Chemistry Letters Vol.34, No.8 (2005)
1089
naphenanthrene ring of 1b consists of a localized Sn=C unit and
a biphenyl unit in contrast to the 9-silaphenanthrene ring of 7,
the X-ray crystallographic analysis of which has revealed its
planar and ꢀ-electron-delocalized structure.10 The thermal insta-
bility of 1a and the theoretical calculations suggest the small
contribution of aromatic stabilization in the 9-stannaphenan-
threne system of 1a.
In summary, we have succeeded in the generation of 9-stan-
naphenanthrene 1a for the first time and revealed its high reac-
tivities. With the hope of isolating 1a as a stable compound, fur-
ther investigation on the introduction of additional substituent(s)
to the stannaphenanthrene skeleton and the cooperative stabili-
zation method (the contribution of kinetic and thermodynamic
stabilization) are currently in progress.
Figure 2. ORTEP drawing (50% probability) of 3.
This work was supported by Grants-in-Aid for COE Re-
search on Elements Science (No. 12CE2005), Scientific Re-
search on Priority Area (No. 14078213), Scientific Research
(A) (No. 14204064) and the 21st Century COE Program on
Kyoto University Alliance for Chemistry from the Ministry of
Education, Culture, Sports, Science and Technology, Japan.
of 2 with LiOMe in THF. The molecular structures of 5 and 6
were confirmed with the 1H, 13C, and 119Sn NMR and mass spec-
tral data,6 and were finally established by X-ray crystallographic
analysis (Figure 3).8 Since 2,3-dimethyl-1,3-butadiene is inert to
anionic species such as 9-chloro-10-lithio-9-Tbt-9,10-dihydro-
9-stannaphenanthrene, which is an alternative intermediate in
the reactions of 2 with LTMP giving 3, 4a, and 5, the formation
of a [2 þ 4] cycloadduct 6 from 2 indicates that the reaction of 2
with LTMP affords not an anionic intermediate but a neutral
stannaphenanthrene 1a. These results strongly indicate that 1a
exists as a monomer in a THF solution at ꢁ78 ꢂC.9 The thermal
instability of 1a is in sharp contrast to the high stability of Tbt-
substituted 9-silaphenanthrene (7),10 which is stable at 100 ꢂC in
C6D6. In theoretical calculations using a Ph-substituted model
1b,11 it was found that the planar conformation of the 9-stanna-
phenanthrene skeleton is not a local minimum, that is, the 9-stan-
References and Notes
1
a) V. J. Minkin, M. N. Glukhovtsev, and Y. B. Simkin, in ‘‘Aromaticity
and Antiaromaticity; Electronic and Structural Aspects,’’ Wiley,
New York (1994). b) N. Tokitoh, Acc. Chem. Res., 37, 86 (2004). c) N.
Tokitoh, Bull. Chem. Soc. Jpn., 77, 429 (2004).
2
3
a) M. Saito, R. Haga, and M. Yoshioka, Chem. Commun., 2002, 1002.
b) M. Saito, R. Haga, and M. Yoshioka, Chem. Lett., 32, 912 (2003).
For reviews, see: a) K. M. Baines and W. G. Stibbs, Adv. Organomet.
´
Chem., 39, 275 (1996). b) J. Escudie, C. Couret, and H. Ranaivonjatovo,
Coord. Chem. Rev., 178–180, 565 (1998). c) N. Tokitoh and R. Okazaki,
in ‘‘The Chemistry of Organic Germanium, Tin and Lead Compounds,’’
ed. by Z. Rappoport, Wiley, Chichester, U.K. (2002), Vol. 2, Part 1,
Chap. 13. d) V. Y. Lee and A. Sekiguchi, Organometallics, 23, 2822
(2004).
Tbt
4
5
Recent applications of the Tbt group to the stabilization of neutral silaar-
omatic compounds, see: a) A. Shinohara, N. Takeda, and N. Tokitoh,
J. Am. Chem. Soc., 125, 10804 (2003). b) N. Takeda, A. Shinohara,
and N. Tokitoh, Organometallics, 21, 4024 (2002).
Recent applications of the Tbt group to the stabilization of neutral
germaaromatic compounds, see: a) N. Nakata, N. Takeda, and N.
Tokitoh, Angew. Chem. Int. Ed., 42, 115 (2003). b) N. Nakata, N.
Takeda, and N. Tokitoh, Organometallics, 22, 481 (2003).
trapping
Sn
reagents
LTMP
2
products
THF
−78 °C
1 h
−78 °C
1a
N
Mes*
6
7
Experimental procedures and physical properties for the precursor 2 and
the products 3, 4b, 5, and 6 are described in the Supporting Information.
MeO
Tbt Sn
O
X
Tbt Sn
H
.
Tbt Sn
H
Crystal data for 3: C80H136Si12Sn2 C6H6 MW ¼ 1750:46; triclinic; space
ꢀ
ꢁ
ꢁ
ꢁ
group P1; a ¼ 12:8898ð2Þ A, b ¼ 17:9414ð3Þ A, c ¼ 22:3902ð5Þ A; ꢁ ¼
ꢂ
ꢂ
ꢂ
ꢁ 3
81:1212ð8Þ , ꢂ ¼ 82:9007ð9Þ , ꢃ ¼ 72:8807ð16Þ ; V ¼ 4872:49ð16Þ A ;
Z ¼ 2; Dcalcd ¼ 1:193 g/cm3; ꢄ ¼ 0:699 mmꢁ1; 2ꢅmax ¼ 50ꢂ; T ¼ 103
K; R1ðI > 2ꢆðIÞÞ ¼ 0:0451; wR2 (all data) = 0.1015; GOF ¼ 1:020 for
16862 reflections and 937 parameters, (CCDC 268569).
4a: X = D
4b: X = H
5
6
8
9
Crystal data for 5: C59H97NOSi6Sn MW ¼ 1123:61; triclinic; space
ꢀ
ꢁ
ꢁ
ꢁ
ꢁ 3
group P1; a ¼ 9:8361ð9Þ A, b ¼ 15:5831ð11Þ A, c ¼ 21:8919ð17Þ A;
Scheme 3.
ꢂ
ꢂ
ꢂ
ꢁ ¼ 107:957ð3Þ , ꢂ ¼ 96:281ð3Þ , ꢃ ¼ 88:936ð7Þ ; V ¼ 3172:5ð4Þ A ;
Z ¼ 2; Dcalcd ¼ 1:176 g/cm3; ꢄ ¼ 0:552 mmꢁ1; 2ꢅmax ¼ 50ꢂ; T ¼ 103
K; R1ðI > 2ꢆðIÞÞ ¼ 0:0309; wR2 (all data) = 0.0907; GOF ¼ 1:014 for
10703 reflections and 716 parameters, (CCDC 268570). Crystal data
for 6 is described in the Supporting Information.
Additional information: 1) When these trapping experiments were
performed after stirring for 1 h at ꢁ40 ꢂC, dimer 3 was obtained in ca.
30% yield. 2) Dimer 3 showed no change in C7D8 at 100 ꢂC and did
not react with MesꢀCNO in C6D6 even at 80 ꢂC, indicating no dissocia-
tion of 3 to the monomer 1a in solution.
10 A. Shinohara, N. Takeda, T. Sasamori, and N. Tokitoh, The 7th IUPAC
International Conference on Heteroatom Chemistry, Shanghai, China,
August 2004, Abstr., No. P43.
11 Theoretical calculations were carried out using the Gaussian 98 program
with density functional theory at the B3LYP level. In calculations,
LANL2DZ (for Sn) and 6-31G(d) (for C and H) basis sets were used.
The optimized structure of 1b is shown in the Supporting Information.
Figure 3. ORTEP drawing (50% probability) of 5.
Published on the web (Advance View) July 2, 2005; DOI 10.1246/cl.2005.1088