F／Cl与Eu^2＋：BaFcl中F色心的浓度和光激励截面的关系

研究了Ｅｕ＾２＋：ＢａＦｘＣｌ２－ｘ在紫外线辐照下的光激励发光。通过改变激励方式激励光的扫描方向，给出了Ｅｕ＾２＋：ＢａＦｘＣｌ２－ｘ光激励发光过程中，两种Ｆ色心的浓度比值与光激励截面比值的测定方法。利用这种测定方法，进一步研究了两种Ｆ色心的浓度比值和光激励截面比值与Ｆ／Ｃｌ比值的关系。     

BuFCl：Eu~（2＋）中两种F色心的浓度比值与光激励截面比值的测定方法

本文研究了紫外线辐照下ＢａＦＣｌ：Ｅｕ２＋的光激励发光性质．通过改变激励方式及激励光的扫描方向，给出了ＢａＦＣｌ：Ｅｕ２＋光激励发光过程中，两种Ｆ色心的浓度比值和光激励截面比值的测定方法．     

F／Cl比与Eu~（2＋）：BaFCl中F色心的浓度和光激励截面的关系

研究了Ｅｕ（２＋）：ＢａＦｘＣｌ２在紫外线辐照下的光激励发光。通过改变激励方式及激励光的扫描方向，给出了Ｅｕ（２＋）：ＢａＦｘＣｌ２－ｘ光激励发光过程中，两种Ｆ色心的浓度比值与光激励截面比值的测定方法。利用这种测定方法，进一步研究了两种Ｆ色心的浓度比值和光激励截面比值与Ｆ／ＣＩ比值的关系。     

Eu^2＋：BaFCl光激励发光衰减的研究

制备了系列材料Ｅｕ＾２＋：ＢａＦＣｌ，测量了其光激励发光的衰减曲线，基于隧穿模型，建立了描述隧穿过程的数学模型，得出了光激励发光衰减规律，并将结果与实验进行了比较。     

Eu^2＋：Sr9Ca（PO4）6Cl2中的新型色心及其光激励发光

本文报道了Ｅｕ＾２＋：Ｓｒ９Ｃａ（ＰＯ４）６Ｃｌ２的新型色心。它的吸收带主峰分别位于７０８，７８５，８４５及９９０ｎｍ。用对应于Ｆ心吸收带和这些吸收带波长的光束分别激励样品时得到相同的光激励发光。通过对比研究表明，这些吸收带是由Ｆ心的缔合中心，即由ＦＡ心产生的。由于这些色心的吸收带偏离Ｅｕ＾２＋的发射波长（４５０ｎｍ）更远，故更适应于Ｅｕ＾２＋：Ｓｒ９Ｃａ（ＰＯ４）６Ｃｌ２光波励发光的研究和开发。     

BaFCl∶Eu~（2＋）中F色心的浓度和光激励截面与温度和紫外线的辐照波长的关系

本文研究了ＢａＦＣｌ∶ＥＵ（２＋）在不同波长的紫外线辐照和不同的测定温度下的光激励发光性质．通过改变激励方式及激励光的扫描方向，给出了ＢａＦＣｌ∶Ｅｕ（２＋）光激励发光过程中，两种Ｆ色心的浓度比值和光激励截面比值与紫外线辐照波长和测定温度的关系．同时我们还研究了在激励读出过程中，对应两种Ｆ色心的光激励发光强度与激励温度的关系，并且给出了相应于Ｆ（Ｃｌ－）心的热激活能．     

SBN晶体中Eu^3＋激光态^5D0的无辐射跃迁

通过测量＾５Ｄ０→７Ｆ２发射带的荧光寿命与晶体温度的依赖关系，研究了Ｅｕ＾３＋激发态＾５Ｄ０的无辐射跃迁。结果表明，＾５Ｄ０→Ｆ２带的温度淬灭效应主要是由于电荷转移态的最低能量太低，＾５Ｄ０态易被热激活至电荷转移，然后通过电荷转移无辐射驰豫至＾７Ｆ０态。     

Eu3+:Y2SiO5晶体透射光谱和荧光谱研究

在室温条件下,对Ｅｕ＾３＋：Ｙ２ＳｉＯ５晶体的透射光谱和４５７．９ｎｍＡｒ＾＋激光激发荧光谱进行测量和研究。这些光谱表明,Ｅｕ＾３＋离子在Ｙ２ＳｉＯ５晶体中占据两种最低对称性Ｃ１格位。利用透射光谱和荧光谱对Ｅｕ＾３＋离子的最低激发态＾５Ｄ０的两种格位光谱进行了成功分离。实验发现,在＾５Ｄ０态两种格位谱的谱宽只有０．１ｎｍ左右,其峰间隔约为０．１８ｎｍ。另外,文中还测量了Ｅｕ＾３＋离子的基态＾７ＦＪ     

Ca8Mg(SiO4)4Cl2中Ce3+和Eu2+的光谱性质和能量传递

首次合成了Ｃｅ＾３＋和Ｅｕ＾２＋共激活氯硅酸镁钙Ｃａ８Ｍｇ（ＳｉＯ４）４Ｃｌ２：Ｃｅ＾３＋，Ｅｕ＾２＋高效绿色荧光粉，报道了它们的漫反射光谱、激发和发射光，观察到氯硅酸镁钙中Ｃｅ＾３＋ Ｅｕ＾２＋     

MAl2O4：Eu^2＋,RE^3＋,长余辉发光性质的研究

研究鳞石英结构碱土铝酸盐ＭＡｌ２Ｏ４：Ｅｕ＾２＋,ＲＥ＾＋（Ｍ＝Ｍｇ,Ｃａ,Ｓｒ,Ｂａ：ＲＥ＝Ｙ,Ｌａ,Ｃｅ,Ｐｒ,Ｎｄ,Ｓｍ,Ｇｄ,Ｔｂ,Ｄｙ,Ｈｏ,Ｅｒ,Ｔｂ,Ｄｙ,Ｈｏ,Ｅｒ,Ｔｍ,Ｙｍ,Ｙｂ,Ｌｕ）的荧光及长余辉发光性质。其发光由Ｅｕ＾２＋的４ｆ－５ｄ跃迁产生。ＲＥ＾３＋作为辅助激离子,提供合适的陷阱能级。即使用ＲＥ＾３＋的特性波长激发,在ＭＡｌ２Ｏ４：Ｅｕ＾３＋的发光中也观察不到ＲＥ＾３     

Effects of excitation and bleaching of ultraviolet during photostimulated luminescence of BaFCl:Eu2+ phosphors

The photostimuated luminescence (PSL) of BaFCl:Eu²⁺ phosphors is studied through changing the energy of ultraviolet(UV)-irradiation. The PSL shows obviously difference while the irradiation energy is larger or smaller than that of the Eu²⁺ minimum excited state. The reasons for this difference are discussed and the location of the transform energy level of UV-irradiation from excitation to bleaching is given. Supported by National Natural Science Foundation of China.     

BaFCl:Eu2+光激励读出过程中两种F色心的差异

研究了紫外线辐照下BaFCl:Eu²⁺的光激励发光性质.测定了在不同温度下经紫外线辐照后的光激励谱,变化范围为10—300K同时研究了两种F色心的光激励发光强度在激励读出过程中随温度的变化关系.分析了光激励谱产生差异的原因. 关键词：     

Eu-Doped KCl storage phosphor for erasable and rewritable optical memory utilizing photostimulated luminescence phenomenon

Intense photostimulated luminescence (PSL) with a peak at 420 nm is observed in ultraviolet (UV) Iight-irradiated europium-doped potassium chloride (KCl: Eu) crystalline phosphors. The PSL characteristics of UV-irradiated KCl: Eu phosphor for optical memory application were studied. The excitation and emission mechanisms of the 420 nm PSL, which are consistent with the results obtained, are discussed.     

Photostimulated luminescence of corrugated fiberboard as an additional screening method for detecting radiated foods

In this study, PSL of non-irradiated and irradiated corrugated fiberboards (CFs) was investigated to evaluate the possibility that CFs can be used as alternative specimens for the screening detection method of food irradiation. The irradiation at a dose of only 0.15 kGy increased PSL signals of the CF over 1 order of magnitude. The PSL signals increased with increasing in gamma irradiation dose and became almost saturated at a dose of 5 kGy. The core of CFs showed PSL signals sufficient for distinguishing irradiated from non-irradiated at least 6 months after irradiation even though the CF was exposed to light and the environmental temperature increased to 50 °C. These results suggest that the PSL property of the core of CFs is useful for detecting irradiation. However, the large variation of PSL signals among CFs made it difficult to set a well-defined “positive” threshold limit to distinguish irradiated from non-irradiated completely. All of the non-irradiated CFs showed PSL signals above 10³ counts, which is much higher than that detected for foods. It is apparent that the threshold limit of EN 13751 is not applicable to detecting irradiated CFs. More detailed collaborative research with large number of samples is needed to establish new threshold limits involving “intermediate” classification.     

Photoluminescence degradation mechanism of BaMgAl10O17：Eu2＋ phosphor by vacuum ultraviolet irradiation

<正>A real high power vacuum ultraviolet light source is applied to the investigation on the vacuum ultraviolet irradiation degradation of BaMgA₁₀O₁₇:Eu²⁺ phosphor.The degradations of emission intensity and color quality of the sample are clearly observed after irradiation.It reveals that the oxidation of Eu²⁺ during irradiation is partly responsible for the degradations.The excitation and absorption spectra show that some traps generated during irradiation have negative influence on the luminescence of sample and these traps have been identified as positively charged oxygen vacancies by positron annihilation.The investigations on host emission and decay curve further confirm that these oxygen vacancies are involved in the perturbation of energy transfer from the host to Eu²⁺ and finally result in the degradation.     

BaFCl:Eu2+中F色心的浓度和光激励截面与温度和紫外线的辐照波长的关系

本文研究了BaFCl:Eu²⁺在不同波长的紫外线辐照和不同的测定温度下的光激励发光性质.通过改变激励方式及激励光的扫描方向,给出了BaFCl:Eu²⁺光激励发光过程中,两种F色心的浓度比值和光激励截面比值与紫外线辐照波长和测定温度的关系.同时我们还研究了在激励读出过程中,对应两种F色心的光激励发光强度与激励温度的关系,并且给出了相应于F(Cl^-)心的热激活能.     

真空环境中紫外脉冲激光对熔石英抗损伤能力的影响

在10-3Pa的高真空环境下,利用355nm的紫外脉冲激光以低于石英基片零概率损伤阈值的能量密度对其进行重复多次的全口径扫描,目的是为了研究石英基片在接受不同剂量的紫外激光辐照后其抗损伤能力的变化和原因.通过辐照过程中损伤点的扩展程度以及辐照后的抗损伤测量表明,高真空环境下紫外脉冲激光辐照后的石英基片抗损伤能力明显降低,降低的幅度更多的与其接受激光辐照的次数有关,辐照能量密度的影响相对较小;通过荧光及X射线光电子能谱(XPS)检测发现,紫外脉冲激光辐照后石英基片表面氧缺位的增加是导致其抗损伤能力下降的主要原因,其程度也直接与接受辐照的紫外脉冲激光剂量相关.     

Effect of microwave irradiation on the electronic structure of ZnO

Modifying the electronic structure may allow a bulk material to efficiently absorb radiation as well as excite and emit atomic plasma. The interaction between microwaves and metal oxides is investigated by analyzing the electronic structure of ZnO with and without microwave (MW) irradiation using absorption, photoluminescence (PL), and PL excitation (PLE) spectroscopies and utilizing an ultraviolet synchrotron light source. MW irradiation lowers the energy of the absorption edge of ZnO producing defects. Additionally, MW irradiation causes a resonantly enhanced change in the intensity and peak shift of the PL band. These phenomena indicate that the defects generated by MW irradiation change the electronic structure of ZnO and the electron transition process.     

Mechanism of photostimulated luminescence: BaFCl:Eu2+

We propose a new parallel model based on the analysis of photostimulated luminescence (PSL) process and existing theoretical models. While solving this model, the general expression for PSL is gained. BaFCl:Eu²⁺, one of the PSL materials, is prepared and a series of spectra are measured. We compared the theoretical and experimental results in terms of the decay process, the difference between two kinds of color centers and the relationship between irradiation dose and luminescent intensity. Supported by the National Nature Science Foundation of China.