Over time it was found that 6 decomposes with the elimination of
red selenium to give the five-membered heterocycle 7. The presence
reported that the six-membered ring in [MeP(l-Se2)Se]2 was
unstable and decomposed to five- and four-membered rings,
[MeP(l-Se)Se]2Se and [MeP(l-Se)Se]2, respectively. Grossmann
et al. reported both solution and solid-state NMR data of two
triselenadiphospholanes [RP(l-Se)Se)2Se (R = Me, Et).23 In line
with our observations (on 6 and 8), the magnitude of long-range
3J(PP) coupling constant was small (3.2 Hz) in [MeP(l-Se2)]Se2.22
1
of this ring was confirmed by analysis of the 31P{ H} NMR
spectra, which showed a sharp singlet at dP 49.8 ppm, with 77Se
satellites (AAꢀX systems for SeA and SeB, other AAꢀX systems for
SeC and SeD, and A2X system for SeE, A and Aꢀ denote phosphorus
nuclei, X denotes 77Se nuclei, for atom numbering see Scheme 2).
This phenomenon was also observed for 8. The room temper-
1
In good agreement with our 31P{ H} spectra of both 7 and 9,
1
ature 31P{ H} spectrum of a solution of 8 taken shortly after its
the NMR signals of (MeP(l-Se)Se)2Se and (EtP(l-Se)Se)2Se23
both appear as singlets in solution, 2J(PP) magnitudes are 34 and
31 Hz, respectively, and also the magnitudes of other short-range
couplings are similar to those found in our compounds. It is worth
noting that the anisochronous nature of the two phosphorus atoms
in 6 and 8 is in contrast to isochronicity of phosphorus atoms in
the related six-membered ring compound (PPh)6 (s, dP −22).24 By
the way of contrast, the five-membered ring compound (PPh)5
shows a very complicated second-order pattern in 31P NMR as all
its phosphorus atoms are anisochronous.
preparation showed three signals: two broad singlets at dP 40.6
and 43.0, belonging to 8, and a sharp singlet at dP 59.7 with
three sets of selenium satellites, belonging to 9 (approx. 4% of
overall integral intensity). On cooling to 203 K, the signals of
8 become sharp singlets and their 77Se satellites become visible
(Fig. 1). The analysis of these confirmed the signals stem from
the six-membered heterocycle 8. The magnitudes of the J(PSe)
1
coupling read from 31P{ H} NMR were in good agreement with
1
these found from 77Se{ H} NMR spectra. Careful analysis reveals
that J(PP) approaches zero in 8, and that the spin systems of
the two phosphorus atoms are independent and the sub-spectra
from each isotopomer are first order (AMX spin systems for
endo selenium atoms, AX spin systems for exo selenium atoms).
Compound 8 was further characterized by 1H NMR, IR, EI-MS
and microanalyses and by X-ray diffraction (Fig. 5, Table 3) which
revealed it to be structurally closely similar to 6.
The new compounds described here illustrate the accessibility of
six-membered selenium-rich heterocycles in addition to the more
familiar four- and five-membered P–Se rings.
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Fig. 5 Crystal structure of 8, 3,6-diphenyl-1,2,4,5,3,6-tetraselenadi-
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1
ca. 30% integral intensity of 9. The 31P{ H} NMR spectrum of 9 at
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room temperature consists of a sharp singlet at dP 59.7 ppm with
three sets of selenium satellites, AAꢀX systems for SeA and SeB,
another AAꢀX systems for SeC and SeD, and A2X system for SeE.
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2590 | Dalton Trans., 2006, 2586–2590
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