E. Kroke, et al.
FULL PAPER
drofluoric acid. All experiments were performed in an HF-ap-
proved fume hood and with HF-approved laboratory equipment.
The obtained harmonic frequencies were combined with standard
statistical thermodynamics to calculate Gibbs free energies at
298.15 K and 1 atm, which allow better comparison with experi-
mental data. Values of Gibbs free energies (G), sum of electronic
and thermal enthalpies (H) and sum of electronic and zero-point
energies (E + ZPE) are listed in the Supporting Information.
HF–HNO3–H2SO4 etching solution (25 mL) was prepared by add-
ing freshly distilled nitric acid (100 wt.-%) and analytical-grade hy-
drofluoric acid (40 wt.-%) dropwise to analytical-grade sulfuric
acid (97 wt.-%) in a PP beaker with ice/NaCl cooling. To distil
nitric acid, sulfuric acid (200 mL, 97 wt.-%) was added to analyti-
cal-grade nitric acid (100 mL, 65 wt.-%) with cooling. The mixture
was heated slowly and distilled at 2 kPa. After adding double the
volume of sulfuric acid to the distillate, the mixture was distilled
again.
Supporting Information (see footnote on the first page of this arti-
cle): FTIR, 19F NMR and Raman spectra, list of calculated ener-
gies, SEM images.
Acknowledgments
HF–NOHSO4–H2SO4 etching mixtures were prepared by dissolv-
ing nitrosyl hydrogensulfate in analytical-grade sulfuric acid
(97 wt.-%) and adding hydrofluoric acid (40 wt.-%). Nitrosyl hydro-
gensulfate was synthesized by bubbling dried SO2 into fuming nitric
acid (100 mL, 2.4 mol) for several hours, followed by filtration and
rinsing with glacial acetic acid and tetrachloromethane under ar-
The authors gratefully acknowledge Prof. Dr. Gerhard Roewer for
his useful discussions. Dipl.-Chem. Tobias Weling is acknowledged
for collecting the XPS spectra. This work was performed within
the Cluster of Excellence “Structure Design of Novel High-Per-
formance Materials via Atomic Design and Defect Engineering
(ADDE)” that is financially supported by the European Union
(European regional development fund) and by the Ministry of Sci-
ence and Art of Saxony.
gon. 14N NMR (H SO ): δ = 11.4 ppm. Raman (solid): ν = 414
˜
2
4
[ρ(SO3)], 571 [δs(SO3)], 597 [δas(SO3)], 871 [ν(SOH)], 1031 [νs(SO3)],
1170 [νas(SO3)], 2275 [ν(NO)] cm–1.
Trifluorosilane: Because of the rapid hydrolysis of HSiF3, the fol-
lowing manipulations were carried out under argon. In a three-
necked flask, trichlorosilane (4.74 g, 35 mmol) was added dropwise
to a suspension of zinc fluoride (10.3 g, 0.10 mol) and tetra-
hydrofuran (50 mL) with ice/NaCl cooling. To ensure complete re-
action of the trichlorosilane, the evolved gas was bubbled through a
second three-necked-flask with a suspension of zinc fluoride (5.0 g,
48 mmol) and tetrahydrofuran (40 mL) at room temperature. The
trifluorosilane was condensed in a 200 mL Schlenk flask. IR (gas
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phase): ν = 424 [δ (SiF )], 846 [δ(SiH)], 858 [ν (Si–F)], 998 [ν(SiF )],
˜
s
3
s
3
2316 [ν(SiH)] cm–1.
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Etching Procedure and Characterization: In a 100 mL Teflon three-
necked-flask, multicrystalline silicon wafer pieces (0.2 g, 7 mmol,
as-cut, boron doped, thickness 330 μm, resistivity 0.5–2 Ωcm–1,
Deutsche Solar AG Freiberg) were added to freshly prepared etch-
ing mixture (25 mL). To avoid oxidation of nitrogen oxides and
hydrolysis of trifluorosilane, all etching experiments were per-
formed under argon. Depending on the reactivity of the etching
mixture, the reaction time for each experiment varied from 120 to
600 s. Gaseous reaction products were transferred into an IR gas
cell (Thermo Fisher Scientific; d = 10 cm; window material: CaF2,
KBr) by using Schlenk techniques. The IR spectra were collected
with a Nicolet 380 FTIR spectrometer (Thermo Electron Corpora-
tion). For Raman spectroscopic investigations, a glass cuvette was
used with a T64000 spectrometer (Jobin Yvon). For XPS measure-
ments the etched silicon wafers were rinsed with deionized water
and dried immediately. Thereby, brief contact with air could not be
avoided. A Specs Phoibos 150 MCD-9 spectrometer was used for
XPS measurements with an Al-Kα source (1486.6 eV) in a vacuum
of 8ϫ10–9 mbar.
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out with Gaussian 09.[42] The geometries of the molecules under
investigation were fully optimized at the DFT level, using Becke’s
three-parameter hybrid exchange functional, the correlation func-
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