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a ( 23 Na)
a ( 29 Si b )
a ( 29 Si b )
a ( 29 Si a )
a ( 29 Si a )
a ( 29 Si a )
a ( 29 Si a )
a ( 29 Si b )
a ( 29 Si b )
(a)
(b)
Figure10.5 EPRspectrumof(a)solvent-separatedionpair[R 2 Si] [Na + (THF) 4 ]( 29 )inDME(a( 29 Si α )
=
29.1G
anda( 29 Si β )
10.2G),and(b)contactionpair[R 2 SiNa(15-crown-5)] ( 28 )intoluene(a( 29 Si α )
29.1G,a( 29 Si β )
=
=
10.2G and a( 23 Na)
=
=
1.9G); g
=
2
.
0074,R
=
SiMetBu 2 . (Reprinted with permission from [38a]. Copyright
2007AmericanChemicalSociety.)
solv
, via a two-electron reduction process
(Scheme 10.10). 38 The possibility of obtaining neutral radicals 28 or anionic paramagnetic species 29
(the anion radical of a silylene) was first noted when the EPR spectra of [R 2 Si] Na(15-crown-5) n were
recorded both in polar (THF, DME) and non-polar (toluene) solvents. 38a It was apparent from the EPR
spectra (Figure 10.5) that in polar solvents the paramagnetic species exists as an ion-separated salt 29 with
a ( 29 Si α ) =
=
crown ether (n
=
2),THF,DME(n
=
4); R
=
SiMe t Bu 2 )
29 Si β ) =
10.2 G, whereas in the non-polar solvent the coupling to the Na +
(
29.1 G and a
cation
23 Na)
23 Na, I
(
=
=
/
was also observable for the contact ion pair 28 ( a
2, 100 %). Subsequently,
the controlled formation of 28 and 29 , both in solid state and in solution, was achieved by using the
appropriate amount of crown ether according to the reactions (iv) and (v) in Scheme 10.10. 38
The solvent-separated ion pair 29 (M
1.9 G;
3
=
=
12-crown-4, Scheme 10) is converted
to the contact ion pair 28 by removal of the crown ether with lithium bromide. The product exists
as a monomer in solution, as shown by the EPR signal with hfc constants of a
Li, crown ether
29 Si α ) =
(
34.0 G,
29 Si β ) =
7 Li)
1.6 G ( 7 Li, I
a
(
9.7 G and a
(
=
=
3
/
2, 92.5 %), but dimerizes in the solid state to the
2 ] •• ( 30 )(R
diradical [(
(Scheme 10.10), as proven by the X-ray crystal
structure. 38 The diradical 30 was produced earlier by UV irradiation of the frozen hexane solution (150
K) of the gem -dilithiosilane, [(R 2 SiLi 2
µ
-Li
·
THF) 2 (SiR 2
)
=
SiMe t Bu 2
)
, and its triplet state nature was
determined from the EPR spectrum, which consists of a signal with four
)
(R 2 HSiLi) 2 ](R
=
SiMe t Bu 2
)
29 Si sidebands arising from
2 transition. 39
M s
=
1 transitions and a signal at half-field (1675 G) resulting from the forbidden
M s
=
In contrast to linear alkynes RC
CR, the heavier group 14 congeners, RE
ER (E
=
Si, Ge, Sn), assume
a trans -bent geometry with respect to the triple bond. 40,41
Similarly to the heavy alkene analogs R 2 E
=
ER 2
(E
Si, Sn) described above, this results in a relatively low energy level for the LUMO in the heavy
alkyne compounds. By exploiting the resulting lowered potential for reduction, the disilyne radical anion,
[RSi
=
SiR]
( 31 ), is obtained directly from the neutral precursor by one-
electron reduction with KC 8 (Scheme 10.11). 40
(R
=
Si( i Pr)[CH(SiMe 3 ) 2 ] 2 )
The analogous germylene and stannylene radical anions,
ER]
[RE
(M
=
Ge, R
=
2,6-Tripp 2 C 6 H 3 ( 32a )or2,6-Dipp 2 C 6 H 3 ( 32b ); E
=
Sn, R
=
2,6-Tripp 2 C 6 H 3
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