ARTICLE IN PRESS
J. Krishna Murthy et al. / Journal of Solid State Chemistry 179 (2006) 739–746
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of light transmission make some of the metal fluorides
preferred candidates in optical as well as protective coating
forming fluoride glasses.
instrument at 77 K. Before each measurement, the
samples were degassed at 4 ꢂ 10ꢀ3 Torr and 150 1C for
10 h. The surface area was calculated according to the BET
method.
2. Experimental
Temperature-programmed desorption of ammonia
(NH3-TPD) was employed to determine the strength of
acid sites and its distribution. The sample (about 0.2 g) was
first heated under nitrogen up to 300 1C, then at 120 1C
exposed to NH3. After flushing the excess NH3 at 120 1C
with N2 for 1 h and cooling to 80 1C the TPD programme
was started (101/min up to 500 1C, keeping for 30 min).
Desorbed NH3 was monitored continuously via IR
spectroscopy (FT-IR System 2000, Perkin-Elmer).
Highly resolved X-ray photoelectron spectra (XPS) and
X-ray excited Auger electron spectra (XAES) were
acquired using a VG Scientific ESCALAB 200X electron
spectrometer as described in [6] with non-monochroma-
tized Al Ka excitation (hn ¼ 1486:6 eV) operated at 15 kV
and 20 mA and in CAE 10 mode. Before recording the
spectra the samples were stored overnight in the VG
Extended PrepLock chamber of the ESCALAB in a
vacuum better than 10ꢀ6 mbar in order to degas. During
analysis the vacuum in the spectrometer was better than
10ꢀ8 mbar. Binding or kinetic energy data were referenced
to the aliphatic C 1s peak at 284.8 eV.
Thermal analysis was done with a NETZSCH thermo-
analyser STA 409 C Skimmers system equipped with a
quadrupole mass spectrometer BALZERS QMG 421 as
described in [2a] recording the thermoanalytical curves
(T, TG, DTA) together with the ionic current (IC) curves in
the multiple ion detection (MID) mode.
Solid-state F MAS NMR experiments were done on a
Bruker AVANCE 400 spectrometer using a 2.5 mm magic
angle spinning probe. Spectra were measured at 376.5 MHz
with ultrafast spinning of 30–36 kHz. Chemical shifts were
referenced to CFCl3.
2.1. Syntheses
HS-MgF2: The synthesis procedure followed basically
that given in [2]. Mg turnings (99.98%, Aldrich) were
reacted with excessive, thoroughly dried CH3OH under
reflux conditions. The Mg(OMe)2 ꢁ 2MeOH was not
separated but after cooling reacted further under stirring
with stoichiometric amounts of HF dissolved in MeOH or
ether. A clear gel or a sol, the viscosity of which depends on
concentration was formed. Low concentrated sols of low
viscosity were used for coating experiments. The wet
viscous gel was dried under vacuum at temperatures up
to 70 1C yielding a white solid containing some organics, a
result which corresponds to that observed in course of HS-
AlF3 synthesis [2a], although in the latter system the
remaining organics measured as carbon content was
substantially higher. By further fluorination with N2
diluted gaseous HF or CCl2F2 or CHClF2 at temperatures
up to 250 1C in a tube-type flow reactor HS-MgF2 was
obtained as fine white powder.
Mg(OH,F)-materials: The preparation is a two-step
process described in [5]. Magnesium hydroxofluorides with
F/Mg molar ratios between 0 and 2 were synthesized from,
e.g., 0.2 mol magnesium methoxide in dry methanol
and then fluorinated with less than two equivalents of a
HF/Et2O solution. The remaining –OCH3 groups (Eq. (1),
product I) were hydrolysed by addition of the equivalent
amount of water to give the magnesium hydroxofluoride of
the general formula Mg(OH)2ꢀx Fx.
Complex magnesium fluorides: 30 mmol of each magne-
sium methoxide and potassium methoxide in 30 ml
methanol were mixed and reacted with 0.1 mol of
HF/MeOH at room temperature to give KMgF3 after
drying under vacuum. Similar reactions were carried out
with varying the K:Mg ratio between 1 and 3. The
amorphous or low crystalline material was calcined at
300 1C under inert carrier gas.
FT-IR measurements were done of wafers of KBr and
CsI. Spectra were recorded between 200 and 4000 cmꢀ1 on
a Perkin-Elmer 2000 spectrometer.
3. Results and discussion
3.1. Synthesis and reaction mechanism
MgF2 coatings: Thoroughly purified and dried small
plates of SiO2 or Si were placed on a spin-coater (KW-4A,
Chemat), covered with low viscous sols of MgF2 in MeOH,
and spun for 40 s at 5000 rpm. After drying at 100 1C the
coating was repeated or the layer was immediately calcined
at 300 or 500 1C.
The sol–gel fluorination reaction results in complex
development of a polymer-like network of gel structures,
essentially determined by the strength of formed
H-bonding and of van der Waals interaction forces,
causing also formation of solvates by Mg?O-bonding.
The latter depends on the partial charge at the metal.
Therefore, in this respect sol–gel reactions and gel stability
are very sensitive to solvent properties such as dielectric
constant DK, ability to hydrogen bonding, polarity
and geometric size of the molecule. Generally, the
state of the gel is irreversible and permanent. The fresh
wet gel morphology is weak and cannot survive harsh
drying treatments at elevated temperatures leading to a
2.2. Characterisation
X-ray powder diffraction (XRD) characterisation was
carried out on a XRD-7 Seiffert-FPM with Cu-Ka
radiation.
Surface area of the catalysts was determined using
N2 adsorption by means of a Micromeritics ASAP 2000