Identification of different reaction channels of high energy neutrons in liquid scintillators by the pulse shape discrimination method
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Cited by (32)
Measurement of neutron energy spectra of 345 MeV/u <sup>238</sup>U incidence on a copper target
2022, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsComparison of detectors with pulse shape discrimination capability for simultaneous detection of gamma-rays, slow and fast neutrons
2021, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :The observed (Fig. 8, bottom-left) poor separation of the thermal neutron peak from the fast neutron components in B-10 loaded scintillators is the effect of quenching of the light pulse slow component derived from the charge particles produced in a capture reaction of thermal neutrons [2,35]. The lack of quenching in the no-boron loaded scintillator was reported in [36], where unambiguous separation was presented for a number of light pulse components reflecting different reaction channels involved in the process of detecting high-energy neutrons in the BC501 A liquid scintillator. The gamma-ray count rates were very similar for all of the detectors, with less than a 20% difference of the lowest yield compared to the highest one.
Measurement of thick target neutron yields from 7 MeV/u α incidence on <sup>209</sup>Bi
2020, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsDeuterated stilbene (stilbene-d<inf>12</inf>): An improved detector for fast neutrons
2018, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :Data obtained using the digitizer CI method were somewhat more linear. However, the linearity can depend on several factors including pulse integration times, PMT HV, etc. [12–16] and will be discussed in more detail in [2]. As shown with other deuterated scintillators, this should then allow for the accurate unfolding of the light spectrum to deduce the incident neutron energy spectrum once the detector response functions are known [5,9,15,16,21,22] and room-return neutrons removed as needed.
Systematic measurement of double-differential neutron production cross sections for deuteron-induced reactions at an incident energy of 102 MeV
2017, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :In the low energy range (≤15 MeV), the number of background gamma-ray events was comparable to that of neutron events in the measurement with the 5.08 cm detector. Both the events were well separated by PSD using the two gate integration method [25]. In Fig. 3, one of the examples is shown as a two-dimensional plot of the total-gate light output versus the slow-gate one.
Response of the Li-7-enriched Cs<inf>2</inf>LiYCl<inf>6</inf>:Ce (CLYC-7) scintillator to 6-60 MeV neutrons
2015, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :Again, this result is not unexpected given the ratio of observed-to-calculated accidentals at 36.1 and 60.5 MeV and the fact that the rates and amplitudes of the pulses are much lower than at higher energies. The band located between the electron and proton bands is attributed to the neutron-capture protons escaping from the scintillator volume without fully depositing their energy [24]. Similar results have been observed in organic scintillators [25].
- ∗∗
French—Belgian Collaboration for the DEMON Project.
- 1
On leave from Soltan Institute for Nuclear Studies, PL 05-400 Świerk-Otwock, Poland (present address).