1964
DOI: 10.1016/0029-554x(64)90333-7
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Pulse shape discrimination

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Cited by 173 publications
(48 citation statements)
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“…Several methods exist to accomplish this, for example by measuring the zero-crossover (ZCO) time of a shaped pulse [16,17] or by comparing the charge collected from different parts of the pulse [18]. The performance of these methods with respect to each other is also well known in the analogue case [19].…”
Section: Liquid Scintillators and Pulse-shape Discriminationmentioning
confidence: 99%
See 1 more Smart Citation
“…Several methods exist to accomplish this, for example by measuring the zero-crossover (ZCO) time of a shaped pulse [16,17] or by comparing the charge collected from different parts of the pulse [18]. The performance of these methods with respect to each other is also well known in the analogue case [19].…”
Section: Liquid Scintillators and Pulse-shape Discriminationmentioning
confidence: 99%
“…The shaping can be done by using double delay lines [16] or an RC-CR integrating and differentiating network [17]. The analogue PSD algorithm of the NDE202 unit used in this work contains a bipolar RC-CR shaping amplifier and a zero-crossing detector.…”
Section: Zco: Analogue and Convolution Algorithmmentioning
confidence: 99%
“…Sensitivity to gamma rays of organic scintillators is generally overcome by analyzing the temporal profiles of pulses using the popular technique of PSD. Because neutrons primarily interact with protons while gamma rays primarily interact with electrons, neutron interactions produce charged particles with higher specific ionization [12]. This creates a higher concentration of triplet states in the scintillator, which enables more frequent triplettriplet annihilations to occur after the initial light production and, consequently, produces a greater amount of delayed scintillation light.…”
Section: Pulse Shape Discrimination Performancementioning
confidence: 99%
“…The rise-time technique, [5], [6], integrates the light pulse (e.g., of the PMT anode), and then measures the time at which this integral reaches a certain fraction of its maximum amplitude. The light output of a heavily ionizing particle, which in n=c-ray discrimination is proton (neutron scatter interaction), has long tail; hence, the time at which this fraction is reached is longer than that of an electron (gamma ray interaction) [2].…”
Section: Classic Rise-time Techniquementioning
confidence: 99%