X射线辐照后BaFC1中缺陷性质的研究

未掺Eu~(2+)的BaFCl粉末样品在80K下经X射线辐照后,在不同的温度条件下(从80K副273K),用580nm的光波激励样品时观测到310nm和380nm的发光峰.经分析认为,样品经X射线辐照后,在晶体中形成两种卤素离子的F-H’心对.当用F心吸收带的光波激励样品时,两种F—H心对衰变成相应的自陷激子态并复合发光.310nm和380nm分别对应于F-离子和Cl-离子的自陷激子的发光,并且它们的发光强度强烈地依赖于温度的变化。     

高低温条件下氟化锂材料的离子激发发光光谱分析

在北京师范大学GIC4117串列加速器原有离子激发发光(ion beam induced luminescence,IBIL)分析靶室基础上,安装了可实现80—900 K温度范围内精确控温的冷热样品台,实现高低温条件下IBIL光谱的测量.添加金硅面垒探测器,在离子辐照材料样品过程中同步采集背散射离子的计数,实现束流的在线监测.在不同温度下,利用2 MeV H~+束轰击氟化锂样品,获得的IBIL光谱中可明显观察到温度对不同发光中心发光效果的影响:激子峰和杂质峰发光在低温条件下更为清晰;高温时各类型F色心的发光强度在较小的注量下即可达到饱和值或开始衰减.辐照初期受扰激子峰(296 nm)发光强度的上升过程表明不能排除受扰激子峰与点缺陷发光中心相关的可能性,激子峰强度的上升源自低注量时核弹性碰撞产生的应变键;温度对空位迁徙速率及非辐射复合的影响是造成发光强度随注量演变差异的重要原因.     

MOCVD方法生长ZnO微米柱的结构与光学性质

通过X射线衍射、扫描电子显微镜和变温光致发光光谱对MOCVD方法生长在蓝宝石衬底上的ZnO微米柱材料的结构及发光特性进行了表征.X射线衍射结果表明,ZnO具有良好的c轴择优取向,扫描电子显微镜图中可观察出ZnO微米在呈六角结构生长,半径约为0.5～1.5μm.样品的发光光谱通过He-Cd激光器的325nm线激发,从光谱中发现低温(81K)下出现极强的与激子相关的带边发光峰,温度升高到360K时与自由激子相关的紫外发射峰仍然是清晰可见.     

α-Al2O3: Mn单晶的三维热释发光谱研究

测量了α-Al2O3: Mn单晶中子辐照前后的三维热释发光谱.观察到α-Al2O3: Mn:Mn单晶γ射线照射后测量的三维热释发光谱中，峰温在350℃波长为680nm处有一宽发光峰，这可能与Mn2+离子有关；波长为695nm峰温在170℃和350℃的线状光谱，叠加在680nm宽发光峰上，是Cr3+离子的发光谱线,其中可能有Mn4+离子的贡献.与纯α-Al2O3单晶的热释发光谱相比，掺入Mn杂质后，γ射线照射的三维热释发光谱中完全地抑制了波长为416nm的α-Al2O3的F心发光峰.经1017cm-2中子注量辐照和退火后，γ射线照射后测量的三维热释发光谱中，在150℃出现了波长为416和695nm的发光峰，以及在250℃波长为680和695nm的发光峰，其中695nm新发光峰的强度略超过了中子辐照前α-Al2O3:Mn在350℃波长为695nm的发光峰，说明中子辐照产生了大量浅陷阱能级和F心.然而，经1018cm-2中子注量辐照和退火后，γ射线照射后测量的三维热释发光谱中，出现了峰温150℃，190℃和250℃波长为520nm的Mn2+离子发光峰，以及300℃波长为680和695nm的Cr3+（或Mn4+）的发光峰，表明增高中子注量的辐照，产生了温度为190℃，250℃和300℃深陷阱能级和F心，并使Mn2+离子发光峰明显加强. 关键词： α-Al2O3:Mn 三维发光谱 缺陷结构 发光机理     

退火对Pb辐照Al2O3单晶发光特性的影响

研究了230MeV的²⁰⁸Pb²⁷⁺辐照Al₂O₃样品及随后在600,900,1100K高温条件下退火后的光致发光特性。从辐照样品的测试结果可以清楚地看到在波长为390,450nm处出现了强的发光峰。辐照量为1×10¹³ions/cm²时,样品的发光峰最强。经过600K退火2h后测试结果显示,380nm发光峰剧烈增强,而其他发光峰显示不明显。在900K退火条件下,380nm的发光峰开始减弱,而在360,510nm出现了明显的发光峰,至到1100K退火完毕后380nm的发光峰完全消失,而360,510nm的发光峰相对增强。从被辐照样品的FTIR谱中看到,波数在460~510cm^-1间的吸收是振动模式,经过离子辐照后,吸收带展宽,随着辐照量的增大,Al₂O₃振动吸收峰消失,说明Al₂O₃振动模式被完全破坏。1000~1300cm^-1之间为Al—O—Al桥氧的伸缩振动模式,辐照后吸收带向高波数方向移动,说明其振动模式受到影响。辐照剂量较小的样品,损伤程度相对较低,经退火晶化后,振动模式基本恢复到单晶状态;辐照剂量较高的样品,损伤程度大,退火处理后表面变得较粗糙,振动模式并未出现,说明结构破坏严重。     

二氧化钛阵列的制备及其光学性能

以水热法制备了由纳米棒组成的二氧化钛阵列。通过控制反应时间,对组成阵列的二氧化钛纳米棒的尺寸进行调节。利用扫描电镜和X射线衍射光谱分析了样品的形貌和晶体结构,发现将反应时间由4 h延长至8 h,二氧化钛纳米棒的直径由100 nm增大到200 nm。利用紫外-可见吸收光谱测量了样品的光吸收特性,发现了尺寸效应引起的吸收边和带隙变化,反应时间由4 h延长至8 h,样品带隙由3.09 eV变化至2.97 eV。利用荧光光谱研究样品的光致发光性能,发现了样品的近带边发光(382 nm左右)、自陷激子发光(420 nm左右)、束缚激子发光(456 nm左右)和缺陷能级发光(492 nm左右)。     

KMgF3晶体的色心和自陷态激子研究

应用从头计算方法对KMgE3离子晶体中的色心和自陷态激子(STE)进行了模拟研究.对包含F心的量子团簇进行几何结构优化,并计算了F心处于1s基态和2p激发态的Mulliken电荷分布.模拟结果表明,F心周围的晶格弛豫较小,处于基态的F心电子主要局域在阴离子空位处,而处于激发态的F心电子波函数则比较扩展.计算结果表明,Vk心移向邻近的间隙位置,但仍保持分子轴向与[110]晶向平行.自陷态激子的弛豫是分子轴向平移与转动的叠加.计算得到的F心、Vk心的光学激发能及STE的发光能与实验符合得较好.     

真空紫外光激发下掺Pr3+铝酸盐的自陷激子对Pr3+发光的影响

研究了SrAl12 O19:Pr3+和Y3Al5O12(YAG):Pr3+在20K,77K和300K的真空紫外(VUV)光谱,二者除了表现出Pr3+特有的发射性质外,还产生了一种特殊的发射现象,即自陷激子(STE)发射,并且其随着稀土离子浓度和温度的降低而增强.还着重讨论了自陷激子对Pr3+发光的影响.     

KMgF3晶体的色心和自陷态激子研究

应用从头计算方法对KMgF3₃离子晶体中的色心和自陷态激子(STE)进行了模拟研 究.对包含F心的量子团簇进行几何结构优化, 并计算了F心处于1s基态和2p激发态的Mulliken电荷分布. 模拟结果表明，F心周围的晶格弛豫较小，处于基态的F心电子主要局域在阴离子空位处，而处于激发态的F心电子波函数则比较扩展. 计算结果表明，VK_K心移向邻近的 间隙位置，但仍保持分子轴向与［110］晶向平行.自陷态激子的弛豫是分子轴向平移与转动的叠加.计算得到的F心、VK关键词： 色心 自陷态激子 从头计算 3离子晶体')" href="#">KMgF3₃离子晶体     

重离子辐照SiO_2/Si结构变温光致发光谱研究

本文研究了重离子辐照前后SiO_2/Si结构光学性质的变化。实验选择初始能量为414 MeV,不同辐照总剂量的Sn离子,在室温下辐照氧化层厚度为36nm和90nm的SiO_2/Si结构。并在不同测试温度下获得了辐照前后SiO_2/Si结构的光致发光谱(PL)谱。在相同的测试温度下,随着辐照总剂量的改变,峰位发生了移动,峰的强度也发生了改变;在相同的辐照总剂量下,随着测试温度的改变,峰位发生移动。由于受束缚激子发光的影响,在测试温度为80K时出现了一个新的光致发光峰。     

BaFCl：Eu2+X射线存储机制的探讨

本文报导了BaF2-xClx和BSFCl:Eu2-(0.1%)两种粉未样品的制备过程;及其系列样品的电子自旋共振的实验结果.认为BaFCl:Eu2-存储X射线的过程是:经X射线辐照后;在其晶体中形成自由电子和空穴,阴离子空位俘获一个电子形成F心,而空穴被束缚在两个氯离子上形成Vk(Cl2-)心,Vk(Cl2-)心经迁移被发光中心Eu2+所束缚.     

Luminescence of silicon Dioxide — silica glass, α-quartz and stishovite

This paper compares the luminescence of different modifications of silicon dioxide — silica glass, α-quartz crystal and dense octahedron structured stishovite crystal. Under x-ray irradiation of pure silica glass and pure α-quartz crystal, only the luminescence of self-trapped exciton (STE) is detected, excitable only in the range of intrinsic absorption. No STE luminescence was detected in stishovite since, even though its luminescence is excitable below the optical gap, it could not be ascribed to a self-trapped exciton. Under ArF laser excitation of pure α-quartz crystal, luminescence of a self-trapped exciton was detected under two-photon excitation. In silica glass and stishovite mono crystal, we spectrally detected mutually similar luminescences under single-photon excitation of ArF laser. In silica glass, the luminescence of an oxygen deficient center is presented by the so-called twofold coordinated silicon center (L.N. Skuja et al., Solid State Commun. 50, 1069 (1984)). This center is modified with an unknown surrounding or localized states of silica glass (A.N. Trukhin et al., J. Non-Cryst. Solids 248, 40 (1999)). In stishovite, that same luminescence was ascribed to some defect existing after crystal growth. For α-quartz crystal, similar to silica and stishovite, luminescence could be obtained only by irradiation with a lattice damaging source such as a dense electron beam at a temperature below 80 K, as well as by neutron or -irradiation at 290 K.     

Luminescent properties of Ce in MSO4 (M: Ca, Sr and Ba) and the effect of Na co-doping

The optical properties of Ce³⁺ in CaSO₄, SrSO₄ and BaSO₄ are reported. The Ce³⁺ ion shows 4f⁰5d¹→²F_5/2,²F_7/2 luminescence in all three sulphates. Co-doping with Na⁺ does not change the local surrounding of the Ce³⁺ ion, but enhances the amount of Ce³⁺ ions built in. Under optical excitation, besides the typical Ce³⁺ doublet emission in the ultraviolet spectral region, band emission around 445 nm was observed. This band emission was not assigned to emission from a Ce³⁺ centre, but to emission from an impurity-trapped exciton. Under X-ray excitation, both Ce³⁺ emission and an emission band around 380 nm was observed. This band was assigned to emission from a self-trapped exciton.     

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.     

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．     

Cross-shaped photoluminescence of excimers in perylene crystals

Cross-shaped excimer (self-trapped exciton) luminescence from α- and β-perylene single crystals of 50–100 μm was found when they were excited at the center of the crystals with a continuous-wave (cw) laser resonant with the exciton absorption. The cross shape is formed by the two lines which intersect at the excited position and are perpendicular to the sides of the crystals of parallelogram shape. Luminescence is emitted from the excited spot and 4 side edges in the cross shape. The most striking feature is that the luminescence intensity at the edges was as high as or higher than at the excited spot. The possibility of the exciton propagation or the waveguide effect is rejected both experimentally and theoretically. This phenomenon can be reasonably explained only when the radiative transition probability of excimers is significantly enhanced at the crystals side edges than at the center due to the lower symmetry.     

Effect of annealing on structural and optical properties of lead tungstate microcrystals

Shuttle-like lead tungstate (PbWO₄) microcrystals are synthesized at room temperature using the precipitation method with the cetyltrimethyl ammonium bromide. Results from both the X-ray diffraction and the scanning electron microscopy show that the lattice distortions of the PbWO₄ microcrystals are reduced significantly when the annealing temperature is increased to 873 K. The result from the ultraviolet-visible diffuse reflectance spectroscopy shows that the exciton absorption appears in the sample annealed at 673 K. The self-trapped exciton luminescence due to the Jahn-Teller effect is also observed in the blue band. The interstitial oxygen ions in the WO₄^2- groups are mainly resposible for the enhancement effect of the green luminescence of the annealed samples. The above results are supported by the spectrum analysis of the as-grown and the post-annealed samples using the X-ray photoelectron spectroscopy.     

Time-resolved luminescence of complex wide-gap oxide crystals under inner-shell excitation

In order to investigate the soft X-ray energy transformation in oxide detectors the optical spectra of several wide-gap oxide crystals were analyzed. The time-resolved luminescence (2.5–10.5 eV) and luminescence excitation spectra (50–200 and 500–630 eV) as well as decay kinetics of luminescence at 10 and 295 K were recorded using the synchrotron radiation from BW3 channel (HASYLAB, DESY). Several analogous features were discovered in the excitation spectra of both intrinsic self-trapped exciton luminescence and recombination luminescence for BeO, BeAl₂O₄, Be₂SiO₄ and AlPO₄ crystals under inner-shell excitation. Simultaneously, the excitation of Ce³⁺-luminescence in scintillating Be₂La₂O₅-Ce crystals significantly differs.