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The high power impulse magnetron sputtering discharge as an ionized physical vapor deposition tool
Affiliation:1. Department of Research, Alexandru Ioan Cuza University, Iasi 700506, Romania;2. Faculty of Physics, Alexandru Ioan Cuza University, Iasi 700506, Romania;3. Faculty of Materials Science and Engineering, Department of Materials Science, Transilvania University, Brasov 500068, Romania;4. National Institute of Research and Development for Technical Physics, Iasi 700050, Romania;1. Institut des Matériaux Jean Rouxel, Université de Nantes, CNRS UMR 6502, 2 rue de la Houssinière, BP 32229, 44322 Nantes cedex 3, France;2. Centre CEA de Saclay, 91191 Gif-sur-Yvette cedex, France;1. Department of Physics (IFM), Linköping University, SE-581 83 Linköping, Sweden;2. CemeCon AG, Adenauerstr. 20 A4, D-52146 W?rselen, Germany;3. Materials Science and Physics Departments, University of Illinois, Urbana, IL 61801, USA;4. The Frederick Seitz Materials Research Laboratory, University of Illinois, Urbana, IL 61801, USA;1. Sheffield Hallam University, Howard Street, Sheffield, S1 1WB, UK;2. University of Illinois at Urbana-Champaign, 104 South Goodwin Avenue, Urbana, IL 61801, United States of America
Abstract:Various magnetron sputtering tools have been developed that provide a high degree of ionization of the sputtered vapor referred to as ionized physical vapor deposition (IPVD). The ions can be controlled with respect to energy and direction as they arrive to the growth surface which allows for increased control of film properties during growth. Here, the design parameters for IPVD systems are briefly reviewed. The first sputter based IPVD systems utilized a secondary plasma source between the target and the substrate in order to generate a highly ionized sputtered vapor. High power impulse magnetron sputtering (HiPIMS) is a recent sputtering technique that utilizes IPVD where a high density plasma is created by applying high power pulses at low frequency and low duty cycle to a magnetron sputtering device. A summary of the key experimental findings for the HiPIMS discharge is given. Measurements of the temporal and spatial behavior of the plasma parameters indicate electron density peak, that expands from the target with a fixed velocity. The discharge develops from an inert sputtering gas dominated to a sputtered vapor dominated during the pulse. The high electron density results in a high degree of ionization of the deposition material.
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