Resonance Raman Spectrum of Distorted Porphyrin
Radical Cation Reveals Orbital Mixing
Ching-Yao Lin, Songzhou Hu, Thomas Rush III, and
Thomas G. Spiro*
Department of Chemistry, Princeton UniVersity
Princeton, New Jersey 08544
ReceiVed June 24, 1996
We report striking reversals of vibrational frequency shifts
in radical cations of Ni(II) porphines bearing n-propyl or tert-
butyl substituents on the meso-carbon atoms (Figure 1). These
reversals are evidence that the two highest occupied molecular
orbitals (HOMO) are mixed by out-of-plane distortions of the
porphyrin. The n-propyl molecule is known to be planar,
1
while
the tert-butyl molecule is severely distorted by the steric clashes
between the substituents and the adjacent pyrrole rings.
2,3
Such
distortions are known to destabilize the HOMO,
3
as evidenced
by diminution of the porphyrin oxidation potential
4
and of the
energies of the π-π* electronic transitions.
4,5
However, the
present results call attention to the electronic reorganization
which accompanies the distortion. Such reorganization may
play a role in modulating electron transfer to or from tetrapy-
rrolic centers in biology, which are subject to distortion by the
surrounding protein.
6
The two Ni(II) porphyrins undergo clean one-electron oxida-
tions, as evidenced by isosbestic visible absorption spectra
(Figure 2). The B and Q absorption energies are substantially
lower for NiT(t-Bu)P than for NiT(n-Pr)P, as is the oxidation
potential (0.65 and 0.85 V Vs SCE, determined by CV). In both
cases, however, oxidation leads to blue-shifted B bands and to
broad low-energy absorptions, characteristic of porphyrin cation
radicals.
7
Resonance Raman (RR) spectra (Figure 3) in the
1300-1600-cm
-1
region are assigned to porphyrin skeletal
vibrations Via the polarization characteristics of the bands, and
with reference to the previous RR study of the neutral molecules
by Jentzen et al.
3
As expected for B-band excitation,
8
the
spectra are dominated by totally symmetric skeletal modes, ν
2-4
.
The mode frequencies are substantially lower for NiT(t-Bu)P
than for NiT(n-Pr)P, an effect of the porphyrin distortion.
3
The
same three totally symmetric modes can readily be identified
in the radical cation spectra, and are shifted very differently in
the two molecules. Most striking is the reversal in the ν
3
shift:
down 41 cm
-1
in NiT(n-Pr)P but up 50 cm
-1
in NiT(t-Bu)P. ν
2
shifts oppositely, but by much smaller amounts: up 8 cm
-1
in
NiT(n-Pr)P and down 5 cm
-1
in NiT(t-Bu)P. Meanwhile ν
4
is
nearly unshifted in NiT(n-Pr)P but undergoes a large downshift,
37 cm
-1
, in NiT(t-Bu)P. To investigate the origin of these
differences, we carried out INDO calculations
9-11
on the two
porphyrins, focusing on the two frontier orbitals. In the planar
NiT(n-Pr)P, these are the standard a
1u
and a
2u
orbitals (Figure
1).
12
The latter lies highest, consistent with the expected
* To whom correspondence should be addressed.
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1995, 7, 733-734.
(3) Jentzen, W.; Simpson, M. C.; Hobbs, J. D.; Song, X.; Ema, T.;
Nelson, N. Y.; Medforth, C. J.; Smith, K. M.; Veyrat, M.; Mazzanti, M.;
Ramasseul, R.; Marchon, J.-C.; Takeuchi, T.; Goddard, W. A., III; Shelnutt,
J. A. J. Am. Chem. Soc. 1995, 117, 11085-11097.
(4) Barkigia, K. M.; Chantranupong, L.; Smith, K. M.; Fajer, J. J. Am.
Chem. Soc. 1988, 110, 7566-7567.
(5) Barkigia, K. M.; Renner, M. W.; Furenlid, L. R.; Medforth, C. J.;
Smith, K. M.; Fajer, J. J. Am. Chem. Soc. 1993, 115, 3627-3635.
(6) (a) Deisenhofer, J.; Epp, O.; Miki, K.; Huber, R.; Michel, H. J. Mol.
Biol. 1984, 180, 385-398. (b) Deisenhofer, J.; Epp, O.; Miki, K.; Huber,
R.; Michel, H. Nature 1985, 318, 618-624. (c) Allen, J. P.; Feher, G.;
Yeates, T. O.; Komiya, H.; Rees, D. C. Proc. Natl. Acad. Sci. U.S.A. 1987,
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1995, 376, 660-669. (e) Tsukihara, T.; Aoyama, H.; Yamashita, E.;
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R.; Yoshikawa, S. Science 1996, 272, 1136-1144. (f) Hildebrandt, P.;
Stockburger, M. Biochemistry 1989, 28, 6710-6721. (g) Hobbs, J. D.;
Shelnutt, J. A. J. Protein Chem. 1995, 14, 19-25. (h) Ravikanth, M.;
Chandrashekar, T. K. In Structure and Bonding 82; Clarke, M. J.,
Goodenough, J. B., Ibers, J. A., Jφrgensen, C. K., Mingos, D. M. P., Nelands,
J. B., Palmer, G. A., Sadler, P. J., Weiss, R., Williams, R. J. P., Eds.;
Springer-Verlag: Berlin, Heidelberg, 1995; pp 105-197.
(7) (a) Fajer, J.; Borg, D. C.; Forman, A.; Dolphin, D.; Felton, R. H. J.
Am. Chem. Soc. 1970, 92, 3451-3459. (b) Seth, J.; Palaniappan, V.; Bocian,
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(9) INDO calculations of the molecular orbitals was performed with the
program ARGUS,
10
which employs the INDO/S semiempirical Hamiltonian,
paramatrized for first-row transition metal ions.
11
Structure parameters were
taken from ref 1 for NiT(n-Pr)P, while for NiT(t-Bu)P, a 4° tilt of the pyrrole
rings was added to the molecular-mechanics-derived ruffled structure
3
(see
text).
(10) (a) Thompson, M. A.; Schenter, G. K. J. Phys. Chem. 1995, 99,
6374. (b) Thompson, M. A.; Glendening, E. D.; Feller, D. J. Phys. Chem.
1994, 98, 10465.
(11) Zerner, M.; Loew, G.; Kirchner, R.; Mueller-Westerhoff, U. J. Am.
Chem. Soc. 1980, 102, 589 and references therein.
Figure 1. The two frontier orbitals for NiT(n-Pr)P (left) and NiT(t-
Bu)P (right), calculated Via INDO.
11
Filled and open circles represent
oppositely oriented p
z orbitals, and the sizes are proportional to the
orbital coefficients.
Figure 2. Absorption spectral changes of NiT(n-Pr)P (left) and NiT-
(t-Bu)P (right) upon one-electron oxidation. The bold lines indicate
the traces of the cation radicals. Experimental conditions: OTTLE cell
17
with sample in CH2Cl2/tetrabutylamonium perchlorate; applied potential,
0.90 and 0.75 V Vs SCE for NiT(n-Pr)P and NiT(t-Bu)P, respectively.
9452 J. Am. Chem. Soc. 1996, 118, 9452-9453
S0002-7863(96)02120-8 CCC: $12.00 © 1996 American Chemical Society