声子模式与电子-声子结合强度对Dy3＋掺杂硒化物玻璃荧光效率的影响

用熔融-淬冷法制备了无稀土掺杂与Dy3 (0.04m01%)掺杂Ge30Ga5Ses5和0.9Ge30Ga5Se65 0.1CsBr玻璃样品.采用Judd-Ofelt理论计算了0.9Ge30GasSe65 0.1CsBr玻璃样品中Dy3 跃迁的强度系数、自发辐射几率与荧光分支比.为了研究多声子弛豫(MPR)随温度的变化,测试了Dy抖的6H11/2能级在20～300K温度范围内的荧光寿命,分析了Ge30Ga5Se65玻璃中声子模式与电子-声子结合强度对Dy3 1.72μm处荧光强度和效率的影响.在硒化物玻璃中引入CsBr使玻璃中形成了Ga-Br键,有效声子能量降低到268cm-1.通过计算得到Ge30Ga5Se65与0.9GeaoGa5Se65 0.1CsBr样品的电子-声子结合强度分别为0.456与0.048.CsBr的引入降低了电子-声子结合强度.声子模式与电子-声子结合强度的改变决定了MPR的变化.     

真空蒸发法制备PbI2多晶薄膜研究

用真空蒸发法在玻璃衬底上制备了PbI2多晶薄膜,对样品的微结构、表面形貌、化学组分及电阻率进行了测试分析.结果表明,样品具有良好的多晶结构,并沿六角密堆积结构的c轴向高度择优取向.室温下样品暗电导率为3.09×10-11(Ω·cm)-1,电导激活能为0.78 eV.     

GeS_2-Ga_2S_3-AgCl玻璃的光学特性研究

采用熔融-淬冷法制备了摩尔组成为(100-x)(0.85GeS2-0.15Ga2S3)-xAgC l(x=0,5,10,15,20)硫卤玻璃,测试了样品的密度、转变温度、析晶温度、可见到中远红外透过光谱、吸收光谱以及折射率参数,根据Z-扫描测试原理用钛宝石飞秒激光器测试了样品的三阶非线性特性.利用经典的Tauc方程计算了样品光学带隙允许的直接跃迁、允许的间接跃迁及Urbach能量.讨论了玻璃的摩尔折射度、金属标准值、光学带隙、Urbach能量对玻璃样品折射率的影响.结果表明:该系统玻璃具有较宽光谱,从可见到中远红外透过区域(0.46~11.50)μm,可作为潜在的多光谱成像材料.随AgC l含量的增加,玻璃的折射率随着摩尔折射度增大而增大,金属标准值、光学带隙与Urbach能量有减小的趋势,而玻璃的三阶非线性性能得到明显提高.     

重金属氧化物玻璃中双光子吸收的研究

用传统熔融法制备了一系列高重金属氧化物(Bi2O3)含量的Bi2O3-B2O3-SiO2三元系统玻璃.用棱镜耦合仪测量了各个玻璃样品在632.8nm波长下的线性折射率n,结果表明玻璃的n值在1.9~2.1范围内且随着Bi2O3含量的增加而增大,其原因是由于Bi3+离子具有高极化率;用分光光度计测量了各个玻璃样品的线性吸收谱,结果表明玻璃的带隙Eopg值在2.229~2.268eV之间,且随Bi2O3含量的增加而减小.用开孔Z扫描实验测量了各个玻璃样品在770、800、850nm三个波长下的非线性吸收系数β,由于三个测量波长的光子能量hv(1.61,1.55,1.46eV)处于各个玻璃样品的带隙(Eopg)和半带隙(Eopg/2)之间,表明实验中的非线性吸收属于双光子吸收(TPA).实验结果表明:在3个测量波长下,Bi2O3含量最小的样品由于能隙状态的作用而体现出谐振型的TPA,其β值很高((3.6~6.1)×10-12m/W),说明其能应用在光限幅器中.另一方面,Bi2O3含量较高的样品只在770nm波长下才表现出微弱的非谐振类的TPA,并且β值随着Bi2O3含量的增加而增大,这表明它们在全光开光器(AOS)中有极高的应用潜力.     

用热分析方法对 AlF_3-MgF_2-CaF_2-SrF_2-BaF_2-RF_3(R=Y,Yb)玻璃析晶动力学的研究

在非等温加热过程中,用 DTA 方法列块状和粉末状40AlF_3-10MgF_2-30CaF_2-10SrF_2-10BaF_2-xRF_3(R=Y.Yb,x=0、5、10、15、20、25 mol.%)玻璃样品进行了测试。在比较各种玻璃析晶倾向时,发现块状样品的测试结果比粉末状的结果更合理。通过修正 Johnson—Mehl—Avraml 方程,求得析晶速率常数 k=vexp(-E/RT),比较各玻璃的 k(T)曲线,得出在加入15mol%YF_3或10mol%YbF_2时,40AlF_3-10MgF_2-30CaF_2-10SrF_2-10BaF_2的析晶倾向得到最有效的抑制的结论。     

白光LED用Ba_2LaF_7:Pr~(3+)微晶玻璃的发光性能研究

采用高温熔制法制备得到50SiO_2-10AlF_3-5TiO_2-30BaF_2-4La F_3-Pr_2O_3(mol%)基质玻璃,玻璃样品分别经640℃、660℃和690℃热处理后,成功获得透明Ba_2LaF_7:Pr~(3+)微晶玻璃且维持着较高的透明度。用XRD和TEM分析热处理前后样品的相变和结构变化,并研究了热处理前后样品的光谱特性。结果表明:玻璃经热处理后生成了Ba_2LaF_7微晶颗粒;热处理前后样品光谱特性的变化表明:热处理后掺杂的Pr~(3+)离子逐渐进入到Ba_2LaF_7晶格位;在波长443 nm的激发下,660℃热处理过的样品实现了白光输出,对应的三色坐标为(0.323,0.343)。     

镀银玻璃微球粉体的制备及应用

通过化学镀方法制得镀银玻璃微球粉体,并分别用扫描电镜(SEM)和透射电镜(TEM)和X射线衍射(XRD)对粉体进行了表征分析,以此为导电填料,制备了环氧树脂导电胶样品并测试其导电性能.电阻率可达3×10-3Ω·cm,可以替代纯金属粉体作为导电胶用导电填料使用.     

纳米晶Co0.8Fe2.2O4薄膜的室温和高温结构及磁性

采用溶胶-凝胶旋转包覆法在玻璃衬底上制备了CO0.8Fe2.2O4薄膜.用振动样品磁强计和X射线衍射仪对样品的磁性和结构进行了室温及高温原位测量;用X射线光电子能谱仪和原子力显微镜测量了样品的成分及表面形貌.室温测量结果表明,400%退火时,样品已生成单一的尖晶石相,随退火温度升高衍射峰增高.样品的晶粒尺寸较小(14.2～29.6 nm),有利于降低磁记录材料的晶界噪音.630%退火样品的矫顽力达到1.56 X 105A·m-1.高温原位测量发现,500%高温时线膨胀系数约为1.3 X 10-5K-1,显示样品结构的热稳定性非常好,适合于磁光记录过程.随温度升高,样品由亚铁磁性逐渐过渡到顺磁性.     

La掺杂对(Bi1.5Zn0.5)(Ti1.5Nb0.5)O7陶瓷组织和介电性能的影响

研究了La3+取代的(Bi1.5Zn0.5)(Ti1.5Nb0.5)O7基陶瓷(Bi1.5-xLaxZn0.5)(Ti1.5Nb0.5)O7(0.0≤x≤1 2,BLZNT)的结构与介电性能。采用传统的固相反应法制备了陶瓷样品,用XRD、SEM分析了样品的组织。在整个取代范围内,La3+取代的样品基本保持单一烧绿石相,稳定范围由容忍因子(RA/RB值)来确定;同时,随着La3+取代量的增加,晶胞常数先增后减。介电性能随结构变化而变化,其中介电性能为:ε=130～170,tanδ=～0.9×10-3(1MHz),并且掺杂La优化了BLZNT x样品高频端(>100kHz)的频谱特性。     

BaO-B_2O_3-SiO_2玻璃助剂中SiO_2对低温烧结PTCR陶瓷性能的影响

研究了氧化钡-氧化硼-氧化硅(BaO-B2O3-SiO2)玻璃助剂对Y掺杂BaTiO3陶瓷微观结构和PTCR特性的影响.微观结构分析表明.玻璃助荆中SiO2的含量能改变晶界相组成,影响样品的烧结特性和室温电阻率.实验结果表明,当含有5%SiO2(摩尔分数)的BaO-B2O3-SiO2玻璃助剂的添加量为3%(质量分数)时,在1050℃保温3h烧结的样品的室温电阻率为210Ω·cm,升阻比为3.5个数量级.     

CsCl Effected Ultrafast Third-order Optical Nonlinearities of GeS_2-Sb_2S_3 Chalcogenide Glasses

A series of alkali halide doped chalcohalide glasses (100?x)(0.9GeS2-0.1Sb2S3)-xCsCl (x=5, 10, 15 and 20 mole fraction) were prepared. The absorption spectra and Raman scatting spectra of these glasses were measured. The optical band gaps Eopt were obtained from ultraviolet absorption edges. Z-scan technique was utilized to investigate the third-order nonlinear optical properties of GeS2-Sb2S3-CsCl glasses. The value of Eopt increases and the third-order optical nonlinearity decreases with increasing CsCl c...     

Emission Properties of Yb3+/Er3+ Doped TeO2-WO3-ZnO Glasses for Broadband Optical Amplifiers

The YbS /Er3 doped TeO2-WO3-ZnO glasses were prepared. The absorption spectra, emission spectra and fluorescence lifetime of Era at 1.5μm, excited by 970 nm were measured. The influence of Er2Oa, Yb2Oa and Ohcontents on emission properties of Era at 1.5 μm was investigated. The optimum doping concentrations for Era and Yba is around 3.34× 1020 ions/cma and 6.63×1020 ions/cma, respectively. The peak emission cross section is 0.83～0.87 pm2. With the increasing concentration of Yba , the FWHM of Era emission at 1.5 μm in the glass increases from 77 nm to 83 nm. The results show that Yba /Era doped meO2-Woa-ZnO glasses are promising candidate for Era -doped broadband optical amplifier.     

掺铒铋酸盐玻璃光谱性质的混合形成体效应

测得了Er3+离子在铋酸盐玻璃系列(50～75)Bi2O3-(20～45)B2O3-5Na2O,70Bi2O3-(17～25)B2O3-xZrF4-5Na2O,70Bi2O3-(0～25)B2O3-(0～25)SiO2-5Na2O中的吸收光谱、荧光光谱及4I13/2能级荧光寿命.提出并研究了Er3+离子光谱性质的混合形成体效应,结果表明Er3+离子在铋酸盐玻璃中通过混合形成体效应可以获得较大的有效线宽(△λeff＝62～80nm)、较高的受激发射截面(σe＝0.76～0.84×10-20cm2)、较宽的荧光半高宽(FWHM＝55～80nm)以及较长的荧光寿命(τm＝1.6～4.3ms),说明掺Er3+铋酸盐玻璃是光纤放大器实现宽带和高增益放大较为理想的基质材料.     

含ZrF4氟铝酸盐玻璃研究

以10MgF_2-20CaF_2-10SrF_2-10BaF_2-15YF_3-35AlF_3(摩尔百分数)氟铝酸盐玻璃为基本组成,在玻璃中引入不同含量的ZrF_4,同时对其它组成进行适当调整,制得了厚度8mm无可见析晶的氟化物玻璃。利用差热分析(DTA)技术研究了ZrF_4对玻璃形成能力和玻璃析晶动力学的影响,结果表明,少量的ZrF_4可以提高玻璃的抗失透能力,过量的ZrF_4会降低玻璃形成能力;ZrF_4的最佳含量范围为7.3～11.4mol％。根据测得的玻璃的红外透过光谱显示,该玻璃具有良好的透红外光性能。     

Erbium-doped tellurite glasses with high quantum efficiency and broadband stimulated emission cross section at 1.5 μm

Optical transitions of Er³⁺ ion in two tellurite glasses of molar composition 75TeO₂:12ZnO:10Na₂O:2PbO:1Er₂O₃ and 75TeO₂:12ZnO:10Na₂O:2GeO₂:1Er₂O₃ were investigated. The measured absorption and emission spectra were analysed by Judd–Ofelt and McCumber theories, in order to obtain radiative transition rates and stimulated emission cross sections. It was found that these glasses have high and broadband absorption and stimulated emission cross sections at 1.5 μm. For the metastable ⁴I_13/2 level, by comparing the measured lifetime with the calculated radiative decay time, quantum efficiency higher than 80% was found.     

高声子能量氧化物对掺铒碲酸盐玻璃光谱性质的影响

在研制的Er3+/Ce3+共掺低声子能量碲酸盐玻璃(TeO2-Bi2O3-TiO2)中,分别引入高声子能量WO3、SiO2和B2O3氧化物组分,测试了玻璃样品400~1700 nm范围内的吸收光谱、1.53μm波段荧光谱、Er3+离子荧光寿命和拉曼光谱,结合McCumber理论计算了Er3+离子光谱参数.结果表明:高声子能量氧化物组分的引入,能使声子参与的Er3+/Ce3+离子间能量传递过程变得更为有效,增加了Er3+离子亚稳态能级4I13/2上粒子数积累,从而增强1.53μm波段荧光发射.另外,高声子能量氧化物组分的引入还可以增加荧光半高宽(FWHM)和带宽品质因子(σe×FWHM).研究结果对于获取具有优异光谱特性的掺Er3+光纤放大器(EDFA)的玻璃基质具有实际意义.     

Effects of Preparation and Heat-Treatment Conditions on the Optical Properties of Glasses Activated with CuInS2 and CuInS1.2Se0.8

CuInS₂- and CuInS_1.2Se_0.8-activated silicate glasses were prepared from starting charges containing various combinations of carbon (reductant), sulfur, and selenium, and their absorption spectra were measured before and after additional heat treatment. The introduction of carbon was shown to improve the optical properties of the glasses (optimal content, 2.0 wt %). Heat treatment has an insignificant effect on the absorption spectra of the glasses, because color centers are formed only during melt cooling.     

Optical properties of Tm3+-doped TeO2-WO3 glasses

Tm³⁺-doped TeO₂-WO₃ glasses have been prepared and their absorption spectra have been measured in the visible to IR (up to 7 μm) spectral region. Luminescence measurements have shown that the glasses have emission bands at 1.45 and 1.8 μm. An attempt was made to remove OH groups from the glasses using KBF₄ and an inert atmosphere during the glass preparation. The results demonstrate that a low OH content can be achieved only by combining these approaches. The 1.8-μm emission intensity in “dry” glass is a factor of 6 higher than that in the OH-containing glasses. The relevant Judd-Ofelt parameters have been calculated.     

Effect of radiation trapping on the emission properties of Er: I13/2 → I15/2 transition in oxide glasses

The effect of radiation trapping on the emission properties of Er³⁺-doped tellurite and phosphate glasses has been investigated as the function of sample thickness and doping concentration. It was found that radiation trapping exists generally in two glass matrices, even at low doping concentration (0.1 mol% Er₂O₃). The larger effect of radiation trapping in tellurite glasses compared with phosphate glasses is due to its larger emission cross-section at 1.5 μm band and the spectral overlap between the emission and absorption spectra of Er³⁺: ⁴I_13/2 ↔ ⁴I_15/2transition. Due to radiation trapping, the measured lifetime of the Er³⁺: ⁴I_13/2 level in tellurite glasses increases by about 11–37% with increasing the sample thickness at the different erbium doping concentration, while 6–17% for phosphate glasses. And the full-width at half maximum of fluorescence (FWHM) of Er³⁺: ⁴I_13/2 → ⁴I_15/2 transition in tellurite glasses increased by about 15–64% with increasing the sample thickness, while 11–55% for phosphate glasses. It caused a high overestimation on the figure of merits (FOM) for amplifier bandwidth (σ_e × FWHM).     

Luminescence performance of Eu<Superscript>3+</Superscript>-doped lead-free zinc phosphate glasses for red emission

In this study, the luminescence performance of zinc phosphate glasses containing Eu³⁺ ion with the chemical compositions (60–x)NH₄H₂PO₄-20ZnO-10BaF₂-10NaF–x Eu₂O₃ (where x = 0.2, 0.5, 1.0 and 1.5 mol%) has been studied. These glasses were characterized by several spectroscopic techniques at room temperature. All the glasses showed relatively broad fluorescence excitation and luminescence spectra. Luminescence spectra of these glasses exhibit characteristic emission of Eu³⁺ ion with an intense and most prominent red emission (614 nm), which is attributed to ⁵D₀ → ⁷F₂ transition. Judd-Ofelt (Ω₂, Ω₄) parameters have been evaluated from the luminescence intensity ratios of ⁵D₀ → ⁷F_J (where J = 2 and 4) to ⁵D₀ → ⁷F₁ transition. Using J-O parameters and excitation spectra, the radiative parameters are calculated for different Eu³⁺-doped glasses. Effect of γ-irradiation at fixed dose has been studied for all the Eu³⁺-doped glass matrices. The lifetimes of the excited level, ⁵D₀, have been measured experimentally through decay profiles. The colour chromaticity coordinates are calculated and represented in the chromaticity diagram for Eu³⁺-doped zinc phosphate glasses for all concentrations.