共查询到19条相似文献,搜索用时 30 毫秒
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采用高温固相法在1 400 ℃下经二次煅烧合成了橙红色荧光粉Ca3Y2-xSi3O12:xSm3+,研究了Sm3+离子掺杂浓度及助熔剂对荧光粉发光性能的影响。XRD结果显示,所合成的荧光粉的主晶相为Ca3Y2Si3O12。荧光光谱分析表明,Ca3Y2Si3O12:Sm3+硅酸盐荧光粉可以在320~500 nm范围内得到有效激发,并发射橙红光。在402 nm激发下,样品发射光谱中的主发射峰分别位于562 nm(4G5/2→6H5/2)、598 nm(4G5/2→6H7/2)和646 nm(4G5/2→6H9/2),其中598 nm处峰值最大。改变Sm3+离子掺杂浓度发现:荧光粉发光强度先增大后减小,最佳Sm3+掺杂量x(Sm3+)为5%,浓度猝灭机理为离子间的相互作用。讨论了几种助熔剂的影响,NH4F、CaF2和NaCl均降低荧光粉的发光强度,只有H3BO3能够显著增强样品的发光,其最佳掺杂质量分数为1%。 相似文献
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在Y3Ga5O12石榴石中,室温下采用紫外激光选择激发光谱研究了能量从Tb3+的5D3和5D4能级无辐射传递给Ce3+的2D3/2能级。实验结果符合Frster-IH直接无辐射传递理论。5D3(Tb3+)→2D3/2(Ce3+)能量传递是电偶-偶极子相互作用机理,其平均临界传递距离为R0=16.3?,而5D4(Tb3+)→2D3/2能量传递是起主导作用的电偶-偶极子相互作用,其平均临界传递距离为11.2?。在5D4的传递过程中,电偶-四极子相互作用也应予以考虑。
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采用柠檬酸燃烧法制备Er,Yb:(LaLu)2O3陶瓷粉体,用X射线衍射对其进行了物相鉴定,研究表明1 000℃时已经得到纯相的(LaLu)2O3。采用冷等静压-真空烧结法制备了Er,Yb:(LaLu)2O3和Er:(LaLu)2O3陶瓷,对陶瓷的结构和光谱性能进行了详细的研究,研究发现掺杂5% Yb3+和10% La3+样品的上转换发光强度与未掺Yb3+、La3+样品相比明显增大,根据上转换光谱显示较强发射峰位于564 nm和661 nm处,对应Er3+的4S3/2(2H11/2)→4I15/2能级跃迁和4F9/2→4I15/2能级跃迁,并讨论了Er3+-Yb3+的能量传递过程及其上转换发光机制。 相似文献
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激发态Na2与H2碰撞,使H2(V=3,J=3)得到布居,在H2和He总气压为800 Pa及温度为700 K的条件下,利用相干反斯托克斯拉曼散射(CARS)光谱技术研究了H2(3,3)与H2(He)间转动能量转移过程.改变CARS激光束与激发Na2的激光之间的延迟时间,测量He不同摩尔配比时H2(3,J)态CARS谱强度的时间演化,得到H2(3,3)的总弛豫速率系数分别为k3,3H2=(21士5)×10-3cm3·s-1和k3,3He=(5.6士1.6)×10-13cm3·s-1.测量H2(3,J)各转动态的相对CARS谱强度,由速率方程分析,得到H2(3,3)+H2→H2(3,J)+H2中,对于J=2,4,转移速率系数分别为(11±4)×10-13cm3·s-1和(8.2±3.1)×10-13cm3·s<sup>-1.在H2(3,3)+He→H2(3,J)+He中,对于J=2,4,转移速率系数分别为(3.1±1.2)×10-13cm3·s-1和(2.1士0.7)×1013cm3·s-1.对于H2(3,3),单量子弛豫|△J|=1约占该态总弛豫率的90%. 相似文献
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以Li2CO3、Nb2O5、TiO2和Eu2O3为原料,采用固相法制备Eu3+掺杂的5Li2CO3-1Nb2O5-5TiO2(LNT)发光介质陶瓷。通过密度、XRD和荧光光谱测试,对0.2%(质量分数)Eu2O3掺杂的陶瓷片进行性能表征。结果表明:1 120℃烧结致密的陶瓷片,其晶相结构为“M-相”与Li2TiO3两相复合构成;在400 nm的近紫外光激发下,样品有较强的橙光(592 nm)和红光(615 nm)发射,分别属于Eu3+的5D0→7F1的磁偶极跃迁和5D0→7F2的电偶极跃迁。 相似文献
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通过水热法合成了一例新颖的稀土钨多酸化合物H26(C2H8N2H2)K(H2O)[K(H2O)Nd8(H2O)2(W3O12)(SiW10O38)4]·18H2O 1。该化合物的不对称单元由两个[SiW10O38]12-通过一个{Nd4(H2O)12+}结构单元和W3O12连接而成。化合物1簇阴离子通过K离子连接成一维无限链,再通过氢键连接成二维平面结构。针对该化合物,做了一系列表征,测试了其二维相关红外光谱,并对其作了详细分析,结果说明化合物1簇阴离子振动偶极矩对磁... 相似文献
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以Tb4O7和Ga2O3(化学计量比为3: 5)、Ho2O3、Yb2O3为原料,其中Yb3+的掺杂浓度为8at.%,Ho3+的掺杂浓度分别为0.5at.%、1at.%、1.5at.%、2.0at.%,以碳酸氢铵为沉淀剂,在1 200 ℃下烧结10 h得到了Ho,Yb: Tb3Ga5O12(Ho,Yb: TGG)纳米粉体。对样品进行了XRD物相分析、热重-差热分析、红外光谱分析以及扫描电镜分析、上转换发射光谱分析。实验结果表明,温度为1 200 ℃下样品平均晶粒尺寸为38.10 nm。在泵浦源为980 nm激发下,Ho3+掺杂浓度为1.5at.%,Yb3+掺杂浓度为8at.%时,在红、绿、蓝波段范围内出现了明显的上转换发光现象,并对其形成机理进行了讨论。分析认为,Ho3+由激发态5S2,5F4向基态5I8跃迁,实现了绿光输出,而Ho3+由激发态5F5和5F3向基态5I8跃迁,分别实现了红光和蓝光输出。 相似文献
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按照50Nb2O5-(46-x)Y2O3-4Yb2O3-xTm2O3(x=0.1,0.2,0.5,1,2)的配比方式,采用高温固相法制备出了掺杂Tm3+/Yb3+的YNbO4晶体粉末。在980 nm红外光激发下,观测到波长为478,645,707 nm的上转换荧光,分别对应于Tm3+离子的1G4→3H6、1G4→3F4、3F3→3H6能级跃迁过程。利用上转换发射功率与980 nm激光器工作电流关系估算出跃迁过程吸收光子数目为2.72,2.69,2.01,从而确定出前两者为三光子吸收过程,最后一个对应于双光子吸收过程。运用Judd-Ofelt理论研究样品光谱特性,根据样品的吸收谱得到样品的谱线强度参数Ωt(t=2,4,6),进而得出理论振子强度及实验振子强度,二者均方根偏差δrms=1.299×10-7。计算了Tm3+离子向下能级跃迁的跃迁几率、跃迁分支比等参数。最后得出结论:(1)3F4能级寿命较长,适合作为上转换中间能级;(2)3H5能级寿命较长,且3H5→3H6跃迁分支比(96.46%)接近100%,可用于产生1 216 nm激光。 相似文献
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通过水解TiCl4制备了锐钛矿结构TiO2纳米粒子, 并用时间分辨荧光光谱研究了5(6)CFL(5(6)-Carboxyfluorescein, 简称5(6)CFL)染料敏化TiO2纳米粒子体系的光致电子转移动力学. 5(6)CFL染料敏化TiO2纳米粒子能形成电荷转移复合物, 这归因于染料分子的激发电子态波函数Ψ(D*)与电荷分离态波函数Ψ(D+ +e-)之间的耦合作用. 当激发5(6)CFL染料敏化TiO2纳米粒子体系时, 电子以两种不同方式注入TiO2纳米粒子导带: 第一, 通过5(6)CFL染料分子的激发态注入; 第二, 从电荷转移复合物(5(6)CFL/TiO2)直接注入. 时间分辨荧光光谱表明, 在水溶液中纯5(6)CFL染料的荧光以寿命为τ1=41 ps (74.4%) 和τ2=3.22 ns (25.6%) 的双e指数衰减, 而5(6)CFL染料敏化TiO2纳米粒子体系的荧光分别以时间常数为τ1=44 ps (90.4%), τ2=478 ps (8.6%) 和τ3=2.41 ns (1.0%) 的三e指数衰减. 本文的研究工作能够为染料敏化太阳能电池的光致电子转移机理提供有价值的参考. 相似文献
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Three different kinds of silanols, which include isolated silanol, silanol I (with the hydroxyl proton bonded to an oxygen atom in the adjacent layer) and silanol II (with the hydroxyl proton bonded to the non-bridging oxygen at the same silicon atom), are generated during the hydration process of SKS-6 (δ-Na2Si2O5). 1H–1H nuclear Overhauser enhancement spectroscopy reveals that the proton of silanol I has an effective chemical exchange or spin diffusion with the proton of hydrogen-bonded water, while the proton of silanol II is likely far away from the other proton-containing species. 29Si magic angle spinning, 1H→29Si CP/MAS NMR and 1H–29Si phase-modulated Lee–Goldburg decoupled correlation experiments demonstrate that the local environments of the silicon sites in the final hydrated sample are mainly composed of Q2 [(SiO)2Si(OH)O−Na+], Q3 [(SiO)3Si(OH) and (SiO)3SiO−Na+] and Q4 [Si(OSi)4] groups. 相似文献
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观测到一种以Tb3+-Er3+进行光谱转换的量子剪裁现象。一个高能紫外光子(Tb3+的7F6→5L1)被量子剪裁成两个低能光子:一个是近红外光子(Er3+的4I9/2→4I15/2),另一个是蓝色光子(Tb3+的5D4→7F6),它们两个 都可以被GaAs太阳能电池有效地吸收。量子剪裁效率高达188%,接近理论极限的200%。从Tb3+(5L1→ 5D4) 到Er3+(4I15/2→4I9/2)的能量传递的能量失配是237 cm-1,比NaYF4中的声子能400 cm-1小,能量传递是近共振的。Tb3+施主间的能量迁移可以近似地用扩散模型处理, 从Tb3+-Er3+对之间能量传递的初始过程发现,偶极-偶极相互作用占主导地位。 相似文献
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Proton and deutron NMR have been conducted to investigate the ionic motion in perfluorinated ionomer membranes from Dow Chemical (XUS) and DuPont (NafionR). Two proton relaxation peaks were found in the XUS specimen absorbed with H2O. The major (narrow) peak presented a spin-lattice relaxation time (T1) of 107 ms while the minor (broader) one gave much longer T1. While the former was attributed to the water molecules involved in restricted motion, the latter was expected to be associated with the protons located in the vicinity of the sulfonate groups. Similar to the previous results from the others, only a single peak was detected in NafionR in 1H spectra, indicating that the protons in the different environments were engaging rapid exchange within NMR time scale. In contrast to the inverse proportion dependence of the linewidth on the water sorption in NafionR, the major line of the XUS membrane exhibited insensitive linewidth dependence on the variation of H2O concentration. The difference was attributed to the existence of narrow breaths of the pores in XUS sample, such that free water contribution to the enhancement of proton mobility was limited. The 2H spectra of NafionR were found to possess a doublet, due to nuclear quadrupolar interaction. Dow (XUS) membrane treated in at 100% relative humidity (RH) D2O presented a single peak with the linewidth insensitive to the amount of heavy water absorbed. An additional rise emerged on the “shoulder” of this single peak when treated at 33% RH. It is concluded that XUS membrane does not provide strong hydrogen bonding to eliminate the rapid motion average over the nuclear quadrupole interaction. 相似文献
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采用共沉淀法制备了不同Eu3+掺杂浓度的CaWO4荧光粉材料.通过X射线衍射和场发射扫描电镜技术对样品的结构和形貌进行了表征.测量了各样品的激发光谱、发射光谱和荧光衰减曲线, 计算了各样品的部分Judd-Oflet (J-O)参数和5D_0 (Eu3+)能级量子效率,以及荧光粉的色坐标, 讨论了样品电荷迁移带相对强度、J-O参数、量子效率与掺杂浓度的依赖关系.对Eu3+掺杂的CaWO4 发光材料的光致发光性质的研究表明,在CaWO4: Eu3+中5D0→7F2跃迁的616~nm 红色发光能被394.5~nm和465~nm的激发光有效激发,具有近紫外(或蓝光)激发效率高和猝灭浓度大的优点, 有潜力成为高效的近紫外(或蓝光)激发白光发光二极管用红色荧光粉材料. 相似文献
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Jie Guan Stephen E. Dorris Uthamalingam Balachandran Meilin Liu 《Solid State Ionics》1998,110(3-4):303-310
Transport properties of SrCe0.95Y0.05O3−δ were studied by impedance spectroscopy and by measuring open-cell voltage (OCV) and gas permeation. Ionic transference numbers were determined by measuring the OCV of concentration cells and water vapor evolution of an O2/H2 fuel cell. We observed interfacial polarization on the basis of the I–V curves obtained by discharging a hydrogen concentration cell or an O2/H2 fuel cell. The observed high protonic conductivity (high proton and low oxide ion transference numbers) makes SrCe0.95Y0.05O3−δ a potential material for hydrogen separation. From proton conductivity measurements, under a given hydrogen partial pressure difference of 4%/0.488%, the hydrogen permeation rate (of a dense membrane with 0.11 cm in thickness) was calculated to be ≈0.072 cm3 (STP) cm−2 min−1 at 800°C, whereas the permeation rate calculated from short-circuit current measurements was ≈0.023 cm3 (STP) cm−2 min−1 at 800°C. The difference between calculated and observed permeation rates is probably due to interfacial polarization. 相似文献