3 For reviews, see: D. A. Armitage, in The Silicon–Heteroatom Bond, ed.
S. Patai and Z. Rappoport, John Wiley and Sons, Chichester, 1991, pp.
213–243; Comprehensive Organometallic Chemistry II, ed. E. W. Abel,
F. G. A. Stone and G. Wilkinson, Pergamon, Oxford, 1995, vol. 2, pp.
34–37, 166–174, 293–296; Comprehensive Organometallic Chemistry,
ed. G. Wilkinson, F. G. A. Stone and E. W. Abel, Pergamon, Oxford,
1982, vol. 2, pp. 167–177, 443–447, 604–607. See also: Kosugi, T.
Ogata, M. Terada, H. Sano and T. Migita, Bull Chem. Soc. Jpn., 1985,
58, 3657; Y. Nishiyama, S. Aoyama and S. Hatanaka, Phosphorus,
Sulfur Silicon Relat. Elem., 1992, 67, 267; Y. Nishiyama, H. Ohashi, K.
Itoh and N. Sonoda, Chem. Lett., 1998, 159.
4 L.-B. Han and M. Tanaka, J. Am. Chem. Soc., 1998, 120, 8249.
5 Although photochemical disproportionation has not been documented,
thermal disproportionation between (Ph3Pb)2 and (PhS)2 in boiling
aqueous benzene was reported to afford Ph3PbSPh (60–76% yield);
L. C. Willemsens and G. J. van der Kerk, J. Organomet. Chem., 1968,
15, 117; P. L. Clarke and J. L. Wardell, J. Chem. Soc., Dalton Trans.,
1974, 190. Disproportionation reactions of R4E2 (E = P, As, Sb, Bi)
with dichalcogenides RA2Z2 (Z = S, Se, Te) are also known: R. S.
Dickson and K. D. Heazle, J. Organomet. Chem., 1995, 493, 189; W.
Uhl, M. Layh, G. Becker, K.-W. Klinkhammer and T. Hildenbrand,
Chem. Ber., 1992, 125, 1547; H. J. Breuning and S. Guelec, Z.
Naturforsch., Teil B, 1986, 41, 1387; A. J. Ashe III and E. G. Ludwig,
Jr., J. Organomet. Chem., 1986, 308, 289; W. W. du Mont, T.
Severengiz and H. J. Breuning, Z. Naturforsch., Teil B, 1983, 38,
1306.
6 Special irradiation apparatus is not necessary for the disproportionation
of (ArS)2 with (Me3Sn)2. Usually, mixing the two reagents in a flask
placed about 2 m under a 40 W fluorescent lamp at room temperature for
a few minutes leads to quantitative formation of the products. Only
when the reactivity was low, was irradiation with a 200 W tungsten lamp
performed.
7 PhSSnMe3 was found to be formed only in ca. 15% yield by heating a
benzene solution of (PhS)2 and (Me3Sn)2 at 80 °C for 2 h in the dark.
8 Neither (PhS)2 nor (Me3Sn)2 was detected by 1H NMR spectroscopy
when pure PhSSnMe3 in benzene was exposed to the room light at room
temperature, indicating the irreversibility of the disproportionation
reaction. Similar phenomena were observed for PhSeSnMe3 and
PhTeSnMe3, although decomposition of PhTeSnMe3 (conversion 30%)
to Ph2Te and (Me3Sn)2Te was found to have occurred after prolonged
irradiation (44 h) at room temperature.
the reaction proceeded more slowly; the completion of the
reaction between (CyS)2 and (Me3Sn)2 required > 7 h and the
formation of ButSSnMe3 in the reaction of (ButS)2 with
(Me3Sn)2 under similar reaction conditions was only marginal.
Although slower than (Me3Sn)2, (Ph3Sn)2 reacted with both
aromatic and aliphatic disulfides to produce the corresponding
triphenyltin sulfides in quantitative yields.
Similar disproportionation reactions did not take place with
disilanes such as (Me3Si)2, (MePh2Si)2, (Ph3Si)2 or (SiCl3)2
under the same conditions. Digermanes such as (Me3Ge)2,
(ClMe2Ge)2 and (Ph3Ge)2 did not react either. However, the
reactions of (Ph3Pb)2 with (PhS)2 and (BuS)2 proceeded
smoothly and quantitative yields of the products were obtained.
(PhSe)2 was as reactive as (PhS)2 in the above disproportiona-
tion reactions. Similar reactions with (PhTe)2 proceeded
relatively slowly,8 but ultimately afforded respectable yields.
(Bu3Sn)2 has no absorption maximum in the normal UV
region. However, its lmax at a wavelength < 215 nm displays
strong end absorption that tails to 250–260 nm.9 (Ph3Sn)2 and
(Ph3Pb)2 display absorption maxima in the UV region (lmax
248–260 nm for the former depending on the solvent and 294
nm for the latter).9 Diphenyl dichalcogenides also have
absorption maxima in the UV, near-UV or visible regions.10
Because of these absorptions, various reactions involving
ditins11 or dichalcogenides10 can very efficiently proceed under
photolytic conditions by irradiation with a sunlamp through
Pyrex.12 With these precedents in mind, we envisioned that the
present disproportionation reaction proceeds via a radical
mechanism as shown in Scheme 1.13 However, the initiation
step is uncertain at the present time since precedents suggest
that homolytic cleavage of both M–M11 and Z–Z10 bonds by
light is possible to initiate the reaction. In agreement with the
reactivity trends in other reactions of chalcogen-centered
radicals (S > Se > Te),10 the disproportionation of (PhTe)2
proceeded most sluggishly. The decreasing trends in the
reactivity of aliphatic disulfides, (BuS)2 > (CyS)2 > (ButS)2,
appear to suggest that steric factors of the chalcogen-centered
radicals also play an important role.14
9 W. Drenth, M. J. Janssen and G. J. M. van der Kerk, J. Organomet.
Chem., 1964, 2, 265.
10 UV absorption for (PhZ)2: (PhS)2, lmax 250 nm; (PhSe)2, lmax 330 nm;
(PhTe)2, lmax 406 nm. Radical additions of (PhZ)2 to unsaturated
carbon–carbon bonds under irradiation of visible light have been
studied. For examples, see: A. Ogawa, I. Ogawa, R. Obayashi, K.
Umezu, M. Doi and T. Hirao, J. Org. Chem., 1999, 64, 84; A. Ogawa,
R. Obayashi, H. Ine, Y. Tsuboi, N. Sonoda and T. Hirao, J. Org. Chem.,
1998, 63, 881; A. Ogawa, R. Obayashi, M. Doi, N. Sonoda and T. Hirao,
J. Org. Chem., 1998, 63, 4277.
Scheme 1
11 Irradiation with
a sunlamp through Pyrex efficiently promotes
In summary, a clean and salt-free route to single source
precursors for semiconductors has been presented and the
process does not require the use of the volatile organic solvents.
These features appear to meet the requirement for ‘green’
chemistry, which is of contemporary public concern.15
Financial support from the Japan Science and Technology
Corporation (JST) through the CREST (Core Research for
Evolutional Science and Technology) program and a post-
doctoral fellowship to F. M. are gratefully acknowledged.
(Bu3Sn)2-initiated radical chain reactions; see D. P. Curran, M.-H. Chen
and D. Kim, J. Am. Chem. Soc., 1989, 111, 6265.
12 Curran et al. have reported that Pyrex shows 1–2.5% transmittance at
250–260 nm, which allows homolytic cleavage of (Bu3Sn)2. See ref.
11.
13 In agreement with the radical mechanism, heating an equimolar mixture
of (Me3Sn)2 and (PhS)2 in C6D6 at 80 °C in the dark in the presence of
10 mol% of AIBN led to 95% conversion after 2 h, whereas the same
treatment in the absence of AIBN showed only 15% conversion.
·
14 (BuS)2 is reported to be 14 times more reactive toward Bu3Sn than
(ButS)2, see: J. Spanswick and K. U. Ingold, Int. J. Chem. Kinet., 1970,
2, 157.
Notes and references
1 G. A. Domrachev, V. K. Khamylov, M. Z. Bochkarev, B. V. Zhuk, B. S.
Kaverin, B. A. Nesterov and A. I. Kirillov, Ger. Pat., 2703873, 1977;
H. Uchida, Jpn. Pat., 01298010, 1989.
2 J. M. Fischer, W. E. Piers, S. D. P. Batchilder and M. J. Zaworotko,
J. Am. Chem. Soc., 1996, 118, 283 and references therein.
15 Note added at proof: We have found very recently that the December 20
issue of Chemical Abstracts has compiled a paper on a new method for
the synthesis of stannyl selenides; see V. A. Potapov, S. V. Amosova, V.
Svetlana, I. P. Beletskaya, A. A. Starkova, A. V. Martynov and L.
Hevesi, Sulfur Lett., 1999, 22, 237; Chem. Abstr., 1999, 131,
337113u.
658
Chem. Commun., 2000, 657–658