16024 J. Phys. Chem., Vol. 100, No. 39, 1996
Kuragaki and Sisido
naphthyl group are needed. The biphenyl fluorescence is
originated from a vibronic mixing of an electronic transition
polarized along the long axis with a variety of vibrational modes.
Therefore, its fluorescence band consists of many differently
polarized vibronic peaks.9 Furthermore, the absorption band
of the naphthyl group in the 285 nm region is assigned to a 1La
band that is electronically polarized along the short axis.
However, this band is only partially allowed [oscillator strength
≈ 0.05 (calculated10) and 0.13 (observed for 1-methylnaphtha-
lene)] and its polarization depends on the mode of coupling in
each vibronic peak. Therefore, the orientation factor of EnT
from an excited biphenyl to a naphthyl group is preaveraged
and may not sharply depend on the relative orientation of the
two chromophores. In the present study, as a first approxima-
tion, the orientational factor for dynamic average (2/3) was
assumed for all polypeptides that possess different relative
orientations of the two chromophores.
are arranged with designed distances and orientations. Polypep-
tides that contain sequences of NAB and NFB were prepared
for the study of the possible superexchange mediation of the F
group. As expected from Figure 4, the spatial arrangement of
the N-B pair may be kept unchanged by the insertion of a
phenyl group, but the phenyl group is outside the line that
connects the N-B pair. In this case, the EnT was not enhanced
by the phenyl group. Indeed, the efficiency of the NFB
polypeptide was slightly smaller than that of the NAB polypep-
tide.
To examine the effect of the phenyl group that is lying on
the B-N line, polypeptides that contain sequences of BG3-
FAG2N and BG4AG2N were synthesized. In both polypeptides,
the B-N pairs are separated by seven spacer amino acids, but
the former has a phenylalanine unit in the middle of the spacer.
The computer-predicted conformation of the BG3FAG2N polypep-
tide is shown in Figure 5. The center-to-center distances
between the B-N pair in the BA3FA3N sequence are predicted
to be 14.0 and 12.8 Å for type I and II orientations of the N
group, respectively. The corresponding distances in the BA7N
sequence are 13.5 and 12.5 Å. The center-to-center distances
between B and F groups in the BA3FA3N sequence are 5.9 Å
for the two naphthyl orientations, and the center-to-center
distances between F and N groups are 7.7 and 6.6 Å for types
I and II, respectively. The calculation suggested that the B-N
distance is very slightly enlarged by the insertion of the phenyl
group.
Highly Efficient Energy Transfer in BXN and NXB
Sequences. Fairly large deviations were found for three
polypeptides that contain BG1N, NAB, and NFB sequences.
All the three polypeptides have the B-N pair separated
by a single amino acid and show higher EnT efficiencies
than those expected from the Fo¨rster theory. The authors
believe that the high efficiencies are attributed neither to
any problem in polypeptide samples nor any experimental
error involved in fluorescence measurements, since the phe-
nomenon is common to the polypeptides with BXN or NXB
sequences and those polypeptides show normal absorption and
CD spectra.
The EnT efficiencies of the two polypeptides are compared
in Table 2 and in Figure 7. The efficiency increased by 5% by
the insertion of a phenyl group just on the line of the B-N
pair. The enhancement, although very small, may be attributed
to some electronic effect, since it is unlikely to expect that the
B-N distance becomes shorter by the replacement of a γ-benzyl
L-glutamate unit by a phenylalanine unit. Absorption spectra
of the two polypeptides were the same, and the positions of
fluorescence peaks were not shifted at all. These observations
suggest that the small enhancement may be caused by a
superexchange mechanism that involves virtual states of the
phenyl π system. Since the enhancement is very small,
however, a modest conclusion is that a very small mediation
of EnT, if it exists actually, may be observed when donor,
mediator, and acceptor groups are arranged in a face-to-face
configuration.
As illustrated in the case of the polypeptide GnNFBG4 in
Figure 4, a common feature of the BXN or NXB polypeptide
is that the edge-to-edge B-N distance is much shorter than the
center-to-center distance. In the case of GnNFBG4, for example,
the edge-to-edge distance is 9.4 Å for both type I and II
orientations of the naphthyl group, that is shorter than the center-
to-center distances, 13.7 and 13.6, for type I and II orientations,
respectively. The EnT efficiency calculated according to the
Fo¨rster theory is based on the interaction between point dipoles
that are positioned on the centers of the B and N groups. If the
B-N distance is shorter, contributions of higher multipole-
multipole interactions will become more important and will
increase the EnT efficiency. Furthermore, direct interactions
between π orbitals of B and N groups including the Dexter’s
mechanism of EnT may enhance the EnT. This may explain
the high EnT efficiencies of the three polypeptides. High
efficiency of the polypeptide that contains the NB sequence is
also explained in a similar manner. In the case of the
polypeptides that contain BG2N and BG3N sequences, the
center-to-center distances are already very small and the above
consideration makes little sense.
Conclusions
A variety of R-helical polypeptides that contain a pair of B
and N groups were synthesized. Energy transfer efficiency from
steady-state fluorescence measurements followed the Fo¨rster
theory up to 20 Å separation of the B-N pair. The polypeptides
that contain BXN and NXB sequences showed higher EnT
efficiency than those expected from the theory, indicating a
contribution of higher multipole-multipole interactions. The
phenyl group in the NFB sequence showed no evidence of
enhancing EnT. The phenyl group in the BG3FAG2N sequence
showed a slight enhancement of EnT, suggesting the presence
of the superexchange mechanism.
Effect of Phenyl Group Lying between B and N Groups.
One of the unknown factors in the singlet EnT is a possible
effect of π orbitals that are inserted between the energy donor
and acceptor. Although the superexchange mechanism on
electron transfer has been discussed by a number of workers,
the superexchange mechanism on EnT has been attracting very
little attention. Recently, Ghiggino and co-workers11 discussed
theoretically the role of the superexchange mechanism in EnT.
Experimental evidence of the superexchange effect is usually
difficult to obtain, since we have to compare efficiencies of EnT
in the presence and in the absence of an intervening aromatic
group without changing other factors, such as donor-acceptor
distance and orientation.
References and Notes
(1) (a) Stryer, L.; Haugland, R. P. Proc. Natl. Acad. Sci. 1967, 58,
720. (b) Gabor, G. Biopolymers 1968, 6, 809. (c) Chiu, H. C.; Bersohn, B.
Biopolymers 1977, 16, 277. (d) Leclerc, M.; Pre´milat, S.; Englert, A.
Biopolymers 1978, 17, 2459.
R-Helical polypeptides provide an ideal molecular framework
on which energy donor, possible mediator, and acceptor groups