Academic literature on the topic 'Photoluminescence and radiophotoluminescence'

CaSO4:Eu phosphor is synthesised by acid distillation method with varying synthesis parameters for studying its Radiophotoluminescence (RPL) properties for gamma absorbed dose measurements. Five phosphor samples are prepared by varying quantity of solvent, distillation temperature and reaction time. XRD, SEM, particle size analysis and photoluminescence studies are carried out. The characterisation study shows polycrystalline luminescent particles of average size varying from 35 μm to 55 μm. Characteristic emission of Eu3+ is observed around 590, 615 and 620 nm at 242 nm excitation. Gamma dose response of maximum Eu3+ PL intensity sample is studied in the range 10 cGy to 1000 cGy using Co-60 source. Gamma radiation exposure induces conversion of Eu3+ to Eu2+ giving luminescence at 385 nm with 320 nm excitation. Repetitive measurements of gamma exposed samples are carried out and no significant fading is observed within one week of post-irradiation. The phosphor has the potential to be used for gamma dosimetry.

Abstract The peculiar photoluminescence characteristics of radiation-induced colour centres in lithium fluoride (LiF), well known for applications in optically-pumped tuneable lasers and broad-band miniaturised light-emitting photonic devices operating at room-temperature, are under exploitation in passive imaging detectors and dosimeters based on visible radiophotoluminescence in LiF crystals and polycrystalline thin films. Their high intrinsic spatial resolution, wide dynamic range and large field of view, combined with easy handling, ambient-light operation and no development need, allow to successfully extend their use from X-ray imaging to proton-beam advanced diagnostics and dosimetry, even at those low dose values that are typical of hadrontherapy. After exposure, the latent images stored in LiF as local formations of F2 and F3 + aggregate defects are read with an optical fluorescence microscope under illumination in the blue spectral range. Their visible emission intensity was found to be linearly proportional to the dose over at least three orders of magnitude, so that bi-dimensional LiF solid-state dosimeters based on spectrally-integrated radiophotoluminescence reading can be envisaged. Taking advantage of the low thickness of LiF thin films, transversal proton beam dose mapping was demonstrated at low proton energies, even at high doses. Recent results and advances concerning LiF crystals and polycrystalline thin film characterisation in the linearity range are presented and discussed with the aim of highlighting challenges related to increasing the LiF film detector radiation sensitivity to both particles (protons) and photons (X-rays), although therapeutic dose values typical of clinical radiotherapy are still a big challenge.

The photoluminescence (PL) properties of radiation-induced color centers (CCs) in lithium fluoride (LiF) crystals and thin films find applications in optically-pumped solid-state lasers and photonic light-emitting microdevices operating at room temperature (RT) in the visible and near-infrared spectral range [1]. Among their peculiarities, the broad tunability and high emission quantum efficiency, combined with the wide optical transparency of the hosting LiF matrix. On the other hand, LiF dosimeters based on thermoluminescence (TL) of point defects in LiF crystals and pellets have been the most widely used family of phosphors in TL dosimetry, mainly for their high radiation sensitivity at low doses and the LiF tissue-equivalence, which is essential for meaningful medical applications. The excellent thermal and optical stabilities of the laser-active F2 and F3 + electronic defects, consisting of two electrons bound to two and three adjacent anion vacancies, respectively, whose efficient visible photoluminescence is located in the green-red spectral range under simultaneous excitation with blue-light pumping, make radiation detectors based on LiF crystals and thin films attractive for X-ray imaging [2] at nanoscale, related to the atomic-scale dimensions of such point defects. These passive radiation imaging sensors are based on the optical reading of visible radiophotoluminescence (RPL) of aggregate CCs locally created and stored in LiF, by using conventional and advanced fluorescence microscopy techniques for latent images acquisition. In the last years they were successfully tested for proton beam advanced diagnostics and dosimetry at increasing energies from 1.5 to 35 MeV, showing a linear RPL response as a function of absorbed doses in a wide dynamic range [4], long-term stability against fading and non-destructive reading capability. With suitable irradiation geometries of LiF crystals, it is possible to record the energy that protons deposit in the material (Bragg curve) as a bi-dimensional spatial distribution of luminescent CCs, even at dose values below 50 Gy, typically utilized in protontheraphy [5]. We have been investigating the feasibility to extend this approach to optically transparent LiF thin films thermally evaporated on Si(100) substrates. Despite of their low thickness, we take advantage of the enhanced PL response of F2 and F3 + CCs, related to the presence of the flat and smooth Si substrate [6], which is optically reflective at the excitation and emission wavelengths utilized in the fluorescence microscope. The irradiations were performed with proton beams produced by the linear accelerator TOP-IMPLART (Oncological Therapy with Protons - Intensity Modulated Proton Linear Accelerator for RadioTherapy), under development at ENEA C.R. Frascati, with the cut edge perpendicular to the proton beam direction. The latent two-dimensional fluorescence images of the CC distributions generated in the polycrystalline LiF layers show a systematic increase in depth of the Bragg peak with respect to LiF crystals. The results obtained in LiF films at increasing proton energies are presented and discussed, also in comparison with those in LiF crystals, in order to explain the observed behaviors and highlight advantages and limits of versatile LiF film radiation detectors. [1] R. M. Montereali, in Handbook of Thin Film Materials, H. S. Nalwa, Editor, Vol.3: Ferroelectric and Dielectric Thin Films, Ch.7, p. 399, Academic Press, S. Diego (2002). [2] G. Baldacchini, F. Bonfigli, A. Faenov, F. Flora, R. M. Montereali, A. Pace, T. Pikuz, L. Reale, J. Nanosci. Nanotechno., 3, 483 (2003). [3] A. Ustione, A. Cricenti, F. Bonfigli, F. Flora, A. Lai, T. Marolo, R. M. Montereali, G. Baldacchini, A. Faenov, T. Pikuz and L. Reale, Jpn. J. Appl. Phys. 45, 2116 (2006). [4] M. Piccinini, F. Ambrosini, A. Ampollini, L. Picardi, C. Ronsivalle, F. Bonfigli, S. Libera, E. Nichelatti, M. A. Vincenti and R. M. Montereali, Appl. Phys. Lett., 106, 261108 (2015). [5] R.M. Montereali, E. Nichelatti, V. Nigro, M. Piccinini, M.A. Vincenti, ECS J. Solid State Sci. and Technol. 10, 116001 (2021). [6] M. A. Vincenti, M. Leoncini,S. Libera, A. Ampollini, A. Mancini, E. Nichelatti, V. Nigro, L. Picardi, M. Piccinini, C. Ronsivalle, A. Rufoloni, R. M. Montereali, Opt. Mater., 119, 111376 (2021).

ABSTRACTA method of radiation dosimetry based upon the radiophotoluminescence (RPL) of synthetic diamond crystals is presented. When the RPL is generated by a stimulation wavelength of 296 nm a linear response vs radiation dose of up to 20 kGy can be obtained with selected crystals. The response is very dependent on the chemistry of the synthesized specimen.

Abstract Radiophotoluminescence (RPL) is a phenomenon in which a luminescence centre is formed in a medium upon interaction with ionizing radiation. The RPL is observed by a conventional photoluminescence (PL) technique, and the PL intensity is proportional to the dose. With the latter feature, the RPL has found successful applications in personnel and environmental dosimetry. However, the conventional materials considered for radiation measurements may be limited to Ag-doped phosphate glass, LiF, and Al2O3:C,Mg. The recent research works, however, have found a number of additional RPL materials for luminescence dosimetry. The aim of the present paper is to review the series of newly reported RPL materials and potential applications in dosimetry.