G. Mloston´ et al.
FULL PAPER
3,3,5,5-Tetramethyl-2-thioxothiolane-4-one (31): Yield 38% (40 mg,
0.21 mmol). M.p. 36–39 °C (n-pentane) (ref.[14] 39–41 °C). 1H
NMR (200 MHz, CDCl3): δ = 1.62 (s, 3 H, CH3), 1.35 (s, 3 H,
CH3) ppm. 13C NMR (50 MHz, CDCl3): δ = 242.8 (s, C=S), 216.5
(s, C=O), 63.2 (s, Cq), 61.2 (s, Cq), 28.0 (q, CH3), 27.7 (q, CH3)
and triplet states is a very demanding task, as standard
MCSCF and CASSCF methods are not sufficiently accu-
rate to draw firm mechanistic conclusions.[16]
ppm. IR (KBr): ν = 1736 [s (C=O)] cm–1. MS (EI): m/z (%) = 188
˜
Conclusions
(100) [M]+, 86 (90) [Me2C=C=S]+.
The irreversible conversion of dithiiranes into the corre-
sponding dithiolactones depends on the substitution
pattern. Thermal and photolytic isomerizations leading to
the ring-enlarged dithiolactone 31 were observed only for
strained spiro derivative 28. The analogous photochemical
conversion was observed for matrix-isolated dithiirane 29,
which afforded dithiolane 32. In this case, thermal isomer-
ization in the gas phase did not take place. Moreover, nei-
ther thermal nor photochemical transformation of 30 into
33 was observed.
Acknowledgments
J. R. and G. M. thank the Rector of the University of Lodz for
financial support (Grant # 505/712).
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Experimental Section
Starting Materials: 1,2,4-Trithiolanes used in the study were ob-
tained according to known literature protocols: 1,1,3,3,7,7,9,9-oc-
tamethyl-5,10,11-trithiadispiro[3.1.3.2]-undecane-2,8-dione (19),[10]
2,2,8,8-tetrachloro-1,1,3,3,7,7,9,9-octamethyl-5,10,11-trithiadispiro-
[3.1.3.2]undecane (20),[11] and dispiro[adamantane-2,3Ј-(1,2,4)-tri-
thiolane-5Ј,2ЈЈ-adamantane] (21).[12]
Matrix Studies: The cryostat for matrix isolation was a helium
closed-cycle refrigeration system (compressor unit RW2 with
coldhead base unit 210 and extension module ROK) from Leybold.
The matrix IR spectra were measured by using an FTIR instrument
IFS 55 from Bruker; the UV/Vis spectra were taken with a Hewlett
Packard HP 8453 diode-array spectrophotometer. The light sources
used were a mercury high-pressure lamp (HBO 200 from Osram)
with a monochromator (Bausch and Lomb) and a mercury low-
pressure spiral lamp with a Vycor filter (Gräntzel). For the combi-
nation of high-vacuum flash pyrolysis with matrix isolation, a small
home-built water-cooled oven directly connected to the vacuum
shroud of the cryostat was used. The pyrolysis zone consisted of a
completely empty quartz tube (inner diameter 8 mm, length of
heating zone 50 mm) resistively heated by a coax heating wire. The
temperature was controlled by a Ni/CrNi thermocouple. The pre-
cursors were sublimed at 30–40 °C from a storage bulb into the
quartz pyrolysis tube. Immediately after leaving the tube, at a dis-
tance of ca. 50 mm, the pyrolysis products were cocondensed with
a large excess of argon on the surface of the 10 K matrix window.
[10] G. Mloston´, M. Woz´nicka, H. Heimgartner, Helv. Chim. Acta
2007, 90, 594–599.
[11] G. Mloston´, A. Majchrzak, M. Rutkowska, M. Woz´nicka, A.
Linden, H. Heimgartner, Helv. Chim. Acta 2005, 88, 2624–
2636.
[12] G. Mloston´, J. Roman´ski, H. Heimgartner, Pol. J. Chem. 1996,
70, 437–445.
Computational Methods: IR spectra of structures 25–33 were com-
puted by density functional theory method by using the B3LYP
functional with the 6-311+G(d,p) basis set as incorporated in the
Gaussian package of programs.[15]
[13] G. Seybold, Tetrahedron Lett. 1974, 15, 555–558.
[14] R. Huisgen, J. Rapp, H. Huber, Liebigs Ann. Recl. 1997, 1517–
1524.
[15] M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria,
M. A. Robb, J. R. Cheeseman, J. A. Montgomery Jr, T. Vreven,
K. N. Kudin, J. C. Burant, J. M. Millam, S. S. Iyengar, J. Tom-
asi, V. Barone, B. Mennucci, M. Cossi, G. Scalmani, N. Rega,
G. A. Petersson, H. Nakatsuji, M. Hada, M. Ehara, K. Toyota,
R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda,
O. Kitao, H. Nakai, M. Klene, X. Li, J. E. Knox, H. P. Hratch-
ian, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gom-
perts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C.
Pomelli, J. W. Ochterski, P. Y. Ayala, K. Morokuma, G. A.
Voth, P. Salvador, J. J. Dannenberg, V. G. Zakrzewski, S. Dap-
prich, A. D. Daniels, M. C. Strain, O. Farkas, D. K. Malick,
A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. V. Ortiz, Q.
Cui, A. G. Baboul, S. Clifford, J. Cioslowski, B. B. Stefanov,
FVP of 19: FVP was carried out by using the standard FVP appa-
ratus equipped with 15-cm heating zone without filling and cooling
finger (acetone/dry ice) under 10–2 mbar.
FVP at 450 °C: Trithiolane 19 (50 mg, 0.135 mmol) was pyrolyzed,
and a 1:1 mixture of dithiolactone 31 (1H NMR) and thioketone
22 (1H NMR: δ = 1.33 ppm) was found.
FVP at 700 °C: Trithiolane 19 (200 mg, 0.54 mmol) was pyrolyzed,
and only dithiolactone 31 and small amounts of some unidentified
products were found in the crude mixture (1H NMR). Dithiolac-
tone 31 was purified by preparative TLC (petroleum ether/CHCl3,
1:3) and subsequently recrystallized from n-pentane.
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