J. Am. Chem. Soc. 1997, 119, 3625-3626
3625
Scheme 1
Acid-Base Equilibrium between
Phenoxyl-Nitronyl Nitroxide Biradical and
Closed-Shell Cation. A Magnetic pH Sensor
Katsuya Ishiguro, Mitsutoshi Ozaki, Nobuyuki Sekine, and
Yasuhiko Sawaki*
Department of Applied Chemistry, Faculty of Engineering
Nagoya UniVersity, Chikusa-ku, Nagoya 464-01, Japan
ReceiVed September 19, 1996
Spin-crossover, which means the switching between two
species or phases with different magnetic properties, have been
focused much attention, especially in developing a novel
functionality for magnetic materials.1 In relation to the recent
advances in the studies on organic ferromagnets,2 molecule-
based spin-crossovers may be also an attractive target in organic
chemistry, but a few related phenomena such as the photo-
isomerization of a carbene3a and the spin isomerism of a non-
Kekule´ molecule3b are known only under matrix-isolated
conditions.
An alternative model for spin-crossover molecules may be
given for a cross-conjugated unsymmetrical biradical with
donor-acceptor characters (D•-A•); if the singlet zwitterionic
state (D+-A-) is energetically close to the triplet biradical state,4
a large difference between them in dipole moments or acid-
base properties may bring about a novel reversed relative
stability by their intermolecular interaction. Typically, when
the zwitterionic state may be stabilized in acidic media by
forming D+-AH species, the spin-state may be controlled by
changing pH of solutions.
A•, 4), and anion radical (D•-A-, 5), were shown to persist
during the voltammetric analyses.
The absorption spectrum of 1 in acetonitrile showed maxi-
mum absorption bands at 283, 322, 365, and 615 nm,5 and those
of 2 were observed at 318, 359, and 604 nm (solid line in Figure
2B). On the other hand, the chemical one-electron oxidation
-
of 1 with Cu(ClO4)2 (Ered ) +1.0 V vs SCE)7a or NO+BF4
(Ered ) +1.3 V vs SCE)7b in acetonitrile resulted in almost
complete conversion of 1 but the formation of 2 was not
identified by absorption spectrum. Instead, an alternative
product was formed which showed the maximum absorption at
334 nm (solid line in Figure 2A). A similar absorption spectrum
could be obtained by the controlled potential electrolysis (+0.9
V vs SCE, ∼1 F/mol) of 1 in acetonitrile containing 0.1 M
n-Bu4NBF4. According to the cyclic voltammogram of 1, the
product at λmax ) 334 nm was assigned as the closed-shell cation
3 generated by the removal of unpaired electron from the
nitronyl nitroxide, which does not deprotonate the phenol proton
under the neutral conditions.
The interconversion between 2 and 3 was successfully
observed by the addition of acid or base. Spectral changes upon
the addition of pyridine to the solution of 3 prepared from 1
and Cu(ClO4)2 are shown as dashed lines in Figure 2A. The
clear isosbestic points observed at 322, 355, and 362 nm indicate
the quantitative nature of the transformation (3 f 2). The
absorption spectrum of 2 was also obtained by the electrolysis
of 1 followed by the deprotonation of 3 with pyridine. The
reverse transformation, i.e., the protonation of biradical 2 by
acids leading to the formation of cation 3, could be followed
by the changes in absorption spectra upon the addition of
trifluoroacetic acid to the solution of 2 (dashed lines in Figure
2B), indicating the equilibrated acid-base pair (2 and 3) with
different spin multiplicities.
Recently, we could prepare a cross-conjugated phenoxyl-
nitronyl nitroxide biradical, 2-(3′,5′-di-tert-butylphenyl-4′-oxy)-
4,4,5,5-tetramethyl-4,5-dihydro-1H-imidazole-1-oxyl 3-oxide, 2,
by the PbO2 oxidation of the corresponding phenol-substituted
radical 1.5 In contrast to the triplet biradical structure of 2 as
confirmed by ESR spectroscopy,6 the one-electron oxidation of
1 in acetonitrile led to the generation of the corresponding
closed-shell cation (3), which was silent on ESR. We report
here an acid-base pair of 2 and 3 with different spin multiplici-
ties, both of which satisfies the requirement of kinetic stability
in solutions (Scheme 1), representing a novel pH sensor
responding by the change of magnetic property.
As reported before,5 the PbO2 oxidation of a phenol-
substituted nitronyl nitroxide radical (D•-AH, 1) led to the
formation of diradical 2 almost quantitatively, which was stable
in solution and could be isolated as a powder. The redox
properties of 1 and 2 were investigated by cyclic voltammetry
in acetonitrile containing 0.1 M n-Bu4NBF4 as a supporting
electrolyte. The voltammogram of 1 showed a reversible couple
at +0.71 V vs SCE (Figure 1a). While the oxidation of 2
occurred at +1.00 V vs SCE, the reduction of 2 showed a
reversible peak at -0.05 V vs SCE (Figure 1e). Thus, all of
the intermediates generated by the redox reactions of 1 and 2,
such as closed-shell cation (D+-AH, 3), cation radical (D+-
The interconversions were also observable by cyclic voltam-
metry in acetonitrile solutions. When 10.0 mM pyridine was
added to the solution of 1, the oxidation peak at +0.7 V became
irreversible and the formation of 2 was identified by the
appearance of its redox peak at +1.0 V (Figure 1d). The
formation of 2 decreased with decreasing basicity of pyridines
B
on the order of pyridine (pKa ) 12.3)8a > 3-chloropyridine
B
B
(pKa ) 9.0,8b Figure 1c) > 4-cyanopyridine (pKa ) 7.0,8c
Figure 1b). The voltammogram of 2 (Figure 1e) was also
affected by the presence of acids. When 10.0 mM acetic acid
(pKa ) 22.3, Figure 2f) was added,9 the oxidation peak of 2 at
+1.0 V remained but the reversible cathodic couple at -0.05
V vs SCE became irreversible, indicating that acetic acid is not
stronger acid than 3 but can protonate the anion radical 5 to
yield 1. With a stronger acid such as trifluoroacetic acid (pKa
(1) (a) Kahn, O. Molecular Magnetism; VCH Publishers: New York,
1993. (b) Gu¨tlich, P.; Hauser, A.; Spiering, H. Angew. Chem., Int. Ed. Engl,
1994, 33, 2024 and references cited therein.
(2) Iwamura, H. AdV. Phys. Org. Chem 1990, 26, 179 and references
cited therein.
(3) (a) Sander, W.; Bucher, G.; Reichel, F.; Cremer, D. J. Am. Chem.
Soc. 1991, 113, 5311. (b) Bush, L. C.; Heath, R. B.; Berson, J. A. J. Am.
Chem. Soc. 1993, 115, 9830.
(4) Salem, L.; Rowland, C. Angew. Chem., Int. Ed. Engl. 1972, 11, 92.
(5) Ishiguro, K.; Ozaki, M.; Kamekura, Y.; Sekine, N.; Sawaki, Y. Mol.
Cryst. Liq. Cryst. In press.
(6) The hyperfine coupling constant in toluene is aN ≈ 3.7 G (2N) at
room temperature and the zero-field splitting parameters at 77 K are |D/
hc| ) 0.107 cm-1 and |E/hc| ≈ 0.5 See Supporting Information for the
ESR spectra.
(7) (a) Bethell, D.; Handoo, K. L.; Fairhurst, S. A.; Sutcliffe, L. H. J.
Chem Soc., Perkin Trans. 2 1977, 707. (b) Lee, K. Y.; Kuchynka, D. J.;
Kochi, J. K. Inorg. Chem. 1990, 29, 4196.
(8) (a) Coetzee, J. F.; Padmanabhan, G. R. J. Am. Chem. Soc. 1965, 87,
5005. (b) Cauquis, G.; Deronzier, A.; Serve, D.; Vieil, E. J. Electroanal.
Chem. Interfacial Electrochem. 1975, 60, 205. (c) Schlesener, C. J.;
Amatore, C.; Kochi, J. K. J. Am. Chem. Soc. 1984, 106, 7472.
(9) Kolthoff, I. M.; Chantooni, Jr., M. K.; Bhowmik, S. J. Am. Chem.
Soc. 1968, 90, 23.
S0002-7863(96)03289-1 CCC: $14.00 © 1997 American Chemical Society