Experimental and Theoretical Spin Density in a Ferromagnetic
Molecular Complex Presenting Interheteromolecular Hydrogen Bonds
Yves Pontillon,
²
Takeyuki Akita,
‡
Andre Grand,
§
Keiji Kobayashi,
‡
Eddy Lelievre-Berna,
|
Jacques Pe ´ caut,
§
Eric Ressouche,
²
and Jacques Schweizer*
,²
Contribution from the Commissariat a ` l’Energie Atomique, MDN/SPSMS/DRFMC, CEN-Grenoble,
17 rue des Martyrs, 38054 Grenoble Cedex 9, France, Department of Chemistry, Graduate School of Arts
and Sciences, The UniVersity of Tokyo, Komaba, Meguro-Ku, Tokyo 153-8902, Japan, Institut
Laue-LangeVin, AV. des Martyrs, BP 156, 38042 Grenoble Cedex 9, France, and Commissariat a ` l’Energie
Atomique, SCIB/DRFMC, CEN-Grenoble, 17 rue des Martyrs, 38054 Grenoble Cedex 9
ReceiVed April 1, 1999. ReVised Manuscript ReceiVed August 18, 1999
Abstract: The association of phenylboronic acid (no unpaired electron, compound 1) with the free radical
phenyl nitronyl nitroxide (PNN, S )
1
/
2
, compound 2) constitutes an interheteromolecular hydrogen bonding
system displaying ferromagnetic intermolecular interactions. We have investigated its spin density distribution
to visualize the pathway of these magnetic interactions. This complex crystallizes at room temperature in the
monoclinic space group P2
1
/n. The unit cell includes one pair (1 + 2). The molecule (1) bridges two radicals
(2) by hydrogen bonds OH‚‚‚ON: the two different hydrogen bond lengths are quite similar (1.95 and 1.92
Å). Infinite chains of this run along the b-axis. In this structure the methyl groups of the PNN are randomly
distributed in two different configurations. Below T ) 220 K the compound undergoes a crystallographic
phase transition due to the ordering of these methyl groups. We have determined the low-temperature structure
using both X-ray and neutron diffraction. The new space group is P1 h. The global structure is preserved and
infinite chains still run along the b-axis, but the unit cell now comprises two different pairs (1 + 2) instead of
one, with four different hydrogen bond OH‚‚‚ON distances: 1.96 and 1.84 Å for the first pair, 1.96 and 1.91
Å for the second pair. The spin density of this complex was measured at T ) 1.8 K (H ) 4.6 T) by polarized
neutron diffraction. The data were treated using both maximum entropy approach and wave function modeling.
As in the isolated PNN, the main part of the spin density is located on the O-N-C-N-O fragment of each
radical in the unit cell. However, compared to the isolated case, a significant difference exists: a large unbalance
is observed between the two oxygen atoms of each radical. Moreover, a positive contribution is found on the
two hydrogen atoms involved on the OH‚‚‚ON hydrogen bonds of each phenylboronic acid molecule. The
stronger contribution corresponds to the longer hydrogen bonds. On the radical the stronger reduction is observed
on the oxygen atoms involved in the shorter hydrogen bonds. The experimental results are compared to those
obtained by density functional theory (DFT) calculations: on the whole, the experimental effects have been
reproduced. However, if there is a good qualitative agreement, from the quantitative point of view, the DFT
results are still very far from the experimental ones.
Introduction
Ullman’s nitronyl nitroxide radicals
1
(2-substituted 4,4,5,5-
tetramethyl-4,5-dihydro-1H-imidazolyl-1oxyl-3-oxide, Figure 1),
first synthesized as possible spin labels, have been widely used
in the preparation of metal complexes displaying ferromagnetic
properties.
2
Later, it was found that these kinds of materials
could by themselves present ferromagnetic order or ferromag-
netic behavior at low temperature.
3
Since then, only a few
compounds exhibiting these behaviors have been synthesized,
4
and some theoretical modeling works were reported.
5-7
The macroscopic physical properties of molecular crystals
are defined by intermolecular electronic interactions present in
²
MDN/SPSMS/DRFMC. Present address for Y. Pontillon: University
of Florence.
‡
University of Tokyo.
§
SCIB/DRFMC.
|
Institut Laue-Langevin.
(1) Ullman, E. F.; Osieki, J. H.; Boocock, D. G. B.; Darcy, R. J. Am.
Chem. Soc. 1972, 94, 7049.
(2) Caneschi, A.; Gatteschi, D.; Rey, P. Prog. Inorg. Chem. 1991, 39,
331. Caneschi, A.; Gatteschi, D.; Laugier, J.; Rey, P.; Sessoli, R.; Zanchini,
C. J. Am. Chem. Soc. 1988, 110, 2795. Caneschi, A.; Gatteschi, D.; Rey,
P.; Sessoli, R. Inorg. Chem. 1988, 27, 1756. Caneschi, A.; Gatteschi, D.;
Sessoli, R.; Rey, P. Acc. Chem. Res. 1989, 22, 392.
(3) Awaga, K.; Maruyama, Y. Chem. Phys. Lett. 1989, 158, 556.
Kinoshita, M.; Turek, P.; Tamura, M.; Nozawa, K.; Shiomi, D.; Nakazawa,
M.; Ishikawa, M.; Takahashi, M.; Awaga, K.; Inabe, T.; Maruyama, Y.
Chem. Lett. 1991, 1225. Awaga, K.; Inabe, T.; Nagashima, U.; Maruyama,
Y. J. Chem. Soc., Chem Commun. 1989, 1617.
Figure 1. General formula of nitronyl nitroxide free radicals.
10126 J. Am. Chem. Soc. 1999, 121, 10126-10133
10.1021/ja991042u CCC: $18.00 © 1999 American Chemical Society
Published on Web 10/13/1999