 (3)C1D—C11D1.397 (17)
C1M—C11M1.430 (3)C2D—C3D1.380 (19)
C2M—C3M1.402 (4)C3D—C4D1.392 (18)
C3M—C4M1.345 (4)C4D—C12D1.395 (18)
C4M—C12M1.417 (3)C5D—C6D1.384 (19)
C5M—C6M1.349 (4)C5D—C13D1.384 (17)
C5M—C13M1.418 (3)C6D—C7D1.382 (19)
C6M—C7M1.402 (4)C7D—C8D1.379 (19)
C7M—C8M1.345 (4)C8D—C14D1.380 (18)
C8M—C14M1.418 (3)C9D—C14D1.496 (16)
C9M—C11M1.393 (3)C9D—C11D1.531 (17)
C9M—C14M1.407 (3)C9D—C15D1.551 (18)
C9M—C15M1.513 (3)C9D—C10Di1.623 (17)
C10M—C12M1.381 (3)C10D—C12D1.500 (17)
C10M—C13M1.385 (3)C10D—C13D1.516 (17)
C11M—C12M1.438 (3)C10D—C9Di1.623 (17)
C13M—C14M1.436 (3)C11D—C12D1.383 (17)
C1D—C2D1.387 (18)C13D—C14D1.418 (17)
C2M—C1M—C11M122.4 (2)C3D—C4D—C12D118 (2)
C1M—C2M—C3M120.6 (2)C6D—C5D—C13D121 (2)
C4M—C3M—C2M119.8 (2)C7D—C6D—C5D118 (2)
C3M—C4M—C12M121.8 (2)C8D—C7D—C6D121 (2)
C6M—C5M—C13M121.7 (2)C7D—C8D—C14D123 (2)
C5M—C6M—C7M119.9 (2)C14D—C9D—C11D107.5 (18)
C8M—C7M—C6M120.6 (3)C14D—C9D—C15D124 (2)
C7M—C8M—C14M122.3 (2)C11D—C9D—C15D99.6 (17)
C11M—C9M—C14M120.47 (19)C14D—C9D—C10Di109.4 (18)
C11M—C9M—C15M120.1 (2)C11D—C9D—C10Di113.3 (18)
C14M—C9M—C15M119.45 (19)C15D—C9D—C10Di102.6 (18)
C12M—C10M—C13M122.05 (18)C12D—C10D—C13D111.3 (18)
C9M—C11M—C1M123.8 (2)C12D—C10D—C9Di114 (2)
C9M—C11M—C12M120.1 (2)C13D—C10D—C9Di108.8 (19)
C1M—C11M—C12M116.1 (2)C12D—C11D—C1D122.2 (18)
C10M—C12M—C4M122.0 (2)C12D—C11D—C9D117.5 (17)
C10M—C12M—C11M118.8 (2)C1D—C11D—C9D120.3 (19)
C4M—C12M—C11M119.2 (2)C11D—C12D—C4D119.0 (18)
C10M—C13M—C5M121.84 (19)C11D—C12D—C10D116.2 (18)
C10M—C13M—C14M119.58 (19)C4D—C12D—C10D125 (2)
C5M—C13M—C14M118.6 (2)C5D—C13D—C14D122.1 (18)
C9M—C14M—C8M123.96 (19)C5D—C13D—C10D121.4 (19)
C9M—C14M—C13M118.99 (19)C14D—C13D—C10D116.5 (17)
C8M—C14M—C13M117.0 (2)C8D—C14D—C13D114.9 (19)
C2D—C1D—C11D119 (2)C8D—C14D—C9D128 (2)
C3D—C2D—C1D118 (2)C13D—C14D—C9D115.9 (17)
C2D—C3D—C4D124 (2)
Symmetry code: (i) x+2, y+1, z.
(6D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.230 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8738 (13) ÅCell parameters from 500 reflections
b = 14.593 (2) Åθ = 4–22°
c = 8.0674 (12) ŵ = 0.07 mm1
β = 96.465 (15)°T = 293 K
V = 1038.0 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1205 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.028
Graphite monochromatorθmax = 26.0°, θmin = 4.6°
ω scansh = 1010
3401 measured reflectionsk = 1816
1940 independent reflectionsl = 95
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.071H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.245Calculated w = 1/[σ2(Fo2) + (0.1343P)2 + 0.1501P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
1940 reflectionsΔρmax = 0.26 e Å3
198 parametersΔρmin = 0.21 e Å3
184 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.009 (10)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C1M1.1012 (3)0.42020 (19)0.3035 (4)0.0656 (8)0.936 (3)
H1M1.04930.44870.38310.079*0.936 (3)
C2M1.2508 (4)0.4026 (2)0.3405 (4)0.0779 (9)0.936 (3)
H2M1.29960.41940.44410.093*0.936 (3)
C3M1.3327 (3)0.3595 (2)0.2245 (5)0.0799 (10)0.936 (3)
H3M1.43540.34720.25120.096*0.936 (3)
C4M1.2622 (3)0.3357 (2)0.0734 (4)0.0663 (8)0.936 (3)
H4M1.31770.30670.00260.080*0.936 (3)
C5M0.8063 (4)0.31899 (18)0.3282 (3)0.0618 (8)0.936 (3)
H5M0.86250.29330.40690.074*0.936 (3)
C6M0.6551 (4)0.3303 (2)0.3660 (4)0.0744 (9)0.936 (3)
H6M0.60830.31190.46960.089*0.936 (3)
C7M0.5687 (4)0.3696 (2)0.2496 (4)0.0724 (9)0.936 (3)
H7M0.46470.37660.27630.087*0.936 (3)
C8M0.6341 (4)0.3973 (2)0.1004 (4)0.0625 (9)0.936 (3)
H8M0.57420.42420.02630.075*0.936 (3)
C9M0.8651 (3)0.41276 (15)0.1056 (3)0.0497 (6)0.936 (3)
C10M1.0333 (3)0.32984 (16)0.1271 (3)0.0533 (7)0.936 (3)
H10M1.08900.30220.20440.064*0.936 (3)
C11M1.0201 (3)0.39652 (16)0.1465 (3)0.0483 (7)0.936 (3)
C12M1.1063 (3)0.35362 (16)0.0276 (3)0.0509 (6)0.936 (3)
C13M0.8809 (3)0.34567 (14)0.1703 (3)0.0493 (6)0.936 (3)
C14M0.7928 (3)0.38698 (17)0.0514 (3)0.0466 (6)0.936 (3)
C15M0.7733 (3)0.4566 (2)0.2312 (4)0.0702 (9)0.936 (3)
H15A0.66990.46320.18300.105*0.936 (3)
H15B0.81460.51590.26160.105*0.936 (3)
H15C0.77700.41860.32870.105*0.936 (3)
C1D1.077 (4)0.398 (3)0.365 (3)0.078 (12)*0.064 (3)
C2D1.216 (4)0.359 (3)0.422 (4)0.095 (13)*0.064 (3)
C3D1.316 (4)0.342 (3)0.305 (4)0.103 (18)*0.064 (3)
C4D1.283 (3)0.361 (3)0.136 (4)0.052 (10)*0.064 (3)
C5D0.881 (4)0.352 (3)0.287 (4)0.078 (12)*0.064 (3)
C6D0.731 (4)0.327 (3)0.332 (4)0.060 (14)*0.064 (3)
C7D0.631 (4)0.348 (3)0.218 (5)0.088 (16)*0.064 (3)
C8D0.677 (3)0.394 (3)0.071 (5)0.052 (14)*0.064 (3)
C9D0.891 (2)0.4639 (15)0.133 (3)0.069 (8)*0.064 (3)
C10D1.090 (3)0.4274 (15)0.095 (3)0.066 (10)*0.064 (3)
C11D1.044 (3)0.4212 (19)0.197 (3)0.036 (5)*0.064 (3)
C12D1.143 (3)0.403 (3)0.082 (3)0.080 (12)*0.064 (3)
C13D0.928 (3)0.398 (2)0.141 (3)0.069 (10)*0.064 (3)
C14D0.827 (3)0.413 (2)0.018 (3)0.041 (5)*0.064 (3)
C15D0.812 (4)0.463 (3)0.294 (4)0.076 (14)*0.064 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.079 (2)0.0644 (16)0.0522 (17)0.0023 (14)0.0026 (13)0.0035 (13)
C2M0.078 (2)0.083 (2)0.0682 (19)0.0066 (15)0.0135 (15)0.0019 (15)
C3M0.0571 (19)0.088 (2)0.090 (3)0.0065 (15)0.0105 (17)0.0113 (19)
C4M0.0533 (17)0.0722 (18)0.073 (2)0.0003 (12)0.0075 (13)0.0030 (16)
C5M0.078 (2)0.0565 (16)0.0507 (15)0.0040 (14)0.0051 (13)0.0054 (11)
C6M0.083 (2)0.0703 (18)0.0641 (19)0.0001 (15)0.0166 (16)0.0004 (14)
C7M0.0572 (18)0.0772 (19)0.080 (2)0.0070 (15)0.0068 (14)0.0035 (15)
C8M0.0514 (18)0.0638 (18)0.072 (2)0.0085 (15)0.0047 (15)0.0057 (14)
C9M0.0562 (15)0.0464 (13)0.0482 (14)0.0006 (10)0.0132 (10)0.0020 (9)
C10M0.0575 (16)0.0502 (13)0.0545 (15)0.0022 (10)0.0162 (11)0.0044 (10)
C11M0.0553 (15)0.0440 (12)0.0449 (13)0.0038 (10)0.0018 (10)0.0009 (10)
C12M0.0492 (14)0.0477 (12)0.0563 (14)0.0012 (9)0.0078 (10)0.0041 (10)
C13M0.0611 (16)0.0405 (12)0.0465 (14)0.0025 (10)0.0071 (10)0.0032 (9)
C14M0.0507 (15)0.0418 (13)0.0474 (14)0.0008 (10)0.0060 (10)0.0028 (10)
C15M0.0731 (19)0.0802 (19)0.0585 (18)0.0050 (14)0.0133 (14)0.0088 (15)
Geometric parameters (Å, º) top
C1M—C2M1.352 (4)C1D—C11D1.394 (17)
C1M—C11M1.427 (4)C2D—C3D1.385 (18)
C2M—C3M1.398 (4)C3D—C4D1.394 (18)
C3M—C4M1.351 (4)C4D—C12D1.401 (17)
C4M—C12M1.415 (3)C5D—C6D1.382 (18)
C5M—C6M1.352 (4)C5D—C13D1.384 (17)
C5M—C13M1.422 (3)C6D—C7D1.382 (19)
C6M—C7M1.400 (4)C7D—C8D1.381 (18)
C7M—C8M1.338 (4)C8D—C14D1.379 (17)
C8M—C14M1.428 (4)C9D—C14D1.489 (16)
C9M—C11M1.398 (3)C9D—C11D1.531 (16)
C9M—C14M1.405 (3)C9D—C15D1.547 (18)
C9M—C15M1.512 (3)C9D—C10Di1.627 (17)
C10M—C13M1.378 (3)C10D—C12D1.497 (16)
C10M—C12M1.384 (3)C10D—C13D1.510 (17)
C11M—C12M1.436 (3)C10D—C9Di1.627 (17)
C13M—C14M1.436 (3)C11D—C12D1.379 (17)
C1D—C2D1.386 (18)C13D—C14D1.427 (17)
C2M—C1M—C11M122.3 (3)C3D—C4D—C12D118 (2)
C1M—C2M—C3M120.6 (3)C6D—C5D—C13D122 (2)
C4M—C3M—C2M119.8 (3)C7D—C6D—C5D116 (2)
C3M—C4M—C12M121.8 (3)C8D—C7D—C6D122 (2)
C6M—C5M—C13M121.2 (3)C14D—C8D—C7D123 (2)
C5M—C6M—C7M120.2 (3)C14D—C9D—C11D108.6 (17)
C8M—C7M—C6M120.8 (3)C14D—C9D—C15D121 (2)
C7M—C8M—C14M122.1 (3)C11D—C9D—C15D100.6 (18)
C11M—C9M—C14M120.3 (2)C14D—C9D—C10Di111.7 (17)
C11M—C9M—C15M120.2 (2)C11D—C9D—C10Di110.9 (17)
C14M—C9M—C15M119.5 (2)C15D—C9D—C10Di103.5 (19)
C13M—C10M—C12M122.2 (2)C12D—C10D—C13D110.7 (18)
C9M—C11M—C1M123.5 (2)C12D—C10D—C9Di112.9 (19)
C9M—C11M—C12M120.0 (2)C13D—C10D—C9Di110.2 (18)
C1M—C11M—C12M116.4 (2)C12D—C11D—C1D122.0 (18)
C10M—C12M—C4M122.3 (2)C12D—C11D—C9D117.5 (16)
C10M—C12M—C11M118.7 (2)C1D—C11D—C9D120.5 (18)
C4M—C12M—C11M119.0 (2)C11D—C12D—C4D118.9 (17)
C10M—C13M—C5M121.7 (2)C11D—C12D—C10D116.2 (17)
C10M—C13M—C14M119.6 (2)C4D—C12D—C10D125 (2)
C5M—C13M—C14M118.7 (2)C5D—C13D—C14D121.1 (18)
C9M—C14M—C8M123.9 (2)C5D—C13D—C10D122.3 (19)
C9M—C14M—C13M119.2 (2)C14D—C13D—C10D116.4 (17)
C8M—C14M—C13M117.0 (2)C8D—C14D—C13D114.5 (18)
C2D—C1D—C11D120 (2)C8D—C14D—C9D128.5 (19)
C3D—C2D—C1D118 (2)C13D—C14D—C9D115.6 (16)
C2D—C3D—C4D123 (2)
Symmetry code: (i) x+2, y+1, z.
(8D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.229 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8718 (13) ÅCell parameters from 500 reflections
b = 14.587 (2) Åθ = 4–22°
c = 8.0776 (12) ŵ = 0.07 mm1
β = 96.489 (15)°T = 293 K
V = 1038.6 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1171 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.028
Graphite monochromatorθmax = 26.0°, θmin = 4.3°
ω scansh = 1010
3389 measured reflectionsk = 1716
1942 independent reflectionsl = 95
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.074H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.265Calculated w = 1/[σ2(Fo2) + (0.1577P)2 + 0.0018P]
where P = (Fo2 + 2Fc2)/3
S = 1.15(Δ/σ)max < 0.001
1942 reflectionsΔρmax = 0.32 e Å3
198 parametersΔρmin = 0.19 e Å3
172 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.009 (12)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C1M1.1010 (3)0.42003 (19)0.3035 (4)0.0675 (8)0.918 (4)
H1M1.04890.44840.38310.081*0.918 (4)
C2M1.2510 (4)0.4025 (2)0.3407 (4)0.0798 (9)0.918 (4)
H2M1.29980.41920.44430.096*0.918 (4)
C3M1.3331 (3)0.3595 (2)0.2247 (5)0.0829 (10)0.918 (4)
H3M1.43580.34720.25160.099*0.918 (4)
C4M1.2629 (3)0.3358 (2)0.0733 (5)0.0683 (9)0.918 (4)
H4M1.31860.30710.00280.082*0.918 (4)
C5M0.8059 (4)0.31914 (18)0.3275 (3)0.0638 (8)0.918 (4)
H5M0.86230.29380.40640.077*0.918 (4)
C6M0.6551 (4)0.33010 (19)0.3656 (4)0.0776 (9)0.918 (4)
H6M0.60850.31140.46900.093*0.918 (4)
C7M0.5688 (4)0.3694 (2)0.2500 (4)0.0745 (9)0.918 (4)
H7M0.46480.37650.27720.089*0.918 (4)
C8M0.6335 (4)0.3970 (3)0.1009 (4)0.0643 (9)0.918 (4)
H8M0.57340.42370.02700.077*0.918 (4)
C9M0.8650 (3)0.41288 (16)0.1055 (3)0.0524 (7)0.918 (4)
C10M1.0337 (3)0.32980 (15)0.1268 (3)0.0552 (7)0.918 (4)
H10M1.08950.30250.20410.066*0.918 (4)
C11M1.0202 (3)0.39649 (19)0.1464 (4)0.0508 (7)0.918 (4)
C12M1.1067 (3)0.35351 (17)0.0277 (3)0.0531 (7)0.918 (4)
C13M0.8808 (3)0.34536 (14)0.1700 (3)0.0517 (7)0.918 (4)
C14M0.7930 (3)0.38686 (18)0.0518 (3)0.0481 (7)0.918 (4)
C15M0.7723 (3)0.4564 (2)0.2302 (4)0.0720 (9)0.918 (4)
H15A0.66900.46280.18140.108*0.918 (4)
H15B0.81320.51570.26110.108*0.918 (4)
H15C0.77570.41830.32750.108*0.918 (4)
C1D1.070 (3)0.396 (2)0.363 (3)0.086 (11)*0.082 (4)
C2D1.209 (3)0.359 (2)0.421 (3)0.076 (8)*0.082 (4)
C3D1.313 (3)0.342 (2)0.309 (4)0.108 (15)*0.082 (4)
C4D1.280 (3)0.360 (2)0.139 (4)0.058 (9)*0.082 (4)
C5D0.881 (3)0.349 (2)0.283 (3)0.077 (10)*0.082 (4)
C6D0.730 (4)0.327 (2)0.329 (4)0.095 (19)*0.082 (4)
C7D0.629 (3)0.352 (3)0.220 (4)0.082 (13)*0.082 (4)
C8D0.676 (3)0.399 (3)0.075 (4)0.044 (7)*0.082 (4)
C9D0.889 (2)0.4669 (13)0.133 (2)0.080 (8)*0.082 (4)
C10D1.090 (2)0.4249 (13)0.094 (2)0.064 (7)*0.082 (4)
C11D1.040 (2)0.4197 (16)0.194 (3)0.035 (7)*0.082 (4)
C12D1.141 (2)0.400 (2)0.082 (2)0.071 (9)*0.082 (4)
C13D0.926 (2)0.3969 (19)0.137 (3)0.072 (9)*0.082 (4)
C14D0.824 (2)0.4161 (16)0.019 (3)0.038 (7)*0.082 (4)
C15D0.810 (4)0.466 (3)0.294 (3)0.080 (12)*0.082 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.080 (2)0.0650 (16)0.0561 (17)0.0014 (14)0.0034 (14)0.0055 (13)
C2M0.079 (2)0.082 (2)0.073 (2)0.0066 (15)0.0125 (15)0.0027 (15)
C3M0.0582 (19)0.093 (2)0.093 (3)0.0028 (15)0.0102 (18)0.0063 (19)
C4M0.0576 (18)0.0734 (19)0.074 (2)0.0010 (12)0.0083 (13)0.0016 (16)
C5M0.082 (2)0.0556 (15)0.0534 (16)0.0042 (14)0.0059 (13)0.0062 (11)
C6M0.087 (2)0.0690 (17)0.0703 (19)0.0021 (15)0.0171 (17)0.0004 (14)
C7M0.0608 (19)0.0753 (19)0.084 (2)0.0072 (15)0.0075 (15)0.0053 (15)
C8M0.0529 (19)0.0654 (17)0.074 (2)0.0061 (16)0.0040 (15)0.0047 (14)
C9M0.0575 (15)0.0515 (13)0.0499 (14)0.0007 (10)0.0137 (10)0.0021 (10)
C10M0.0602 (16)0.0517 (13)0.0562 (15)0.0025 (10)0.0173 (11)0.0056 (10)
C11M0.0571 (17)0.0452 (13)0.0496 (15)0.0033 (10)0.0040 (11)0.0002 (12)
C12M0.0524 (15)0.0513 (13)0.0564 (15)0.0008 (10)0.0099 (10)0.0022 (10)
C13M0.0653 (16)0.0420 (12)0.0481 (15)0.0023 (10)0.0081 (11)0.0036 (9)
C14M0.0528 (16)0.0419 (13)0.0502 (14)0.0010 (11)0.0080 (11)0.0019 (11)
C15M0.0745 (19)0.0816 (19)0.0612 (18)0.0057 (14)0.0131 (15)0.0099 (15)
Geometric parameters (Å, º) top
C1M—C2M1.356 (4)C1D—C11D1.399 (17)
C1M—C11M1.427 (4)C2D—C3D1.381 (18)
C2M—C3M1.398 (4)C3D—C4D1.395 (18)
C3M—C4M1.353 (5)C4D—C12D1.397 (17)
C4M—C12M1.417 (3)C5D—C6D1.383 (18)
C5M—C6M1.348 (5)C5D—C13D1.387 (17)
C5M—C13M1.420 (4)C6D—C7D1.375 (19)
C6M—C7M1.396 (4)C7D—C8D1.378 (18)
C7M—C8M1.336 (4)C8D—C14D1.364 (17)
C8M—C14M1.434 (4)C9D—C14D1.496 (16)
C9M—C11M1.400 (3)C9D—C11D1.533 (16)
C9M—C14M1.408 (4)C9D—C15D1.546 (17)
C9M—C15M1.511 (3)C9D—C10Di1.624 (17)
C10M—C13M1.381 (3)C10D—C12D1.489 (16)
C10M—C12M1.383 (3)C10D—C13D1.511 (16)
C11M—C12M1.438 (4)C10D—C9Di1.624 (17)
C13M—C14M1.433 (3)C11D—C12D1.378 (16)
C1D—C2D1.384 (18)C13D—C14D1.420 (16)
C2M—C1M—C11M122.3 (3)C3D—C4D—C12D119 (2)
C1M—C2M—C3M120.6 (3)C6D—C5D—C13D122 (2)
C4M—C3M—C2M119.9 (3)C7D—C6D—C5D116 (2)
C3M—C4M—C12M121.6 (3)C6D—C7D—C8D122 (2)
C6M—C5M—C13M121.6 (3)C14D—C8D—C7D124 (2)
C5M—C6M—C7M120.1 (3)C14D—C9D—C11D106.6 (15)
C8M—C7M—C6M121.0 (3)C14D—C9D—C15D120.8 (19)
C7M—C8M—C14M121.9 (3)C11D—C9D—C15D100.8 (16)
C11M—C9M—C14M120.1 (2)C14D—C9D—C10Di111.3 (15)
C11M—C9M—C15M120.6 (2)C11D—C9D—C10Di112.8 (15)
C14M—C9M—C15M119.3 (2)C15D—C9D—C10Di104.3 (17)
C13M—C10M—C12M122.2 (2)C12D—C10D—C13D109.3 (15)
C9M—C11M—C1M123.4 (3)C12D—C10D—C9Di113.3 (16)
C9M—C11M—C12M120.1 (3)C13D—C10D—C9Di110.1 (16)
C1M—C11M—C12M116.5 (2)C12D—C11D—C1D121.3 (16)
C10M—C12M—C4M122.2 (2)C12D—C11D—C9D119.4 (15)
C10M—C12M—C11M118.7 (2)C1D—C11D—C9D119.3 (16)
C4M—C12M—C11M119.1 (3)C11D—C12D—C4D119.1 (16)
C10M—C13M—C5M122.0 (2)C11D—C12D—C10D115.5 (15)
C10M—C13M—C14M119.5 (2)C4D—C12D—C10D125.4 (17)
C5M—C13M—C14M118.5 (2)C5D—C13D—C14D121.3 (16)
C9M—C14M—C13M119.4 (2)C5D—C13D—C10D120.8 (17)
C9M—C14M—C8M123.7 (2)C14D—C13D—C10D117.9 (15)
C13M—C14M—C8M116.9 (3)C8D—C14D—C13D114.1 (17)
C2D—C1D—C11D119.8 (19)C8D—C14D—C9D129.4 (17)
C3D—C2D—C1D119 (2)C13D—C14D—C9D115.5 (15)
C2D—C3D—C4D122 (2)
Symmetry code: (i) x+2, y+1, z.
(11D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.228 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8652 (13) ÅCell parameters from 500 reflections
b = 14.573 (2) Åθ = 4–22°
c = 8.0993 (13) ŵ = 0.07 mm1
β = 96.499 (16)°T = 293 K
V = 1039.6 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1108 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.029
Graphite monochromatorθmax = 26.0°, θmin = 4.6°
ω scansh = 1010
3390 measured reflectionsk = 1716
1944 independent reflectionsl = 95
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.079H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.287Calculated w = 1/[σ2(Fo2) + (0.1521P)2 + 0.2205P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
1944 reflectionsΔρmax = 0.25 e Å3
198 parametersΔρmin = 0.19 e Å3
160 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.010 (12)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C1M1.1008 (4)0.4200 (2)0.3035 (5)0.0704 (10)0.890 (5)
H1M1.04830.44850.38250.084*0.890 (5)
C2M1.2514 (5)0.4025 (3)0.3412 (5)0.0833 (12)0.890 (5)
H2M1.30000.41910.44470.100*0.890 (5)
C3M1.3334 (4)0.3599 (3)0.2256 (7)0.0846 (12)0.890 (5)
H3M1.43640.34800.25260.102*0.890 (5)
C4M1.2635 (4)0.3356 (3)0.0733 (6)0.0703 (10)0.890 (5)
H4M1.31940.30660.00200.084*0.890 (5)
C5M0.8073 (5)0.3191 (2)0.3272 (4)0.0646 (9)0.890 (5)
H5M0.86390.29380.40570.078*0.890 (5)
C6M0.6563 (5)0.3303 (2)0.3649 (5)0.0784 (11)0.890 (5)
H6M0.60980.31190.46830.094*0.890 (5)
C7M0.5693 (5)0.3693 (3)0.2494 (5)0.0761 (11)0.890 (5)
H7M0.46510.37600.27630.091*0.890 (5)
C8M0.6342 (5)0.3971 (3)0.1007 (6)0.0667 (11)0.890 (5)
H8M0.57420.42410.02720.080*0.890 (5)
C9M0.8652 (3)0.4127 (2)0.1050 (4)0.0536 (8)0.890 (5)
C10M1.0345 (3)0.3298 (2)0.1259 (3)0.0571 (8)0.890 (5)
H10M1.09030.30230.20290.068*0.890 (5)
C11M1.0205 (3)0.3961 (2)0.1467 (4)0.0521 (8)0.890 (5)
C12M1.1076 (3)0.3537 (2)0.0279 (4)0.0543 (8)0.890 (5)
C13M0.8816 (3)0.34548 (18)0.1694 (3)0.0524 (8)0.890 (5)
C14M0.7932 (4)0.3866 (2)0.0517 (4)0.0501 (8)0.890 (5)
C15M0.7713 (5)0.4566 (3)0.2290 (6)0.0765 (13)0.890 (5)
H15A0.66820.46290.17980.115*0.890 (5)
H15B0.81200.51600.25970.115*0.890 (5)
H15C0.77440.41860.32620.115*0.890 (5)
C1D1.070 (3)0.398 (2)0.361 (3)0.097 (11)*0.110 (5)
C2D1.207 (3)0.359 (2)0.421 (3)0.105 (11)*0.110 (5)
C3D1.311 (3)0.340 (2)0.310 (3)0.099 (12)*0.110 (5)
C4D1.280 (3)0.359 (2)0.141 (3)0.059 (8)*0.110 (5)
C5D0.883 (3)0.3506 (19)0.286 (3)0.077 (9)*0.110 (5)
C6D0.732 (3)0.326 (2)0.331 (4)0.079 (14)*0.110 (5)
C7D0.631 (3)0.348 (3)0.222 (4)0.100 (13)*0.110 (5)
C8D0.674 (3)0.395 (3)0.077 (4)0.061 (9)*0.110 (5)
C9D0.886 (2)0.4659 (13)0.128 (2)0.078 (7)*0.110 (5)
C10D1.0925 (19)0.4251 (12)0.094 (2)0.060 (6)*0.110 (5)
C11D1.038 (2)0.4228 (15)0.194 (2)0.040 (7)*0.110 (5)
C12D1.139 (2)0.400 (2)0.084 (2)0.083 (9)*0.110 (5)
C13D0.930 (2)0.3976 (17)0.140 (2)0.068 (7)*0.110 (5)
C14D0.823 (2)0.4152 (16)0.025 (2)0.043 (8)*0.110 (5)
C15D0.794 (4)0.460 (3)0.279 (4)0.078 (13)*0.110 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.081 (2)0.070 (2)0.060 (2)0.0021 (17)0.0023 (18)0.0025 (16)
C2M0.083 (3)0.085 (2)0.076 (3)0.005 (2)0.0127 (19)0.0019 (19)
C3M0.058 (2)0.091 (3)0.100 (3)0.0046 (18)0.010 (2)0.009 (2)
C4M0.058 (2)0.074 (2)0.079 (3)0.0001 (15)0.0072 (16)0.004 (2)
C5M0.077 (3)0.058 (2)0.058 (2)0.0032 (18)0.0063 (17)0.0048 (14)
C6M0.089 (3)0.072 (2)0.069 (2)0.0016 (19)0.015 (2)0.0003 (17)
C7M0.061 (2)0.078 (2)0.086 (3)0.0080 (19)0.0048 (18)0.0041 (19)
C8M0.056 (2)0.065 (2)0.079 (3)0.008 (2)0.0045 (19)0.0064 (18)
C9M0.0559 (18)0.0528 (17)0.0539 (18)0.0012 (12)0.0137 (12)0.0027 (12)
C10M0.0623 (19)0.0551 (16)0.0558 (18)0.0012 (13)0.0155 (13)0.0050 (13)
C11M0.060 (2)0.0436 (16)0.0513 (18)0.0033 (13)0.0019 (13)0.0010 (14)
C12M0.0493 (17)0.0534 (16)0.0608 (18)0.0023 (12)0.0091 (12)0.0023 (13)
C13M0.0624 (19)0.0450 (15)0.0499 (18)0.0013 (12)0.0069 (13)0.0029 (11)
C14M0.054 (2)0.0442 (18)0.0523 (18)0.0007 (14)0.0073 (13)0.0006 (14)
C15M0.084 (3)0.085 (3)0.061 (3)0.006 (2)0.015 (2)0.007 (2)
Geometric parameters (Å, º) top
C1M—C2M1.360 (5)C1D—C11D1.394 (17)
C1M—C11M1.427 (5)C2D—C3D1.389 (18)
C2M—C3M1.394 (6)C3D—C4D1.394 (18)
C3M—C4M1.363 (6)C4D—C12D1.411 (17)
C4M—C12M1.415 (4)C5D—C13D1.389 (17)
C5M—C6M1.348 (6)C5D—C6D1.397 (18)
C5M—C13M1.423 (4)C6D—C7D1.371 (18)
C6M—C7M1.399 (5)C7D—C8D1.377 (18)
C7M—C8M1.337 (5)C8D—C14D1.377 (17)
C8M—C14M1.428 (5)C9D—C14D1.498 (16)
C9M—C11M1.401 (4)C9D—C11D1.530 (16)
C9M—C14M1.407 (4)C9D—C15D1.541 (17)
C9M—C15M1.517 (5)C9D—C10Di1.628 (16)
C10M—C13M1.380 (4)C10D—C12D1.493 (16)
C10M—C12M1.382 (4)C10D—C13D1.505 (16)
C11M—C12M1.439 (4)C10D—C9Di1.628 (16)
C13M—C14M1.432 (4)C11D—C12D1.376 (16)
C1D—C2D1.387 (18)C13D—C14D1.419 (16)
C2M—C1M—C11M122.2 (3)C3D—C4D—C12D118.5 (19)
C1M—C2M—C3M120.4 (3)C13D—C5D—C6D122.2 (19)
C4M—C3M—C2M120.3 (4)C7D—C6D—C5D117 (2)
C3M—C4M—C12M121.2 (4)C6D—C7D—C8D122 (2)
C6M—C5M—C13M121.2 (3)C7D—C8D—C14D122 (2)
C5M—C6M—C7M120.4 (3)C14D—C9D—C11D108.5 (15)
C8M—C7M—C6M120.8 (4)C14D—C9D—C15D116.7 (19)
C7M—C8M—C14M121.9 (4)C11D—C9D—C15D103.0 (18)
C11M—C9M—C14M120.2 (3)C14D—C9D—C10Di112.2 (15)
C11M—C9M—C15M120.7 (3)C11D—C9D—C10Di110.1 (14)
C14M—C9M—C15M119.0 (3)C15D—C9D—C10Di105.9 (18)
C13M—C10M—C12M122.3 (3)C12D—C10D—C13D109.1 (15)
C9M—C11M—C1M123.3 (3)C12D—C10D—C9Di112.1 (15)
C9M—C11M—C12M120.0 (3)C13D—C10D—C9Di110.2 (15)
C1M—C11M—C12M116.7 (3)C12D—C11D—C1D120.0 (16)
C10M—C12M—C4M122.2 (3)C12D—C11D—C9D119.0 (15)
C10M—C12M—C11M118.6 (3)C1D—C11D—C9D120.8 (16)
C4M—C12M—C11M119.2 (3)C11D—C12D—C4D120.1 (16)
C10M—C13M—C5M121.7 (3)C11D—C12D—C10D116.1 (15)
C10M—C13M—C14M119.7 (3)C4D—C12D—C10D123.8 (17)
C5M—C13M—C14M118.6 (3)C5D—C13D—C14D119.6 (15)
C9M—C14M—C8M123.7 (3)C5D—C13D—C10D121.5 (16)
C9M—C14M—C13M119.2 (3)C14D—C13D—C10D118.7 (14)
C8M—C14M—C13M117.2 (3)C8D—C14D—C13D116.9 (17)
C2D—C1D—C11D121 (2)C8D—C14D—C9D127.7 (17)
C1D—C2D—C3D118 (2)C13D—C14D—C9D114.9 (14)
C2D—C3D—C4D122 (2)
Symmetry code: (i) x+2, y+1, z.
(15D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.228 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8574 (16) ÅCell parameters from 500 reflections
b = 14.556 (3) Åθ = 4–22°
c = 8.1209 (15) ŵ = 0.07 mm1
β = 96.58 (2)°T = 293 K
V = 1040.1 (3) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1044 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.035
Graphite monochromatorθmax = 26.0°, θmin = 4.6°
ω scansh = 1010
3414 measured reflectionsk = 1716
1942 independent reflectionsl = 105
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.095H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.352Calculated w = 1/[σ2(Fo2) + (0.2P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.21(Δ/σ)max < 0.001
1942 reflectionsΔρmax = 0.36 e Å3
198 parametersΔρmin = 0.19 e Å3
154 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.04 (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
xyzUiso*/UeqOcc. (<1)
C1M1.1021 (5)0.4198 (3)0.3038 (6)0.0763 (12)0.849 (6)
H1M1.04960.44780.38320.092*0.849 (6)
C2M1.2519 (5)0.4027 (3)0.3411 (6)0.0928 (14)0.849 (6)
H2M1.30070.41960.44410.111*0.849 (6)
C3M1.3347 (5)0.3595 (3)0.2256 (8)0.0903 (15)0.849 (6)
H3M1.43760.34740.25280.108*0.849 (6)
C4M1.2652 (4)0.3357 (3)0.0756 (6)0.0752 (12)0.849 (6)
H4M1.32140.30690.00040.090*0.849 (6)
C5M0.8066 (6)0.3188 (2)0.3259 (5)0.0706 (11)0.849 (6)
H5M0.86280.29300.40420.085*0.849 (6)
C6M0.6564 (6)0.3298 (3)0.3640 (5)0.0833 (13)0.849 (6)
H6M0.61010.31150.46730.100*0.849 (6)
C7M0.5695 (6)0.3686 (3)0.2494 (6)0.0826 (13)0.849 (6)
H7M0.46500.37450.27610.099*0.849 (6)
C8M0.6340 (6)0.3974 (4)0.1019 (7)0.0715 (15)0.849 (6)
H8M0.57390.42540.02970.086*0.849 (6)
C9M0.8654 (4)0.4125 (2)0.1046 (4)0.0589 (10)0.849 (6)
C10M1.0362 (4)0.3297 (2)0.1255 (4)0.0629 (10)0.849 (6)
H10M1.09280.30250.20190.076*0.849 (6)
C11M1.0207 (4)0.3966 (3)0.1463 (5)0.0578 (10)0.849 (6)
C12M1.1079 (4)0.3534 (2)0.0291 (4)0.0589 (10)0.849 (6)
C13M0.8823 (4)0.3452 (2)0.1698 (4)0.0586 (10)0.849 (6)
C14M0.7933 (4)0.3862 (3)0.0517 (5)0.0554 (10)0.849 (6)
C15M0.7706 (6)0.4562 (4)0.2285 (8)0.0811 (16)0.849 (6)
H15A0.66740.46250.17900.122*0.849 (6)
H15B0.81110.51570.25960.122*0.849 (6)
H15C0.77360.41800.32520.122*0.849 (6)
C1D1.063 (3)0.3957 (19)0.364 (3)0.111 (10)*0.151 (6)
C2D1.201 (3)0.3567 (17)0.424 (3)0.109 (9)*0.151 (6)
C3D1.309 (3)0.3405 (19)0.317 (3)0.111 (10)*0.151 (6)
C4D1.280 (3)0.364 (2)0.149 (3)0.077 (9)*0.151 (6)
C5D0.881 (2)0.3525 (16)0.289 (3)0.078 (7)*0.151 (6)
C6D0.730 (3)0.330 (2)0.334 (4)0.112 (17)*0.151 (6)
C7D0.628 (3)0.352 (3)0.224 (4)0.122 (15)*0.151 (6)
C8D0.675 (3)0.394 (2)0.074 (3)0.061 (9)*0.151 (6)
C9D0.8845 (18)0.4678 (11)0.129 (2)0.079 (7)*0.151 (6)
C10D1.0911 (17)0.4241 (10)0.0888 (18)0.066 (5)*0.151 (6)
C11D1.034 (2)0.4218 (15)0.199 (2)0.064 (8)*0.151 (6)
C12D1.135 (2)0.4006 (15)0.089 (2)0.076 (6)*0.151 (6)
C13D0.9273 (18)0.3968 (15)0.141 (2)0.084 (7)*0.151 (6)
C14D0.824 (2)0.4140 (13)0.023 (2)0.052 (7)*0.151 (6)
C15D0.786 (4)0.466 (3)0.273 (4)0.107 (17)*0.151 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.085 (3)0.072 (2)0.070 (3)0.0004 (19)0.001 (2)0.0041 (18)
C2M0.092 (3)0.089 (3)0.091 (3)0.004 (2)0.016 (2)0.000 (2)
C3M0.065 (3)0.098 (3)0.104 (4)0.002 (2)0.008 (3)0.005 (3)
C4M0.065 (3)0.080 (3)0.079 (3)0.0016 (17)0.0050 (19)0.005 (2)
C5M0.089 (3)0.059 (2)0.063 (2)0.004 (2)0.007 (2)0.0053 (16)
C6M0.096 (4)0.074 (2)0.074 (3)0.003 (2)0.015 (2)0.0027 (19)
C7M0.073 (3)0.080 (3)0.092 (3)0.003 (2)0.005 (2)0.004 (2)
C8M0.060 (3)0.070 (3)0.083 (3)0.009 (2)0.004 (2)0.008 (2)
C9M0.061 (2)0.059 (2)0.059 (2)0.0014 (14)0.0158 (15)0.0017 (14)
C10M0.068 (2)0.0571 (18)0.066 (2)0.0010 (14)0.0193 (16)0.0060 (15)
C11M0.067 (3)0.0503 (19)0.055 (2)0.0016 (14)0.0056 (16)0.0019 (17)
C12M0.0523 (19)0.0575 (19)0.068 (2)0.0042 (13)0.0105 (15)0.0024 (15)
C13M0.069 (2)0.0513 (18)0.055 (2)0.0005 (14)0.0079 (16)0.0041 (14)
C14M0.060 (2)0.048 (2)0.059 (2)0.0006 (17)0.0091 (15)0.0003 (16)
C15M0.087 (3)0.090 (3)0.069 (3)0.005 (2)0.018 (2)0.009 (2)
Geometric parameters (Å, º) top
C1M—C2M1.351 (6)C1D—C11D1.386 (17)
C1M—C11M1.435 (5)C2D—C3D1.388 (18)
C2M—C3M1.403 (6)C3D—C4D1.396 (18)
C3M—C4M1.346 (7)C4D—C12D1.420 (16)
C4M—C12M1.425 (5)C5D—C6D1.387 (18)
C5M—C6M1.340 (8)C5D—C13D1.389 (16)
C5M—C13M1.417 (5)C6D—C7D1.375 (18)
C6M—C7M1.394 (6)C7D—C8D1.385 (18)
C7M—C8M1.334 (6)C8D—C14D1.373 (17)
C8M—C14M1.432 (6)C9D—C14D1.507 (15)
C9M—C11M1.398 (4)C9D—C11D1.536 (15)
C9M—C14M1.407 (5)C9D—C15D1.538 (17)
C9M—C15M1.522 (5)C9D—C10Di1.627 (16)
C10M—C12M1.384 (5)C10D—C12D1.493 (15)
C10M—C13M1.388 (4)C10D—C13D1.516 (15)
C11M—C12M1.437 (5)C10D—C9Di1.627 (16)
C13M—C14M1.439 (5)C11D—C12D1.372 (16)
C1D—C2D1.381 (17)C13D—C14D1.416 (16)
C2M—C1M—C11M122.4 (4)C3D—C4D—C12D119.0 (17)
C1M—C2M—C3M120.5 (4)C6D—C5D—C13D120.9 (18)
C4M—C3M—C2M120.1 (4)C7D—C6D—C5D118 (2)
C3M—C4M—C12M121.7 (4)C6D—C7D—C8D121 (2)
C6M—C5M—C13M122.0 (4)C14D—C8D—C7D123 (2)
C5M—C6M—C7M120.3 (4)C14D—C9D—C11D106.7 (14)
C8M—C7M—C6M120.9 (5)C14D—C9D—C15D115.8 (18)
C7M—C8M—C14M121.8 (5)C11D—C9D—C15D104.4 (18)
C11M—C9M—C14M120.4 (3)C14D—C9D—C10Di112.4 (13)
C11M—C9M—C15M120.7 (4)C11D—C9D—C10Di111.6 (13)
C14M—C9M—C15M118.9 (4)C15D—C9D—C10Di105.8 (17)
C12M—C10M—C13M122.0 (3)C12D—C10D—C13D110.3 (13)
C9M—C11M—C1M123.8 (4)C12D—C10D—C9Di112.9 (13)
C9M—C11M—C12M120.1 (3)C13D—C10D—C9Di110.0 (13)
C1M—C11M—C12M116.1 (3)C12D—C11D—C1D120.3 (15)
C10M—C12M—C4M121.9 (3)C12D—C11D—C9D117.2 (14)
C10M—C12M—C11M118.9 (3)C1D—C11D—C9D122.4 (15)
C4M—C12M—C11M119.1 (4)C11D—C12D—C4D119.4 (14)
C10M—C13M—C5M122.5 (3)C11D—C12D—C10D117.4 (13)
C10M—C13M—C14M119.4 (3)C4D—C12D—C10D123.1 (15)
C5M—C13M—C14M118.0 (3)C5D—C13D—C14D121.4 (14)
C9M—C14M—C8M123.8 (3)C5D—C13D—C10D122.6 (14)
C9M—C14M—C13M119.2 (3)C14D—C13D—C10D115.9 (13)
C8M—C14M—C13M117.0 (4)C8D—C14D—C13D115.6 (16)
C2D—C1D—C11D120.8 (19)C8D—C14D—C9D126.6 (15)
C1D—C2D—C3D119.5 (19)C13D—C14D—C9D116.7 (13)
C2D—C3D—C4D120.4 (19)
Symmetry code: (i) x+2, y+1, z.
(18D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.228 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8470 (16) ÅCell parameters from 500 reflections
b = 14.539 (3) Åθ = 4–22°
c = 8.1361 (16) ŵ = 0.07 mm1
β = 96.67 (2)°T = 293 K
V = 1039.4 (4) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
1027 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.039
Graphite monochromatorθmax = 26.0°, θmin = 4.6°
ω scansh = 1010
3380 measured reflectionsk = 1716
1947 independent reflectionsl = 105
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.104H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.375Calculated w = 1/[σ2(Fo2) + (0.2P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.27(Δ/σ)max = 0.002
1947 reflectionsΔρmax = 0.35 e Å3
198 parametersΔρmin = 0.20 e Å3
148 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.03 (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
xyzUiso*/UeqOcc. (<1)
C1M1.1023 (5)0.4193 (3)0.3043 (6)0.0779 (13)0.821 (6)
H1M1.04920.44640.38380.093*0.821 (6)
C2M1.2519 (6)0.4028 (3)0.3419 (7)0.0956 (16)0.821 (6)
H2M1.30040.42000.44490.115*0.821 (6)
C3M1.3358 (5)0.3597 (4)0.2264 (9)0.0936 (17)0.821 (6)
H3M1.43900.34810.25380.112*0.821 (6)
C4M1.2665 (5)0.3353 (3)0.0764 (7)0.0798 (13)0.821 (6)
H4M1.32260.30600.00200.096*0.821 (6)
C5M0.8077 (7)0.3191 (3)0.3259 (5)0.0729 (13)0.821 (6)
H5M0.86430.29430.40460.087*0.821 (6)
C6M0.6565 (7)0.3294 (3)0.3631 (6)0.0853 (15)0.821 (6)
H6M0.60990.31010.46570.102*0.821 (6)
C7M0.5688 (7)0.3688 (3)0.2499 (7)0.0839 (15)0.821 (6)
H7M0.46430.37500.27750.101*0.821 (6)
C8M0.6338 (8)0.3978 (4)0.1012 (8)0.0744 (18)0.821 (6)
H8M0.57390.42600.02920.089*0.821 (6)
C9M0.8655 (4)0.4124 (3)0.1037 (5)0.0623 (11)0.821 (6)
C10M1.0361 (4)0.3295 (2)0.1253 (4)0.0645 (11)0.821 (6)
H10M1.09280.30210.20140.077*0.821 (6)
C11M1.0214 (4)0.3966 (3)0.1464 (6)0.0596 (11)0.821 (6)
C12M1.1079 (4)0.3536 (3)0.0291 (5)0.0624 (11)0.821 (6)
C13M0.8828 (4)0.3450 (2)0.1692 (5)0.0610 (11)0.821 (6)
C14M0.7933 (5)0.3862 (3)0.0514 (5)0.0581 (11)0.821 (6)
C15M0.7739 (10)0.4557 (7)0.2310 (11)0.090 (3)0.821 (6)
H15A0.66990.46260.18400.135*0.821 (6)
H15B0.81570.51490.26260.135*0.821 (6)
H15C0.77840.41680.32680.135*0.821 (6)
C1D1.058 (3)0.3936 (18)0.362 (3)0.120 (11)*0.179 (6)
C2D1.198 (2)0.3563 (16)0.422 (3)0.108 (8)*0.179 (6)
C3D1.309 (3)0.3431 (18)0.316 (3)0.118 (10)*0.179 (6)
C4D1.283 (2)0.3650 (15)0.149 (3)0.064 (6)*0.179 (6)
C5D0.889 (2)0.3530 (16)0.290 (2)0.092 (7)*0.179 (6)
C6D0.736 (3)0.329 (2)0.335 (4)0.113 (16)*0.179 (6)
C7D0.631 (3)0.349 (2)0.229 (3)0.111 (11)*0.179 (6)
C8D0.674 (3)0.391 (2)0.078 (3)0.075 (11)*0.179 (6)
C9D0.8829 (17)0.4676 (10)0.1253 (18)0.076 (6)*0.179 (6)
C10D1.0927 (16)0.4240 (9)0.0861 (17)0.068 (5)*0.179 (6)
C11D1.030 (2)0.4225 (16)0.199 (2)0.083 (9)*0.179 (6)
C12D1.136 (2)0.4013 (15)0.092 (2)0.085 (7)*0.179 (6)
C13D0.9305 (17)0.3974 (14)0.141 (2)0.083 (6)*0.179 (6)
C14D0.8219 (19)0.4167 (13)0.032 (2)0.060 (7)*0.179 (6)
C15D0.760 (4)0.466 (3)0.244 (5)0.104 (15)*0.179 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.081 (3)0.075 (3)0.076 (3)0.000 (2)0.003 (2)0.004 (2)
C2M0.099 (4)0.089 (3)0.093 (4)0.003 (3)0.011 (3)0.003 (3)
C3M0.067 (3)0.104 (4)0.104 (5)0.003 (2)0.013 (3)0.008 (3)
C4M0.070 (3)0.080 (3)0.088 (3)0.001 (2)0.004 (2)0.008 (3)
C5M0.089 (4)0.064 (3)0.065 (3)0.004 (2)0.009 (2)0.0047 (18)
C6M0.100 (4)0.077 (3)0.074 (3)0.002 (2)0.013 (3)0.002 (2)
C7M0.068 (3)0.080 (3)0.101 (4)0.005 (2)0.001 (3)0.008 (2)
C8M0.065 (3)0.072 (3)0.085 (4)0.013 (3)0.004 (3)0.009 (2)
C9M0.063 (2)0.058 (2)0.069 (3)0.0003 (16)0.0201 (18)0.0022 (16)
C10M0.071 (3)0.060 (2)0.065 (2)0.0005 (16)0.0185 (18)0.0057 (16)
C11M0.068 (3)0.054 (2)0.058 (2)0.0022 (16)0.0083 (18)0.0026 (19)
C12M0.055 (2)0.060 (2)0.073 (3)0.0020 (15)0.0118 (17)0.0049 (18)
C13M0.069 (2)0.053 (2)0.062 (2)0.0010 (16)0.0099 (18)0.0066 (15)
C14M0.064 (3)0.048 (2)0.063 (2)0.0006 (19)0.0103 (17)0.0004 (17)
C15M0.096 (4)0.093 (4)0.086 (4)0.011 (3)0.027 (3)0.005 (3)
Geometric parameters (Å, º) top
C1M—C2M1.345 (6)C1D—C2D1.386 (17)
C1M—C11M1.434 (6)C2D—C3D1.399 (17)
C2M—C3M1.410 (7)C3D—C4D1.391 (17)
C3M—C4M1.348 (7)C4D—C12D1.433 (16)
C4M—C12M1.436 (5)C5D—C13D1.385 (16)
C5M—C6M1.346 (8)C5D—C6D1.401 (18)
C5M—C13M1.419 (6)C6D—C7D1.372 (18)
C6M—C7M1.394 (6)C7D—C8D1.381 (18)
C7M—C8M1.346 (7)C8D—C14D1.373 (17)
C8M—C14M1.432 (7)C9D—C11D1.519 (15)
C9M—C14M1.399 (6)C9D—C14D1.520 (15)
C9M—C11M1.402 (5)C9D—C15D1.535 (17)
C9M—C15M1.524 (7)C9D—C10Di1.627 (15)
C10M—C13M1.381 (5)C10D—C12D1.492 (15)
C10M—C12M1.385 (5)C10D—C13D1.503 (15)
C11M—C12M1.434 (6)C10D—C9Di1.627 (15)
C13M—C14M1.442 (5)C11D—C12D1.381 (16)
C1D—C11D1.384 (17)C13D—C14D1.408 (15)
C2M—C1M—C11M122.6 (4)C3D—C4D—C12D116.1 (15)
C1M—C2M—C3M120.5 (5)C13D—C5D—C6D119.8 (17)
C4M—C3M—C2M120.1 (5)C7D—C6D—C5D119 (2)
C3M—C4M—C12M121.4 (5)C6D—C7D—C8D121 (2)
C6M—C5M—C13M121.5 (4)C14D—C8D—C7D121 (2)
C5M—C6M—C7M120.8 (4)C11D—C9D—C14D109.0 (14)
C8M—C7M—C6M120.7 (5)C11D—C9D—C15D112 (2)
C7M—C8M—C14M121.4 (5)C14D—C9D—C15D108 (2)
C14M—C9M—C11M120.8 (3)C11D—C9D—C10Di111.6 (13)
C14M—C9M—C15M120.2 (5)C14D—C9D—C10Di110.4 (12)
C11M—C9M—C15M119.0 (5)C15D—C9D—C10Di105.2 (19)
C13M—C10M—C12M121.7 (3)C12D—C10D—C13D110.8 (12)
C9M—C11M—C12M119.5 (4)C12D—C10D—C9Di112.3 (12)
C9M—C11M—C1M124.0 (4)C13D—C10D—C9Di109.6 (12)
C12M—C11M—C1M116.6 (3)C12D—C11D—C1D118.5 (15)
C10M—C12M—C11M119.4 (3)C12D—C11D—C9D117.3 (14)
C10M—C12M—C4M121.8 (4)C1D—C11D—C9D123.9 (15)
C11M—C12M—C4M118.8 (4)C11D—C12D—C4D122.4 (14)
C10M—C13M—C5M122.2 (4)C11D—C12D—C10D116.7 (13)
C10M—C13M—C14M119.7 (3)C4D—C12D—C10D120.9 (14)
C5M—C13M—C14M118.2 (4)C5D—C13D—C14D120.7 (14)
C9M—C14M—C8M123.7 (4)C5D—C13D—C10D121.7 (14)
C9M—C14M—C13M118.9 (4)C14D—C13D—C10D117.5 (13)
C8M—C14M—C13M117.4 (4)C8D—C14D—C13D118.2 (15)
C11D—C1D—C2D120.8 (18)C8D—C14D—C9D126.7 (15)
C1D—C2D—C3D119.7 (18)C13D—C14D—C9D115.1 (13)
C4D—C3D—C2D121.8 (18)
Symmetry code: (i) x+2, y+1, z.
(24D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.230 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8359 (17) ÅCell parameters from 500 reflections
b = 14.519 (3) Åθ = 4–22°
c = 8.1512 (19) ŵ = 0.07 mm1
β = 96.74 (2)°T = 293 K
V = 1038.5 (4) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
953 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.045
Graphite monochromatorθmax = 25.0°, θmin = 4.3°
ω scansh = 1010
3122 measured reflectionsk = 1716
1752 independent reflectionsl = 94
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.109H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.385Calculated w = 1/[σ2(Fo2) + (0.2P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.34(Δ/σ)max < 0.001
1752 reflectionsΔρmax = 0.38 e Å3
198 parametersΔρmin = 0.20 e Å3
166 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.07 (4)
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C1M1.1026 (7)0.4203 (4)0.3034 (8)0.0803 (16)0.765 (7)
H1M1.04980.44900.38140.096*0.765 (7)
C2M1.2529 (7)0.4029 (4)0.3422 (8)0.0952 (18)0.765 (7)
H2M1.30140.41940.44550.114*0.765 (7)
C3M1.3359 (6)0.3600 (5)0.2269 (10)0.095 (2)0.765 (7)
H3M1.43930.34830.25370.115*0.765 (7)
C4M1.2654 (6)0.3355 (4)0.0765 (9)0.0822 (16)0.765 (7)
H4M1.32140.30590.00230.099*0.765 (7)
C5M0.8085 (8)0.3190 (3)0.3253 (6)0.0713 (14)0.765 (7)
H5M0.86490.29350.40330.086*0.765 (7)
C6M0.6563 (8)0.3305 (4)0.3628 (7)0.0868 (17)0.765 (7)
H6M0.60960.31180.46550.104*0.765 (7)
C7M0.5692 (7)0.3697 (4)0.2507 (8)0.0840 (17)0.765 (7)
H7M0.46470.37640.27840.101*0.765 (7)
C8M0.6346 (9)0.3981 (5)0.1022 (9)0.076 (2)0.765 (7)
H8M0.57470.42650.03050.091*0.765 (7)
C9M0.8658 (5)0.4122 (3)0.1042 (5)0.0619 (13)0.765 (7)
C10M1.0361 (5)0.3300 (3)0.1239 (5)0.0655 (13)0.765 (7)
H10M1.09290.30270.19980.079*0.765 (7)
C11M1.0213 (5)0.3960 (4)0.1458 (7)0.0613 (14)0.765 (7)
C12M1.1090 (5)0.3536 (3)0.0293 (6)0.0621 (13)0.765 (7)
C13M0.8827 (5)0.3450 (3)0.1696 (6)0.0616 (13)0.765 (7)
C14M0.7931 (5)0.3859 (4)0.0516 (6)0.0576 (13)0.765 (7)
C15M0.7763 (11)0.4536 (7)0.2329 (13)0.097 (3)0.765 (7)
H15A0.67180.46100.18730.145*0.765 (7)
H15B0.81840.51260.26610.145*0.765 (7)
H15C0.78180.41360.32720.145*0.765 (7)
C1D1.061 (2)0.3978 (14)0.359 (2)0.107 (8)*0.235 (7)
H1D0.98780.40800.43080.129*0.235 (7)
C2D1.199 (2)0.3601 (15)0.421 (3)0.129 (8)*0.235 (7)
H2D1.21950.34610.53310.155*0.235 (7)
C3D1.305 (3)0.3435 (16)0.314 (3)0.126 (10)*0.235 (7)
H3D1.39870.31800.35610.152*0.235 (7)
C4D1.279 (2)0.3633 (17)0.146 (3)0.092 (8)*0.235 (7)
H4D1.35270.35320.07530.110*0.235 (7)
C5D0.884 (2)0.3492 (14)0.289 (2)0.095 (7)*0.235 (7)
H5D0.95530.33450.35940.114*0.235 (7)
C6D0.733 (3)0.3238 (16)0.331 (3)0.104 (12)*0.235 (7)
H6D0.70300.29280.42930.125*0.235 (7)
C7D0.629 (3)0.3454 (16)0.225 (3)0.101 (8)*0.235 (7)
H7D0.52730.33010.25360.122*0.235 (7)
C8D0.672 (3)0.389 (2)0.077 (3)0.096 (13)*0.235 (7)
H8D0.59940.40030.00490.116*0.235 (7)
C9D0.8816 (16)0.4674 (10)0.1210 (18)0.091 (5)*0.235 (7)
C10D1.0929 (15)0.4244 (9)0.0869 (17)0.083 (5)*0.235 (7)
H10D1.15990.38950.15180.100*0.235 (7)
C11D1.0267 (19)0.4211 (14)0.194 (2)0.083 (8)*0.235 (7)
C12D1.1336 (19)0.3999 (14)0.0890 (19)0.094 (6)*0.235 (7)
C13D0.9293 (16)0.3957 (13)0.1438 (19)0.089 (6)*0.235 (7)
C14D0.8203 (19)0.4165 (13)0.033 (2)0.073 (7)*0.235 (7)
C15D0.752 (3)0.469 (2)0.233 (4)0.076 (9)*0.235 (7)
H15D0.73050.40760.26540.114*0.235 (7)
H15E0.66260.49580.17320.114*0.235 (7)
H15F0.78330.50570.32920.114*0.235 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.088 (4)0.075 (3)0.077 (4)0.002 (3)0.009 (3)0.000 (2)
C2M0.093 (4)0.088 (4)0.098 (4)0.000 (3)0.015 (3)0.003 (3)
C3M0.067 (3)0.100 (4)0.113 (6)0.004 (3)0.012 (4)0.008 (4)
C4M0.072 (4)0.080 (3)0.094 (4)0.001 (2)0.006 (3)0.007 (3)
C5M0.074 (4)0.070 (3)0.069 (3)0.001 (3)0.004 (2)0.013 (2)
C6M0.101 (5)0.075 (3)0.078 (4)0.006 (3)0.013 (3)0.003 (3)
C7M0.068 (3)0.077 (3)0.104 (4)0.013 (3)0.003 (3)0.005 (3)
C8M0.068 (3)0.075 (4)0.083 (4)0.016 (3)0.006 (3)0.010 (3)
C9M0.063 (3)0.059 (3)0.066 (3)0.0007 (19)0.016 (2)0.0018 (19)
C10M0.073 (3)0.059 (2)0.066 (3)0.0042 (19)0.020 (2)0.0047 (19)
C11M0.066 (3)0.055 (3)0.061 (3)0.0037 (19)0.003 (2)0.001 (2)
C12M0.053 (3)0.059 (2)0.075 (3)0.0029 (17)0.0093 (19)0.001 (2)
C13M0.066 (3)0.051 (2)0.068 (3)0.0035 (19)0.011 (2)0.0074 (18)
C14M0.064 (3)0.047 (3)0.063 (3)0.004 (2)0.011 (2)0.001 (2)
C15M0.093 (5)0.093 (5)0.108 (6)0.025 (4)0.029 (4)0.002 (3)
Geometric parameters (Å, º) top
C1M—C2M1.352 (7)C1D—C11D1.385 (16)
C1M—C11M1.440 (7)C2D—C3D1.378 (17)
C2M—C3M1.404 (8)C3D—C4D1.395 (17)
C3M—C4M1.355 (9)C4D—C12D1.419 (16)
C4M—C12M1.415 (6)C5D—C13D1.380 (16)
C5M—C6M1.354 (9)C5D—C6D1.385 (17)
C5M—C13M1.410 (7)C6D—C7D1.369 (17)
C6M—C7M1.384 (7)C7D—C8D1.378 (17)
C7M—C8M1.343 (8)C8D—C14D1.376 (17)
C8M—C14M1.424 (9)C9D—C14D1.505 (15)
C9M—C11M1.397 (6)C9D—C11D1.508 (15)
C9M—C14M1.407 (7)C9D—C15D1.542 (16)
C9M—C15M1.511 (8)C9D—C10Di1.616 (15)
C10M—C12M1.380 (6)C10D—C12D1.480 (14)
C10M—C13M1.380 (6)C10D—C13D1.524 (14)
C11M—C12M1.433 (7)C10D—C9Di1.616 (15)
C13M—C14M1.443 (6)C11D—C12D1.383 (15)
C1D—C2D1.378 (17)C13D—C14D1.424 (15)
C2M—C1M—C11M122.4 (5)C3D—C4D—C12D116.1 (16)
C1M—C2M—C3M120.1 (5)C13D—C5D—C6D121.3 (17)
C4M—C3M—C2M120.1 (5)C7D—C6D—C5D118.5 (19)
C3M—C4M—C12M121.8 (5)C6D—C7D—C8D121.7 (19)
C6M—C5M—C13M121.0 (5)C14D—C8D—C7D120.7 (19)
C5M—C6M—C7M121.1 (5)C14D—C9D—C11D108.6 (13)
C8M—C7M—C6M120.5 (6)C14D—C9D—C15D106.5 (15)
C7M—C8M—C14M121.9 (6)C11D—C9D—C15D115.4 (16)
C11M—C9M—C14M120.3 (4)C14D—C9D—C10Di112.1 (12)
C11M—C9M—C15M118.6 (6)C11D—C9D—C10Di111.9 (12)
C14M—C9M—C15M121.0 (6)C15D—C9D—C10Di102.2 (14)
C12M—C10M—C13M123.0 (4)C12D—C10D—C13D110.0 (12)
C9M—C11M—C12M120.3 (5)C12D—C10D—C9Di112.2 (12)
C9M—C11M—C1M123.3 (5)C13D—C10D—C9Di111.1 (12)
C12M—C11M—C1M116.4 (4)C12D—C11D—C1D117.5 (14)
C10M—C12M—C4M122.5 (4)C12D—C11D—C9D117.6 (13)
C10M—C12M—C11M118.4 (4)C1D—C11D—C9D124.9 (14)
C4M—C12M—C11M119.1 (5)C11D—C12D—C4D122.6 (14)
C10M—C13M—C5M122.6 (4)C11D—C12D—C10D116.3 (13)
C10M—C13M—C14M118.9 (4)C4D—C12D—C10D121.0 (14)
C5M—C13M—C14M118.5 (4)C5D—C13D—C14D119.5 (13)
C9M—C14M—C8M123.9 (4)C5D—C13D—C10D124.5 (13)
C9M—C14M—C13M119.1 (4)C14D—C13D—C10D116.0 (12)
C8M—C14M—C13M117.1 (5)C8D—C14D—C13D118.2 (15)
C2D—C1D—C11D122.4 (17)C8D—C14D—C9D126.4 (14)
C1D—C2D—C3D118.6 (18)C13D—C14D—C9D115.4 (12)
C2D—C3D—C4D122.6 (19)
Symmetry code: (i) x+2, y+1, z.
(26D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.231 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.830 (2) ÅCell parameters from 500 reflections
b = 14.486 (4) Åθ = 4–22°
c = 8.169 (2) ŵ = 0.07 mm1
β = 96.75 (3)°T = 293 K
V = 1037.7 (4) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
896 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.056
Graphite monochromatorθmax = 25.0°, θmin = 4.3°
ω scansh = 910
3104 measured reflectionsk = 1716
1750 independent reflectionsl = 94
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.131H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.425Calculated w = 1/[σ2(Fo2) + (0.2P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.42(Δ/σ)max < 0.001
1750 reflectionsΔρmax = 0.37 e Å3
198 parametersΔρmin = 0.21 e Å3
142 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.14 (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
xyzUiso*/UeqOcc. (<1)
C1M1.1030 (7)0.4198 (4)0.3043 (9)0.0836 (18)0.744 (8)
H1M1.04960.44780.38260.100*0.744 (8)
C2M1.2554 (8)0.4026 (5)0.3442 (9)0.101 (2)0.744 (8)
H2M1.30440.41930.44690.122*0.744 (8)
C3M1.3367 (8)0.3592 (5)0.2279 (12)0.106 (2)0.744 (8)
H3M1.43990.34650.25410.127*0.744 (8)
C4M1.2652 (7)0.3359 (4)0.0778 (10)0.089 (2)0.744 (8)
H4M1.32110.30710.00280.107*0.744 (8)
C5M0.8111 (10)0.3192 (4)0.3233 (8)0.0812 (19)0.744 (8)
H5M0.86840.29430.40120.097*0.744 (8)
C6M0.6577 (9)0.3299 (4)0.3620 (8)0.092 (2)0.744 (8)
H6M0.61100.31080.46430.110*0.744 (8)
C7M0.5707 (9)0.3694 (5)0.2492 (10)0.095 (2)0.744 (8)
H7M0.46600.37580.27670.113*0.744 (8)
C8M0.6349 (10)0.3982 (6)0.1023 (11)0.080 (3)0.744 (8)
H8M0.57510.42720.03120.096*0.744 (8)
C9M0.8657 (5)0.4122 (4)0.1037 (7)0.0683 (16)0.744 (8)
C10M1.0372 (6)0.3298 (3)0.1227 (6)0.0735 (17)0.744 (8)
H10M1.09420.30250.19840.088*0.744 (8)
C11M1.0225 (6)0.3967 (4)0.1474 (8)0.0647 (16)0.744 (8)
C12M1.1102 (5)0.3535 (4)0.0315 (7)0.0670 (15)0.744 (8)
C13M0.8841 (6)0.3448 (3)0.1683 (6)0.0669 (15)0.744 (8)
C14M0.7939 (7)0.3854 (5)0.0519 (7)0.0649 (17)0.744 (8)
C15M0.7718 (14)0.4561 (9)0.2286 (16)0.094 (4)0.744 (8)
H15A0.66800.46280.18000.141*0.744 (8)
H15B0.81300.51570.25980.141*0.744 (8)
H15C0.77530.41740.32440.141*0.744 (8)
C1D1.063 (2)0.3990 (15)0.364 (2)0.114 (9)*0.256 (8)
H1D0.99110.41060.43650.137*0.256 (8)
C2D1.202 (2)0.3607 (16)0.422 (3)0.140 (9)*0.256 (8)
H2D1.22400.34560.53330.168*0.256 (8)
C3D1.308 (3)0.3451 (17)0.316 (3)0.128 (10)*0.256 (8)
H3D1.40160.31970.35720.154*0.256 (8)
C4D1.282 (2)0.3656 (18)0.148 (3)0.096 (9)*0.256 (8)
H4D1.35520.35530.07750.115*0.256 (8)
C5D0.887 (2)0.3482 (15)0.287 (2)0.107 (8)*0.256 (8)
H5D0.96040.33380.35580.128*0.256 (8)
C6D0.738 (3)0.3229 (17)0.332 (3)0.105 (11)*0.256 (8)
H6D0.70920.29170.43040.126*0.256 (8)
C7D0.632 (3)0.3451 (18)0.228 (3)0.116 (10)*0.256 (8)
H7D0.52990.32920.25730.140*0.256 (8)
C8D0.673 (3)0.391 (2)0.080 (4)0.102 (14)*0.256 (8)
H8D0.59840.40400.01210.122*0.256 (8)
C9D0.8815 (17)0.4671 (10)0.1247 (18)0.093 (6)*0.256 (8)
C10D1.0932 (16)0.4253 (9)0.0860 (17)0.089 (5)*0.256 (8)
H10D1.16010.38970.14990.107*0.256 (8)
C11D1.028 (2)0.4204 (16)0.198 (2)0.102 (11)*0.256 (8)
C12D1.137 (2)0.4029 (14)0.0918 (19)0.099 (7)*0.256 (8)
C13D0.9309 (17)0.3946 (13)0.1402 (19)0.094 (6)*0.256 (8)
C14D0.8217 (19)0.4168 (13)0.032 (2)0.074 (7)*0.256 (8)
C15D0.761 (5)0.461 (3)0.245 (5)0.123 (19)*0.256 (8)
H15D0.74580.39770.27370.184*0.256 (8)
H15E0.66620.48640.19450.184*0.256 (8)
H15F0.79450.49540.34340.184*0.256 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.089 (4)0.079 (4)0.082 (4)0.002 (3)0.012 (4)0.000 (3)
C2M0.103 (5)0.096 (4)0.100 (5)0.008 (4)0.006 (4)0.001 (4)
C3M0.083 (5)0.105 (5)0.124 (7)0.000 (4)0.009 (5)0.019 (5)
C4M0.076 (4)0.082 (4)0.108 (5)0.004 (3)0.004 (3)0.015 (4)
C5M0.083 (5)0.078 (4)0.082 (4)0.008 (4)0.009 (3)0.008 (3)
C6M0.099 (5)0.083 (4)0.087 (4)0.011 (3)0.015 (4)0.005 (3)
C7M0.071 (4)0.081 (4)0.131 (6)0.013 (3)0.004 (4)0.008 (4)
C8M0.061 (4)0.079 (4)0.098 (6)0.016 (4)0.005 (4)0.009 (4)
C9M0.063 (3)0.068 (3)0.077 (4)0.001 (2)0.022 (2)0.001 (2)
C10M0.083 (4)0.065 (3)0.077 (4)0.001 (2)0.025 (3)0.009 (2)
C11M0.068 (4)0.059 (3)0.065 (3)0.002 (2)0.003 (2)0.002 (3)
C12M0.050 (3)0.066 (3)0.086 (4)0.003 (2)0.012 (2)0.000 (3)
C13M0.064 (3)0.063 (3)0.074 (4)0.000 (2)0.013 (3)0.004 (2)
C14M0.069 (4)0.054 (3)0.073 (4)0.005 (3)0.012 (2)0.002 (3)
C15M0.089 (6)0.099 (6)0.097 (6)0.010 (3)0.022 (4)0.001 (4)
Geometric parameters (Å, º) top
C1M—C2M1.370 (8)C1D—C11D1.392 (16)
C1M—C11M1.430 (8)C2D—C3D1.367 (17)
C2M—C3M1.404 (9)C3D—C4D1.395 (17)
C3M—C4M1.354 (10)C4D—C12D1.411 (16)
C4M—C12M1.400 (7)C5D—C6D1.380 (17)
C5M—C6M1.364 (10)C5D—C13D1.388 (16)
C5M—C13M1.402 (8)C6D—C7D1.375 (18)
C6M—C7M1.390 (9)C7D—C8D1.386 (18)
C7M—C8M1.333 (9)C8D—C14D1.380 (17)
C8M—C14M1.427 (10)C9D—C14D1.514 (15)
C9M—C11M1.406 (6)C9D—C11D1.522 (15)
C9M—C14M1.407 (8)C9D—C15D1.538 (17)
C9M—C15M1.527 (10)C9D—C10Di1.611 (15)
C10M—C13M1.377 (7)C10D—C12D1.495 (15)
C10M—C12M1.389 (7)C10D—C13D1.515 (15)
C11M—C12M1.436 (8)C10D—C9Di1.611 (15)
C13M—C14M1.437 (7)C11D—C12D1.389 (16)
C1D—C2D1.386 (17)C13D—C14D1.419 (15)
C2M—C1M—C11M122.8 (6)C3D—C4D—C12D116.2 (16)
C1M—C2M—C3M119.1 (6)C6D—C5D—C13D121.4 (18)
C4M—C3M—C2M120.2 (6)C7D—C6D—C5D118 (2)
C3M—C4M—C12M122.4 (6)C6D—C7D—C8D121.4 (19)
C6M—C5M—C13M121.2 (6)C14D—C8D—C7D122 (2)
C5M—C6M—C7M120.3 (6)C14D—C9D—C11D108.3 (14)
C8M—C7M—C6M121.1 (7)C14D—C9D—C15D108 (2)
C7M—C8M—C14M121.3 (7)C11D—C9D—C15D110 (2)
C11M—C9M—C14M120.8 (5)C14D—C9D—C10Di110.0 (12)
C11M—C9M—C15M119.5 (7)C11D—C9D—C10Di112.1 (13)
C14M—C9M—C15M119.7 (7)C15D—C9D—C10Di107.7 (19)
C13M—C10M—C12M122.9 (4)C12D—C10D—C13D110.5 (12)
C9M—C11M—C1M124.1 (6)C12D—C10D—C9Di112.0 (12)
C9M—C11M—C12M119.5 (6)C13D—C10D—C9Di112.0 (13)
C1M—C11M—C12M116.3 (5)C12D—C11D—C1D118.8 (15)
C10M—C12M—C4M122.3 (5)C12D—C11D—C9D117.2 (14)
C10M—C12M—C11M118.5 (4)C1D—C11D—C9D123.9 (14)
C4M—C12M—C11M119.2 (5)C11D—C12D—C4D122.1 (14)
C10M—C13M—C5M122.4 (5)C11D—C12D—C10D116.4 (13)
C10M—C13M—C14M119.3 (5)C4D—C12D—C10D121.5 (14)
C5M—C13M—C14M118.3 (5)C5D—C13D—C14D120.4 (14)
C9M—C14M—C8M123.3 (5)C5D—C13D—C10D123.5 (14)
C9M—C14M—C13M119.0 (5)C14D—C13D—C10D116.1 (12)
C8M—C14M—C13M117.7 (6)C8D—C14D—C13D117.1 (15)
C2D—C1D—C11D120.4 (18)C8D—C14D—C9D126.8 (15)
C3D—C2D—C1D119.7 (19)C13D—C14D—C9D116.1 (13)
C2D—C3D—C4D122.8 (19)
Symmetry code: (i) x+2, y+1, z.
(28D) top
Crystal data top
C15H12F(000) = 408
Mr = 192.25Dx = 1.231 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.819 (2) ÅCell parameters from 500 reflections
b = 14.474 (4) Åθ = 4–22°
c = 8.183 (3) ŵ = 0.07 mm1
β = 96.84 (3)°T = 293 K
V = 1037.1 (5) Å3, pale yellow
Z = 40.50 × 0.35 × 0.20 mm
Data collection top
Kuma KM4CCD
diffractometer
865 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.058
Graphite monochromatorθmax = 25.0°, θmin = 4.6°
ω scansh = 910
3123 measured reflectionsk = 1716
1751 independent reflectionsl = 94
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.135H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.435Calculated w = 1/[σ2(Fo2) + (0.2P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.44(Δ/σ)max = 0.001
1751 reflectionsΔρmax = 0.39 e Å3
198 parametersΔρmin = 0.20 e Å3
142 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.12 (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
xyzUiso*/UeqOcc. (<1)
C1M1.1018 (8)0.4205 (5)0.3044 (9)0.085 (2)0.724 (8)
H1M1.04780.44840.38200.102*0.724 (8)
C2M1.2548 (9)0.4034 (5)0.3446 (10)0.103 (2)0.724 (8)
H2M1.30340.42140.44680.124*0.724 (8)
C3M1.3380 (9)0.3588 (6)0.2310 (13)0.106 (3)0.724 (8)
H3M1.44080.34500.25910.128*0.724 (8)
C4M1.2663 (7)0.3357 (5)0.0788 (11)0.093 (2)0.724 (8)
H4M1.32250.30730.00380.111*0.724 (8)
C5M0.8117 (10)0.3190 (5)0.3229 (8)0.082 (2)0.724 (8)
H5M0.86910.29430.40060.099*0.724 (8)
C6M0.6584 (10)0.3298 (5)0.3612 (8)0.096 (2)0.724 (8)
H6M0.61180.31050.46340.115*0.724 (8)
C7M0.5706 (10)0.3694 (5)0.2499 (11)0.097 (2)0.724 (8)
H7M0.46580.37510.27880.116*0.724 (8)
C8M0.6328 (10)0.3997 (6)0.1011 (12)0.089 (3)0.724 (8)
H8M0.57290.42920.03070.107*0.724 (8)
C9M0.8662 (6)0.4116 (4)0.1050 (7)0.0684 (16)0.724 (8)
C10M1.0374 (6)0.3298 (4)0.1216 (7)0.0768 (18)0.724 (8)
H10M1.09480.30250.19680.092*0.724 (8)
C11M1.0221 (6)0.3967 (5)0.1467 (9)0.0702 (19)0.724 (8)
C12M1.1101 (5)0.3537 (4)0.0321 (7)0.0705 (16)0.724 (8)
C13M0.8841 (6)0.3446 (4)0.1680 (7)0.0703 (17)0.724 (8)
C14M0.7936 (7)0.3855 (5)0.0529 (8)0.0690 (19)0.724 (8)
C15M0.7621 (11)0.4545 (7)0.2180 (11)0.104 (3)0.724 (8)
H15A0.66060.45920.16150.156*0.724 (8)
H15B0.79890.51510.25020.156*0.724 (8)
H15C0.76090.41660.31410.156*0.724 (8)
C1D1.061 (2)0.3980 (15)0.363 (2)0.121 (9)*0.276 (8)
H1D0.98830.40940.43390.145*0.276 (8)
C2D1.200 (2)0.3599 (15)0.422 (3)0.146 (9)*0.276 (8)
H2D1.22190.34530.53260.175*0.276 (8)
C3D1.306 (3)0.3437 (17)0.316 (3)0.130 (10)*0.276 (8)
H3D1.39880.31720.35770.156*0.276 (8)
C4D1.283 (2)0.3649 (16)0.149 (3)0.092 (8)*0.276 (8)
H4D1.35780.35630.07920.110*0.276 (8)
C5D0.891 (2)0.3483 (14)0.289 (2)0.109 (8)*0.276 (8)
H5D0.96560.33320.35550.131*0.276 (8)
C6D0.740 (3)0.3242 (17)0.335 (3)0.110 (12)*0.276 (8)
H6D0.71230.29380.43400.132*0.276 (8)
C7D0.632 (3)0.3457 (18)0.232 (3)0.123 (10)*0.276 (8)
H7D0.52990.33190.26480.147*0.276 (8)
C8D0.674 (2)0.3873 (17)0.083 (3)0.079 (8)*0.276 (8)
H8D0.59920.39700.01310.095*0.276 (8)
C9D0.8816 (16)0.4670 (10)0.1228 (16)0.088 (5)*0.276 (8)
C10D1.0937 (16)0.4251 (9)0.0842 (17)0.093 (5)*0.276 (8)
H10D1.16080.38990.14850.111*0.276 (8)
C11D1.029 (2)0.4193 (16)0.197 (2)0.093 (10)*0.276 (8)
C12D1.1369 (19)0.4004 (13)0.0925 (19)0.095 (6)*0.276 (8)
C13D0.9309 (16)0.3953 (13)0.1416 (18)0.093 (6)*0.276 (8)
C14D0.8208 (19)0.4152 (12)0.032 (2)0.069 (7)*0.276 (8)
C15D0.784 (2)0.4657 (15)0.265 (2)0.068 (6)*0.276 (8)
H15D0.76740.40300.29670.103*0.276 (8)
H15E0.68780.49490.23170.103*0.276 (8)
H15F0.83620.49850.35760.103*0.276 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1M0.091 (5)0.086 (4)0.078 (5)0.004 (3)0.006 (4)0.002 (3)
C2M0.108 (6)0.096 (5)0.099 (5)0.002 (4)0.011 (4)0.007 (4)
C3M0.084 (5)0.108 (6)0.122 (8)0.003 (4)0.007 (6)0.011 (5)
C4M0.077 (4)0.085 (4)0.114 (6)0.006 (3)0.004 (4)0.023 (4)
C5M0.079 (6)0.076 (4)0.090 (5)0.005 (4)0.006 (4)0.009 (3)
C6M0.104 (6)0.089 (4)0.088 (5)0.009 (4)0.014 (4)0.006 (3)
C7M0.075 (5)0.085 (5)0.129 (7)0.008 (4)0.007 (4)0.005 (4)
C8M0.065 (5)0.092 (5)0.109 (7)0.020 (4)0.004 (4)0.014 (4)
C9M0.065 (3)0.069 (4)0.075 (4)0.002 (2)0.025 (3)0.004 (2)
C10M0.084 (4)0.073 (3)0.077 (4)0.003 (3)0.024 (3)0.011 (3)
C11M0.073 (5)0.069 (4)0.068 (4)0.006 (3)0.010 (3)0.001 (4)
C12M0.055 (3)0.073 (3)0.084 (4)0.007 (2)0.010 (3)0.005 (3)
C13M0.068 (4)0.065 (3)0.078 (4)0.002 (3)0.013 (3)0.006 (3)
C14M0.073 (5)0.057 (4)0.078 (4)0.010 (3)0.010 (3)0.009 (3)
C15M0.112 (6)0.120 (6)0.079 (6)0.006 (4)0.007 (5)0.023 (5)
Geometric parameters (Å, º) top
C1M—C2M1.373 (9)C1D—C11D1.389 (16)
C1M—C11M1.435 (9)C2D—C3D1.367 (17)
C2M—C3M1.409 (10)C3D—C4D1.394 (17)
C3M—C4M1.369 (10)C4D—C12D1.411 (16)
C4M—C12M1.409 (7)C5D—C6D1.384 (17)
C5M—C6M1.360 (11)C5D—C13D1.389 (16)
C5M—C13M1.399 (8)C6D—C7D1.379 (18)
C6M—C7M1.387 (9)C7D—C8D1.375 (17)
C7M—C8M1.348 (9)C8D—C14D1.375 (16)
C8M—C14M1.441 (10)C9D—C14D1.512 (15)
C9M—C11M1.394 (7)C9D—C11D1.529 (15)
C9M—C14M1.422 (8)C9D—C15D1.530 (16)
C9M—C15M1.512 (9)C9D—C10Di1.612 (15)
C10M—C13M1.377 (7)C10D—C12D1.495 (14)
C10M—C12M1.386 (8)C10D—C13D1.519 (14)
C11M—C12M1.429 (9)C10D—C9Di1.612 (15)
C13M—C14M1.433 (7)C11D—C12D1.379 (16)
C1D—C2D1.382 (17)C13D—C14D1.429 (15)
C2M—C1M—C11M122.3 (6)C3D—C4D—C12D115.0 (16)
C1M—C2M—C3M119.9 (7)C6D—C5D—C13D119.7 (18)
C4M—C3M—C2M119.4 (7)C7D—C6D—C5D119 (2)
C3M—C4M—C12M122.2 (7)C8D—C7D—C6D120.6 (19)
C6M—C5M—C13M120.8 (6)C7D—C8D—C14D122.8 (19)
C5M—C6M—C7M120.9 (6)C14D—C9D—C11D107.8 (13)
C8M—C7M—C6M121.9 (8)C14D—C9D—C15D117.1 (13)
C7M—C8M—C14M118.8 (7)C11D—C9D—C15D102.8 (12)
C11M—C9M—C14M120.4 (5)C14D—C9D—C10Di111.1 (11)
C11M—C9M—C15M124.5 (6)C11D—C9D—C10Di112.7 (13)
C14M—C9M—C15M115.1 (6)C15D—C9D—C10Di105.2 (12)
C13M—C10M—C12M122.9 (5)C12D—C10D—C13D110.7 (12)
C9M—C11M—C12M120.2 (6)C12D—C10D—C9Di113.4 (12)
C9M—C11M—C1M123.1 (6)C13D—C10D—C9Di111.0 (12)
C12M—C11M—C1M116.7 (5)C12D—C11D—C1D119.0 (14)
C10M—C12M—C4M122.1 (5)C12D—C11D—C9D117.6 (14)
C10M—C12M—C11M118.4 (5)C1D—C11D—C9D123.3 (14)
C4M—C12M—C11M119.5 (6)C11D—C12D—C4D122.8 (14)
C10M—C13M—C5M122.4 (6)C11D—C12D—C10D115.8 (13)
C10M—C13M—C14M119.2 (5)C4D—C12D—C10D121.3 (14)
C5M—C13M—C14M118.4 (6)C5D—C13D—C14D121.5 (14)
C9M—C14M—C13M118.8 (5)C5D—C13D—C10D122.6 (14)
C9M—C14M—C8M122.2 (6)C14D—C13D—C10D115.9 (12)
C13M—C14M—C8M119.1 (6)C8D—C14D—C13D115.9 (14)
C2D—C1D—C11D120.0 (18)C8D—C14D—C9D128.9 (14)
C3D—C2D—C1D119.6 (19)C13D—C14D—C9D115.2 (12)
C2D—C3D—C4D123.5 (19)
Symmetry code: (i) x+2, y+1, z.
(100D) top
Crystal data top
C30H24F(000) = 408
Mr = 384.49Dx = 1.289 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.7650 (13) ÅCell parameters from 958 reflections
b = 13.6035 (19) Åθ = 4–22°
c = 8.1177 (10) ŵ = 0.07 mm1
β = 113.308 (15)°T = 293 K
V = 990.3 (2) Å3, colorless
Z = 20.32 × 0.15 × 0.12 mm
Data collection top
Kuma KM4CCD
diffractometer
1000 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.071
Graphite monochromatorθmax = 26.0°, θmin = 4.5°
ω scansh = 1212
3166 measured reflectionsk = 1513
1695 independent reflectionsl = 105
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.078All H-atom parameters refined
wR(F2) = 0.250Calculated w = 1/[σ2(Fo2) + (0.1425P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
1695 reflectionsΔρmax = 0.25 e Å3
185 parametersΔρmin = 0.22 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.07 (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
xyzUiso*/Ueq
C10.8047 (4)0.7058 (3)0.8646 (5)0.0541 (11)
C20.6630 (5)0.7154 (4)0.8620 (5)0.0609 (12)
C30.6103 (5)0.6494 (3)0.9502 (5)0.0593 (12)
C40.7014 (4)0.5734 (3)1.0462 (5)0.0533 (11)
C51.1869 (4)0.5029 (3)1.4312 (5)0.0533 (10)
C61.3251 (5)0.5458 (4)1.5166 (5)0.0628 (12)
C71.3788 (5)0.6100 (3)1.4270 (5)0.0588 (11)
C81.2928 (4)0.6330 (3)1.2481 (5)0.0501 (10)
C91.0533 (4)0.6119 (3)0.9665 (4)0.0427 (9)
C100.9481 (4)0.4824 (3)1.1568 (4)0.0447 (10)
C110.8968 (4)0.6299 (3)0.9582 (4)0.0453 (9)
C120.8445 (4)0.5638 (3)1.0519 (4)0.0442 (9)
C131.1006 (4)0.5257 (3)1.2545 (4)0.0440 (9)
C141.1540 (4)0.5918 (3)1.1613 (4)0.0435 (9)
C151.1099 (5)0.6978 (3)0.8890 (6)0.0577 (11)
H10.838 (5)0.753 (4)0.805 (6)0.078 (14)*
H20.595 (5)0.771 (3)0.783 (5)0.065 (11)*
H30.505 (5)0.658 (3)0.951 (6)0.082 (13)*
H40.671 (5)0.520 (3)1.114 (6)0.077 (13)*
H51.137 (4)0.450 (3)1.486 (5)0.060 (10)*
H61.392 (5)0.532 (3)1.637 (6)0.069 (12)*
H71.481 (5)0.644 (3)1.488 (6)0.073 (12)*
H81.326 (4)0.685 (3)1.177 (5)0.049 (9)*
H100.910 (4)0.453 (3)1.250 (4)0.048 (9)*
H15A1.039 (4)0.708 (3)0.758 (6)0.063 (11)*
H15B1.230 (5)0.682 (4)0.901 (6)0.085 (14)*
H15C1.121 (5)0.761 (4)0.962 (7)0.091 (15)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.058 (2)0.054 (3)0.047 (2)0.009 (2)0.0164 (18)0.0016 (18)
C20.063 (2)0.061 (3)0.052 (2)0.017 (2)0.0151 (19)0.002 (2)
C30.051 (2)0.069 (3)0.053 (2)0.008 (2)0.0153 (18)0.012 (2)
C40.053 (2)0.059 (3)0.051 (2)0.005 (2)0.0245 (18)0.0119 (18)
C50.058 (2)0.056 (3)0.0435 (19)0.001 (2)0.0176 (17)0.0036 (17)
C60.059 (2)0.078 (3)0.0396 (19)0.002 (2)0.0073 (18)0.007 (2)
C70.054 (2)0.064 (3)0.054 (2)0.002 (2)0.0172 (18)0.009 (2)
C80.0477 (19)0.052 (3)0.0478 (19)0.0009 (18)0.0164 (16)0.0036 (17)
C90.0485 (19)0.041 (2)0.0379 (16)0.0045 (17)0.0165 (14)0.0008 (14)
C100.055 (2)0.045 (2)0.0369 (17)0.0045 (17)0.0210 (15)0.0000 (14)
C110.0458 (19)0.048 (2)0.0392 (17)0.0002 (17)0.0141 (15)0.0035 (15)
C120.0482 (18)0.046 (2)0.0373 (16)0.0005 (17)0.0156 (14)0.0060 (14)
C130.0535 (19)0.043 (2)0.0352 (17)0.0029 (17)0.0168 (15)0.0045 (14)
C140.0486 (19)0.041 (2)0.0397 (17)0.0020 (16)0.0163 (15)0.0067 (15)
C150.067 (3)0.050 (3)0.058 (2)0.005 (2)0.027 (2)0.007 (2)
Geometric parameters (Å, º) top
C1—C21.382 (6)C8—C141.376 (5)
C1—C111.384 (5)C8—H81.04 (4)
C1—H10.93 (5)C9—C141.521 (5)
C2—C31.369 (6)C9—C111.522 (5)
C2—H21.04 (5)C9—C151.531 (5)
C3—C41.385 (6)C9—C10i1.625 (5)
C3—H31.04 (4)C10—C131.503 (5)
C4—C121.386 (5)C10—C121.514 (5)
C4—H41.02 (5)C10—C9i1.625 (5)
C5—C61.379 (6)C10—H101.05 (3)
C5—C131.381 (5)C11—C121.398 (5)
C5—H51.06 (4)C13—C141.401 (5)
C6—C71.367 (6)C15—H15A1.02 (4)
C6—H60.95 (4)C15—H15B1.16 (5)
C7—C81.395 (5)C15—H15C1.02 (6)
C7—H71.03 (5)
C2—C1—C11120.5 (4)C14—C9—C10i110.0 (3)
C2—C1—H1119 (3)C11—C9—C10i109.6 (3)
C11—C1—H1120 (3)C15—C9—C10i105.4 (3)
C3—C2—C1120.8 (4)C13—C10—C12108.3 (3)
C3—C2—H2121 (2)C13—C10—C9i113.5 (3)
C1—C2—H2118 (2)C12—C10—C9i112.9 (3)
C2—C3—C4119.5 (4)C13—C10—H10109.4 (18)
C2—C3—H3120 (3)C12—C10—H10109.8 (19)
C4—C3—H3120 (3)C9i—C10—H10103 (2)
C3—C4—C12120.3 (4)C1—C11—C12118.7 (3)
C3—C4—H4125 (2)C1—C11—C9124.6 (3)
C12—C4—H4115 (2)C12—C11—C9116.7 (3)
C6—C5—C13120.1 (4)C4—C12—C11120.1 (4)
C6—C5—H5127 (2)C4—C12—C10121.9 (3)
C13—C5—H5113 (2)C11—C12—C10118.0 (3)
C7—C6—C5120.5 (4)C5—C13—C14120.0 (3)
C7—C6—H6115 (2)C5—C13—C10122.0 (3)
C5—C6—H6125 (3)C14—C13—C10118.0 (3)
C6—C7—C8119.9 (4)C8—C14—C13119.1 (3)
C6—C7—H7122 (2)C8—C14—C9124.0 (3)
C8—C7—H7118 (2)C13—C14—C9116.8 (3)
C14—C8—C7120.4 (4)C9—C15—H15A109 (2)
C14—C8—H8117 (2)C9—C15—H15B110 (2)
C7—C8—H8123 (2)H15A—C15—H15B111 (3)
C14—C9—C11107.5 (2)C9—C15—H15C112 (3)
C14—C9—C15112.0 (3)H15A—C15—H15C112 (4)
C11—C9—C15112.3 (3)H15B—C15—H15C104 (4)
Symmetry code: (i) x+2, y+1, z+2.
 

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