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Colin Judge: Testing structural materials in Idaho’s newest hot cell facility
Idaho National Laboratory’s newest facility—the Sample Preparation Laboratory (SPL)—sits across the road from the Hot Fuel Examination Facility (HFEF), which started operating in 1975. SPL will host the first new hot cells at INL’s Materials and Fuels Complex (MFC) in 50 years, giving INL researchers and partners new flexibility to test the structural properties of irradiated materials fresh from the Advanced Test Reactor (ATR) or from a partner’s facility.
Materials meant to withstand extreme conditions in fission or fusion power plants must be tested under similar conditions and pushed past their breaking points so performance and limitations can be understood and improved. Once irradiated, materials samples can be cut down to size in SPL and packaged for testing in other facilities at INL or other national laboratories, commercial labs, or universities. But they can also be subjected to extreme thermal or corrosive conditions and mechanical testing right in SPL, explains Colin Judge, who, as INL’s division director for nuclear materials performance, oversees SPL and other facilities at the MFC.
SPL won’t go “hot” until January 2026, but Judge spoke with NN staff writer Susan Gallier about its capabilities as his team was moving instruments into the new facility.
S. Agosteo, A. Fazzi, G. D'Angelo, M. V. Introini, A. Pola, C. Pirovano, V. Varoli, S. Altieri, S. Stella, S. Bortolussi, P. Bruschi
Nuclear Technology | Volume 168 | Number 1 | October 2009 | Pages 11-16
Detectors | Special Issue on the 11th International Conference on Radiation Shielding and the 15th Topical Meeting of the Radiation Protection and Shielding Division (Part 1) / Radiation Protection | doi.org/10.13182/NT09-A9093
Articles are hosted by Taylor and Francis Online.
A monolithic silicon telescope, consisting of a thin E stage (of [approximately]2 m in thickness) coupled to a residual-energy stage E (thickness 500 m), was studied and tested for measuring the boron concentration in biological samples for boron neutron capture therapy (BNCT). At the Laboratorio di Energia Nucleare Applicata BNCT facility, Pavia, Italy, this information is derived by placing the tissue sample in front of a surface barrier diode and by irradiating the system with neutrons generated in the thermal column of the TRIGA Mark II reactor. The boron concentration is estimated through the measurement of the energy deposited in the detector by the products of the 10B(n,)7Li reaction. However, the low-energy part of the measured spectra is typically distorted by secondary electrons produced by photon background and by protons generated via the 14N(n,p)14C reaction in tissue. This work discusses the possibility of using a different silicon device, namely, the monolithic silicon telescope, for improving the accuracy of the method by exploiting its particle discrimination capabilities. A device with a sensitive area of 1 mm2 was irradiated (in vacuo) bare, faced both with a certified boron implanted silicon wafer and with a thin sample of rat lung loaded with boron. The preliminary results showed that (a) alpha particles and lithium ions produced by neutron capture on boron are well identified, (b) the events due to protons generated in tissue by neutron capture on nitrogen can be well discriminated, and (c) the presence of nitrogen inside the detector dead layer gives rise to an additional contribution of protons from neutron absorption. These preliminary studies gave confidence about the possibility of improving the accuracy for the assessment of the 10B concentration in biological samples for BNCT.