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Glinian litu - nowy detektor dozymetryczny

Mandowska E., Mandowski A., Bilski P., Marczewska B., Twardak A., Gieszczyk W.

Przegląd Elektrotechniczny

2015

R. 91, nr 9

117-120

Optycznie stymulowana luminescencja (OSL) jest luminescencją emitowaną przez napromieniowany izolator lub półprzewodnik podczas stymulacji światłem o odpowiedniej energii. Intensywność sygnału OSL jest funkcją dawki promieniowania jonizującego, jaka została pochłonięta i dlatego też jest techniką coraz częściej wykorzystywaną w dozymetrii. Wytworzono techniką Micro–Pulling–Down (MPD) nowy detektor OSL glinian litu o dobrej powtarzalności, wysoko czuły na promieniowanie jonizujące oraz wykazujący znacznie lepszą czułość niż komercyjnie stosowany tlenek aluminium. W celu lepszego poznania jego własności lumniescencyjnych przeprowadzono badania termoluminescencji rozdzielczej widmowo.

Optically stimulated luminescence (OSL) is the luminescence emitted from irradiated insulator or semiconductor during stimulation with light of appropriate energy. The OSL intensity is a function of the dose of absorbed ionizing radiation and therefore is a technique increasingly used in dosimetry. New lithium aluminate OSL detector was fabricated using a Micro-Pulling-Down (MPD) technique. The detector has good reproducibility and is highly sensitive to ionizing radiation, having a much better sensitivity than commercially used aluminum oxide detectors. Spectrally resolved thermoluminescence studies were performed to better understand its luminescence properties.

Application of LiF : Mg,Cu,P (MCP-N) thermoluminescent detectors (TLD) for experimental verification of radial dose distribution models

Gieszczyk W., Olko P., Bilski P., Grzanka L., Obryk B., Horwacik T.

Nukleonika

2012

Vol. 57, No. 4

507-512

In track structure theory, the radial distribution of dose, D(r), around an ion track plays a fundamental role in predicting the response of biological systems and physical detectors after a dose (or fluence) of ions. According to the formulations of D(r), the local dose at radial distances below 1 nm can reach values as high as 106 Gy. We propose a new method of verifying experimentally the radial dose distribution around alfa-particle tracks, using LiF:Mg,Cu,P (MCP-N) thermoluminescent detectors (TLD) which are able to measure gamma-ray doses in the kGy range via evaluation of their high-temperature TL glow peak structure over the temperature range of 350–550 centigrade. MCP-N detectors were irradiated with Am-241 alfa-particles at fluences ranging from 107 to 1011 particles/cm2, and by Co-60 gamma-ray doses ranging from several Gy up to the MGy. A number N of individual high-temperature TL peaks were analysed in the obtained glow curves by deconvolution, using the GlowFit code. For each of these peaks, an equation relating the intensity, A, of the TL signal obtained after alfa-particle irradiation and after gamma-ray doses, via the dose-frequency function, f alfa(D), was written in the form: A i alfa = integral A i gamma(D)x f alfa (D)dD, i 1,.., N. Using this set of N equations, where A alfa i and A gamma i(D) were known (measured), the single unknown function f alfa(D) was unfolded and converted to D(r). Parametric unfolding and the SAND-II iterative code were applied. While we were able to confirm the 1/r2 dependence of D(r) in agreement with D(r) expressions, we were unable to conclusively evaluate the dependence of D(r) at intermediate ranges of radial distance r. This preliminary result of our unique experimental approach to determine the radial dose distribution around the path of heavy charged particles in LiF detectors, requires further development.