1971
DOI: 10.1007/bf00606770
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Scintillation (deexcitation) time of CsI(Tl) after gamma excitation

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“…Excitons eventually find their way to luminescent (dopant) centers where they can re-combine via radiative transitions with energies lower than the bandgap, emitting light in the process that, importantly, is at a wavelength that is not reabsorbed by the crystal. In many scintillators this recombination can proceed through different intermediate excited states, leading these scintillators to exhibit ‘fast’ and ‘slow’ components in their light emissions (Belyavskii et al ., 1971) . The light output of a scintillator, given in terms of the number of optical photons produced per keV of energy deposited (photons/keV), ultimately governs both the energy and spatial resolutions that can be achieved.…”
Section: Advances In Scintillatorsmentioning
confidence: 99%
“…Excitons eventually find their way to luminescent (dopant) centers where they can re-combine via radiative transitions with energies lower than the bandgap, emitting light in the process that, importantly, is at a wavelength that is not reabsorbed by the crystal. In many scintillators this recombination can proceed through different intermediate excited states, leading these scintillators to exhibit ‘fast’ and ‘slow’ components in their light emissions (Belyavskii et al ., 1971) . The light output of a scintillator, given in terms of the number of optical photons produced per keV of energy deposited (photons/keV), ultimately governs both the energy and spatial resolutions that can be achieved.…”
Section: Advances In Scintillatorsmentioning
confidence: 99%