ANTONIO, P.L.SILVA, A.M.B.SILVEIRA, I.S.CALDAS, L.V.PESSANHA, SOFIAMANSO, MARTA2025-12-222025-12-22ANTONIO, P.L.; SILVA, A.M.B.; SILVEIRA, I.S.; CALDAS, L.V. Effect of the UV lighting for photo-transfer of the charges of radiation dosimeters: TL and PTTL responses. In: PESSANHA, SOFIA (ed.); MANSO, MARTA (ed.). In: INTERNATIONAL SYMPOSIA ON RADIATION PHYSICS, 19th, September 1-5, 2024, Lisbon, Portugal. <b>Abstract...</b> Lisbon: Universidade Nova de Lisboa - Faculdade de Ciências e Tecnologia, Lisboa, 2024. p. 74-74. Disponível em: https://repositorio.ipen.br/handle/123456789/48967.https://repositorio.ipen.br/handle/123456789/48967Some solid-state materials store energy in the form of trapped electronic charges, when they are exposed to ionizing radiation. This energy can be measured when the stimulation of those charges occurs and one way is the heating of the sample, in order to observe its luminescent signal by the thermoluminescence (TL) technique. Another way to study the luminescence of these materials is by means of the phototransferred thermoluminescence (PTTL) technique, that allows the observation of the light-induced transfer of charges from one kind of trap to another [1-2]. The main objective of this work was to study the TL and PTTL of radiation dosimeters in 60Co and UV beams, in order to apply these dosimeters using an established photo-transfer procedure in high-dose dosimetry. The luminescent responses of commercial LiF:Mg,Ti, CaF2:Dy, CaF2:Mn and CaSO4:Dy dosimeters were studied according to this sequence: 1) TL after irradiation; 2) TL after irradiation and post-irradiation thermal treatment (PITT); and 3) PTTL after irradiation, PITT and illumination. The irradiations were performed using a 60Co source, and all the measurements were taken using the Risø reader system, model TL/OSL-DA-20. The absorbed doses were: 0.7 Gy (LiF:Mg,Ti and CaSO4:Dy), 20 Gy (CaF2:Dy) and 50 Gy (CaF2:Mn), for the first step, and 5 Gy (LiF:Mg,Ti), 100 Gy (CaF2:Dy), 200 Gy (CaF2:Mn) and 25 Gy (CaSO4:Dy), for the second and third steps. As results of the first step, TL emission maximum peaks were observed for all four materials at about 250ºC (LiF:Mg,Ti), 300ºC (CaF2:Dy and CaSO4:Dy) and 385ºC (CaF2:Mn). After PITT, in the second step of the experiments, the TL peaks arised at about 365ºC for LiF:Mg,Ti, and for the other materials no peaks were observed. In the final step, after exposure to UV light, PTTL signals appeared for LiF:Mg,Ti at 260ºC and 370ºC, for CaF2:Mn at 398ºC and for CaSO4:Dy at 200ºC; no PTTL was observed for CaF2:Dy. According to the results obtained, it was possible to study the occurrence of the phototransferrence signal of the materials, present for LiF:Mg,Ti, CaF2:Mn and CaSO4:Dy. These data open the possibility of applying these materials and the PTTL technique in high-dose dosimetry of gamma irradiators, with applications in the industrial area.74-74engopenAccessResumo de eventos científicoshttps://orcid.org/0000-0002-7362-2455