Y. Matano et al.
Table 1. Optical[a] and electrochemical[b] data for 4a–c, 5a–c, and 6.
and energies. The opposite is noted for 5c-m; the LUMO
has a character of the acenaphthylene subunit, whereas the
LUMO+1 possesses a character of phosphole. A similar
trend was found for the s3-P models (4a-m, 4b-m versus 4c-
m). It is evident that the peripheral functionalizations dra-
matically alter the characters of LUMO and LUMO+1 of
the [c]-fused phosphole-naphthalene p-systems.
[c]
[c]
[d]
[e]
[e]
Compd
labs (log e)
lem (FF
)
Eox
Ered
DE[f]
4a
4b
4c
5a
5b
5c
6
399 (4.12)
404 (4.23)
464 (3.89)
439 (3.62)
459 (3.58)
414 (3.96)
386 (4.15)
480 (0.38)
482 (0.23)
–
+0.64
+0.52
+0.74
+0.94
+0.77
+0.98
+1.19
ꢀ2.38
ꢀ2.42
ꢀ1.76
ꢀ1.82
ꢀ1.89
ꢀ1.61
ꢀ2.02
3.02
2.94
2.50
2.76
2.66
2.59
3.21
[g]
552 (0.08)
583 (0.07)
[g]
–
To reveal the nature of the observed excitations, we also
performed time-dependent (TD)-DFT calculations on the
models (Table S1 in the Supporting Information). Qualita-
tively, the theoretically calculated results well explain the
experimentally observed absorption spectra. In a series of
the s3-P derivatives, HOMO–LUMO and HOMO–
LUMO+1 transitions of 4a,b are overlapping at around
400–410 nm, whereas the respective transitions of 4c are ob-
served separately at 464 and 380 (shoulder) nm. In a series
of the P-oxo derivatives, HOMO–LUMO and HOMO–
LUMO+1 transitions of 5a,b appear separately at 460–490
and 380–400 nm, respectively, whereas those of 5c are over-
lapping at around 410–480 nm. Specifically, the P-oxidation
considerably stabilizes the phosphole-based p* orbitals
(DELUMO =0.59 and 0.55 eV for the naphthalene- and ace-
naphthene-fused derivatives; DELUMO+1 =0.53 eV for the
acenaphthylene-fused derivative) as compared to the respec-
tive HOMO (DEHOMO =0.20–0.21 eV), which results in large
red-shifts of the HOMO–LUMO transitions for the naph-
thalene- and acenaphthene-fused derivatives (Dl=63 and
60 nm) and the HOMO–LUMO+1 transition for the ace-
naphthylene-fused derivative (Dl=49 nm). It should be
noted that the P-oxidation from 4c to 5c makes a relatively
small impact on the transition from the HOMO to the ace-
naphthylene-based LUMO (Dl=22 nm).
491 (0.19)
[a] UV/Vis absorption and fluorescence measurements were made in
CH2Cl2. [b] Redox potentials were determined by DPV in CH2Cl2 with
ꢀ
0.1m nBu4N+PF6 (Ag/AgNO3). [c] Absorption and emission maxima are
given in nm. [d] Fluorescence quantum yield relative to Rꢂauꢃs 3,4-C4-
bridged 1-phenyl-2,5-bis(2-thienyl)phosphole–AuCl Complex (FF =0.129;
ref. [3c]). [e] First oxidation (Eox) and reduction (Ered) potentials are
given in V versus Fc/Fc+ couple. [f] EoxꢀEred (in V). [g] Non-fluorescent.
To gain a deep insight into the electronic structures of the
naphthalene-, acenaphthene-, and acenaphthylene-fused
phosphole derivatives, we carried out density functional
theory (DFT) calculations on model compounds 4x-m and
5x-m (x=a, b, c) without the phenyl group on the P atom
(Figure 1). The Cs symmetric structures of these compounds
were optimized at the B3LYP/6-31G* level. As visualized in
Figure 4 and S3 in the Supporting Information, the HOMO
Redox potentials of 4, 5, and 6 were measured by cyclic
voltammetry (CV) and differential pulse voltammetry
(DPV) (Table 1 and Figure S4 in the Supporting Informa-
tion). It was found that the electrochemical reduction pro-
cesses of P-oxo derivatives 5a–c and 6 occurred reversibly.
The first reduction potentials (Ered) of 5a–c are more posi-
tive than Ered of 6, indicating that the electron-accepting
ability of [c]-fused phospholes is appreciably improved by
the introduction of the naphthalene, acenaphthene, or ace-
naphthylene subunit. Among 5a–c, the difference (DE) in
the first oxidation potential (Eox) and Ered decreases in the
order: 5a (2.76 V) > 5b (2.66 V) > 5c (2.59 V). In the
cases of the naphthalene- and acenaphthene-fused deriva-
tives, P-oxidation (from 4a,b to 5a,b) shifts Ered to the posi-
tive side more considerably than Eox. As a result, the DE
values of 5a,b are smaller than those of 4a,b, which is in
good accordance with the results obtained from the absorp-
tion spectra and DFT calculations (see above). Most impor-
tantly, the above electrochemical data suggested that 5a–c
would be possible candidates for the phosphole-based elec-
tron-transporting materials in terms of the electric potential
and the reversibility of their reduction processes.[9]
Figure 4. HOMO (lower), LUMO (middle), and LUMO+1 (upper) of a)
5a-m, b) 5b-m, and c) 5c-m. The calculated orbital energies (in eV) are
shown in parentheses.
of each model is spread over the entire p-conjugated plane
with anti-bonding character between the phosphole and
naphthalene rings. On the other hand, the LUMO and
LUMO+1 display the character of each subunit. In the case
of 5a-m, the LUMO basically consists of a typical LUMO
of phosphole, and the LUMO+1 displays a character of the
naphthalene backbone. The LUMO and LUMO+1 of 5b-m
resemble those of 5a-m with respect to the orbital diagrams
With this in mind, we evaluated the thermal stability of
5a–c. Compounds 5a and 5b were found to be stable up to
2508C, indicating that the thermal stability of the naphtha-
10002
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2009, 15, 10000 – 10004