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1.
低温扩散Mn2+制备ZnSⅩⅣMn,Cu电致发光材料   总被引:4,自引:0,他引:4  
韦志仁  李志强 《发光学报》1997,18(4):283-285
研究了不同Mn的化合物掺杂在不同退火处理条件下对ZnSⅩⅣMn,CuACEL粉末的发光亮度的影响.在低温下扩散Mn2+掺杂的方法,有效降低了Mn盐中其它杂质对发光的影响,和直接高温法制备的ZnSⅩⅣMn,CuACEL材料相比,提高了材料的发光亮度.  相似文献   

2.
Mn2+, Pb2+共掺杂ZnS纳米材料制备及光致发光   总被引:1,自引:0,他引:1       下载免费PDF全文
徐扬子  胡鹤 《发光学报》2007,28(4):589-593
采用聚乙烯基吡咯烷酮(PVP)为表面包覆剂,在室温大气条件下的水溶液中制备了ZnS:Mn,Pb纳米晶。讨论了Mn2+和Pb2+掺杂量对ZnS纳米发光材料光致发光强度的影响,确定了Mn2+和Pb2+掺杂量相对于Zn2+的最佳的量的比,并对其发光机理进行了初步的探讨。  相似文献   

3.
李湘祁  张懿 《发光学报》2014,35(6):643-648
以MCM-41为硅源,在800~1 100℃下合成了Ba1.2Ca0.64SiO4:0.10Eu,0.06Mn荧光粉,研究了煅烧温度对荧光粉发光性能的影响。实验结果表明,Eu2+的蓝绿光发射带的强度与宽度随煅烧温度的升高先增大后减小,在1 000℃时强度达到最大。最大发射峰位随温度的升高而发生红移,由800℃和900℃时的450 nm移至1 000℃和1 100℃时的480 nm。Mn2+的红光发射起源于Eu2+发射光的激发,其强度随温度的升高而增大。与Mn2+发生能量传递作用的Eu2+主要位于10配位的M(1)格位。  相似文献   

4.
以葡萄糖为碳源、对苯二胺为氮源,一步水热法合成了新型双发射荧光碳量子点(GP-CQDs),对该GPCQDs的形貌及光谱特性进行了研究。实验发现,在单一波长λex=300 nm激发下,该GP-CQDs于348 nm和452nm处有双发射荧光信号。将MnO4-加入GP-CQDs溶液,GP-CQDs于452 nm处的荧光信号完全猝灭,而348 nm处的信号基本不变。于上述猝灭体系中继续加入S2-,其于425 nm处产生新的荧光发射峰,相较于GP-CQDs原452 nm处的荧光信号,发射峰位置发生蓝移,且发射峰强度随S2-的浓度增加线性增强,而348 nm处的信号无增敏现象。根据该现象,以425 nm处的荧光峰为响应信号、348 nm荧光峰为参比信号,可直接构建基于S2-测定的比率荧光传感探针。实验对该探针的构建条件及分析性能进行了优化,当S2-浓度在3.1×10-8~8.0×10-6mol/L范围...  相似文献   

5.
采用高温固相法制备了Ba9(Y2-xScx)(SiO4)6:Ce3+,Mn2+(x=0,0.5,1.0,1.5,2.0)样品。在该体系中,当Sc3+含量从x=0逐渐增加至x=2时,Ce3+的蓝光发射强度提高了1.7倍;同时,Mn2+的红光发射强度提高了1.9倍,显示了优良的红光特性。样品的发射光谱和漫反射光谱表明,Ce3+、Mn2+发射强度的增加与Ce3+吸收能力和Ce3+向Mn2+能量传递的提升有直接关系。研究了样品Ba9Sc2(SiO4)6:Ce3+,Mn2+的热稳定性。随着温度的升高,Mn2+的红光发射呈现先升后降的态势。当温度从室温升至488 K时,Mn2+发射强度仅下降至室温时的84%,表现出优良的热稳定性。高亮的红光发射和优良的热稳定性表明该荧光材料可为紫外基白光LED提供良好的红色光源。  相似文献   

6.
SrB4O7:Pr3+,Mn2+中的Pr→Mn能量传递   总被引:1,自引:0,他引:1       下载免费PDF全文
从能量传递的角度出发,利用同步辐射光源(德国HASYLAB实验室的SUPERLUMI实验站)对Pr3+和Mn2+掺杂的SrB4O7粉末样品进行了光谱研究.206nm激发下,在SrB4O7:Pr3+(0.1%,摩尔分数)样品中观察到了来自Pr3+离子1S0能级的光子级联发射.SrB4O7:Pr3+样品的发射谱与SrB4O7:Mn2+样品监测Mn2+离子640nm发射的激发谱在330~430nm的波长范围里存在显著的光谱重叠.这个光谱重叠有利于Pr3+→Mn2+的能量传递发生,从而将Pr3+离子级联发射中第一步不实用的紫外或近紫外光子转换为Mn2+的红光发射.双掺杂样品SrB4O7:Pr3+,Mn2+与单掺杂样品SrB4O7:Pr3+的发射谱比较揭示出Pr3+→Mn2+的能量传递的确存在,并且提供了一种传递效率的估算方法,表明通过“Pr3+-Mn2+”组合有可能获得量子效率大于1的高效真空紫外激发发光材料.  相似文献   

7.
王雪  田莲花 《发光学报》2011,32(11):1109-1114
采用高温固相法,制得一种新型荧光粉Na4Ca3(AlO2)10∶Eu2+,Mn2+。样品的结构和发光性质分别由X射线衍射谱和荧光光谱来表征。在Na4Ca3(AlO2)10∶Eu2+的激发光谱中出现了Eu2+的f-d跃迁吸收带;在发射光谱中,出现蓝光发射,峰值位于441 nm。当在Na4Ca3(AlO2)10∶Eu2+中掺杂Mn2+时,发生了Eu2+→Mn2+的能量传递,在542 nm处出现了Mn2+的发射峰。在Na4Ca3(AlO2)10∶Eu2+,Mn2+中,随着Mn2+浓度的增加,Eu2+粒子的发射强度减弱,而Mn2+粒子的发射强度增强,且Eu2+离子发射的衰减时间缩短,同时色度由蓝光移向白光。  相似文献   

8.
用融熔法制备分散有ZnS:Mn2+纳米晶的纳硼硅(Na2O-B2O3-SiO2)玻璃在不同温度、时间对样品进行退火处理,得到不同尺寸的纳米晶.研究了玻璃基质中ZnS:Mn2+纳米晶的EPR谱、微波功率饱和EPR谱及发射光谱,发现Mn2+有二种组态,即替位组态和间隙位组态.分析结果表明替位组态Mn2+及周围立方晶场的畸变程度直接影响光学发光特性.  相似文献   

9.
Cd3Al2Ge3O12:Mn2+锗酸盐石榴石光谱性质   总被引:1,自引:1,他引:0  
本文报道室温下Cd3Al2Ge3O12:Mn2+(简称CAGG:Mn2+)锗酸盐石榴石的漫反射光谱、激发和发射光谱.在UV光激发下,在CAGG中Mn2+离子发射强黄光,这是基质到Mn2+离子无辐射能量传递的结果.Mn2+的黄发射带是由一个弱的红带和一个强的绿带所组成.讨论了这两个Mn2+发射带的起因.  相似文献   

10.
用高温固相反应法合成了Ba2SiO4:xCe3+,yMn2+(x=0~0.2, y=0~0.15)荧光粉,研究了荧光粉的晶体结构和发光性质。在紫外光激发下,Ba2SiO4:xCe3+的发射光谱为位于384 nm附近的宽带。Ba2SiO4:Mn2+样品的发射光谱位于376 nm的宽带较强,红光发射极弱。在Ce3+和Mn2+共掺的Ba2SiO4:xCe3+,yMn2+样品中,位于606 nm附近的红光发射较强,来源于Mn2+4T1(4G)-6A1(6S)跃迁。这说明Ce3+离子将部分能量传递给了Mn2+离子,有效地敏化了Mn2+离子的发光。当Ce3+的摩尔分数为0.2、Mn2+的摩尔分数为0.075时,Ba2SiO4:xCe3+,yMn2+荧光粉位于606 nm的Mn2+的发射峰最强。  相似文献   

11.
We report a novel method of growing red luminescent (635 nm) Mn-doped CdS (CdS:Mn) nanoparticles capped by an inorganic shell of Mn(OH)2. CdSO4, Na2S2O3 and Mn(NO3)2 were used as the precursors, and thioglycerol (C3H8O2S) was employed as the capping agent and also the catalyst of the reaction. Using these materials resulted in very slow rate of the reaction and particles growth. The self-assembled one-pot process was performed at pH of 8 and Mn:Cd ratio of 10, and took about 10 days for completion. CdS:Mn nanoparticles are slowly formed in the first day of the process; however, the luminescence is weak. After 7 days, the solution turns white turbid through the formation of additional particles, which precipitate on the walls on the next day. At this stage, a relatively strong red luminescence at 635 nm appears from transparent solution of the CdS:Mn nanoparticles. The white deposit on the walls turns to dark-brown color and luminescence increases on the 9th day. Finally, the CdS:Mn nanoparticles agglomerate and precipitate out of the solution on 10th day. X-ray diffraction and optical spectroscopy showed crystalline phase CdS nanoparticles with an average size of 3.6 nm. We explain the luminescence enhancement based on the formation of a Mn(OH)2 shell on the surface of the CdS:Mn nanoparticles during the precipitation stage. This can passivate the S dangling bonds located on the particles surface. As the surface Cd sites are previously capped with thioglycerol molecules, a complete surface passivation is achieved and results in emergence of high-intensity luminescence.  相似文献   

12.
Un-doped and Mn-doped ZnO nanoparticles were successfully synthesized in an ethanolic solution by using a sol-gel method. Material properties of the samples dependence on preparation conditions and Mn concentrations were investigated while other parameters were controlled to ensure reproducibility. It was observed that the structural properties, particle size, band gap, photoluminescence intensity and wavelength of maximum intensity were influenced by the amount of Mn ions present in the precursor. The XRD spectra for ZnO nanoparticles show the entire peaks corresponding to the various planes of wurtzite ZnO, indicating a single phase. The diffraction peaks of doped samples are slightly shifted to lower angles with an increase in the Mn ion concentration, signifying the expansion of the lattice constants and increase in the band gap of ZnO. All the samples show the absorption in the visible region. The absorbance spectra show that the excitonic absorption peak shifts towards the lower wavelength side with the Mn-doped ZnO nanoparticles. The PL spectra of undoped ZnO consist of UV emission at 388 nm and broad visible emission at 560 nm with varying relative peak intensities. The doping of ZnO with Mn quenches significantly the green emission while UV luminescence is slightly affected.  相似文献   

13.
Green-light-emitting Zn2SiO4:Mn phosphor particles were synthesized by modified large-scale spray pyrolysis using a colloidal solution containing fumed silica particles. The particles had a fine size, filled morphology, spherical shape and non-aggregation characteristics even after post-treatment at 1150 °C. The luminescence characteristics of Zn2SiO4:Mn phosphor particles having spherical shape, such as brightness and decay time under VUV excitation light, were investigated as a function of Mn content. The luminescence intensity exhibits a maximum at 5 mol% Mn-doped powder. The decay time increases consistently with decreasing Mn content and more saturated color coordinates are obtained with the composition having 12 mol% Mn. As a consequence, the 10 mol% Mn-doped powder proved to provide a good combination of favorable luminance and acceptable decay time. The influence of post-treatment temperature on the decay time and photoluminescence characteristics of Zn2SiO4:Mn particles was also investigated. Particles post-treated at 1155 °C had the maximum photoluminescence intensity, which was identical to 113% that of the commercial product, and a comparable decay time of 5.8 ms. PACS 81.20.Rg; 78. 55.Hx; 78.40.Ha; 81.05.Hd; 81.40.Tv  相似文献   

14.
Zhang S  Liang H  Liu Y  Liu Y  Hou D  Zhang G  Shi J 《Optics letters》2012,37(13):2511-2513
A series of Zn(1-x)Mn(x)Al(2)O(4) (x=0.001~0.08) phosphors were synthesized by a traditional solid-state reaction route. Their photoluminescence under vacuum ultraviolet (VUV, energy E>50000 cm(-1), wavelength λ<200 nm) and cathodoluminescence under low-voltage electron beam excitation were evaluated. The luminescence decays were also measured. The intense green emission was observed with a peak at about 510 nm upon 172/147 nm excitation. The luminescence of optimum phosphor Zn(0.99)Mn(0.01)Al(2)O(4) (ZAM) was compared with that of commercial green phosphor Zn(2)SiO(4):Mn(2+) (ZSM). The maximum emission intensity of ZAM is larger than that of ZSM under 172/147 nm and low-voltage electron beam excitation. The values of chromaticity coordinates reveal the phosphors can evidently enlarge the tricolor gamut. The results show that the ZnAl(2)O(4):Mn(2+) phosphors may be considered as candidates for Hg-free lamps, plasma flat backlights, and field emission backlights for liquid crystal displays.  相似文献   

15.
许武  张新夷 《发光学报》1983,4(4):14-22
前一阶段我们比较系统地研究了ZnS:Mn2+,Sm3+材料中Mn2+中心和Sm3+中心之间的能量传递。通过测量ZnS:Mn2+、ZnS:Sm3+和ZnS:Mn2+,Sm3+三种材料的发射光谱、激发光谱、选择激发发光光谱,证实了Mn2+中心和Sm3+中心之间存在偶极—偶极相互作用的无辐射能量传递。为了进一步研究Mn2+中心和Sm3+中心之间的相互作用及其物理特点,我们又仔细测量了上述三种不同类型材料的分时光谱,这不仅可以更清楚地了解激发停止后Mn2+中心和Sm3+中心之间的相互作用,而且有效地解决了Mn2+中心发射光谱和Sm3+中心某些特征光谱线交叠引起的测量发光衰减的困难。  相似文献   

16.
This study has been carried out on the optical properties of polyvinyl-pyrrolidone (PVP), the energy transition process in nanocomposite of PVP capped ZnS:Mn nanocrystalline and the influence of the PVP concentration on the optical properties of the PVP capped ZnS:Mn nanocrystalline thin films synthesized by the wet chemical method. The microstructures of the samples were investigated by X-ray diffraction, the atomic absorption spectroscopy, and transmission electron microscopy. The results showed that the prepared samples belonged to the sphalerite structure with the average particle size of about 2–3 nm. The optical properties of samples are studied by measuring absorption, photoluminescence (PL) spectra and time-resolved PL spectra in the wavelength range from 200 to 700 nm at 300 K. From data of the absorption spectra, the absorption edge of PVP polymer was found about of 230 nm. The absorption edge of PVP capped ZnS:Mn nanoparticles shifted from 322 to 305 nm when the PVP concentration increases. The luminescence spectra of PVP showed a blue emission with peak maximum at 394 nm. The luminescence spectra of ZnS:Mn–PVP exhibits a blue emission with peak maximum at 437 nm and an orange–yellow emission of ion Mn2+ with peak maximum at 600 nm. While the PVP coating did not affect the microstructure of ZnS:Mn nanomaterial, the PL spectra of the PVP capped ZnS:Mn samples were found to be affected strongly by the PVP concentration.  相似文献   

17.
The emission spectra both of fluorescence at room temperature and at 520 K and of thermostimulated luminescence (TSL) of multicomponent alumino-phosphate glasses with various Mn concentration (0·2–20mol%) has been measured. The colour of fluorescence and TSL changes from orange to yellow with increasing temperature at constant concentration of Mn and from yellow to red with increasing concentration at constant temperature. The colour shift with temperature can be explained by means of decreasing field strength, Dq with increasing distance Mn-O. The intensity of orange fluorescence at R.T. increases with increasing concentration up to about 5% Mn and then decreases in consequence of concentration quenching. On the contrary, the TSL intensity reaches its maximum at concentraction of about one order of magnitude smaller. The different behaviour of fluorescence and TSL intensity in dependence on Mn is probably due to their different elementar mechanisms.  相似文献   

18.
吕文选  史其武 《发光学报》1992,13(4):355-362
Mn2+浓度C(0.5%,0.6%)相同,而煅烧温度不同的DCEL ZnS:Mn、Cu粉未样品的EPR谱是不同的.用微机模拟EPR谱,计算出Mn2+团所占Mn2+的比例Cc/C.煅烧温度低于950℃时,Mn2+团比例随锻烧温度升高而减少,煅烧温度高于950℃时,六角晶相比例和Mn2+团比例同时随锻烧温度的升高而增加.分析表明,六角晶相有利于Mn2+间的间接电子自旋交换作用,在相同的掺Mn、Cu浓度条件下,对比立方晶相,它将使更多的Mn2+形成团,使材料的发光亮度降低.文中还讨论了锻烧DCEL ZnS:Mn、Cu材料的最佳温度问题.  相似文献   

19.
采用溶胶凝胶燃烧合成法制备了稀土掺杂Y2O3粉体,考察了煅烧温度、Er3+浓度和Yb3+浓度对粉体发光性能的影响。研究结果表明,在800℃的温度下可以得到结晶良好的单相Y2O3粉体;随着煅烧温度的升高,样品结晶度越高,其上转换发光强度变强;在900℃的煅烧温度下,样品的粒径大约为lμm左右,颗粒尺寸分布较均匀;当Er3+掺杂浓度达到1mol%时,绿光发射强度达到最大值,而对于红光发射,其发射强度的最大值出现在4mol%的掺杂浓度;当Yb3+与Er3+掺杂比例达到4:1时,绿光发射强度达到最大值,而红光发射强度随着Yb3+浓度的增加一直增强。  相似文献   

20.
An investigation is made of the chemiluminescence (luminol-dependent and spontaneous) of aqueous solutions of NaNO2 and H2O2 in the pH range of 4.0–9.0. In the presence of luminol at pH>7 the initiator of luminescence is H2O2. At pH<7 the luminescence revealed seems to be initiated by peroxynitric acid (HOONO) produced by the interaction of NaNO2 with H2O2 in weakly acid and acid solutions. Cysteine added to the solution prior to introducing H2O2 completely suppresses luminescence development in the pH range investigated. Moreover, cysteine quenches the luminescence already developed. Mannite and ethanol do not exert a substantial influence on the development of the luminescence. The solution of NaNO2 and H2O2 is also characterized by spontaneous chemiluminescence, the intensity of which is one-two orders of magnitude lower than that of the luminol-dependent chemiluminescence. The intensity of the spontaneous chemiluminescence of the solutions of NaNO2 and H2O attains its maximum in the pH region of 6.5 to 7.0. It is assumed that the revealed spontaneous luminescence of the solutions of NaNO2 and H2O2 is also attributable to formation of peroxynitrit acid in an activated state (HOONO*). Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 66, No. 3, pp. 436–440, May–June, 1999.  相似文献   

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