Boron-Carbide coatings for neutron detectors

10B4C coated copper foil

Neutrons pass through an enriched boron-10 coating layer. They are converted into lithium-7 atoms and alpha particles (He-4 nucleus). The alpha particles can be meaured by the detector.

GEM folie before coating (left) and after coating (right) with modified non-conductive enriched 10B4C.

Neutron detector of the company CDT with 10B4C coated entrance foil

B4C workpieces for neutron physics.

We are one of few companies producing enriched Boron-Carbide coatings for neutron detectors in radiation protection and basic research.

With our magnetron-deposition technique we coat GEM-folies (see below) and one or double side of aluminium or copper foils with sizes up to 400 x 1200 mm and up to 2 μm thicknesses.

The enriched 10B from boron-carbide targets works as neutrons converter: Neutrons pass through a coating layer of enriched boron-10 and are converted into a lithium-7 atom and an alpha particle (helium nuclei). The charged alpha particle can then be measured with standard techniques.

We are always in close contact with our customers and partners. Cooperations with partners in research and development companies or scientific institutes ensure that our production processes fullfill the requests of specific detectors for high end applications.

For example, in collaboration with the company CDT GmbH, Heidelberg, www.n-cdt.com, we supplied 10B4C coatings for the DREAM detector at the European Spallations Source in Lund: https://europeanspallationsource.se/instruments/dream

DREAM will be an outstanding tool for structure analysis enabling new physical and chemical research in material and nanoscience using scattered neutron diffratometry.

GEM (Gaseous Electron Multiplier) foils were developed at CERN, https://gdd.web.cern.ch/gem, for the big particle detectors looking for new physics. These foils combine simplicity and high technology:  A capton foil is coated on both sides with copper dealing as high voltage electrodes. Several thousand holes drilled through the foils generate transparency enabling particles to pass it. Charged particles passing the holes are accelerated, ionize the detector gas and generate an avalanche of electrons which are measured by the detector.

Unfortunately, neutrons are free of electric charge and therefore can’t be manipulated and detected using the standard GEM foil detector technique.
But such foils are now available for the next generation of neutron detectors at high luminosity neutron sources (like ESS, PSI, ILL, Los Alamos, FRMII or Oak Ridge).
For the conversion of “neutral” neutrons into detectable charged particles isotopically enriched 10B4C coatings are used. After the Conversion the charged particle are measured as described.
Standard B4C is an electrically conductive material and so a short circuit between the electrodes prevent the GEM principle to work.

The development of non-conductive and enriched 10B4C coatings is the solution.
Such special coatings were developed at Magtec.

We also offer workpieces for neutron physics machined out of B4C material.

Selection of publications:

  • Performance study of the Jalousie detector baseline design for the ESS thermal powder diffractometer HEIMDAL through GEANT4 simulations, I. Stefanescu, M. Christensen, R. Hall-Wilton, S. Holm-Dahlin, K. Iversen, M. Klein, D. Mannix, J. Schefer, C.J. Schmidt, W. Schweika and U. Stuhr, Journal of Instrumentation, Volume 14, (2019)
  • Ultracold neutron detectors based on 10B converters used in the qBounce experiments, T. Jenke, G. Cronenberg, H. Filter, P. Geltenbort, M. Klein, K. Mitsch, T. Lauer, H. Saul, D. Seiler, D. Stadler, M. Thalhammer, H. Abele, Nucl. Instr. and Meth. A (2013)
  • Experimental investigation of a low-cost solid state detector with high spatial resolution for ultracold neutrons, Th. Lauer, P. Geltenbort, P. Hoebel, M. Kaoui, H.C. Koch, A. Kraft, U. Schmidt, Yu. Sobolev, Eur. Phys. J. A (2011)