Study of Photostimulable Luminescence Materials Sr_9Ca(PO_4)_6Cl_2:Eu

The polycrystalline Sr_9Ca(PO_4)_6Cl_2:Eu has been synthesized by solid state reaction.The reaction condition,the appropriate raw materials and their quantity used,which may affect the photostimulable luminescence (PSL),have been systematically inves- tigated.The properties of this PSL phosphor as a material for storing and reproducing the X-ray image in computer-aided radiography have been reported briefly.

Sonoluminescence as the PeTa Radiation

In this paper, a model of cavitational luminescence (CL) and sonoluminescence (SL) is developed. The basis of the model is the PeTa (Perel’man-Tatartchenko) effect—a characteristic radiation under first-order phase transitions. The main role is given to the liquid, which is where the cavitation occurs. The evaporation of the liquid and subsequent vapor condensation inside the bubble are responsible for the CL and SL. Apparently, the dissolved gases and other impurities in the liquid are responsible for peaks that appear at the background of the main spectrum. They most likely are excited by a shock wave occurred during cavitation. The model explains the main experimental data. Thus, no mystery, no plasma, no Hollywood.

A Two-dimensional Anthracene-9,10-dicarboxylate Zinc(Ⅱ) Coordination Polymer Based on Binuclear [Zn_2Cl_2] Nodes: Synthesis, Characterization and Luminescent Properties

A two-dimensional（2D） 44 topological ZnⅡ coordination polymer {[Zn2Cl2（L）（4bpy）2]}∞（H2L = anthracene-9,10-dicarboxylic acid, 4bpy = 4,4ˊ-bipyridine） based on binuclear [Zn2Cl2] nodes has been synthesized and characterized by IR, elemental analysis, X-ray powder diffraction and single-crystal X-ray diffraction analysis. Moreover, the luminescent properties of the correspon- ding compound have been briefly investigated.

Sonoluminescence as the PeTa Radiation, Part Two

This paper is a continuation of one published in this journal nine months ago. The two papers present a model of cavitational luminescence (CL), multi-bubble sonoluminescence (MBSL), one-bubble sonoluminescence (OBSL), and laser-induced bubble luminescence (LIBL). The basis of this model is the PeTa (Perel’man-Tatartchenko) effect, a nonequilibrium characteristic radiation under first-order phase transitions, especially vapour condensation. In this model, the main role is given to the liquid, where the evaporation, condensation, flash, and subsequent collapse of bubbles occur. The instantaneous vapour condensation inside the bubble is a reason for the CL/MBSL/OBSL/LIBL. Apparently, the dissolved gases and other impurities in the liquid are responsible for peaks that appear at the background of the main spectrum. They are most likely excited by a shock wave occurred during the collapse. This paper, in contrast to the previous one, presents a slightly expanded model that explains additional experimental data concerning especially the LIBL spectrum. As a result, today we are not aware of any experimental data that would contradict the PeTa model, and we continue to assert that there is no mystery to the CL/MBSL/OBSL/LIBL phenomena, as well as no reason to hope that they can be used for high-temperature chemical reactions, and even more so for a thermonuclear ones.

Sonoluminescence as the PeTa Radiation, Part Three

This paper is the third in a series published in this journal during 2017-2018. These three papers present various stages in the development of the PeTa model for phenomena of the same physical nature: cavitational luminescence (CL), multi-bubble sonoluminescence (MBSL), single-bubble sonoluminescence (SBSL), and laser-induced bubble luminescence (LIBL). The basis of this model is the PeTa (Perel’man-Tatartchenko) effect—a nonequilibrium characteristic radiation under first-order phase transitions, for instance, vapour condensation. The third iteration of this model “Vapour bubble luminescence” (VBL) is presented in this paper. The essence of this model is as follows: with a local decrease of pressure or an increase of temperature in a tiny volume of the liquid, one or several bubbles filled with vapour will appear. Subsequently, a very rapid increase in pressure or a decrease in temperature of the bubble leads to super-saturation of the vapour inside the bubble, followed by its instantaneous condensation with the emission of condensation energy (this is the PeTa effect). A sharp decrease in pressure causes the collapse of the bubble accompanied by a shock wave in the liquid. VBL model is conveniently represented on the solid-liquid-vapour phase diagram. A better understanding of the physical nature of the phenomena under consideration could help to find their useful applications. To develop this idea further, we propose a design of a cavity-free pulsed laser on the basis of CL/MBSL/SBSL. An analysis of LIBL in cryogenic liquids is also given in this paper.

白光LED用新型红色荧光粉Sr_5(BO_3)_3Cl:Eu^(3+)的制备与发光特性

采用高温固相法合成了Sr5(BO3)3Cl:Eu3+新型红色发光材料,并对其结构和发光特性进行了研究。X射线衍射测试表明合成材料为纯相Sr5(BO3)3Cl晶体。材料的主发射峰位于587,596,613nm和626nm,对应Eu3+的5 D0→7F1,7F2辐射跃迁。监测626nm发射峰,激发光谱主峰位于392nm,可被InGaN管芯有效激发。通过时间分辨光谱测得Eu3+离子5 D0能级的荧光寿命约为2.28ms。研究了Eu3+离子掺杂浓度对Sr5(BO3)3Cl:Eu3+发光性能的影响,结果随着Eu3+离子浓度的增大,样品的发光强度先增大后减小,最佳掺杂浓度为16%(摩尔分数)。计算了Eu3+离子浓度猝灭的临界距离为1.46nm。测量了不同Eu3+浓度样品的色坐标,均位于色品图红光区,符合NTSC标准。

类溶胶-凝胶法制备LiMn_2O_(4-δ)Cl_δ正极材料

本文以水合氢氧化锂 (LiOH .H2 O)、水合硝酸锰 (Mn(No3) 2 .6H2 O) ,水合氯化锂 (LiCl.H2 O)为原料 ,用类溶胶 凝胶法制备了LiMn2 O4 δClδ,并且以此作正极进行了电化学测试 .结果表明 ,掺氯的尖晶石LiMn2 O4 正极材料具有优异的稳定性 ,且循环稳定后 ,容量几乎没有衰减 .

在Cl^-环境下金属腐蚀行为和机理

Cl-环境下的金属腐蚀尤其是奥氏体不锈钢的腐蚀是世界石化工业急需解决的难题之一。概述了在Cl-环境下碳钢和奥氏体不锈钢的腐蚀机理、破坏类型、影响因素和实验方法,提出了目前在研究中存在的主要问题和将来重点研究方向,为Cl-环境下的金属的腐蚀与防护,以及复杂环境下腐蚀主导机制的确定提供理论参考。

碳酸盐岩微观测试技术对比与应用——以济阳坳陷乐安油田潜山为例

微观测试结果能反映很多油藏信息。目前关于微孔缝的镜下测试技术不断丰富,但仍缺少对微孔缝最全面的微观分析。为了便于对比各类测试技术,以济阳坳陷乐安油田草桥潜山区域为典型代表实例,先采用不同的精细微观专项测试技术对孔缝储集空间特征进行分析,具体包括微溶孔电子探针成分分析、扫描电镜、薄片和阴极发光测试等技术,然后总结了通过各种不同的微观测试技术观察到的现象及规律。具体结果和得出认识如下:通过电子探针成分分析技术,能够分辨出灰岩微溶孔内诸如有机质、方解石、黄铁矿、白云石、石膏等成分;薄片内可见灰岩含油段砾间砾内孔洞发育,溶蚀孔洞边部有轻微方解石化;通过扫描电镜分析,能够分辨出代表区块的白云岩结晶孔比灰岩溶蚀孔大两个以上数量级,能通过晶间孔或溶蚀孔推断岩石的脆性以及是否易于压裂;通过岩样阴极发光测试,能够区分出共有几期成分不同的孔洞充填物;通过扫描电镜和压汞都可以得到孔喉大小,比较两项技术,扫描电镜得到的是局部纳米级的孔喉直径,而压汞测试得到的是单块样品微米级孔喉半径。从应用对象来看,前者适合对应到矿物的孔喉,后者更适合开发区块的孔喉对比研究。

紫外线辐照能量对BaFCl：Eu^（2＋）光激励发光的影响

通过改变紫外线辐照能量，研究了ＢａＦＣｌ：Ｅｕ（２＋）的光激励发光性质．发现当紫外线能量大于或小于Ｅｕ（２＋）最低激发态能量两种情况下，光激励发光有明显的差异，还分析了产生差异的原因，并且给出了紫外线辐照能量与Ｆ／Ｃｌ比值的关系．

X射线和紫外线激发下BaFCl_xBr_(1-x):Eu^(2+)的发光

制备了ＢａＦＣｌｘＢｒ１－ｘ：Ｅｕ２＋（ｘ＝００，０２，０４，０６，０８，１０）四元系列氟卤化合物．对于不同的Ｃｌ／Ｂｒ比值样品，研究了其在Ｘ射线和紫外线激发下的发光性质；同时研究了在Ｘ射线激发下的发光强度随温度的变化关系，并发现这种关系随Ｃｌ／Ｂｒ比值的变化呈现一定的规律性；最后，测量了在紫外线激发下。

NH4^+和NO3^-对纯锌在NaCl溶液中腐蚀行为的影响

采用质量损失实验、电化学测试以及扫描电镜(SEM)、激光扫描共聚焦显微镜(CLSM)等研究了NH4^+与NO-3对纯锌(Zn≥99.99%)在NaCl溶液中腐蚀行为的影响。结果表明:在NH4^+-NO3^-Cl^-体系中,NH4^+对促进锌的腐蚀起主导作用;NO-3的存在可显著加速样品在溶液中的电化学阴极反应,同时导致样品金属表面腐蚀形态发生改变,局部腐蚀坑趋向横向扩张生长。另外,在一定浸泡时间周期内,样品金属的腐蚀速度与NH4NO3浓度呈正相关。

^(147)Pm激发的ZnS∶Cu,Cl发光粉的研究

以高纯ZnS粉末为基质,采用高温转相、扩散,以及表面涂敷工艺,制得了147Pm激发的ZnS∶Cu,Cl发光粉。分析了ZnS∶Cu,Cl的晶体结构,测量了ZnS∶Cu,Cl的激发光谱、发射光谱、发光亮度。其晶体结构主要是六方纤锌矿型结构,激发光谱峰值波长为341nm,发射光谱峰值波长为513nm,初始发光亮度达到312mcd/m2。由激发光谱的峰值波长341nm推算得到六方ZnS晶体的禁带宽度为3.64eV。分析了147Pm激发的ZnS∶Cu,Cl发光粉的发光寿命,其发光寿命达到5年以上。还探讨了该放射性发光粉的发光机理。147Pm激发的ZnS∶Cu,Cl的稳定发光,实际上是激发过程与复合过程的准平衡。ZnS∶Cu,Cl的绿色发光来源于深施主-深受主对的复合发射。实验结果的分析表明,ZnS∶Cu,Cl中深施主-深受主之间的能级间隔约为2.42eV。

Size-induced effect on cathode luminescence spectra of CsI(Na) and CsI(Tl) crystals

We investigated the cathode luminescence characteristics of CsI(Na)and CsI(Tl)crystals by the spectrum and structure properties at room temperature.We fabricated three different sizes of CsI(Na)and CsI(Tl)crystals and measured their luminescence spectra under cathode rays.We found that CsI(Na)cathode luminescence peaks appear at 420 and 305 nm,and CsI(Tl)cathode luminescence peaks are 540 and 410 nm,the grain size affects CsI(Na)luminescence significantly,and the Na-related420 nm luminescence intensified relatively when the average grain size reaches^20μm,which becomes weak when the grain size is down to nano-scale.But the cathode luminescence spectra of CsI(Tl)crystals with different size have no obvious changes.Our explanations for these phenomena are that the different impurities in the same host material CsI lead to different luminescence mechanisms.These cathode luminescence characteristics indicate the suitability of CsI(Na)and CsI(Tl)crystals to match photomultiplier tube for large area crystal detector development.

Ca_2BO_3Cl:Ce^(3+),Tb^(3+):A novel tunable emitting phosphor for white light-emitting diode

Ca2BO3Cl：Ce3＋, Ca2BO3Cl：Tb3＋, and Ca2BO3Cl：Ce3＋, Tb3＋ phosphors are synthesized by a high temperature solid-state reaction. The emission intensity of Ce3＋ or Tb3＋ in Ca2BO3Cl is influenced by the Ce3＋ or Tb3＋ doping content, and the optimum concentrations of Ce3＋ and Tb3＋ are 0.03 tool and 0.05 mol, respectively. The concentration quenching effect of Ce3＋ or Tb3＋ in Ca2BO3Cl occurs, and the concentration quenching mechanism is d-d interaction for either Ce3＋ or Tb3＋. The Ca21303Cl：Ce3＋, Tb3＋ can produce colour emission from blue to green by properly tuning the relative ratio between Ce3＋ and Tb3＋, and the emission intensity of Tb3＋ in Ca2BO3Cl can be enhanced by the energy transfer from Ce3＋ to Tb3＋. The results indicate that Ca2BO3Cl：Ce3＋, Tb3＋ may be a promising double emission phosphor for UV-based white light emitting diodes.

氮氯共掺杂石墨烯量子点的合成及其对汞离子检测

以果糖、乙二胺、盐酸为原料,采用水热法将N、Cl原子掺杂在石墨烯量子点上,制备出氮氯共掺杂石墨烯量子点(N,Cl-GQDs),利用透射电镜、X射线光电子能谱、紫外-可见吸收光谱、荧光光谱等手段对其结构和性能进行了表征。结果表明:合成的N,Cl-GQDs为分散效果良好的球形,与单独氮掺杂及未掺杂的石墨烯量子点相比,双元素掺杂石墨烯量子点具有更好的光学性能。同时利用电化学发光淬灭原理构建了传感器,实现了对汞离子的检测,计算得出检测限为0.03ng/mL。

A novel white emitting phosphor Ca_2PO_4Cl:Dy^(3+): luminescence, concentration quenching and thermal stability

A novel white emitting phosphor Ca2PO4Cl：Dy^3＋ was synthesized by a solid state method. The luminescence, concentration quenching and thermal stability of Ca2PO4Cl：Dy^3＋ were investigated. Ca2PO4Cl：Dy^3＋ showed three emission peaks, which were located at 483, 575 and 660 nm. Though the ratio of yellow to blue emission intensities showed a similar value, the intensities of yellow and blue peaks were influenced by Dy^3＋ concentration, and the concentration quenching effect was observed. The emission intensity of Ca2PO4Cl：Dy^3＋ as a function of temperature was explored and the emission intensity（at 150 °C） of Ca2PO4Cl：Dy^3＋ was 90.0% of the value at 25 °C, and activation energy was 0.18 eV. The results indicated that Ca2PO4Cl：Dy^3＋ might be conducive to development of white LEDs.

溅射方法生长的氧化锌薄膜的阴极射线和光致发光特性

近紫外光发射氧化锌薄膜是一种新兴的发光材料 ,它的发光波长比氮化镓的蓝光波长更短 ,在光存储应用中可以进一步提高光存储的密度 ,因而在光电子领域具有重要应用价值而备受关注。在此介绍我们用直流反应溅射方法在硅衬底上生长的氧化锌薄膜 ,观察了它们的阴极射线发光和光致发光光谱 ,研究了发光与薄膜晶体结构 ,以及发光与激发电子束流的关系等。

塔里木盆地中-下奥陶统鹰山组层序地层格架中的成岩作用——以塔河地区和柯坪巴楚露头区为例

塔里木盆地中-下奥陶统鹰山组内幕储层的成因机制是当前油气勘探所关注的重点。以塔河地区钻井与柯坪巴楚露头为研究对象,利用岩石学与地球化学手段,对成岩作用在准层序、准层序组以及三级层序内的发育规律与演化特征展开研究。研究认为:沉积相带对成岩作用具有明显的控制作用,海水潜流成岩作用占据潮下带,潮间带则以海水潜流、渗流以及淡水潜流成岩作用为特征,潮上带以淡水渗流胶结物、同生期大气淡水溶蚀作用为特征;退积型准层序组,准层序顶部在海平面上升早期受大气淡水影响,海水成岩作用则在晚期主导旋回顶部;进积型准层序组,准层序在高水位早期以海水成岩作用为主,直至晚期顶部出现暴露;鹰山组下亚段三级层序,海平面上升期以同生期淡水成岩作用为特征,同时下倾方向胶结作用增加,高水位末期发育较弱的喀斯特;下亚段三级层序中的埋藏白云岩化作用发育强烈,云化流体以原生海水为主;上亚段三级层序在海泛面附近发育广泛海水胶结作用,快速的海侵使得同生期淡水成岩作用发育较弱,高水位期,受裂缝控制的表生溶蚀现象普遍存在。

西藏南部上三叠统郎杰学群物源分析

运用Dickinson三角图解、地球化学和阴极发光方法,对西藏山南琼结和贡嘎地区上三叠统深海—半深海郎杰学群砂岩和板岩进行了研究。碎屑成分和地球化学分析结果显示,物源总体来自再旋回造山带,含有大陆基块和混合区(切割弧)成分。阴极发光照射结果反映,物源区石英主要为变质成因(棕色光),次为深成/火山成因(浅紫兰色—绿色光),在一定程度上表明,母源区结晶基底可能已经抬升暴露,并且粘附在大陆块上。这些结果暗示,在拉萨地块与印度次大陆之间的新特提斯洋中可能存在一个含造山带的未名地块。