Martins et al.
Scheme 1
As shown in Figure 1 and Table 1, at 23 °C, the tacn
methylenic proton resonances and the dimethylsilyl proton
resonances of complexes [Ti{N(Ph)SiMe2}3-tacn]X are
strongly dependent on the solvent and counterions.
In d5-bromobenzene, all complexes display an AA′BB′
pattern for the methylenic Hsyn and Hanti resonances that is
maintained in CD2Cl2, except for 3 that leads to a deceptively
simple AA′BB′ spectrum. In CD3CN, the Hsyn and Hanti
resonances of 1 and 2 appear superimposed in an apparent
singlet whereas 3 and 4 give rise to a more complex AA′BB′
pattern. In d2-dichloromethane and d5-bromobenzene, Hsyn
resonances appear at higher field than Hanti for complexes
1, 2, and 3, although for complex 4, those resonances invert
their relative positions, with Hanti being observed at higher
field than Hsyn. In both solvents, Hsyn and Hanti resonances
are more shielded in complex 4 than in complexes 1, 2, and
3. The shifts to high field registered in all complexes are
[Ti{N(Ph)SiMe2}3-tacn]I with LiNMe2 is also reported and
discussed in the light of the interactions described.
Results and Discussion
Cationic [Ti{N(Ph)SiMe2}3-tacn]X (X ) Cl, 1; I, 2; PF6,
3; BPh4, 4; tacn ) triazacyclononane) have been recently
reported by some of us.22 The complexes, which are readily
prepared by oxidation of the neutral Ti(III) precursor, were
characterized by X-ray diffraction (2 and 4) and NMR that
confirmed the titanium coordination to six nitrogen atoms
in a distorted trigonal prismatic geometry.
more pronounced for Hanti than for Hsyn
.
The NOESY spectrum of complex 4 in CD2Cl2 (Figure
2) shows (i) strong interactions between the ortho- and meta-
phenyl anion protons (δ 7.34 and 7.06, respectively) and the
cation Hanti resonance (δ 3.08-2.96), (ii) weak interaction
between the ortho-Ph anion protons (δ 7.34) and the cation
Hsyn (δ 3.36-3.24), and (iii) medium interactions between
all BPh4- protons and the Si(CH3)2 protons (δ 0.41). These
In solution, a fluxional process consisting in the trigonal
twist of the amido and amine nitrogen planes is accompanied
by a change in the conformation of the five-member Ti-
NCH2CH2N metallocycles, in such a way that the overall
process corresponds to the intramolecular conversion of
enantiomers (∆(λλλ)/Λ(δδδ)) (Scheme 1). An analogous
equilibrium was identified for [Ti{N(Ph)SiMe2}3-tacu]I (tacu
) triazacycloundecane).23 In this case, due to the different
macrocycle chain lengths (C2 and C3), the global fluxional
process has a further component that is the boat/chair
conversion of the six-member metallocycles formed by the
bonding of the NC3N moieties to the titanium. Although a
static 1H spectrum was not obtained until -70 °C in CD2Cl2
and overlapping resonances did not allow the estimation of
activation parameters, variable-temperature NMR studies
allowed the differentiation of the three independent processes
and gave information about their limit temperatures. δ/λ
isomerization is the higher-activation-energy process, being
blocked at -40 °C, ∆/Λ equilibrium stops at -70 °C and
the chair/boat conversion is still operative at -70 °C.
In addition to the intramolecular processes mentioned, the
solutions of cations [Ti{N(Ph)SiMe2}3-tacn]X also disclose
ion pair formation that have a deep influence on the 1H NMR
and UV-vis absorption and emission spectra.
-
results show that the BPh4 anions are located at the
macrocycle side, close to Hanti and to the dimethylsilyl
groups, with which nonbonded interactions between atoms
of the two ionic moieties are the strongest exhibited (Scheme
-
2). The lack of NOE between the BPh4 and NPh protons
further confirms the anion preference to locate on the side
of the triazacyclononane ring.
Thus, the shifts to high field observed for the macrocyclic
-
protons are consistent with the BPh4 ring current effects.
The outcome is mainly noticed in the Hanti resonance because
the anion is closer to Hanti than to Hsyn protons. The shielding
of Si(CH3)2 signals, more pronounced in d5-PhBr than in
dichloromethane, also reflect the proximity of the anion and,
as expected due to the lower dielectric constant of bro-
mobenzene, ion pairing is more effective in this solvent than
in dichloromethane.
To evaluate the importance of ion pairing in the solutions
of complexes 2 and 3, absorption and emission spectra were
recorded in CH2Cl2 and CH3CN (Figures 3 and 4). In
CH3CN, the two electronic absorption spectra are identical,
with maximum, λa, at 285 nm for 2 and at 286 nm for 3.
Electronic excitation at higher and lower energies relative
to the maximum of the band centered at λa around 285 nm
produces similar emission spectra. Accordingly, lumines-
cence collected at higher and lower energies relative to the
emission maximum also gives rise to similar spectral
distributions corresponding well to the respective absorption
profiles. Thus, the 2 and 3 emitting states in CH3CN can be
ascribed to the directly excited (relaxed) electronic states of
the cation. In CH3CN, the emission spectra of 2 displays
more intense fluorescence than that of 3. In spite of the
(18) Song, F.; Lancaster, S. J.; Cannon, R. D.; Schormann, M.; Humphrey,
S. M.; Zuccaccia, C.; Macchioni, A.; Bochmann, M. Organometallics
2005, 24, 1315.
(19) Zuccaccia, C.; Stahl, N. G.; Macchioni, A.; Chen, M.-C.; Roberts, J.
A.; Marks, T. J. J. Am. Chem. Soc. 2004, 126, 1448.
(20) Babushkin, D. E.; Brintzinger, H. H. J. Am. Chem. Soc. 2002, 124,
12869.
(21) Chen, Y.-X. E.; Metz, M. V.; Li, L.; Stern, C. L.; Marks, T. J. J. Am.
Chem. Soc. 1998, 120, 6287.
(22) Dias, A. R.; Martins, A. M.; Ascenso, J. R.; Ferreira, H.; Duarte, M.
T.; Henriques, R. T. Inorg. Chem. 2003, 42, 2675.
(23) Martins, A. M.; Ascenso, J. R.; Azevedo, C. G.; Dias, A. R.; Duarte,
M. T.; Ferreira, H.; Ferreira, M. J.; Henriques, R. T.; Lemos, M. A.;
Li, L.; Ferreira da Silva, J. L. Eur. J. Inorg. Chem. 2005, 1689.
-
extremely high dielectric constant of the solvent, the PF6
anion may act as a more efficient quencher, thereby
9018 Inorganic Chemistry, Vol. 44, No. 24, 2005