掺Dy与Mn的硼酸镁热释光发光谱

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。     

掺入Dy和Mn的MgSO_4磷光体的热释光发光光谱

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。     

掺入Dy和Mn的MgSO4磷光体的热释光发光光谱

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。     

掺Dy的MgB4O7磷光体的研制及其热释光特性

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.     

MgB4O7:Tm,Mn磷光体的热释光特性

采用高温固相法制备了MgB4O7:Tm,Mn磷光体材料,测量了热释光发光曲线和热释光三维光谱以及剂量响应曲线。其主发光峰温度约为400oC,发光波长455 nm。MgB4O7:Tm,Mn主发光峰面积比LiF:Mg,Ti高6.2倍,具有很好的热稳定性,在0.1–2000 Gy范围内具有良好的线性-超线性剂量响应。     

MgSO4:Tm,Mn,P磷光体的研究

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℃）。     

MgB4O7:Tb磷光体的研制及其热释光(TL)特性

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：Tb磷光体。用Risφ／OSL-15-B／C热释光（TL）,光释光（OSL）自动测量仪和TL/OSL三维光谱自动测量仪分别测量了这种磷光体的二维热释光发光曲线和三维热释光发光谱。由MgB4O7：Tb的三维热释光发光谱可看出这种磷光体在230℃、340℃和420℃附近有三个热释光峰,发光谱的波长分别为489nm、548nm、589nm和620nm。此外,不同的高温烧结温度不仅对发光峰的发光强度有很大影响,而且还对。Tb^3＋发光谱形产生影响。当温度高于850℃时Tb^3＋离子发光谱线开始变成了发光谱带。     

MgSO_4:Dy,P和MgSO_4:Dy,P,Cu的热释光剂量学特性

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     

MgSO4：Dy,P和MgSO4：Dy,P,Cu的热释光剂量学特性

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。     

存放温度对CaSO_4:Na,Dy测定照射发生时间的影响

热释光元件的低温发光峰衰退快而高温峰衰退较慢,因而低、高温峰峰下面积比能反映受照后间隔时间的长短。利用这一特性,热释光剂量计在测定吸收剂量的同时可以估算出受照的大致发生时间。在剂量监测中照射发生时间的测定,对于调查事故原因,制定应急措施等会有很大的帮助。 我们用CaSO_4:Na,Dy测定受照发生时间的研究工作表明,在存放温度为10℃时,它能较准确地测定3个月以内的受照发生时间。     

掺稀土硫酸盐的剂量响应特性

测量了掺稀土碱土硫酸盐的热释光和光释光剂量响应曲线,利用复合作用剂量响应模型,得出了剂量响应的非线性参数。实验发现剂量响应的线性与稀土离子的种类及其引起的缺陷结构相关。掺入Eu的磷光体材料的一次作用因子R接近于1,说明其响应是亚线性,以一次作用响应为主;掺入Tm和Dy的磷光体材料的一次作用因子R小于0．5,说明其响应是超线性,以二次作用响应为主。热释光峰温愈高,R因子越小,超线性愈严重,表明二次作用响应所占的份额增加。实验中光释光剂量响应的非线性参数和TL的参数基本相同。     

Dosimetric characterization of a new preparation of BaSO4 activated by Eu ions

The results of a thermoluminescent investigation carried out on a new preparation of BaSO₄ activated by Eu ions at different concentrations (0.1, 0.5 and 1.0 mol%) are reported in this paper. Several batches were prepared by varying Dy, Tm and Sm ions concentrations. The TL sensitivity property of each of the doped barium sulphate samples were compared to the BaSO₄:Eu. The highest sensitivity was found for BaSO₄:Eu (0.5 mol%). The main dosimetric characteristics, i.e. thermoluminescent (TL) response as a function of the dose, reproducibility, lower detection limit, and fading, have been investigated for the BaSO₄:Eu. Furthermore, the kinetic parameters, i.e. activation energy, E, the frequency factor, s, the pre-exponential factor s^* and the kinetic order, b, have been calculated using initial-rise and deconvolution methods. The peak shape methods related to the geometric properties of a TL peak were also used. In order to analyse the TL response at different energies, the effective atomic number (Z_eff = 45–47) for this material was determined.     

Thermoluminescence kinetic parameters of Bi4Ge3O12 single crystals

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.     

The effects of heating rate on the dose response characteristics of TLD-200, TLD-300 and TLD-400

In the given study; the effects of heating rates on the dose response characteristics of CaF₂:Dy (TLD-200), CaF₂:Tm (TLD-300) and CaF₂:Mn (TLD-400) crystals have been investigated using the dose dependence curve and dose response function f(D). It was observed from the dose response functions that the linearity and behaviour of the TL glow peaks of TLD-200 and TLD-400 are affected, but the TLD-300 is not affected from the heating rate.     

Radiation damage effects in CMR manganite materials

Polycrystalline La_0.5Pb_0.5Mn_1−xCr_xO₃ (x = 0.075 and 0.15) samples have been irradiated with 50 MeV Li³⁺ ions with different fluences and the effects on the transport properties have been studied by means of the temperature and magnetic field dependent resistivity measurements. Due to Li³⁺ ion irradiation, the resistivity increases and the metal–insulator transition temperature (T_mi) decreases. At low temperatures (below T_mi), a dominant contribution of the electron–magnon scattering process is observed for all the irradiated and unirradiated samples. The low temperature resistivity behavior as well as the magnetoresistance is modified due to irradiation. The changes in the magnetotransport properties due to irradiation have been compared with the changes caused due to Mn site substitution.     

Thermoluminescence, photoluminescence, photo-stimulated luminescence and optical studies on X-ray irradiated KBr:Ce crystals

This paper reports thermoluminescence (TL) glow and emission, optical absorption and optically stimulated emission studies made on Ce³⁺ doped KBr single crystals irradiated at room temperature. Optical absorption and photoluminescence studies confirm the presence of cerium ions in the trivalent state. A broad and intense blue emission around at 290 and 390 nm, attributable to the transition from 5d excited state to the 4f¹ ground state of Ce³⁺ ions could be observed in the photoluminescence emission. Two TL glow peaks were observed at 374 and 422 K. Presence of characteristic emission due to Ce³⁺ ions in the optically stimulated emission at the F-band confirms the participations of the Ce³⁺ ions in the defect production and recombination processes.     

Al2O3:C、LiF:Mg,Ti、LiF:Mg,Cu,P对本底辐射的热释光响应比较

用Al2O3:C、LiF:Mg,Ti、LiF:Mg,Cu,P热释光剂量计(TLD)测量湛江市区本底辐射的热释光响应,以选取适合低辐射场辐射剂量测量的TLD。它们的最低响应剂量依次为Al2O3:C(1–2μGy)、LiF:Mg,Cu,P(约2μGy)和LiF:Mg,Ti(>10μGy)。Al2O3:C的热释光峰温较低,对较长时间段(>30 d)的累积剂量,存在较明显的热释光衰退,剂量响应曲线偏离线性;LiF:Mg,Cu,P和LiF:Mg,Ti的发光峰温较高,数年内都很稳定。综合考虑灵敏度和稳定性,LiF:Mg,Cu,P更宜于低辐射场的累积剂量测量。     

Paleothermometry of NaCl as evidenced from thermoluminescence data

The firing temperature of ancient ceramic artifacts, i.e. the paleothermometry of these materials has been estimated by various techniques including thermoluminescence (TL) and, more recently, Optically Stimulated Luminescence (OSL) where the OSL response of quartz to firing temperature is used. In this work we report the paleothermometry of sodium chloride (NaCl) by studying the TL response of the material as a function of annealing temperatures in the range of 100–500 °C. Annealing/measurement has been done in a commercial TL/OSL reader (Model No. Risø TL/OSL reader TL-DA-15) in a nitrogen atmosphere.Sodium chloride (NaCl) has been selected as the candidate to test the feasibility of the technique since in this system TL peaks are correlated with the thermal annealing of F-centers unlike the case of quartz where a one to one correlation with all the glow peaks and thermal annealing of defects has not been possible.