首页> 外文期刊>Optical Materials >The effect of Mn concentration on the luminescence properties of NaMgF_3:Mn: Defect/Mn complex photoluminescence, radioluminescence, and optically stimulated luminescence for radiation dose monitoring
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The effect of Mn concentration on the luminescence properties of NaMgF_3:Mn: Defect/Mn complex photoluminescence, radioluminescence, and optically stimulated luminescence for radiation dose monitoring

机译:Mn浓度对NaMgF_3:Mn的发光特性的影响:缺陷/ Mn复合物的光致发光,放射致发光和光激发发光,用于辐射剂量监测

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摘要

Luminescence measurements were made on NaMgF3 :Mn before and after irradiation with X-rays over a wide Mn concentration range from x = 0.1 0 /0-5%. Photoluminescence (PL) is seen from distorted Mn2+ sites that saturate for x >= 1% and non-distorted Mn2+ sites. The non-distorted Mn2+ crystal field parameter and crystal field splitting are independent of Mn concentration and they are B = 779 +/- 14 cm(-1) and 10Dq = 9250 +/- 160 cm(-1 ). F-centre/Mn complexes are seen for all concentrations with a PL emission at similar to 670 nm. The complexes have perturbed Mn2+ energy levels that shift by less than 1630 cm(-1) in the 320 nm-570 nm wavelength range. There is also a PL emission at similar to 730 nm that is likely to arise from F-3 -centres perturbed by nearby Mn. The PL from these two perturbed centres is linear in dose up to 3.8 kGy when probed in the 550 nm-650 nm region and it can be repeatedly probed without bleaching. Optically stimulated luminescence (OSL) occurs for all Mn concentrations from the non-distorted Mn2+ site after X-ray irradiation. The OSL intensity is linear up to similar to 270 Gy for 0.5% Mn and the trapped carriers can be selectively bleached. Radioluminescence (RL) is also observed in all samples from both Mn2+ sites. Not all Mn(2+ )displays RL and a larger fraction of distorted Mn2+ sites do not display RL, which may be due to a higher concentration of nearby non-radiative recombination sites. The ratio of the RL of the non-distorted Mn2+ to the distorted Mn2+ is nearly dose-history-independent after an initial predose for 0.1% Mn, and it is linear in dose up to 9.6 kGy for 5% Mn. Our results show that NaMgF3 :Mn has great potential for real-time and total dose measurements where there are complementary methods available to obtain the dose rate, the dose-history, the dose after each irradiation, and the cumulative dose up to very high doses.
机译:在X = 0.1 0 / 0-5%的宽Mn浓度范围内,在X射线照射之前和之后,在NaMgF3:Mn上进行发光测量。从x> = 1%的饱和Mn2 +位置和未变形的Mn2 +位置可以看到光致发光(PL)。不变的Mn2 +晶体场参数和晶体场分裂与Mn浓度无关,它们分别为B = 779 +/- 14 cm(-1)和10Dq = 9250 +/- 160 cm(-1)。在所有浓度下都可以看到F中心/ Mn配合物,PL发射类似于670 nm。络合物的Mn2 +能级水平在320 nm-570 nm波长范围内偏移小于1630 cm(-1)。还有一个类似于730 nm的PL发射,很可能是由附近的Mn扰动的F-3中心引起的。当在550 nm-650 nm范围内进行探测时,来自这两个扰动中心的PL的线性剂量最高可达3.8 kGy,并且可以重复探测而不会漂白。 X射线辐照后,来自未变形Mn2 +位点的所有Mn浓度均发生光激发发光(OSL)。对于0.5%的Mn,OSL强度呈线性直至接近270 Gy,并且可以选择性地漂白捕获的载流子。在两个Mn2 +位点的所有样品中也观察到了放射发光(RL)。并非所有Mn(2+)都显示RL,并且大部分扭曲的Mn2 +位点不显示RL,这可能是由于附近非辐射重组位点的浓度较高。初始剂量为0.1%Mn后,未畸变的Mn2 +与畸变的Mn2 +的RL之比几乎与剂量历史无关,并且对于5%的锰,直至9.6 kGy剂量呈线性关系。我们的结果表明,NaMgF3:Mn具有实时和总剂量测量的巨大潜力,其中存在补充方法可用于获得剂量率,剂量历史,每次照射后的剂量以及直至非常高剂量的累积剂量。

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