In order to gain insight into the electrochemical and
conformational properties of the prototypical high
polymeric poly(ferrocenylsilane),
poly(ferrocenyldimethylsilane)
[Fe(η-C5H4)2SiMe2]
n
6, three series of oligo(ferrocenylsilanes)
R-fc-[SiMe2-fc]
n
-
1-R‘
(fc = Fe(η-C5H4)2)
7
2
−7
9
(R = R‘ = H),
8
2
−8
7
(R = H and R‘ = SiMe3),
and
9
2
−9
7
(R = R‘ = SiMe3) have been prepared and studied (the
subscript n in the oligomer refers to the number
of ferrocene units present). These species were prepared via the
anionic ring-opening oligomerization of the silicon-bridged [1]ferrocenophane
Fe(η-C5H4)2SiMe2
5. Initiation with ferrocenyllithium FcLi (Fc =
Fe(η-C5H5)(η-C5H4))
followed by quenching with H2O or SiMe3Cl
afforded
H-fc-[SiMe2-fc]
n
-
1-H
(7
2
-9
) or
H-fc-[SiMe2-fc]
n
-
1-SiMe3
(8
2
-7
), respectively.
Initiation with the dilithioferrocene complex
fcLi·2/3TMEDA followed by quenching with
H2O
or SiMe3Cl similarly afforded the oligomers
H-fc-[SiMe2-fc]
n
-
1-H
(7
2
-9
) or alternatively
the bis(silyl)-capped species
Me3Si-fc-[SiMe2-fc]
n
-
1-SiMe3
(9
2
-7
), respectively.
The individual molecular compounds of these three series
of
oligomers
7
2
−7
9
,
8
2
−8
7
,
and
9
2
−9
7
were isolated in pure form from the oligomeric mixtures by
column
chromatography and these were structurally characterized by
1H, 13C, and 29Si NMR
spectroscopy, mass spectrometry,
and in selected cases by elemental analysis. The structure of the
linear pentamer 7
5
has also been
determined by
single crystal X-ray diffraction. The central portion of this
species possesses a trans planar zigzag conformation in
the solid state and appears to be a valuable model for the analogous
conformation of the high polymer 6 in
crystalline
domains. The electrochemical behavior of each pure oligomer was
studied by cyclic and differential pulse voltammetry
and was found to depend on whether an odd or an even number of
ferrocene units were present. For oligomer
systems containing an odd number of iron centers two reversible redox
processes of varying intensities at −0.02−0.00 V and 0.21−0.23 V (vs ferrocene) were observed with a redox
splitting of 0.21−0.23 V. For oligomer systems
containing an even number of iron centers larger then two, three
reversible redox processes of varying intensities
were observed at ca. 0.00, 0.13, and 0.24 V vs ferrocene. As the
oligomer chain length increased, the electrochemical
behavior for both the “odd” and “even” series approached that
of the high polymer 6 for which two reversible
redox
processes at 0.00 and 0.24 V (vs ferrocene) of equal intensity exist.
These results are completely consistent with the
previously proposed theory that initial oxidation of 6
affords a product in which alternating iron sites are
oxidized.
Spectroelectrochemical experiments show an intervalence electron
transfer absorption (1100−1350 nm, εmax ⩽
150
M-1 cm-1) for
partially oxidized oligo(ferrocenylsilanes) that is typical for
class II mixed-valent compounds.
Additionally, single crystals were obtained of the m...
The oxidative electron-transfer properties of several superphane complexes consisting of cyclopentadienylcobalt cyclobutadiene moieties linked by either three (compounds 1 and 4) or five (compounds 2 and
5) bridging methylene groups have been studied by experimental and theoretical methods. In both cases two
separate one-electron oxidations are found. The mixed-valent monocations of the (−CH2−)5-bridged complexes
are valence-trapped with very weak interactions between metal centers. The (−CH2−)3 complexes, however,
have strong interactions between the two molecular halves. The intervalence transfer (IT) band of 1
+ has
characteristics of both class II (localized) and class III (delocalized) behavior, but the IR spectra of carboxy-labeled 4
+ clearly establish trapped valence for the monocations of the propano-bridged systems. Photoelectron
spectra and ab initio calculations at the UHF level show that, in the ground electronic state, 1
+ has a half-filled orbital (i.e., electron spin) that is essentially localized in one Co d
xy
, orbital, but that the charges on the
two metals are unequal owing to inductive electronic effects which give unequal electron flow from the ligands
to the two metal centers. Calculations and IR (carbonyl) spectral shifts suggest about a 70:30 charge ratio
between the two metal centers in 1
+ and 4
+, whereas both spin and charge localization is virtually complete
in the pentano-bridged complexes 2
+ and 5
+. The intervalence transition in 1
+ is proposed to proceed through
a “hole”-transfer process mediated by a π-cyclobutadiene MO, ultimately involving a through-bond transannular
mechanism.
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