2022
DOI: 10.1109/tns.2022.3182348
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Benchmarking a New Digital Data Acquisition System for Fast Neutron Metrology

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Cited by 7 publications
(5 citation statements)
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“…A practical solution is presented here where both anode and dynode signals are only recorded for the purpose of calibrating the integrated anode pulse, with subsequent measurements only requiring the acquisition of the anode pulse. For the AMANDE analyses [2], the integration time tL was chosen to ensure agreement between the integral of the anode and the dynode pulse height by comparing the location of the gamma-calibrated edge associated with monoenergetic neutrons. For the present n-lab measurements, this process was replicated, resulting in an optimised integration time of 1100 ns.…”
Section: Analyses and Resultsmentioning
confidence: 99%
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“…A practical solution is presented here where both anode and dynode signals are only recorded for the purpose of calibrating the integrated anode pulse, with subsequent measurements only requiring the acquisition of the anode pulse. For the AMANDE analyses [2], the integration time tL was chosen to ensure agreement between the integral of the anode and the dynode pulse height by comparing the location of the gamma-calibrated edge associated with monoenergetic neutrons. For the present n-lab measurements, this process was replicated, resulting in an optimised integration time of 1100 ns.…”
Section: Analyses and Resultsmentioning
confidence: 99%
“…Figure 2 shows the scaled and calibrated light output spectra measured with the EJ-301 for 14 MeV neutrons produced by the STNG for the three scenarios. The expected lineshape for 14 MeV neutrons is taken from the IRSN response matrix used for unfolding analyses [2]. It is interesting to note that the edge of the 14 MeV lineshape matches the edge of the dynode and anode (1100 ns) light output spectra, which are observed to have slightly inferior edge resolution to the lineshape.…”
Section: Analyses and Resultsmentioning
confidence: 99%
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“…A 6.0 cm thick sample of SiO2 beads (< 0.1 cm diameter) was prepared with a crosssectional area of 5.0 x 5.0 cm 2 . Neutrons (and gamma rays) were detected using a 2" x 2" EJ301 organic liquid scintillator, and data were acquired digitally [11]. The light output parameter L was taken to be the pulse height of the dynode signal after shaping and amplification and calibrated with a series of gamma ray sources.…”
Section: Experimental Validationmentioning
confidence: 99%