Abstract

Beryllium-deuterium co-deposited layers were obtained using DC magnetron sputtering technique by varying the Ar/D2 gas mixture composition (10/1; 5/1; 2/1 and 1:1) at a constant deposition rate of 0.06 nm/s, 343 K substrate temperature and 2 Pa gas pressure. The surface morphology of the layers was analyzed using Scanning Electron Microscopy and the layer crystalline structure was analyzed by X-ray diffraction. Rutherford backscattering spectrometry was employed to determine the chemical composition of the layers. D trapping states and inventory quantification were performed using thermal desorption spectroscopy. The morphology of the layers is not influenced by the Ar/D2 gas mixture composition but by the substrate type and roughness. The increase of the D2 content during the deposition leads to the deposition of Be-D amorphous layers and also reduces the layer thickness by decreasing the sputtering yield due to the poisoning of the Be target. The D retention in the layers is dominated by the D trapping in low activation binding states and the increase of D2 flow during deposition leads to a significant build-up of deuterium in these states. Increase of deuterium flow during deposition consequently leads to an increase of D retention in the beryllium layers up to 300%. The resulted Be-D layers release the majority of their D (above 99.99%) at temperatures lower than 700 K.

Highlights

  • The high paced growth of the human civilization in the last century is strongly tied to the current demand on energy supply

  • The same conclusions drawn from the deposited at 2 sccm (D2) sample can be extended for the rest of the Be-D layers deposited on silicon substrates since there are no visible differences between the scanning electron microscopy (SEM) images

  • The D values obtained with Rutherford backscattering spectrometry (RBS) are between 100 and 300% higher than the ones resulted from the thermal desorption spectrometry (TDS) measurements, and since NRA is presented in literature as the best suited method to determine the D inventory in the samples, we considered that in this particular case the information obtained by TDS is more reliable

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Summary

Introduction

The high paced growth of the human civilization in the last century is strongly tied to the current demand on energy supply. Renewable energy that harnesses the power of wind and sun can have a major impact in covering the energy demand especially for domestic consumption, the discontinuity in energy production and heavy reliance on external meteorological factors and geography means that in most cases these energy sources will be complementary to conventional ones. In this context, nuclear fusion represents an attractive alternative that promises to deliver massive amounts of clean energy to cover this ever-increasing demand. Several thermonuclear fusion reactors were built for experimental purposes, among them one of the most important is Joint European Torus (JET) which represents a test platform for the development of the International Thermonuclear Experimental Reactor (ITER), considered the biggest scientific and technological achievement in the nuclear fusion field

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