Fig. 6 19F NMR spectrum of isomer 2. Peaks marked ᭹ are due to
isomer 1 produced by isomerisation, and peaks marked × are due to the
second Cs isomer arising from addition across bond c.
Fig. 5 The structure of isomer 2 (addition across bond b); ‘visible’
fluorines only are shown.
Isomer 2
As for isomer 1 the EI mass spectrum consisted only of the
anthracene and C60F18 fragmentation ions. The 1H NMR
spectrum (500 MHz, CDCl3) showed 2 to be unsymmetrical,
giving ten lines overall at δH 7.65 (1 H, d, J 7.4 Hz, HC), 7.60
(1 H, d, J 7.5 Hz, HD), 7.57 (1 H, d, J 7.4 Hz, HE), 7.47 (1 H, d,
J 7.1 Hz, HF), 7.442 (1 H, dd, J 7.4 and 1.3 Hz, HG), 7.405 (1 H,
dd, J 7.6 and 1.3 Hz, HH), 7.392 (1 H, dd, J 7.5 and 1.3 Hz, HI),
7.365 (1 H, dd, J 7.4 and 1.3 Hz, HJ), 5.623 (1 H, s, HA), 5.495
(1 H, s, HB). The relationships between HC-F and HG-J, Fig. 5)
were determined by a 2D-COSY experiment. Couplings (NOE)
between HA–HD, HA–HE, HB–HC, and HB–HF were determined
as 8.0, 7.3, 9.3 and 7.5%, respectively. Some other double
doublets, of about half the above intensities were evident in the
7.34–7.45 ppm region, and these are attributed to a trace of a
third isomer of Cs symmetry (produced by addition across
bond c) as shown also by the 19 F NMR spectrum, Fig. 6.
Isomer 2 is less stable than isomer 1, significant amounts of
anthracene being evident from the 1H NMR spectrum, showing
that decomposition was occurring fairly rapidly. In principle,
isomer 2 could involve addition across bond d. However, given
the extreme steric hindrance that models indicate for the latter,
this possibility can be ruled out.
Fig. 7 Location of the fluorines identified from the 2 D 19F NMR
spectrum of 2.
solved at this time; separation of anthracene from a 1 : 1 adduct
with [60]fullerene and recombination with a second cage takes
place in the solid state.9 Interconversions from a 6,6-closed-
to a 6,5-open structure (methanofullerene to homofullerene)
have been reported previously,14 but these are mechanistically
different since they involve simultaneous 1,3-shifts of two C–C
bonds.
The eighteen lines for isomer 2 appeared at δF -127.25 (1 F, d,
J 20 Hz, 1), Ϫ130.46 (1 F, d, J 20 Hz, 2), Ϫ134.48 (1 F, sh 3),
Ϫ135.20 (1 F, s, 4), Ϫ136.25 (1 F, s, 5), Ϫ136.65 (1 F, sh 6),
Ϫ137.43 (1 F, d, J 20 Hz, 7), Ϫ137.57 (1 F, s, 8), Ϫ139.24 (1 F,
ddd, J 6, 6 and 33 Hz, 9), Ϫ141.14 (1 F, dd, J 9 and 26 Hz, 10),
Ϫ142.68 (1 F, ddd, J 6, 6 and 26 Hz, 11), Ϫ143.53 (1 F, d, J 28
Hz, 12), Ϫ143.87 (1 F, d, J 28 Hz, 13), Ϫ144.40 (1 F, ddd, J 5, 5
and 26 Hz, 14), Ϫ149.85 (1 F, ddd, J 7, 7 and 28 Hz, 15),
Ϫ157.19 (1F, dt, J 11 and 21 Hz, 16), Ϫ157.49 (1 F, dt, J 10 and
19 Hz, 17), Ϫ158.25 (1 F, dt, J 10 and 20 Hz, 18). The bold
numbers identify the fluorines in Fig. 7 as deduced from a 2 D
spectrum. The small amount of compound prevented identi-
fication of some of the couplings, hence some assignments
may be interchanged; the couplings 17→2, 18→7, 13→11→9,
4→12→15, 16→1→6→10→14, and 16→8 were clearly identi-
fied. As for isomer 1 (and C60F18 derivatives in general) the
fluorines nearest to the central benzenoid ring (nos. 3, 4, 5, 6,
8, 9) are more downfield than those further out (nos. 10, 11,
12, 13, 14, 15). The peak 7 (and hence peak 18) was assigned on
the basis of its marked upfield shift assumed to arise from the
proximity of the anthracene addend.
The 19F NMR spectrum, run ca. 2 weeks after formation of
the adduct, is shown in Fig. 6, all of the associations between
peaks from the same component being determined from a 2 D
spectrum. There are four main peaks arising from C60F18
produced by the retro Diels–Alder reaction, eighteen peaks due
to isomer 2, and (marked ×) nine of the ten peaks due to the
presence of the alternative Cs isomer produced by addition
across bond c (Fig. 1); their intensities relative to those for iso-
mer 2 appear greater because of the higher symmetry.
Most significant, however, are the peaks marked ᭹ due to
isomer 1 produced from isomerisation of isomer 2 (and possibly
also some of the second symmetrical isomer). We are confident
that isomer 1 was not present originally in isomer 2 because the
former eluted after the latter in the HPLC separation and so
would not be present due to ‘tailing’ and, moreover, there was
no trace of it in the 1H NMR spectrum that was run ca. 10 days
before the 19F NMR spectrum. This appears to be the first
example of spontaneous migration of a cycloaddend across the
same cage surface. Such a migration can only be detected in the
presence of a second addend (in our case the fluorine atoms),
and has been observed previously only during electrochemistry
of bis malonates (shown to be intramolecular through the use
of a standard cross-over procedure).13 In view of the lability of
the anthracene it is possible that separation–recombination
occurs in our case, but this mechanistic aspect cannot be readily
The presence of the components in the 19F NMR spectrum
of 2 is readily seen in the region where the resonances appear
for the fluorines attached to sp3-hybridised carbons, themselves
attached to sp3-hybridised carbons (Fig. 8). This shows the
intense off-scale peak due to regenerated C60F18, the three equal
intensity double triplets for peaks 16–18 of isomer 2 (marked
A), the two double triplets for peaks 9 and 10 of isomer 1
(marked B – one of these is partially superimposed on one of
996
J. Chem. Soc., Perkin Trans. 2, 2001, 994–997