[Mg(XeF2)n](AsF6)2
(9) Å) also indicates accumulation of negative charge at those
F ligands relative to the terminal ones. A similar situation
was observed in the Ca compounds [Ca(XeF2)n](AsF6)2, n
) 4 and 2.5.7 In the compounds [Mg(XeF2)n](AsF6)2, n ) 4
and 2, all XeF2 molecules are nonbridging (i.e. they do not
connect two metal centers), which is again unique among
the compounds of the type [Mx(XeF2)n](AF6)x (M ) Mg,
Ca, Sr, Ba, Pb, Ag, La, Nd; A ) As, Sb, P). This indicates
that the electron charge of the XeF2 molecule is delocalized
toward the magnesium cation, which renders the XeF2
molecule less capable of bridging two magnesium cations.
In addition to bridging XeF2 molecules, nonbridging mol-
ecules of XeF2 were observed in [Ca(XeF2)4](AsF6)2 and in
[Ln(XeF2)2.5](AsF6)3 (Ln ) La,2 Nd3) while crystal structures
of [Ca(XeF2)2.5](AsF6)2, [M(XeF2)3](AsF6)2 (M ) Pb, Sr4,5),
[Ba(XeF2)5](SbF6)2,6 and [Ag(XeF2)2]AF6 (A ) As,1 P8)
contain no nonbridging XeF2 molecules. This is the conse-
quence of the decreasing Lewis acidity of the cation and
charge transfer from the XeF2 molecule to the cation due
the covalent character of the M-F bond. It appears that
compounds with magnesium cations prefer to crystallize in
molecular ([Mg(XeF2)4](AsF6)2) or chain ([Mg(XeF2)2]-
(AsF6)2) arrangements, while [Ln(XeF2)2.5](AsF6)3 (Ln ) La,2
Nd3) contains double chains, [Ca(XeF2)4](AsF6)27 is a layer
structure, [M(XeF2)3](AsF6)2 (M ) Pb, Sr)4 contains strongly
interconnected double layers, and [Ca(XeF2)2.5](AsF6)2,7
[Ba(XeF2)5](SbF6)2,6 and [Ag(XeF2)2]AF6 (A ) As,1 P8) form
a 3D network.
Raman Spectroscopy. The Raman spectra of [Mg(XeF2)n]-
(AsF6)2 with n ) 4 and 2 are shown in Figure 4. The high
polarizability of xenon usually results in intense Raman bands
for the symmetric Xe-F stretching modes. Modes involving
Mg-F and As-F vibrations are usually far less intense and
broader.
The totally symmetric (a1g) stretching mode for XeF2
occurs at 497 cm-1.25 When XeF2 is distorted by bridging
through one F atom to Mg2+ ion, the band at 497 cm-1 is
replaced by two bands: that at higher frequency is labeled
as the shorter bond Xe-F stretching (ν(Xe-F)), and the band
at lower frequency is labeled as the longer bond Xe-F
stretching (ν(Xe‚‚‚F)). In the 1:4 compound ν(Xe-F) is 565
cm-1, and in the 1:2 compound, it is 578 cm-1. The higher
frequency in the case of the latter is a consequence of a
shorter and therefore stronger Xe-F(terminal) bond. The
vibration of the longer Xe-F bond (ν(Xe‚‚‚F)) in the 1:4
compound is probably hidden under the broad band at 469
cm-1. In the case of the 1:2 compound, ν(Xe‚‚‚F) is at 412
cm-1. The origin of the band at 469 cm-1 is not clear but
could be a consequence of the vibrational coupling of four
nonbridging XeF2 molecules. A similar band was found in
the compounds with nonbridging XeF2 molecules, e.g.
[Ca(XeF2)4](AsF6)2 at 463 cm-1 and [Nd(XeF2)2.5](AsF6)3 at
461 cm-1.3,7
-
In both compounds, the Oh symmetry of the AsF6 octa-
hedra is reduced, due to interactions with Mg2+ ions. Thus,
instead of three Raman bands (ν1 685, ν2 576, and ν5 372
cm-1),26 more bands appear. The bands at 686, 704, 599,
and 380 cm-1 in the case of the 1:4 compound and 687,
739, and the 374 cm-1 in the 1:2 compound can be assigned
[Mg(XeF2)4](AsF6)2 is not stable in a dynamic vacuum at
room temperature, slowly losing XeF2 to yield [Mg(XeF2)2]-
(AsF6)2. The lost XeF2 ligands around the Mg2+ cation are
-
-
to As-F vibrations. The symmetry reduction of AsF6
replaced by F ligands from AsF6 units that transform
+
octahedra in the XeF+, XeF3 , and KrF+ salts has been
from monodentate to cis bridging units (compare Figures 1
and 2). The Mg-F(Xe) distances are significantly shorter
(1.917(4) Å) than the Mg-F(As) distances (2.019(3) Å),
reported by several authors in the past.27-29
As reported,30 the ν1 vibrations of matrix-isolated MgF2
were found at frequencies between 514 and 544 cm-1,
depending on the matrix used. The band at 510 cm-1 in the
Raman spectra of [Mg(XeF2)n](AsF6)2 can tentatively be
assigned to the Mg-F vibrations.
-
indicating that four cis-bridging AsF6 units in the Mg
coordination sphere are electrostatically and sterically less
favorable than the two F ligands of the XeF2 molecules for
coordinating a magnesium cation (Figure 2). In addition, the
Raman stretching frequency of the nonbridging XeF2 mol-
ecule (ν(Xe-F)) in the compound [Mg(XeF2)2](AsF6)2 is
higher (578 cm-1) than that in [Mg(XeF2)4](AsF6)2 (565
cm-1; see Raman spectroscopy), which can be attributed
to a higher positive charge on the magnesium cation in
Acknowledgment. The authors gratefully acknowledge
the financial support of the Ministry of Education, Science,
and Sport of the Republic of Slovenia. We thank Dr. M.
Ponikvar for the chemical analyses of these compounds.
Supporting Information Available: An X-ray crystallo-
graphic file in CIF format, a figure showing the arrangement of
[Mg(XeF2)4](AsF6)2 molecules, and tables of X-ray powder dif-
fraction data for [Mg(XeF2)n](AsF6)2 (n ) 4, 2). This material is
-
[Mg(XeF2)2](AsF6)2. This shows that the four AsF6 units
accompanied by two XeF2 molecules in the magnesium
coordination sphere of [Mg(XeF2)2](AsF6)2 are weaker
-
electron donors that the two AsF6 units accompanied by
four XeF2 molecules in the magnesium coordination sphere
of [Mg(XeF2)4](AsF6)2. [Mg(XeF2)2](AsF6)2 has a structure
similar to that of [Mg(SO2)2](AsF6)2.24 The Mg-O distances
are 2.077(12) and 2.121(13) Å, showing that SO2 is a
weaker electron donor than the cis-bridged AsF6 unit. The
Mg-F(As) distances range from 1.953(11) to 1.987(10) Å.24
IC034826O
(25) Agron, P. A.; Begun, G. M.; Levy, H. A.; Mason, A. A.; Jones, C.
G.; Smith, D. F. Science 1963, 139, 842-844.
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(27) Gillespie, R. J.; Landa, B. Inorg. Chem. 1973, 12, 1383-1388.
(28) Gillespie, R. J.; Landa, B.; Schrobilgen, G. J. Inorg. Chem. 1976, 15,
1256-1263.
(29) Lehmann, J. F.; Dixon, D. A.; Schrobilgen, G. J. Inorg. Chem. 2001,
40, 3002-3017.
(30) Lisiecki, M. L.; Nibler, J. W. J. Chem. Phys. 1976, 64, 871-883.
(24) Hoppenheit, R.; Isenberg, W.; Mews, R. Z. Naturforsch. 1982, 37b,
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Inorganic Chemistry, Vol. 43, No. 2, 2004 703