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Oxidation of Sputtered Thin Films of Molybdenum Alloys at Ambient ...

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RM 12/2 17th Plansee Seminar 2009, Vol. 1 List, Mitterer, Mori et al.<br />

Consequently, several studies have been done to improve the low-temper<strong>at</strong>ure oxid<strong>at</strong>ion and corrosion<br />

properties <strong>of</strong> Mo films. Park et al. report on spontaneous passiv<strong>at</strong>ion <strong>of</strong> sputtered Mo-Ti alloy films in 12<br />

M HCl, where corrosion r<strong>at</strong>es lower than those <strong>of</strong> the pure components have been observed for the<br />

range between 20 and 60 <strong>at</strong>.-% Ti [3]. Also Tomachuk et al. mention a superior corrosion behavior <strong>of</strong><br />

Mo-Ti films compared to Mo-Nb [4].<br />

The aim <strong>of</strong> this study was to evalu<strong>at</strong>e the effect <strong>of</strong> low contents <strong>of</strong> the alloying elements Ti, Cr, Ni, Nb,<br />

Ta, or W, respectively, in sputter deposited Mo films on their oxid<strong>at</strong>ion and corrosion resistance. In<br />

pursuit <strong>of</strong> this goal, rel<strong>at</strong>ions between thin film synthesis conditions, resulting film structure and<br />

composition have been established. Electrical, oxid<strong>at</strong>ion and corrosion properties have been determined<br />

by a four-point method, by exposure in a clim<strong>at</strong>ic test chamber and by potentiodynamic polariz<strong>at</strong>ion<br />

experiments and electrochemical impedance spectroscopy in 0.9 % NaCl aqueous solution.<br />

Experimental details<br />

Mo thin films have been grown in a labor<strong>at</strong>ory-scale unbalanced magnetron sputtering system described<br />

in detail in ref. [5]. A Mo target with a purity <strong>of</strong> ≥ 99.97 wt.-% and 152 mm diameter, mounted to an<br />

unbalanced Gencoa PP150 magnetron, has been used. For depositing alloyed films, 24 inserts <strong>of</strong> 5 mm<br />

diameter <strong>of</strong> the elements Ti, Cr, Ni, Nb, Ta, or W, respectively, have been placed in blind holes evenly<br />

distributed over the erosion track <strong>of</strong> the Mo “mosaic” target. The target-to-substr<strong>at</strong>e distance was 7.5 cm.<br />

As substr<strong>at</strong>es, alkaline earth boro-aluminosilic<strong>at</strong>e glass sheets for display technologies (Corning<br />

EAGLE2000TM AMLCD) <strong>of</strong> dimension 50.8 × 50.8 × 0.7 mm have been used, which have been cleaned<br />

before deposition using a commercial detergent from Borer Chemistry for glass cleaning. For thin film<br />

deposition, the sputtering power was 1 kW and the Ar pressure 0.3 Pa. The substr<strong>at</strong>e temper<strong>at</strong>ure was<br />

set to 120°C, and a bias voltage <strong>of</strong> -50 V was applied to the substr<strong>at</strong>es. After pre-sputtering <strong>of</strong> the target<br />

for 10 min and substr<strong>at</strong>e ion etching for 5 min <strong>at</strong> -1250 V, films with thicknesses <strong>of</strong> ~2.5 µm (deposition<br />

time, 20 min) and ~200 nm (deposition time, 100 sec) were grown. The thicker films have been used for<br />

determining the chemical composition and the growth r<strong>at</strong>e, while structural investig<strong>at</strong>ions as well as<br />

characteriz<strong>at</strong>ion <strong>of</strong> electrical, corrosion and oxid<strong>at</strong>ion properties has been done on the thinner films.<br />

The film thickness was characterized using scanning electron microscopy (SEM, Zeiss EVO-50) on<br />

fractured cross-sections and 3D optical pr<strong>of</strong>ilometry (Wyko NT1000) on the steps <strong>of</strong> partly masked and<br />

thus unco<strong>at</strong>ed substr<strong>at</strong>e areas. The chemical composition was determined using energy-dispersive Xray<br />

spectroscopy (EDS, Oxford Instruments INCA) <strong>at</strong>tached to the SEM. The efficiency <strong>of</strong> sputtering <strong>at</strong><br />

the target was simul<strong>at</strong>ed using the SRIM code (The Stopping and Range <strong>of</strong> Ions in M<strong>at</strong>ter, version<br />

2008.05 [6]). For estim<strong>at</strong>ion <strong>of</strong> thermaliz<strong>at</strong>ion behavior <strong>of</strong> energetic species sputtered from the target, the<br />

sc<strong>at</strong>tering characteristics during the transport phase from the target to the substr<strong>at</strong>e was characterized<br />

by the energy transfer coefficient ε [7]<br />

4⋅<br />

m ⋅m<br />

=<br />

( ) 2<br />

1 2<br />

ε (1)<br />

m1<br />

+ m2<br />

There, m1 is the mass <strong>of</strong> <strong>at</strong>oms sputtered from the target and m2 is the mass <strong>of</strong> Ar. X-ray diffraction<br />

(XRD) was done using a Bruker-AXS D8 Advance diffractometer with Cu Kα radi<strong>at</strong>ion in Bragg-Brentano<br />

geometry. The macro-strain in the films was calcul<strong>at</strong>ed via the XRD peak shift, while the micro-strain<br />

was estim<strong>at</strong>ed via peak broadening using a Pseudo-Voigt function. The film resistivity was measured by<br />

a four-point probe method using a MDC Multiheight Probe.<br />

The oxid<strong>at</strong>ion and corrosion properties <strong>of</strong> the films were evalu<strong>at</strong>ed by three different tests. Exposure<br />

tests were done in a clim<strong>at</strong>ic test chamber <strong>at</strong> 85 % humidity <strong>at</strong> 85°C for 168 h (1 week). Potentiodynamic<br />

and electrochemical impedance spectroscopy were additionally done in 0.9 % NaCl aqueous solution <strong>at</strong><br />

room temper<strong>at</strong>ure. As reference electrode, a s<strong>at</strong>ur<strong>at</strong>ed calomel electrode (SCE) <strong>at</strong> a potential <strong>of</strong> 241<br />

mVSHE<br />

(standard hydrogen electrode) was used. The starting potential was 100 mV lower than the open

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