1980
DOI: 10.1016/0029-554x(80)90759-4
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Efficiency calibration of scintillation detectors in the neutron energy range 1.5–25 MeV by the associated particle technique

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Cited by 48 publications
(13 citation statements)
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“…The neutron flux was monitored by a φ30.0 mm × 30.0 mm stilbene scintillator in another collimator situated at an angle of about 60 • . For the neutron energy range from 1 to 5 MeV, the T(p,n) 3 He reaction was used to produce monoenergetic neutrons by changing the detection angles, for 6 to 20 MeV the same reaction was used at 0 • by changing the incident proton energies, and for 21 to 30 MeV the T(d,n) 3 He reaction was chosen at 0 • by changing the incident deuteron energies. The gas target was a gas cell with the size of φ10.0 mm × 30.0 mm, filled with tritium gas to a pressure of 101.325 kPa.…”
Section: Methodsmentioning
confidence: 99%
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“…The neutron flux was monitored by a φ30.0 mm × 30.0 mm stilbene scintillator in another collimator situated at an angle of about 60 • . For the neutron energy range from 1 to 5 MeV, the T(p,n) 3 He reaction was used to produce monoenergetic neutrons by changing the detection angles, for 6 to 20 MeV the same reaction was used at 0 • by changing the incident proton energies, and for 21 to 30 MeV the T(d,n) 3 He reaction was chosen at 0 • by changing the incident deuteron energies. The gas target was a gas cell with the size of φ10.0 mm × 30.0 mm, filled with tritium gas to a pressure of 101.325 kPa.…”
Section: Methodsmentioning
confidence: 99%
“…In the energy region above 20 MeV, contributions from the n-C reactions in the liquid scintillator become more and more important, while the reaction cross sections and the angular distributions are not precise enough. A little efficiency calibration work above the 20 MeV region has been reported [1][2][3][4][5] . However, their results can not be used directly since the size of the detector and the detection threshold are different, even the composition of the scintillator is slightly different.…”
Section: Introductionmentioning
confidence: 99%
“…[6] and Fowler et.al. [7] had determined the location of the Compton edge Ec as the point located at half height of the Compton peak E c.p in distribution. That is Ec is higher in energy than Ec.p.…”
Section: -1 Determination Of the Compton Edgementioning
confidence: 99%
“…Since in reality, pulse height spectra are measured with an acquisition threshold, as shown in figure 17, the lower limit of the integration must be accurately determined. This is typically done by calibrating the detector light output against the energy deposited by recoil electron using standard γ-rays calibration sources (such as 22 Na, 137 Cs and 207 Bi) and then converting the experimental light output threshold into a deposited energy threshold using the corresponding light output function [18,19]. The light output so calibrated is given in units of MeV electron-equivalent (MeVee) as shown in figure 17.…”
Section: Detector Efficiencymentioning
confidence: 99%