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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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Ruzic, David N.
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Publications (5/5 displayed)
- 2020Study of a linear surface wave plasma source for tin removal in an extreme ultraviolet sourcecitations
- 2005A model for ion-bombardment induced erosion enhancement with target temperature in liquid lithiumcitations
- 2002Enhancement of aluminum oxide physical vapor deposition with a secondary plasmacitations
- 2001Absolute sputtering yield of Ti/TiN by Ar+/N+ at 400-700 eVcitations
- 2001Measurements and modeling of D, He and Li sputtering of liquid lithiumcitations
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article
Enhancement of aluminum oxide physical vapor deposition with a secondary plasma
Abstract
<p>Reactive sputtering of aluminum oxide in a planar magnetron system is conducted with a mixture of O<sub>2</sub> and Ar reacting with and bombarding an aluminum target. The aluminum target is powered by a pulsed directed current (DC) bias which functions to discharge the accumulated ions on the insulating AlO<sub>x</sub> film surface during the positive duty cycle and suppresses arc formation. A seven-turn helical antenna sits below the magnetron sputtering system in the vacuum system and delivers radio-frequency (RF) power to generate a secondary plasma in the chamber. This plasma can efficiently ionize the sputtered flux, achieving ionized physical vapor deposition (IPVD). A gridded energy analyzer (GEA) and a quartz crystal microbalance (QCM) are located in the substrate plane to allow the ion and neutral deposition rates to be determined. Electron temperature and electron density are measured by a RF compensated Langmuir probe. A RF power of 500 W significantly increases the deposition rate of AlO<sub>x</sub> up to half of the Al deposition rate in metallic mode at the total pressure of 1.33 Pa (10 mtorr). At 3.33 Pa (25 mtorr), the ionization fraction of Al atoms reaches 90%. In addition the RF power extends the range of O<sub>2</sub> partial pressure in which the sputtering occurs in the metallic mode. SEM photos show that the secondary RF plasma makes the films smoother and denser due to a moderate level of ion bombardment. The deposition rates and ionization fractions fluctuate as a function of O<sub>2</sub> partial pressure. These variations can be explained by the combined variation of sputtering at the target, electron temperature and electron density.</p>