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Dielectric Aluminum Oxides: Nano-Structural Features and ...

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The surfaces of various films on Al substrates were observed with a Hitachi FE-4800. An<br />

electron beam with 1.5 keV acceleration voltage <strong>and</strong> 7-10 µA current was used for imaging.<br />

Working distance was kept at ~ 1.5 mm while both SE detectors were mixed for better detail.<br />

Prior to the FE-SEM analysis, all films were coated with a 2 nm Pt/Pd layer from a 208<br />

HR/MTM20 Cressington Sputter unit.<br />

Specimens to be examined by TEM were thinned using a Hitachi FB2000A focused ion<br />

beam (FIB). A beam of Ga ions radiating parallel to the plane of the sample face was used to<br />

cut sections of ~ 50 nm thickness. These thin sections of the oxide films on Al substrate were<br />

examined with a Hitachi HD-2300 TEM. A beam with 200 kV acceleration voltage <strong>and</strong> 20-<br />

30 µA current was used for imaging. Electron diffraction patterns were generated using a<br />

beam diameter of 200-300 nm at 200 kV <strong>and</strong> 80-85 nA current.<br />

Stability Testing was accomplished by using a ramp-build-time test in 85 °C citric acid<br />

solution with 0.5 mA/cm2 current density after boiling for two hours in deionized (DI)-<br />

water. The rise times to 95% of V f were measured <strong>and</strong> used to assess the stability of the<br />

grown oxides, <strong>and</strong>, in turn, the level of defects/voids exposed by boiling.<br />

Anodization of Etched Foil:<br />

RESULTS<br />

One of the accepted methods of producing amorphous aluminum oxide for high voltage use<br />

involves initially anodizing the etched foil at low temperature in an oxidizing acid such as<br />

sulfuric acid to deposit a thick amorphous, porous layer of alumina inside the etch structure.<br />

Figures 1 <strong>and</strong> 2 show a plan view <strong>and</strong> a cross-sectional view of such porous oxides inside of<br />

etch tunnels. While this oxide has little in the way of barrier properties, it serves as the base<br />

layer for a formation step which fills in the pores with additional amorphous oxide to leave a<br />

barrier layer of the desired forming voltage. This oxide has the ability to withst<strong>and</strong> high<br />

duty cycles of charge – discharge with minimal increases in leakage current <strong>and</strong> dissipation<br />

factor. Unfortunately, amorphous oxide has a higher dielectric ratio [~1.4 nm/V] as<br />

compared to crystalline aluminum oxide [~1.0nm/V] which leads to 40% lower capacitance.<br />

The disadvantage of crystalline oxide is the presence of appreciable tensile stress which may<br />

lead to relaxation <strong>and</strong> cracking when subjected to thermal, chemical, electrical or mechanical<br />

stressors. The 40% capacitance advantage of crystalline oxide explains why so much work<br />

has gone into stabilization of the crystalline oxide on capacitor foils.<br />

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