Table 1. Optical Data and Redox Potentials of 2 and 3 in CH2Cl2
compd
λab/nm (log ε)
λ
em/nma (ΦF)b
Eox/Vc
Ered/Vc
2a
2b
2c
2d
2e
3a
3b
3c
3d
383 (4.31)
367 (4.30)
369 (4.40)
376 (4.63)
339 (3.79)
374 (4.39)
362 (4.25)
361 (4.30)
347 (3.97)
469 (0.73)
446 (0.66)
447 (0.60)
468 (0.70)
408 (0.81)
455 (0.65)
434 (0.77)
437 (0.71)
418 (0.69)
þ0.77
þ1.04
þ1.12
þ0.97
n.d.
ꢀ2.12
ꢀ2.07
ꢀ2.03
ꢀ2.05
ꢀ2.23
ꢀ2.02
ꢀ1.96
ꢀ1.95
ꢀ2.06
þ1.08
n.d.
n.d.
n.d.
a Excited at λab b Absolute fluorescence quantum yields. c First
.
oxidation (Eox) and reduction (Ered) potentials (vs Fc/Fcþ) determined
by DPV (0.1 M Bu4NþPF6ꢀ; Ag/Agþ). n.d. = Not determined.
Figure 1. Crystal structures of (a) 2b and (b) 3b: Top views
˚
(upper) and side views (lower). Selected bond lengths (A), bond
angles (deg), and torsion angles (deg): 2b: PꢀO, 1.4859(10);
C1ꢀC2, 1.3510(19); C1ꢀC9, 1.4414(19); C9ꢀC10, 1.3421(19);
C10ꢀC11, 1.466(2); C1ꢀC9ꢀC10, 125.43(12); C9ꢀC10ꢀC11,
125.79(13); C2ꢀC1ꢀC9ꢀC10, 177.03(13); C1ꢀC9ꢀC10ꢀC11,
178.81(12). 3b: PꢀO, 1.4827(8); C1ꢀC2, 1.3499(16); C1ꢀC9,
1.4196(16); C9ꢀC10, 1.2013(17); C10ꢀC11, 1.4375(17);
C1ꢀC9ꢀC10, 175.93(12); C9ꢀC10ꢀC11, 178.07(13).
clearly observed for 2aꢀc and 3aꢀc, in which Stokes shifts
increase with the increase of solvent polarity (Figures S2
and S3, Supporting Information). It should be noted that
the changes in Stokes shifts of the para-methoxy deriva-
tives (2a and 3a) are larger than those of the para-chloro
derivatives (2cand 3c). Apparently, the CT character in the
S1 states of 2-alkenyl- and 2-alkynyl-benzo[b]phosphole
P-oxides are appreciably enhanced when combined with
the electron-donating para-methoxyphenyl groups; the
benzo[b]phosphole unit behaves as the electron-accepting
function. The λab and λem values as well as the degree of
solvatochromism (Δλem = 1250 cmꢀ1) observed for 2a are
comparable to those for 3a (Δλem = 1250 cmꢀ1), suggest-
ing that the linkage effects of the vinylene and acetylene
spacers on the π-conjugation are close to each other. The
electrochemical redox processes of 2 and 3 were measured
by cyclic voltammetry (CV) and differential pulse voltam-
metry (DPV). In the CV measurements, irreversible CV
waves were observed for both oxidation and reduction
processes (Figure S4, Supporting Information). As shown
in Table 1, the para-substituents affect the oxidation
potetials (Eox) more efficiently than the reduction poten-
tials (Ered). This is consistent with theoretical prediction
(B3LYP/6-31G*); the orbital coefficient at the para carbon
in HOMO is more distinct than that in LUMO (Figure S7,
Supporting Information). The differences in the redox
potentials (Eox ꢀ Ered) increase in the order, 2a (2.89 V)
< 2b (3.11 V) < 2c (3.15 V) for the vinylene-linked series,
which agrees well with the order of their HOMOꢀLUMO
gaps obtained by the DFT calculations.
To attain some insight into excited-state dynamics of the
newly constructed π-systems, we measured fluorescence
lifetimes (τf) of 2aꢀe and 3aꢀc in CH2Cl2 at room temp-
erature. The τf values of the styryl derivatives 2aꢀd
(2.7ꢀ3.7 ns) are comparable to those of the arylethynyl
derivatives 3aꢀc (3.0ꢀ3.9 ns). The radiative and non-
radiative decay rate constants (kr and knr) calculated
from τf and Φf values are summarized in Table S2 in the
Supporting Information. Among 2aꢀc and 3aꢀc, the
effects of para substituents and π-spacers on the kr values
(1.9ꢀ2.4 ꢁ 108 sꢀ1) are negligible compared to those on the
knr values(0.6ꢀ1.5ꢁ 108 sꢀ1), although the absolutevalues
π-networks are partially stacked with the πꢀπ distances of
˚
3.4ꢀ3.5 A.
To understand the effects of the para-substituents and
the π-spacers (vinylene, acetylene) on the optical and
electrochemical properties of benzo[b]phosphole P-oxides,
we measured absorption/emission spectra and redox po-
tentialsof2 and 3 in CH2Cl2. Theresultsaresummarizedin
Figure 2 and Table 1. All the compounds examined are
moderately to highly fluorescent in solution. In each series
of the para-substituted derivatives (2aꢀc and 3aꢀc), the
absorption maxima (λab) and emission maxima (λem) shift
to longer wavelength with increasing the electron donating
ability of the para substituents on the terminal benzene
ring. In each series, the red shifts of the emission maxima
are larger than those of the absorption maxima, suggesting
that the excited singlet (S1) states are more sensitive than
the ground states to the para-substituent effects. In addi-
tion, the solvatochromism of the fluorescence spectra was
(12) 2b: C22H17OP, MW = 328.33, 0.30 ꢁ 0.25 ꢁ 0.10 mm, mono-
˚
˚
˚
clinic, P21/c, a = 9.308(2) A, b = 11.131(2) A, c = 17.312(4) A, β =
3
103.927(3)°, V = 1741.0(6) A , Z = 4, Fcalcd = 1.253 g cmꢀ3, μ = 1.62
˚
cmꢀ1, collected 13447, independent 3943, parameters 217, Rw = 0.0914,
R = 0.0395 (I > 2σ(I)), GOF = 1.053. 2c: C22H16ClOP, MW = 362.77,
˚
0.40 ꢁ 0.15 ꢁ 0.10 mm, monoclinic, P21/n, a = 6.3504(2) A, b =
3
˚
˚
˚
7.9511(3) A, c = 35.8818(12) A, β = 94.457(2)°, V = 1806.29(11) A ,
Z = 4, Fcalcd = 1.334 g cmꢀ3, μ = 3.06 cmꢀ1, collected 14141,
independent 4142, parameters 226, Rw = 0.0956, R = 0.0381 (I >
2σ(I)), GOF = 1.058. 2d: C26H19OP, MW = 378.38, 0.35 ꢁ 0.20 ꢁ 0.15
˚
˚
mm, monoclinic, P21/c, a = 8.3951(13) A, b = 8.9874(13) A, c =
3
˚
˚
25.691(4) A, β = 94.065(3)°, V = 1933.5(5) A , Z = 4, Fcalcd = 1.300 g
cmꢀ3, μ = 1.56 cmꢀ1, collected 22777, independent 4418, parameters
253, Rw = 0.0917, R = 0.0368 (I > 2σ(I)), GOF = 1.090. 3b: C22H15OP,
MW = 326.31, 0.30 ꢁ 0.25 ꢁ 0.15 mm, monoclinic, P21/c, a = 7.9918(8)
˚
˚
˚
A, b = 18.1517(17) A, c = 11.7749(12) A, β = 96.3610(10)°, V =
1697.6(3) A , Z = 4, Fcalcd = 1.277 g cmꢀ3, μ = 1.66 cmꢀ1, collected
3
˚
13548, independent 3851, parameters 217, Rw = 0.0929, R = 0.0340
(I > 2σ(I)), GOF = 1.039. 3c: C22H14ClOP, MW = 360.75, 0.30 ꢁ
˚
˚
0.20 ꢁ 0.10 mm, monoclinic, P21/c, a = 9.961(2) A, b = 8.7326(17) A,
3
˚
˚
c = 21.055(4) A, β = 102.507(3)°, V = 1788.0(6) A , Z = 4, Fcalcd
=
1.340 g cmꢀ3, μ = 3.09 cmꢀ1, collected 13927, independent 4054,
parameters 226, Rw = 0.0912, R = 0.0344 (I > 2σ(I)), GOF = 1.044.
Org. Lett., Vol. XX, No. XX, XXXX
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