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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Birkett, Martin
Northumbria University
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (23/23 displayed)
- 2024Precision depth-controlled isolated silver nanoparticle-doped diamond-like carbon coatings with enhanced ion release, biocompatibility, and mechanical performancecitations
- 2023Soft diamond-like carbon coatings with superior biocompatibility for medical applicationscitations
- 2023Biocompatible Ti3Au–Ag/Cu thin film coatings with enhanced mechanical and antimicrobial functionalitycitations
- 2023Biocompatible Ti3Au–Ag/Cu thin film coatings with enhanced mechanical and antimicrobial functionalitycitations
- 2022Enhanced mechanical and biocompatibility performance of Ti(1- x )Ag(x) coatings through intermetallic phase modificationcitations
- 2022Thermal activation of Ti(1-x)Au(x) thin films with enhanced hardness and biocompatibility citations
- 2022Tribological Behavior of Microalloyed Cu50Zr50 Alloy
- 2022Tribological Behavior of Microalloyed Cu50Zr50 Alloy
- 2022Mn3Ag(1-x)Cu(x)N antiperovskite thin films with ultra-low temperature coefficient of resistancecitations
- 2022Mn3Ag(1-x)Cu(x)N antiperovskite thin films with ultra-low temperature coefficient of resistancecitations
- 2022Investigating the Thermal and Mechanical Properties of Polyurethane Urea Nanocomposites for Subsea Applications
- 2022Thermal activation of Ti(1-x)Au(x) thin films with enhanced hardness and biocompatibilitycitations
- 2021Mechanical performance of biocompatible Ti-Au thin films grown on glass and Ti6Al4V substrates
- 2021Effect of noble metal (M=Ag, Au) doping concentration on mechanical and biomedical properties of Ti-M matrix thin films co-deposited by magnetron sputtering
- 2019A Numerical and Experimental Study of Adhesively-Bonded Polyethylene Pipelinescitations
- 2018Tuning the antimicrobial behaviour of Cu85Zr15 thin films in “wet” and “dry” conditions through structural modificationscitations
- 2016Mechanical behaviour of adhesively bonded polyethylene tapping teescitations
- 2016Electrical resistivity of CuAlMo thin films grown at room temperature by dc magnetron sputteringcitations
- 2016Resistor trimming geometry; past, present and futurecitations
- 2015Investigation into the Development of an Additive Manufacturing Technique for the Production of Fibre Composite Productscitations
- 2012Optimization of the deposition and annealing of CuAIMo thin film resistors
- 2008Discrete resistor technologies and potential future advancements
- 2006Effects of annealing on the electrical properties of NiCr vs AlCu thin film resistors prepared by DC magnetron sputtering
Places of action
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article
Electrical resistivity of CuAlMo thin films grown at room temperature by dc magnetron sputtering
Abstract
We report on the thickness dependence of electrical resistivity of CuAlMo films grown by dc magnetron sputtering on glass substrates at room temperature. The electrical resistance of the films was monitored in situ during their growth in the thickness range 10–1000 nm. By theoretically modelling the evolution of resistivity during growth we were able to gain an insight into the dominant electrical conduction mechanisms with increasing film thickness. For thicknesses in the range 10–25 nm the electrical resistivity is found to be a function of the film surface roughness and is well described by Namba’s model. For thicknesses of 25–40 nm the experimental data was most accurately fitted using the Mayadas and Shatkes model which accounts for grain boundary scattering of the conduction electrons. Beyond 40 nm, the thickness of the film was found to be the controlling factor and the Fuchs–Sonheimer (FS) model was used to fit the experimental data, with diffuse scattering of the conduction electrons at the two film surfaces. By combining the Fuchs and Namba(FN) models a suitable correlation between theoretical and experimental resistivity can be achieved across the full CuAlMo film thickness range of 10–1000 nm. The irreversibility of resistance for films of thickness >200 nm, which demonstrated bulk conductivity, was measured to be less than 0.03% following subjection to temperature cycles of−55 and+125 °Cand the temperature co-efficient of resistance was less than±15 ppm °C−1.