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通过掺杂得到的 Mg SO4∶ Tm,P粉末样品 ,经 60 Co和13 7Csγ辐照后 ,测定了 10 -4~ 2× 10 4Gy范围内的热释光的发光曲线和三维光谱 ,确定了 TL峰的峰参数和陷阱参数值 ,主剂量峰位于 2 89.3℃左右 ,辐射剂量响应为超线性 ,从其发光谱上可看到其发光波长主要位于 36 5、4 6 0、6 6 0 mm。通过与其他材料的比较 ,观测到其灵敏度高 ,剂量响应范围宽 ,稳定性好 ,可作为实用的 TL材料在剂量学中获得应用 相似文献
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通过三掺杂得到MgSO4:Tm,Mn,P,其热释光的两个主要发光峰温分别约为253℃和383℃,发光波长位于365nm、460nm和660nm。比较MgSO4:Tm、MgSO4:Tm,Mn、MgSO4:Tm,P、MgSO4:Tm,Mn,P的发光曲线,讨论了杂质Tm、Mn、P分别产生的作用。采用一般级动力学方程拟合发光曲线,确定出各发光峰的激活能与频率因子。用^60Co γ射线在0.1-20kGy的辐照范围内,测定了它们的热释光剂量响应曲线。用复合作用剂量响应函数拟合实验数据,得到两个发光峰的一次作用因子R分别为0.397(253℃)和0.127(383℃)。 相似文献
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以碳酸镁和硼酸为原料在高温条件下合成了基质材料MgB4O7并制备了MgB4O7∶Dy磷光体.用RGD-3热释光剂量仪和三维热释光谱仪分别测量了这种磷光体的二维发光曲线和三维发光谱,实验观察到:1)MgB4O7∶Dy磷光体热释光发光峰峰温为220 ℃和380 ℃;2)Dy3 离子的发光波长为480 nm、575 nm和660 nm;3)磷光体220 ℃和380 ℃发光峰的相对强度随高温固相反应温度的升高而变化,但发光峰温和波长基本保持不变.对比MgB4O7∶Dy和MgSO4∶Dy两种热释光材料的三维发光谱,验证了掺入Dy3 离子的热释光材料的发光峰峰温主要由基质材料决定,发光波长则取决于Dy3 离子的能级跃迁的结果. 相似文献
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掺Dy与Mn的硼酸镁热释光发光谱 总被引:1,自引:0,他引:1
本文制备了掺Dy和Mn的MgB4O7的磷光体,并测量其热释光发光谱。测量结果表明,MgB4O7:Mn的热释光发光峰位于180℃和300℃左右,其发光波长分布较宽,中心约为580nm;而MgB4O7:Dy的热释光发光峰位于200℃和350℃,发光波长由Dy3+离子的能级跃迁决定,位于480、580、680和750nm左右。当两者共掺时,只改变Mn的浓度,测量结果发现,随着Mn掺杂浓度的增加,480nm和680nm左右的发光受到抑制,并且低温峰也受到强烈抑制,而580nm的高温峰逐渐增强并且发光谱变宽。 相似文献
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掺入Dy和Mn的MgSO_4磷光体的热释光发光光谱 总被引:1,自引:0,他引:1
用光学多道分析器和微机控制线性升温法研究了MgSO4 :Dy和MgSO4 :Dy ,Mn热释光材料的发光光谱。测定不同温度和波长的发光光谱 ,得到了热释光三维光谱图。观察到MgSO4 掺入稀土元素Dy的两个发光谱带为 4 80nm和 580nm ,每个光谱带有多个发光峰。与掺入Dy的Ca SO4 的三维发光谱相比较 ,掺入稀土元素Dy的热释光材料的发光谱带的波长主要取决于掺入Dy3+的能级间的跃迁。MgSO4 同时掺入Dy和Mn后 ,4 80nm发光谱带受到很大的抑制 ,所有发光峰的发光效率显著减小 ;波长为 580nm谱带的多个发光峰中 ,温度低于 30 0℃的发光峰的发光效率显著减小 ,在 380℃附近的发光峰的发光强度最大。这说明掺入Mn杂质后 ,不同深度的陷阱的相对分布发生了变化。 相似文献
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用光学多道分析器和微机控制线性升温法研究了MgSO4:Dy和MgSO4:Dy,Mn热释光材料的发光光谱,测定不同温度和波长的发光光谱,得到了热释光三维光谱图。观察到MgSO4掺入稀土元素Dy的两个发光谱带为480nm和580nm,每个光谱带有多个发光峰。与掺入Dy的CaSO4的三维发光谱相比较,掺入稀土元素Dy的热释光材料的发光谱带的波长主要取决于掺入Dy^3 的能级间的跃迁。MgSO4同时掺入Dy和Mn后,480nm发光谱带受到很大的抑制,所有发光峰的发光效应显著减小;波长为580nm谱带的多个发光峰中,温度低于300℃的发光峰的发光效率显著减小,在380℃附近的发光峰的发光强度最大。这说明掺入Mn杂质后,不同深度的陷阱的相对分布发生了变化。 相似文献
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MgSO4:Dy中掺入适量的P,热释发光光曲线中两个高温峰显著增强,主剂量峰的峰温接近283.6℃,另一个发光峰的峰温在352.7℃,其热释光效率超过LiF:Mg,Ti的两倍,MgSO4:Dy,P的单个发光峰峰面积对^60Coγ辐射剂量(0.1Gy-20kGy)的实验响应曲线用复合作用响应函数拟合,得到的非线性特征参数表明,两个发光峰的γ辐射量响应均为超线性,在MgSO4:Dy,P中再掺入微量Cu,首先抑制峰温在352.7℃的发光峰,随着Cu浓度的增加,283.6℃的主剂量峰会随之降低,此的γ辐射剂量响应的超线性随之减小,MgSO4:Dy,P,Cu(0.1mol%,0.5mol%,0.01mol%)磷光体对γ辐射的剂理响应(0.1Gy-20kGy)为亚线性,最引人注目的是MgSO4:Dy,P,Cu(0.1mol%,0.5mol%,0.004%mol)磷光体,它具有与MgSO4:Dy,P(0.1mol%,0.5mol%)相近的热释光灵敏度,并具有最宽的剂量响应线性范围,这种新热释光材料可用于高剂量辐射测量。本文进一步阐明和验证了《复合作用模型》,并揭示了热释光材料中杂质和缺隐结构与剂量学特性的相关性,结合热释光三维发光光谱的分析对热释光机制提出一些见解。 相似文献
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M. Zahedifar M. Mehrabi 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2010,268(23):3517-3522
Thermoluminescence (TL) and photoluminescence (PL) characteristics of CaSO4:Ce nanocrystalline prepared by hydrothermal method has been studied. Its TL glow curve contains three overlapping glow peaks at around 490, 505 and 521 K. Emission spectra band at 303 and 324 nm were observed for the orthorhombic phase of nanosheets. TL response of the prepared nanocrystalline to β and γ radiation was studied and the sensitivity of the nanosheets was found much more than that of analogous microcrystalline and is around 10 times higher than the well known high sensitive TL dosimeter LiF:Mg, Cu, P (GR-200) hot-pressed chips. TL kinetic parameters of this nanocrystalline are also presented. 相似文献
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MgSO4 :Dy中掺入适量的P ,热释光发光曲线中两个高温峰显著增强 ,主剂量峰的峰温接近2 83.6℃ ,另一个发光峰的峰温在 35 2 .7℃ ,其热释光效率超过LiF:Mg ,Ti的两倍。MgSO4 :Dy ,P的单个发光峰峰面积对60 Coγ辐射剂量 (0 .1Gy— 2 0kGy)的实验响应曲线用复合作用响应函数拟合 ,得到的非线性特征参数表明 ,两个发光峰的γ辐射剂量响应均为超线性。在MgSO4 :Dy ,P中再掺入微量Cu ,首先抑制峰温在 35 2 .7℃的发光峰 ,随着Cu浓度的增加 ,2 83.6℃的主剂量峰会随之降低 ,此峰的γ辐射剂量响应的超线性随之减小。MgSO4 :Dy ,P ,Cu (0 .1mol% ,0 .5mol% ,0 .0 1mol% )磷光体对γ辐射的剂量响应 (0 .1Gy— 2 0kGy)为亚线性。最引人注目的是MgSO4 :Dy ,P ,Cu(0 .1mol% ,0 .5mol% ,0 .0 0 4mol% )磷光体 ,它具有与MgSO4 :Dy ,P(0 .1mol% ,0 .5mol% )相近的热释光灵敏度 ,并具有最宽的剂量响应线性范围。这种新热释光材料可用于高剂量辐射测量。本文进一步阐明和验证了《复合作用模型》 ,并揭示了热释光材料中杂质和缺陷结构与剂量学特性的相关性。结合热释光三维发光光谱的分析对热释光机制提出一些见解 相似文献
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Ronaldo Santos da Silva Zlia Soares Macedo Andr Luiz Martinez Antonio Carlos Hernandes Mrio Ernesto Giroldo Valerio 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2006,250(1-2):390-395
In this work, we present a detailed kinetic study of the thermoluminescence of Bi4Ge3O12 (BGO) single crystals grown by the Czochralski technique. A single crystalline phase was confirmed through X-ray diffraction pattern analysis based on the Rietveld profile refinement method. The thermoluminescent (TL) glow curves were induced by UV or beta radiation and measured between 20 °C and 200 °C. The glow curves of BGO crystal presented two peaks at 61 °C and 90 °C for both kinds of radiation. The kinetic parameters, kinetic order (b), activation energy (E) and frequency factor (s), of the TL glow curves have been determined by four different methods. The lifetime of the peaks at room temperature was also determined and used to discuss the stability of the TL peaks at room temperature. 相似文献
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A. Upadhyay R. Rai 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2008,266(11):2594-2598
KNaSO4:Tb3+ phosphors were synthesized by melt technique with different concentration of Tb3+ ions and MgSO4:Dy3+ phosphor is prepared by solid state diffusion method. Lyoluminescence and photoluminescence characterization of KNaSO4:Tb and MgSO4:Dy3+ phosphors are reported in this paper. Only one sharp peak is observed in the lyoluminescence (LL) glow curve and KNaSO4:Tb(0.05 mol%) phosphor shows maximum efficiency. The LL intensity increases linearly with gamma ray dose. LL emission occurs in the blue and yellow region of the spectrum. Photoluminescence (PL) characterization of KNaSO4:Tb(0.05 mol%) phosphor shows PL emission at 486 and 546 nm. These PL emissions from KNaSO4:Tb3+ are due to 5D4 → 7F6 and 5D4 → 7F5 transitions of Tb3+ ion respectively. Lyoluminescence of MgSO4:Dy3+ phosphor shows the high sensitivity to γ-ray exposure and LL emission observed at 486 and 572 nm in the blue and yellow emission of the spectrum is due to Dy3+ ion. Experimental results obtained in the present investigation show that KNaSO4:Tb3+ and MgSO4:Dy3+ phosphors are suitable as a lyoluminescence dosimetry phosphor for ionizing radiations. 相似文献