Eu3+掺杂GdPO4微晶玻璃的制备及其发光特性的研究

采用高温熔融法,制备了摩尔组分为53P2O5-16BaO-9Na2O-7K2O-14.25Gd2O3-0.75Eu2O3系统基质玻璃,熔化温度为1 400℃,经过热处理后获得微晶玻璃。采用X射线衍射(XRD)、扫描电镜(SEM)和荧光光谱,对微晶玻璃的结构、形貌和发光性能进行研究。XRD结果表明,基质玻璃经过700℃、800℃热处理2h得到Eu3+掺杂GdPO4微晶玻璃,其晶粒尺寸分别约为39nm和55nm;荧光光谱研究结果表明,与基质玻璃相比,微晶玻璃的激发强度和发射强度明显增强,微晶玻璃中源自Eu3+的7F0-5L6跃迁强度与电荷迁移带强度的比值降低,发射峰出现明显劈裂,且5D0-7F2与5D0-7F1跃迁强度的比值减小,表明Eu3+成功地进入了GdPO4晶相中。微晶玻璃中,Eu3+发射强度和激发强度随着热处理温度的升高而增强。     

Ho3+/Yb3+共掺的SiO2-Al2O3-BaO-BaF2微晶玻璃上转换发光研究

制备了Ho3+/Yb3+共掺的氧氟硅酸盐玻璃, 根据玻璃样品的差热分析进行微晶化处理, 测试了Ho3+/Yb3+共掺微晶玻璃的X射线衍射(XRD)图谱、吸收光谱和上转换发光光谱。结果发现, 在980 nm LD激发下, Ho3+/Yb3+共掺的含BaF2纳米晶的氧氟硅酸盐微晶玻璃可以同时观察到绿光(544 nm)和红光(656, 748 nm)上转换发光, 分别对应于Ho3+ 离子的5F4/5S2→5I8, 5F5→5I8和5F4/5S2→5I7能级跃迁, 与未热处理的玻璃样品相比, 微晶玻璃样品的绿光发光强度增强约347倍。研究结果表明含BaF2纳米晶的氧氟硅酸盐微晶玻璃是一种潜在的上转换基质材料。     

YAlO3∶Eu3+发光纳米纤维的制备与表征

采用静电纺丝技术制备了聚乙烯吡咯烷酮PVP/[Y(NO3)3+Al(NO3)3+Eu(NO3)3]复合纤维,将其进行热处理,得到了YAlO3:Eu3+发光纳米纤维。采用X射线衍射(XRD)、扫描电镜(SEM)、荧光光谱等技术对样品进行了表征。PVP/[Y(NO3)3+Al(NO3)3+Eu(NO3)3]复合纤维经1200℃焙烧2h后,获得了YAlO3:Eu3+纳米纤维,属于正交晶系,空间群为Pnma。用Shapiro-Wilk方法检验了纤维直径分布情况,在95%的置信度下,纤维直径属于正态分布。PVP/[Y(NO3)3+Al(NO3)3+Eu(NO3)3]复合纤维表面光滑,纤维分散性较好,有很好的长径比,尺寸均一,平均直径为(152.9±26.0)nm;YAlO3:Eu3+纳米纤维的平均直径为(106.7±20.2)nm。在234nm的紫外光激发下,YAlO3:Eu3+纳米纤维的主要发射峰位于590nm和609nm处,分别属于Eu3+的5 D0→7F1跃迁和5 D0→7F2跃迁,Eu3+掺杂离子浓度对YAlO3:Eu3+发射峰的峰型与位置均没有影响,当Eu3+掺杂离子浓度为5%时,YAlO3:Eu3+纳米纤维发光最强。     

Eu~(3+),Tb~(3+)共掺杂NaY(MoO_4)_2材料的制备及发光性能研究

采用水热法制备出NaY(MoO4)2:Eu3+,Tb3+下转换发光材料。通过X射线粉末衍射、红外光谱、荧光激发和发射光谱对其进行表征。讨论了不同反应温度及Eu3+掺杂浓度对NaY(MoO4)2:Eu3+,Tb3+的晶体结构和发光性能的影响,得到水热温度为180℃及Eu3+浓度为摩尔分数0.7%时,样品具有最佳的发光效果。在395nm光激发下,观察到了591nm处橙光发射峰以及616nm处强红光发射峰,分别对应于Eu3+的5D0→7F1和5D0→7F2跃迁。并研究了NaY(MoO4)2:Eu3+,Tb3+材料中Tb3+对Eu3+的敏化作用及能量传递过程。     

白光LED封装用Ce:YAG荧光微晶玻璃的研究

以CaO-Al2O3-SiO2-Y2O3玻璃作为基础玻璃(添加微量Ce),采用不同的热处理方法制备了白光LED荧光微晶玻璃。通过对比样品的测试数据,总结出了较为理想的热处理工艺。研究表明,采用整体析晶工艺,在1150℃、热处理1h,得到了主晶相为Ce:YAG的荧光微晶玻璃。其激发波长为462.2nm,发射波长为530.2nm,适合作为白光LED的封装材料。     

白光LED用红色荧光粉Sr0.7Ca0.3－2xMoO4:Eux3+Nax+的制备及发光性能研究

采用高温固相法合成白光LED用红色荧光粉Sr0.7Ca0.3-2 xMoO4Eux3+Nax+,对样品分别进行X射线衍射(XRD)分析和荧光光谱的测定,讨论了不同掺杂量下合成的荧光粉的发光性质。XRD图谱分析表明,在1 000℃下灼烧9h得到的样品为纯相的SrMoO4。研究结果表明,制备的Sr0.7Ca0.3-2 xMoO4:Eux3+Nax+荧光粉可以被近紫外光(393nm)和蓝光(464nm)有效激发;发射光谱中,在波长在611nm和615nm处有很强的发射峰,其中最强发射峰位于615nm左右,与Eu3+的5D0→7F2跃迁对应。进一步探讨Na+和Eu3+掺杂浓度对发光强度的影响,得出Sr0.7Ca0.3-2 x MoO4:Eux3+Nax+样品的发光强度比SrMoO4:Eu3+Na+增强,当掺杂量x=0.07时,Sr0.7Ca0.3-2 x MoO4:Eux3+Nax+样品在波长614nm处发光强度最强。最后测试计算样品在393nm紫外激发下的色坐标,当Eu3+和Na+的掺杂量x=0.02时,样品红色显示最强。研究结果表明,所合成的红色荧光粉Sr0.7Ca0.3-2 xMoO4:Eux3+Nax+新型红色荧光粉适合在白光LED中应用。     

新型红色荧光粉NaY（MoO4）2:Sm3+的制备及发光性能的研究

采用高温固相法制备了NaY(MoO4)2:Sm3+新型红色荧光粉,研究了Sm3+在NaY(MoO4)2基质中的发光特性。X射线衍射(XRD)测量结果表明,烧结温度为550℃时,制备的样品为纯相NaY(MoO4)2晶体。样品激发谱由两部分组成:220～340nm为电荷迁移带,峰值位于297nm;350～500nm的一系列线状峰为Sm3+的特征激发峰,最强峰位于403nm(6 H5/2→4 F7/2)。样品可被UV-LED管芯及蓝光激发。发射谱由564nm(4 G5/2→6 H5/2),600nm和607nm(4 G5/2→6 H7/2)、647nm(4 G5/2→6 H9/2)和708nm(4 G5/2→6 H11/2)4个峰组成,最强发射峰位于647nm(4 G5/2→6 H9/2),呈现红光发射。研究了不同Sm3+掺杂浓度对NaY1-X(MoO4)2:xSm3+材料发光强度的影响,X=0.05时出现浓度猝灭,分析表明,其猝灭机理是电偶极-电偶极的相互作用。     

Al3+/Eu2+共掺杂高硅氧玻璃的荧光特性

由纳米多孔玻璃制备了Al3+/Eu2+共掺杂的高硅氧玻璃,并研究了在纳米多孔玻璃基质中共掺杂Al3+离子对Eu2+离子450 nm处蓝色荧光强度和荧光峰位的影响。结果表明,共掺杂Al3+离子可分散多孔玻璃中丛聚的Eu2+离子,加之Al2O3较低的声子能量,使Eu2+离子的蓝色荧光发射显著增强;并且由于共掺杂的Al3+降低了Eu2+离子5d轨道劈裂幅度,随着Al3+离子含量的增加,Eu2+离子荧光峰蓝移。     

GdCOB:Eu~(3+)晶体的生长及其光谱性能研究

生长了新型激光晶体 Gd Ca4O( BO3) 3:Eu3+ (简称 Gd COB:Eu3+ ) ,测量了室温透过谱。确定了室温下 Eu3+ 在 Gd COB晶体中的能级结构。在 46 5 nm的 Ar3+ 离子激光泵浦下 ,测量了晶体 5 D0 → 7F1 ,2 跃迁和 5 D1 → 7F0 ,1 ,2 跃迁的荧光发射 ,揭示了晶体内部的多声子弛豫机制和能级跃迁途径     

退火气氛对稀土Eu3+掺杂ZnO薄膜结构和发光性质的影响

采用脉冲激光沉积(PLD)法在Si(111)衬底上制备稀土Eu3+掺杂ZnO薄膜材料,分别在纯氧和真空气氛中进行退火处理。XRD图谱中仅观察到尖锐的ZnO(002)衍射峰,表明ZnO:Eu3+,Li+薄膜具有良好的c轴取向。薄膜的结构参数显示：在纯氧气氛中退火的样品具有较大的晶粒尺寸且应力较小,表明在纯氧中退火的样品具有较好的结晶质量。通过光致发光谱发现,在纯氧中退火的样品的IUV/IDL比值较大,说明在纯氧中退火的样品缺陷去除更充分,结晶质量更好。当用395nm光激发样品时,仅发现Eu3+位于595nm附近的5D0→7F1磁偶极跃迁峰。并没有发现Eu3+在613 nm附近的特征波长发射,表明掺杂的Eu3+占据了ZnO基质反演对称中心格位。     

In0.52Al0.48As/In0.53Ga0.47As/In0.52Al0.48As abrupt double-heterojunction bipolar transistors

In0.52Al0.48As/In0.53Ga0.47As/In0.52Al0.48As n-p-n abrupt double-heterojunction bipolar transistors grown by molecular beam epitaxy (MBE) have been realized for the first time. DC current gains in excess of 300 have been measured on devices operated in the emitter-up configuration. DC current gains around 50 are obtained on device structures with Be+ implanted extrinsic base regions operated in the emitter-down configuration. The carrier injection and collection behavior of the abrupt InGaAs/InAlAs heterojunctions is discussed.     

Characteristics of metal-ferroelectric-insulator-semiconductor structure using Sr0.8Bi2.2Ta2O9 and Sr0.8Bi2.2Ta2O9-BaZrO3 for ferroelectric gates

Characteristics of BaZrO₃ (BZO) modified Sr_0.8Bi_2.2Ta₂O₉ (SBT) thin films fabricated by sol-gel method on HfO₂ coated Si substrates have been investigated in a metal-ferroelectric-insulator-semiconductor (MFIS) structure for potential use in a ferroelectric field effect transistor (FeFET) type memory. MFIS structures consisting of pure SBT and doped with 5 and 7 mol% BZO exhibited memory windows of 0.81, 0.82 and 0.95 V with gate voltage sweeps between −5 and +5 V, respectively. Leakage current density levels of 10⁻⁸ A/cm² for BZO doped SBT gate materials were observed and attributed to the metallic Bi on the surface as well as intrinsic defects and a porous film microstructure. The higher than expected leakage current is attributed to electron trapping/de-trapping, which reduces the data retention time and memory window. Further process improvements are expected to enhance the electronic properties of doped SBT for FeFET.     

Beat-frequency between measurements between C12O216and C12O218lasers

Several beat frequencies in the range below 6 GHz have been measured using a C¹²O2¹⁶laser and a C¹²O2¹⁸laser operating on several pairs of closely spaced lines in the 9.3-μm region.     

Some new FIR laser lines of optically pumped12CH316OH,12CH316OD, and12CH3I,12CH3Br,12CD2Cl2absorption spectroscopy of water and acetonitrile

The wavelength, polarization, and output power of several lines of the optically pumped CW FIR¹²CH3¹⁶OH (methanol) and¹²CH3¹⁶OD (1-D deuterated methanol), methyl iodide, methyl bromide, and deuterated methylene chloride lasers have been determined. In addition to lines already reported in the literature, seven strong lines have been observed. Optimum performance of the laser system is achieved by means of an improved coupling of the CO2pump power into the resonator and extraction of the FIR power from the resonator. Measurements on the power absorption coefficient of water using the laser indicate thatalpha(bar{nu})rises to almost 1100 Np ċ cm^-1at 170 cm^-1, and then shows a gradual fall with an increase in frequency. A strong temperature dependence of the 200 cm^-1peak inalpha(bar{nu})is predicted, with a decrease in the frequency of maximum power absorption coefficient with an increase in temperature. The range of measurements for acetonitrile is extended to lower frequencies so as to overlap with those determined from other millimeter wave techniques. For highly power-absorbing liquids,alpha(bar{nu})is estimated to be within ± 5 percent.     

Laser4F3/2→4I9/2and4F3/2→4I13/2transitions in KY(WO4)2:Nd3+

We report the observation of lasing at 0.9137 μm and 1.3545 μm in neodymium-doped KY(WO4)2at 77 K. Transition cross sections, fluorescent line width, and branching ratios are given.     

Al0.25In0.75P/Al0.48In0.52As/Ga0.35In 0.65As graded channelpseudomorphic HEMT's with high channel-breakdown voltage

A new Al_0.25In_0.75P/Al_0.48In_0.52 As/Ga_0.35In 0_.65As pseudomorphic HEMT where the InAs mole fraction of the Ga_1-xIn_xAs channel was graded (x=0.53→0.65→0.53) is described. The modification of the quantum well channel significantly improved breakdown characteristics. In addition, use of an Al_0.25In_0.75P Schottky layer increased the Schottky barrier height. Devices having 0.5 μm gate-length showed g_m of 520 mS/mm and I_max of 700 mA/mm. The gate-drain (BV_g-d) and source-drain (BV_d-s ) breakdown voltages were as high as -14 and 13 V, respectively. An f_T of 70 GHz and f_max of 90 GHz were obtained     

选频~(14)CO_2-~(12)CO_2同位素激光器

我们研制了一台~(14)CO_2-~(12)CO_2同位素激光器,测量到激光谱线80条,其中40条是~(14)CO_200°1-(10°0,02°0)_I带的激光跃迁谱线,强线输出功率达4.0W以上;实验还观察到同位素的竞争效应,发现即使~(14)CO_2成份低于~(12)CO_2,其激光辐射仍占优势.     

Waveguide In0.53Ga0.47As-In0.52Al0.48As avalanche photodiode

A high-speed waveguide In_0.53Ga_0.47As-In_0.52Al_0.48 As separate absorption, charge, and multiplication avalanche photodiode suitable for operation at 1.55 μm has been demonstrated, a unity-gain bandwidth of 27 GHz was achieved with a gain-bandwidth product of 120 GHz     

An In0.52Al0.48As/n+-In0.53Ga0.47As MISFET with a modulation-doped channel

A heterostructure metal-insulator-semiconductor field-effect transistor (MISFET) with a modulation-doped channel is proposed. In this device, a very thin undoped subchannel is located between the undoped wide-bandgap insulator and a thin heavily doped channel. In the depletion mode of operation, electron transport takes place along the heavily doped channel. When the device enters the accumulation mode of operation, electrons pile up against the heterointerface in the high-mobility undoped subchannel. This results in markedly improved transport characteristics at the onset of accumulation. The concept is demonstrated in the In_0.52Al_0.48As/In_0.53 Ga_0.47As system on InP. A 1.5-μm-gate-length MISFET shows a unity current-gain cutoff frequency of 37 GHz     

Temporal stability of circulating current in thin film Tl2Ba2CaCu2O8 and YBa2Cu3O7

The temporal stability of trapped transport current in annular thin film Tl₂Ba₂CaCu₂O₈ (TBCCO) and YBa₂Cu₃O₇ (YBCO) wafers has been accurately measured and has been found to be of suitable quality for the stringent requirements of nuclear magnetic resonance (NMR) magnets. No detectable decay, to the limit of the experimental apparatus (2*10^-14 Ω), was detected in those wafers with transport current at or below the critical current density J_c. The critical current density, as previously determined from 12 μm meander lines, was confirmed in a wafer with a width of 1.9 cm. The profile of trapped magnetic field resulting from induced current was modeled in order to assess its effect on the uniformity of an NMR magnet