Chemistry Letters Vol.35, No.10 (2006)
1137
0342921 and CHE-0079498), U. S. A., US Department of
Energy Grant (DE-FG02-86ER13465), and the Department of
Energy, Office of Energy Efficiency and Renewable Energy
under the Hydrogen Storage Grand Challenge (DE-PS36-
03GO93013). The authors thank Prof. Noboru Morita at Tohoku
University for his helpful suggestions and comments.
H
C
–0.59
1.847
1.722
t-Bu 1.868 P89.2
94.6
81.5
P
1.846 Me
+0.84
+0.70
C
1.072
–0.59
H
References and Notes
Figure 2. A visual map of electron spin density in the opti-
mized structure of 5 at the UHF/6-31Gꢀ level. The geometry
at the optimized structure is shown on the right: bond distances
in A and bond angles (italics) in degrees ( ). The sums of the an-
gles: ꢀ(C): 360.0ꢆ, ꢀ(P): 292.8ꢆ (PMe), 350.0ꢆ (Pt-Bu). Mulliken
atomic charges on the ring are also given.
1
2
3
Multiple Bonds and Low Coordination in Phosphorus Chemistry,
ed. by M. Regitz, O. J. Scherer, Georg Thieme Verlag, Stuttgart,
1990. b) K. B. Dillon, F. Mathey, J. F. Nixon, Phosphorus: The
Carbon Copy, Wiley, Chichester, 1998.
a) M. Yoshifuji, I. Shima, N. Inamoto, K. Hirotsu, T. Higuchi,
Yoshifuji, K. Shibayama, N. Inamoto, T. Matsushita, K.
ꢆ
˚
is characteristic of ꢀ-organic radicals (Figure 1b) and could be
attributed to the radical cation 4. The radical cation spectrum
(b) was simulated by using the XSophe computer simulation
software.13 The best fit was obtained with the Lorentzian line
width of 2.2 G, two different 31P(I ¼ 1=2) hyperfine coupling
constants (hfc) constants aP1 ¼ 39:5 G, aP2 ¼ 22:3 G and the
13C (I ¼ 1=2) hfc of 30 G (Figure 1c).14 The large 31P(aP1) hfc
corresponds to the phosphorus atom with Me and the smaller
31P(aP2) corresponds to that with t-Bu, according to an ab initio
¨
1733. d) M. Yoshifuji, H. Kawanami, Y. Kawai, K. Toyota, M.
a) E. Niecke, A. Fuchs, F. Baumeister, M. Nieger, W. W.
Schmidt, A. Fuchs, D. Gudat, M. Nieger, W. Hoffbauer, E.
D. Scheschkewitz, H. Amii, H. Gornitzka, W. W. Schoeller, D.
4
5
ꢄ
calculation using [t-BuP(CH)2PMe]þ (5) as a model for 4.15
Figure 2 shows the optimized structure of 5 with the total
energy of ꢅ954:3680984 au at the UHF/6-31Gꢀ level. The
two carbon atoms assume sp2 configurations while the two phos-
phorus centers are pyramidalized. The computation depicts that
most of the electron spin density is concentrated equally on the
two carbon atoms of the C2P2 ring, and there is much smaller
electron spin density observed on the phosphorus atom attached
to methyl (PMe), while the spin density does not seem to reside
on the other phosphorus attached to t-Bu (Pt-Bu). Accordingly,
the unambiguous assignment of aP1 and aP2 was possible based
on the model calculation. The experimental spectrum (Figure 1b)
was well-reproducible if the protons with hfc < 1:0 G were used
in the simulations. Most of the positive charges in 5 locate on
the phosphorus atoms (with the larger charge at Pt-Bu), which
supports the partially delocalized structure formula 4.
6
7
8
9
a) F. A. Bell, A. Ledwith, D. C. Sherrington, J. Chem. Soc. (C)
EPR measurements at X-band (9 GHz) were carried out with a
Varian E-12 EPR spectrometer, equipped with a rectangular cav-
ity. The magnetic field was measured with a Bruker EPR 035M
gaussmeter, and the microwave frequency was measured with a
model HP 5245L frequency counter for g value determination.
ꢄ
ꢅ
.
10 UV–vis spectrum for (4-BrC6H4)3Nþ SbCl6 was reported
(ꢁmax ¼ 700 nm) and the spectrum of the reaction mixture did
not seem to contain the ammoniumyl antimonite: W. Schmidt,
E. Steckhan, Chem. Ber. 1980, 113, 577.
11 An EI-MS (70 eV) spectrum of the adducts showed obvious
ion peaks corresponding to 3þ (m/z 648) and (4-BrC6H4)3Nþ
(m/z 479).
12 The three-line spectrum of the starting reagent was also observed
(not shown in Figure 1). It could be due to a trace of mono-radical
admixture in 3, the assignment of which is in progress. See: H. D.
Brauer, J. Stieger, J. S. Hyde, L. D. Kispert, G. R. Luckhust,
are reproducible and stayed alive at room temperature even after
2 months.
13 XSophe Computer Simulation Software Suite (Version 1.1.4),
1993–2004, developed in the Centre for Magnetic Resonance
and Department of Mathematics, The University of Queensland,
Brisbane, Queensland, Australia and Bruker Biospin, GmbH,
Rheinstetten, Germany.
Our results described herein constitute a chemical transfor-
mation of 3 to a novel heterocyclic radical ion through single-
electron transfer procedure. This chemical process mirrors nota-
ble feature of the redox properties of 1,3-diphosphacyclobutane-
2,4-diyls. Recently, Niecke and co-workers reported chemical
reduction and protonation of 1,3-diphosphacyclobutane-2,4-
diyls affording the intriguing heterocyclic anion and cation,
respectively, through removal or addition of the substituents
on the ring.16,17 Therefore, such reactivity of the biradicals,
1,3-diphosphacyclobutane-2,4-diyls, promises to develop heter-
ocyclic phosphorus chemistry by furnishing novel molecular
functionalities.
In conclusion, we were successful in generating a cation rad-
ical chemically by the reaction of 1,3-diphosphacyclobutane-
2,4-diyl with tris(4-bromophenyl)ammoniumyl hexachloro-
antimonate and characterized it by EPR measurement and ab
initio calculation.
14 S. Ito, M. Kikuchi, M. Yoshifuji, A. J. Arduengo, III, T. A.
15 Ab initio calculations were performed at the UHF/6-31Gꢀ
level using a SPARTAN’04 Program Package available from
Wavefunction Inc., Irvine, CA, 2004.
This work was supported in part by Grant-in-Aid for
Scientific Research (Nos. 13304049 and 14044012) from the
Ministry of Education, Culture, Sports, Science and Technology,
Japan, the National Science Foundation (CHE-0413521, CHE-
´
16 M. Sebastian, M. Nieger, D. Szieberth, L. Nyulaszi, E. Niecke,
17 M. Sebastian, A. Hoskin, M. Nieger, L. Nyulaszi, E. Niecke,
´