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Biennial Report 2016/2017

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<strong>Report</strong>s<br />

precursor thin films was determined<br />

gravimetrically.<br />

Precursor UV irradiation was carried out in a<br />

homemade chamber [1.2 m 3 h -1 nitrogen gas flow,<br />

*<br />

0.25 % oxygen], equipped with a Xe 2 excimer<br />

lamp having a continuous emission in the VUV<br />

wavelength range at 160 nm < λ < 195 nm<br />

[photon energy 7.75 > E Ph > 6.36 eV, 614 kJ mol -1<br />

< ȂE < 748 kJ mol -1 ], enough for photoinitiated<br />

radical bond cleavage reactions of C-C<br />

(348 kJ mol -1 ), C-O (358 kJ mol -1 ) and C-H<br />

(413 kJ mol -1 ) bonds in the organic ligands of<br />

titanium(IV) ethoxide [Ti(OEt) 4 ] as precursor.<br />

During irradiation the temperature at sample<br />

surface did not exceeded 34 °C. ATR-FTIR<br />

spectra on pristine and irradiated Ti(OEt) 4 thin<br />

films were recorded under flowing nitrogen<br />

atmosphere in absorbance mode. Gaseous<br />

reaction products were enriched on a solid phase<br />

microextraction fiber assembly and analyzed<br />

using a gas chromatography system coupled with<br />

a mass selective detector (GC-MS).<br />

Film morphology was obtained by scanning<br />

electron microscopy (SEM) at an acceleration<br />

voltage of 1 kV. Thin film depth profiles were<br />

produced by multiple X-ray photoelectron<br />

spectroscopy (XPS) analysis cycles together with<br />

material removal via sputtering using argon ions<br />

(0.5 kV). The thin films structure was investigated<br />

using X-ray diffraction (XRD) in Bragg-Brentano<br />

geometry with Cu Kα 1 radiation (λ = 0.15406 nm),<br />

in the 2θ range of 20°-70° and a step width of<br />

0.05°. X-ray reflectivity (XRR) measurements<br />

were performed using a combined high-resolution<br />

reflectometer/diffractometer setup with parallelbeam<br />

geometry. X-ray radiation was collimated by<br />

a multilayer-gradient X-ray mirror. Cu Kα 1<br />

radiation was exclusively obtained by passing a 2-<br />

bounce Ge(220) crystal monochromator.<br />

Measurements were carried out in the range<br />

between 0°-1.25° (step widths of 0.002°). The<br />

intensity of the radiation which was reflected from<br />

the sample was determined by a scintillation<br />

detector. UV-Vis transmittance of thin films onto<br />

quartz was measured in the range of 300-1000<br />

nm. Film thicknesses of the spin-coated and VUV<br />

irradiated samples was measured by<br />

spectroscopic ellipsometry (SE) in the spectral<br />

range from 400-1700 nm at three angles of<br />

incidence (65°, 70° and 75°). Water vapour<br />

transmission rates of TiO x covered PET films<br />

were determined at 38 °C and 90 % relative<br />

humidity.<br />

Quantum chemical calculations employing<br />

Density Functional Theory (DFT, B3LYP, Jaguar<br />

program package) helped us to understand the<br />

underlying molecular mechanisms. Structures and<br />

energies of possible transformations of the<br />

molecules were calculated at B3LYP/LACVP*<br />

level of theory. The frequency analysis was done<br />

at the same level of theory to characterize the<br />

stationary points on the potential surface and to<br />

obtain total enthalpy (H) and Gibbs free energy<br />

(G) at a standard temperature of 298.15 K using<br />

unscaled vibrations. ∆H and ∆G were calculated<br />

as the difference of the calculated H and G<br />

between reactants and products. For better<br />

understanding of observed experimental IRspectra,<br />

frequency analysis was done on possible<br />

structures, which could be built during<br />

transformations of studied geometries after UV<br />

excitation (E Photon = 7.2 eV). The electronic<br />

excitation energies were calculated using the<br />

Time Dependent (TD) DFT method at the<br />

B3LYP/LACVP* level of theory.<br />

Results and Discussion<br />

Ti(OEt) 4 conversion and decomposition kinetics<br />

(Fig. 1) for different precursor layer thicknesses<br />

were obtained under the assumption that ATR-<br />

FTIR peak areas of C-O-based vibrations<br />

between 1200-980 cm -1 represent the remaining<br />

precursor contents. Measured data of the initial C-<br />

O bond scission initiated by VUV photons can be<br />

fit by a first-order law (correlation r 2 > 0.97) with<br />

apparent rate constants of 2.4x10 -2 s -1 ,<br />

1.6x10 -2 s -1 , 0.6x10 -2 s -1 for precursor film<br />

thicknesses of 270, 550 and 1060 nm,<br />

Fig. 1: Area of normalized ATR-FTIR peaks for C-O based<br />

vibrations in the range of 1200-980 cm -1 (A IR1200-980 cm-1) after<br />

VUV irradiation (t irradiation) and different radiant exposure (H e)<br />

and a logarithmic plot of the initial reaction rates (k app) for<br />

different precursor thin film thicknesses (d Ti(OEt)4) (inset)<br />

[average radiant exposure per minute (H e/t) =<br />

0.31 J cm -2 min -1 ].<br />

23

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