Abstract

European Spallation Source instruments like the macromolecular diffractometer (NMX) require an excellent neutron detection efficiency, high-rate capabilities, time resolution, and an unprecedented spatial resolution in the order of a few hundred micrometers over a wide angular range of the incoming neutrons. For these instruments solid converters in combination with Micro Pattern Gaseous Detectors (MPGDs) are a promising option. A GEM detector with gadolinium converter was tested on a cold neutron beam at the IFE research reactor in Norway. The μTPC analysis, proven to improve the spatial resolution in the case of 10B converters, is extended to gadolinium based detectors. For the first time, a Gd-GEM was successfully operated to detect neutrons with a measured efficiency of 11.8% at a wavelength of 2 Åand a position resolution better than 250 μm.

Highlights

  • This content has been downloaded from IOPscience

  • Zat'ko et al Measurement of fast neutron detection efficiency with 6Li and 7Li enriched CLYC scintillators A Mentana, F Camera, A Giaz et al Applications of triple Gas Electron Multipliers (GEM) detectors beyond particle and nuclear physics F Murtas Development of epithermal neutron camera based on resonance-energy-filtered imaging with GEM H Tomita, C Shoda, J Kawarabayashi et al Development of GEM-based detector for thermal neutron M Shoji, S Uno, T Uchida et al Operational performance characteristics of the WISH detector array on the ISIS spallation neutron source D Duxbury, D Khalyavin, P Manuel et al JINST 11 P05011

  • A GEM detector with gadolinium converter was tested on a cold neutron beam at the Institute for Energy Technology (IFE) research reactor in Norway

Read more

Summary

Conversion electrons

Despite the very large neutron capture cross section of 155Gd and 157Gd, the material is not a popular converter due to the nature and the energy of the secondary particles. Kinetic Energy [keV] CSDA Range [cm]a Maximum Penetration Depth [cm]b Standard Deviation [cm]c. The conversion electron track is fully contained in the drift space if its maximum penetration depth is smaller than the drift length. A CsI layer applied to the gadolinium was used as an electron emitter to localize the electron energy loss and, improve the spatial resolution [25, 26] The disadvantage in this case is the very small amount of primary electrons and deposited energy that requires a detector with very large gain. The challenge is here that in contrast to the α particles and Li ions created in the 10B4C converter, the gadolinium conversion electrons have on average a far larger range, and do not leave a straight ionization track.

Converter efficiency
R2D2 beam line
Detection efficiency
Position resolution
Findings
Conclusions and outlook
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call