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Electronic Properties of Ceramic Films
Tim Jurasevich Advisor: Dr. Kvam
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Outline Background Info Goals Procedure Results Conclusions
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Perovskites ABO3 Middle atom can move Cubic above Curie temperature
Structure changes below Curie temperature Permanent dipole
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Conductive Metal Oxides
Middle atom won’t move Not capacitive Ferroelectric Fatigue
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SrRuO3 Orthorhombic a = 5.57 Å b = 7.86 Å c = 5.54 Å Nearly Tetragonal
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LaNiO3 Rhombohedral a = 5.45 Å Low degree of tilt Nearly Cubic
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Research Goals Create Strontium Ruthenate (SrRuO3) and Lanthanum Nickelate (LaNiO3) thin films Sol-gel process Refine process Investigate properties of the thin films
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Sol-gel process SrRuO3 sol-gel Black More black LaNiO3 sol-gel
RuCl3 Ethanol Water SrAc2 H2O2 Black More black LaNiO3 sol-gel La(NO3)3 2-methoxyethanol MEA NiAc2 Dark Blue
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Sol-gel process Spin coated Annealed SrRuO3 on Silicon LaNiO3 on Glass
800°C 700°C
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Visual Inspection
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Sputtering Platinum Platinum stripes sputtered along the edges and in the middle Lots of platinum required for good electrode
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Optical Microscopy
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X-Ray Diffraction
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X-Ray Diffraction
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X-Ray Diffraction
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Resistivity SrRuO3 LaNiO3 ρ = 350 µΩ∙cm Ideal: 300 µΩ∙cm ρ = 700 µΩ∙cm
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Conclusions SrRuO3 and LaNiO3 can be prepared by sol-gel methods
Both thin films exhibit fairly low resistivities Process variations affect crystallographic texture
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Thank You Questions? Comments?
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