1965
DOI: 10.1063/1.3047620
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The Theory and Practice of Scintillation Counting

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Cited by 606 publications
(283 citation statements)
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“…As can be seen in Eq. (1), for electrons with energies greater than 125 keV in the scintillator, the stopping power becomes very small [38] which makes kB · (dE/dx) 1, as a result, the light output L(E) can be simplified to be a linear relation to higher energies.…”
Section: Energy Calibration For High Energiesmentioning
confidence: 99%
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“…As can be seen in Eq. (1), for electrons with energies greater than 125 keV in the scintillator, the stopping power becomes very small [38] which makes kB · (dE/dx) 1, as a result, the light output L(E) can be simplified to be a linear relation to higher energies.…”
Section: Energy Calibration For High Energiesmentioning
confidence: 99%
“…A quenching factor matrix exists between the recoil energy and the visible energy "seen" by the PMTs. The light output in the liquid scintillator can be described by Birks' relation [38,43]:…”
Section: Light Output Response To Fast Neutronsmentioning
confidence: 99%
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“…A bonding optical adhesive was chosen to fill the space between the CsI(Tl) and photodiode. In order to optimize light transmission, a grease with an index equal to the geometric mean of the two adjoining materials is ideal, or mathematically, 12) (1.78 2.02) 1.82 2 n optimum…”
Section: Gamma-ray Detector Simulationsmentioning
confidence: 99%
“…In order to obtain a local light emission, non-radiative processes must dominate the energy transfer from solvent t o d y e [26,39]. The probability ( ) of non-radiative energy transfer increases with dye concentration according to the expression [40] = C=(C+C 0 ). For the LS's considered C 0 ranges between 1.0 and 1.6 g/l, and dye concentrations larger than these values are necessary to ensure a high locality of light emission.…”
Section: Local Light Emissionmentioning
confidence: 99%