Analysis of the response of CVD Diamond Detectors for UV and sX-Ray plasma diagnostics installed at JET

被引:8
作者
Caiffi, B. [1 ]
Coffey, I. [3 ]
Pillon, M. [2 ]
Osipenko, M. [4 ]
Prestopino, G. [5 ]
Ripani, M. [4 ]
Taiuti, M. [1 ]
Verona, C. [5 ]
Verona-Rinati, G. [5 ]
机构
[1] Univ Genoa, Dip Fis, Genoa, Italy
[2] Ist Nazl Fis Nucl, Sez Genova, Genoa, Italy
[3] Queens Univ Belfast, Belfast BT7 1NN, Antrim, North Ireland
[4] Assoc EURATOM ENEA Fus, Rome, Italy
[5] Univ Roma Tor Vergata, Dip Ingn Meccan, Rome, Italy
[6] Culham Sci Ctr, JET EFDA, Abingdon OX14 3DB, Oxon, England
来源
3RD INTERNATIONAL CONFERENCE FRONTIERS IN DIAGNOSTIC TECHNOLOGIES, ICFDT3 2013 | 2015年 / 62卷
关键词
CVD diamond detector; plasma diagnostic; laser ablation;
D O I
10.1016/j.phpro.2015.02.014
中图分类号
O59 [应用物理学];
学科分类号
摘要
Diamond detectors are very promising candidates for plasma diagnostics in a harsh environment. In fact, they have several proprieties which make them suitable for magnetic fusion devices: radiation hardness, high thermal conductivity, high resistivity, high carrier mobility and a large bandgap (5.5 eV). The latter makes them insensitive to visible radiation and allows low noise measurements without any cooling. In 2008 two CVD (Chemical Vapour Deposition) single crystal diamond (SCD) detectors were installed at the JET tokamak as extreme UV and soft X-Ray diagnostics [1]. In this work the neutron background in these detectors was measured shielding the UV and soft X-Ray radiation by closing a local vacuum valve. The UV detector was found to be insensitive to the neutron flux, while the soft X Ray detector signal exhibited spikes during the highest neutron rate pulse (neutron rate 10(16) n/s, which corresponds to a flux of phi(n) similar to 10(5) n/cm(2)s in the detector location). These spikes were found to be due to the (n,p) reaction within the plastic filter in front of the soft X-Ray detector. The UV SCD was also used to perform time of flight (ToF) measurements in laser ablation experiments. ToFs were found to be an order of magnitude higher than expected if only the drift velocity is considered. This discrepancy could be due to a delay between the arrival time of the impurities in the plasma and their emission in an energy range which SCD is sensitive to (E-ph >5.5 eV). The delay is found to be comparable with the expected ionization times for edge plasma conditions. (C) 2015 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND license.
引用
收藏
页码:79 / 83
页数:5
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