Angewandte
Chemie
There are eight electrostatic interactions in the range
329.3(8)–380(3) pm between the positively charged xenon
atom of XeF2 and negatively charged FÀ ligands of the XeF4
and [AsF6]À units. In accordance with the higher positive
charge at the Xe atom in XeF4, this molecule forms six
electrostatic interactions with FÀ ligands in the range of
310.3(8)–357.7(11) pm. The shorter XeF4···XeF2 interaction of
310.3(8) pm is especially important in connecting the layers
(XeF4)](AsF6)2 because two XeF4 molecules are now coordi-
nated to the same metal center (Figure 4). Efforts to prepare
single crystals of this compound failed. Although large excess
of XeF4 was used, the only crystalline product obtained
(Figure 3). In the XeF2·XeF4 adduct,[5] this Xe Fe distance is
À
335.9 pm. The bridge angle, F-Xe-F, between XeF4 and XeF2
is 134.2(4)8.
Figure 4. Comparison of the Raman spectra of different products in
the system Mg(AsF6)2/XeF2/XeF4. * Spectrum of [Mg(XeF2)2](AsF6)2
from Reference [9].
always had the composition [Mg(XeF2)(XeF4)](AsF6)2. Thor-
ough prefluorination of the reaction vessel and very careful
purification of XeF4 did not help. The most probable reason
for the formation of XeF2 is the reduction of XeF4 during the
four weeks of crystallization in a FEP reaction vessel. The
structure of the coordination compound with only XeF4
ligands is still unknown.
Figure 3. Interactions between XeF4 and XeF2 molecules in the crystal
structure of [Mg(XeF2)(XeF4)](AsF6)2.
The most intense Raman bands of the single crystal of
[Mg(XeF2)(XeF4)](AsF6)2 occurring at 605, 596 (sh), 575, and
552 cmÀ1 (see Figure 4) can be assigned to Xe F vibrations.
À
Solid molecular XeF4 has D4h symmetry with Raman bands at
551(n4), 543(n1), 506(n5), 503(n1), 238(n6), and 216(n3) cmÀ1.[11]
When the XeF4 molecule donates one fluorine atom to a
strong Lewis acid yielding the [XeF3]+ cation of C2v symmetry,
the Raman bands are found to be at higher frequencies.
In XeF3SbF6 the Raman bands assigned to [XeF3]+ are at
643(n1), 571(n2), 607(n4), 608(n4), and 316(n5) cmÀ1.[12] In the
magnesium compound, the XeF4 species is not as far along the
ionization pathway as in the [SbF6]À salt and thus the lower
Experimental Section
Mg(AsF6)2 was prepared by the reaction between MgF2 and AsF5 in
anhydrous HF (aHF) as a solvent. XeF4 was prepared by the
fluorination of XeF2 with elemental fluorine under UV light in aHFas
a solvent at room temperature. The purity of XeF4 was checked by
gas-phase IR spectroscopy and Raman spectroscopy of the solids.
Solid product showed only the vibrational bands associated with
XeF4. Reactants Mg(AsF6)2 (0.2116 g, 0.557 mmol), XeF2 (0.1074 g,
0.634 mmol), and XeF4 (0.1191 g, 0.575 mmol) were weighed out in a
dry box. The solvent, aHF, was added on a vacuum line.
À
Xe F stretching frequencies are expected. The bands at 605,
596 (sh), and 552 cmÀ1 can be attributed to the XeF4 ligand
coordinated to the Mg2+ ion. The band at 575 cmÀ1 can be
assigned to the vibration of the nonbridging XeF2 ligand, as in
the [Mg(XeF2)2](AsF6)2 compound.[9] The band at 460 cmÀ1
could be a consequence of a coupling between vibrations of
XeF2 and XeF4. The bands at 728, 704, 687, 370, and 265 cmÀ1
probably arise from the two crystallographically distinct and
distorted [AsF6]À units.
Caution: Anhydrous hydrogen fluoride, AsF5, XeF2, and XeF4
must be handled in a well-ventilated hood and protective clothing
must be worn at all times! XeF4 and all of its products are susceptible
to moisture and they react with it forming XeO3, a compound which
easily detonates.[13] The experimentalist must become familiar with
these reagents and the hazards associated with them. For treatment of
HF injuries see reference [14].
Crystals were grown in a crystallization vessel made from a T-
shaped poly(tetrafluoroethylene-co-hexafluoropropylene) (FEP)
reaction vessel, constructed using FEP tubing of inner diameter
16 mm. A 30 cm long FEP tube of inner diameter 4 mm connected by
a teflon valve provided flexibility for decanting the aHF solution from
one arm of the T-reactor to the other. Reagents were placed in the
wider tube of a crystallization vessel in stoichiometric amounts and
dissolved in aHF. This solution was decanted into the narrower part of
the T-shaped crystallization vessel. The crystals were grown with a
temperature gradient of at least 288C and were isolated from the
The Raman spectrum of the product isolated from the
experiment using a higher molar excess of XeF4 shows the
Xe F modes at 622, 590, 575, and 549 cmÀ1 (see Figure 4). A
À
weak band at 575 cmÀ1 probably arises from some of the
coordinated XeF2 and the bands at 622, 590, and 549 cmÀ1 are
most likely the signature of coordinated XeF4 molecules.
These Raman bands are different from those of [Mg(XeF2)-
Angew. Chem. Int. Ed. 2009, 48, 1432 –1434
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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