Interdiffusion and phase formation at iron-tungsten interfaces
Creators
- 1. Technische Universität München, Garching (Germany)
- 2. Max Planck Institut für Plasmaphysik, Boltzmannstr. 2, Garching 85748 (Germany)
- 3. Instituto de Física da Universidade de São Paulo, Rua do Mãtao, trav. R 187, São Paulo 05508-090 (Brazil)
Description
Highlights: • The interdiffusion coefficient between Iron and Tungsten is investigated. • For temperatures above 1000 K, the phase Fe2W was observed in Fe/W couples. • The growth rate of Fe2W was assesed. • The interdiffusion coefficient of Fe2W was quantified. -- Abstract: Low-activation steels are attractive candidates for wall materials in future nuclear-fusion power plants. Through a process called preferential sputtering, an enriched tungsten (W) layer is expected to develop on these steels, lowering erosion and thus increasing their lifetime and reducing contamination of the fusion plasma. However, the process of preferential sputtering may be counteracted by interdiffusion of W and iron (Fe). In this article, we investigate a simplified model system of such low-activation steels with a W-rich layer on the surface, by sputter depositing a thin W layer on top of pure Fe substrates. We investigate the processes that are activated when this model system is subject to temperatures relevant in the context of nuclear fusion reactors and assess the temperatures at which interdiffusion is expected to influence W surface concentrations. This is done by annealing a binary W-Fe system and analyzing the resulting concentration profiles by means of Rutherford backscattering spectrometry (RBS) and focused ion beam cross-sectioning (FIB). For annealing temperatures above 1000 K, an intermediate phase was observed to have formed, both between the Fe and W layer as well as on the surface of the W layer. This intermediate phase was determined to be Fe2W using Sputter X-ray photoelectron spectroscopy (XPS) and time-of-flight Rutherford backscattering spectrometry (ToF-RBS). The laterally averaged growth rate of this phase was determined to be at 1050 K and at 1100 K.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.nme.2019.01.033Additional details
Identifiers
- DOI
- 10.1016/j.nme.2019.01.033;
- PII
- S2352179118302837;
Publishing Information
- Journal Title
- Nuclear Materials and Energy
- Journal Volume
- 19
- Journal Page Range
- p. 189-194
- ISSN
- 2352-1791
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 56004906
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Descriptors DEI
- ANNEALING; CONTAMINATION; CROSS SECTIONS; ION BEAMS; IRON; RUTHERFORD BACKSCATTERING SPECTROSCOPY; STEELS; THERMONUCLEAR POWER PLANTS; THERMONUCLEAR REACTORS; TIME-OF-FLIGHT METHOD; TUNGSTEN; X-RAY PHOTOELECTRON SPECTROSCOPY
- Descriptors DEC
- ALLOYS; BEAMS; CARBON ADDITIONS; ELECTRON SPECTROSCOPY; ELEMENTS; HEAT TREATMENTS; IRON ALLOYS; IRON BASE ALLOYS; METALS; PHOTOELECTRON SPECTROSCOPY; POWER PLANTS; REFRACTORY METALS; SPECTROSCOPY; THERMAL POWER PLANTS; TRANSITION ELEMENT ALLOYS; TRANSITION ELEMENTS
Optional Information
- Copyright
- Copyright (c) 2019 The Authors. Published by Elsevier Ltd.