掺铒TeO2-WO3玻璃光谱性能

研究了掺铒TeO2-WO3玻璃的吸收光谱和荧光光谱性质.根据吸收光谱,应用Judd-Ofelt理论计算得到了3个强度参数Ωt(t=2,4,6),分别为Ω2=5.38×10-20cm2,Ω4=1.78×10-20 cm2,Ω6=0.75×10-20cm2.Er3 离子在TeO2-WO3玻璃中的Ω6小于磷酸盐、氟磷酸盐中的Ω6,而大于锗酸盐、硅酸盐和碲酸盐玻璃中的Ω6,说明Er-O键在TeO2-WO3玻璃中的共价性大于磷酸盐、氟磷酸盐中Er-O键的共价性而小于锗酸盐、硅酸盐和碲酸盐玻璃中Er-O键的共价性.4I13/2→4I15/2荧光光谱表明Er3 的荧光半高宽(FWHM)为66 nm,荧光寿命为3.2 ms;应用McCumber理论计算了Er3 的峰值发射截面σe为8.0×10-21cm2.对Er3 在不同基质玻璃中光谱参数比较发现,TeO2-WO3玻璃的FWHM×σe乘积较大,说明其带宽特性较好.     

Tm3+掺杂的新型铋酸盐玻璃的制备与光谱特性

通过传统熔融法,分别制备了Tm3+单掺和Tm3+/Yb3+共掺的新型铋酸盐玻璃Li2O-SrO-ZnO-Bi2O3(LSZB),采用拉曼光谱、吸收光谱、荧光光谱对其进行了表征.应用Judd-Ofelt理论,计算了Judd-Ofelt参数Ωt(t=2,4,6),分别为Ω2=4.29×10-20 cm2,Ω4 =1.16×...     

掺Er~(3+)重金属氧氟硅酸盐玻璃的光谱性质与Judd-Ofelt理论分析

制备了掺Er3+重金属氧氟硅酸盐玻璃,研究了玻璃的吸收光谱和荧光光谱性质,应用Judd Ofelt理论计算了强度参数Ωt(t=2,4,6)、Er3+离子的振子强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数。应用McCumber理论,计算了能级4I13 2→4I15 2跃迁的受激发射截面。结果表明:掺Er3+重金属氧氟硅酸盐玻璃具有较宽的荧光半高宽和较大的受激发射截面。对Er3+离子在不同玻璃基质中带宽特性的比较发现,掺Er3+重金属氧氟硅酸盐玻璃的带宽特性与碲酸盐和铋酸盐玻璃相当,大于磷酸盐、锗酸盐和硅酸盐玻璃。     

LD泵浦的镱铒共掺磷酸盐玻璃的光谱性质和激光性质

制备了Er3+/Yb3+共掺磷酸盐玻璃。通过分析其吸收光谱,根据McCumber理论计算得到了Er3+离子在波长1533 nm处的峰值发射截面为0.84×10-20cm2,4I13/2能级的荧光寿命为8.5 ms。利用激光二极管作为泵浦源,成功地实现了Er3+/Yb3+共掺磷酸盐玻璃激光器的连续运转。在室温下,获得最大激光输出功率为80 mW,斜率效率为16.5%。     

新型掺铒铋酸盐玻璃上转换发光研究

制备了新型掺Er3 铋铅锶玻璃,研究了玻璃的吸收光谱和上转换光谱性质,应用Judd-Ofelt理论计算了铋铅锶玻璃的3个强度参量Ωt(t=2,4,6),分别为Ω2=3.27×10-20 cm2,Ω4=1.15×10-20cm2,Ω6=0.38×10-20 cm2.计算了Er3 离子的振子强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数.研究了上转换发光强度随泵浦激光功率的变化,上转换荧光525,546和657 nm曲线的斜率分别为1.86,1.88和1.85,表明红、绿光发射均为双光子吸收过程.     

Er~(3+)铋铅锶玻璃吸收光谱和上转换光谱

制备了新型掺Er3+铋铅锶玻璃,研究了玻璃的吸收光谱和上转换光谱性质,应用Judd-Ofelt理论计算了铋铅锶玻璃的3个强度参量Ωt(t=2,4,6),分别为Ω2=3·27×10-20cm2,Ω4=1.15×10-20cm2,Ω6=0.38×10-20cm2。计算了Er3+离子的振子强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数。研究了上转换发光强度随泵浦激光功率的变化,上转换荧光525,546和657nm曲线的斜率分别为1·86,1·88和1·85,表明红、绿光发射均为双光子吸收过程。     

Er^3＋／Yb^3＋：Sr3Y2（BO3）4晶体的光谱和激光性质

采用提拉法生长了双掺Yb3+和Er3+离子浓度分别为18.63%和0.87%(原子分数)的Sr3Y2(BO3)4晶体.利用测量的偏振吸收谱结合Judd-Ofeh理论,拟合得到了该晶体中Er3+离子的偏振和有效J-O参数.测量了Er3+离子4I13/2能级和Yb3+离子2F5/2能级的荧光衰减曲线,并计算了4I13/2能级的荧光量子效率和Yb3+到Er3+的能量传递效率.利用Fuchtbauer-Ladenberg公式计算了Er3+离子4I13/2→4I15/2跃迁的偏振受激发射截面.在平-凹谐振腔中,利用97nm波长光纤耦合准连续半导体激光端面泵浦1.12mm厚的该晶体,当输出镜透过率为1.5%时,获得了最大输出功率为1.3 w和斜率效率为20%的1560 nm附近的激光输出.结果表明,Er3+/Yb3+:Sr3+Y2+(BO3)4晶体是一种优良的1.5～1.6 μm波段激光的增益介质.     

Tm3+掺杂锗镓酸盐玻璃的2 μm中红外光谱特性

用高温熔融法制备了Tm2O2掺杂浓度分别为1.526%,3.006%,5.836%,11.028%,15.678%(质量分数,以下同)的65GeO2-12Ga2O3-10BaO-8Li2O-5La2O3(摩尔比)玻璃.从其吸收光谱特性出发,应用Judd-Ofelt理论,计算了Tm3+离子的J-O强度参数(Ω2,Ω4,Ω6)及Tm3+离子各激发态能级的自发跃迁几率、荧光分支比以及辐射寿命等光谱参量.在808 nm波长光的激发下,研究了不同Tm3+掺杂浓度玻璃在～1.47 μm与～1.8 μm的荧光特性,发现当Tm2O3掺杂浓度约达到～3.006%时,在1.8 μm处的荧光强度达最大;然后随着掺杂浓度的增大,其荧光强度反而降低.本文从Tm3+离子间的能量交叉弛豫效应与浓度猝灭效应解释了这一荧光强度变化的现象.同时,根据Mc-Cumber理论,计算了Tm3+离子能级3F4→3H6(1.8 μm)跃迁的吸收截面和受激发射截面,该荧光的受激发射截面峰值比氟锆铝酸盐玻璃大.由于该玻璃材料表现出较好的光谱性能,因此该材料可望成为～2.0 μm波段中红外光纤激光器的候选基质材料.     

Er3+单掺与Er3+/Yb3+双掺杂Bi2O3-GeO2-B2O3-ZnO玻璃的光谱研究

用高温融熔法制备了Er^3＋单掺与Er^3＋/Yb^3＋双掺杂的（60-x）Bi2O3-xGeO2-30B2O3-10ZnO （x=5,10, 20, 30）系统玻璃. 用差热曲线（DTA）研究了该玻璃系统的热稳定性. 结果表明, GeO2的掺入, 使得玻璃的软化温度与结晶起始温度的差增加, 玻璃的稳定性与料性增加. 测定了玻璃的吸收光谱. 应用McCumber理论计算了Er^3＋离子的受激发射截面及Er^3＋离子^4I13/2-^4I15/2发射光谱的荧光半高宽. 从吸收光谱特性出发, 应用J-O理论计算了玻璃中Er^3＋离子的强度参数（Ω2, Ω4, Ω6）, Er^3＋离子的自发跃迁几率、荧光分支比以及辐射寿命. 在970 nm波长的激发下, 研究了样品在红外波段的荧光光谱. Yb2O3的掺入, 大幅度地提高了970 nm波长的抽运效率以及在1.54 μm波段的发光强度.     

掺Er^3＋重金属氧氟硅酸盐玻璃的光谱性质与Judd—Ofelt理论分析

制备了掺Er^3 重金属氧氟硅酸盐玻璃，研究了玻璃的吸收光谱和荧光光谱性质，应用Judd-Ofelt理论计算了强度参数Ωt(t＝2，4，6)、Er^3 离子的振子强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数。应用McCCumber理论，计算了能级^413/2→^4I15/2跃迁的受激发射截面。结果表明：掺Er^3 重金属氧氟硅酸盐玻璃具有较宽的荧光半高宽和较大的受激发射截面。对Er^3 离子在不同玻璃基质中带宽特性的比较发现，掺Er^3 重金属氧氟硅酸盐玻璃的带宽特性与碲酸盐和铋酸盐玻璃相当，大于磷酸盐、锗酸盐和硅酸盐玻璃。     

Thermal stability, Judd-Ofelt theory analysis and spectroscopic properties of a new Er3+/Yb3+-codoped germano-tellurite glass

The Er3+/Yb3+-codoped 70TeO2-5Li2O-10B2O3-15GeO2 glass was prepared. The thermal stability, absorption spectra, emission spectra and up-conversion spectra were measured and investigated. The Judd-Ofelt analysis based on absorption spectra was performed in order to determine the Judd-Ofelt intensity parameters Omega(t) (t = 2, 4, 6), spontaneous emission probability, radiative lifetime and branching ratios of several Er3+ transitions. It was found that this studied glass has good thermal stability, broad fluorescence full width at half maximum (FWHM), large stimulated emission cross-section and strong up-conversion emissions at about 532, 546 and 659 nm, corresponding to the 2H(11/2)-->4I(15/2), 4S(3/2)-->4I(15/2) and 4F(9/2)-->4I(15/2) transitions of Er3+, respectively under the excitation at 970 nm. The results suggest that this Er3+/Yb3+-codoped germano-tellurite glass may be a potentially useful material for developing potential amplifiers and up-conversion optical devices.     

Optical-transition Probability of Tm^3＋ Ions in Tm^3＋／Er^3＋：YVO4 Crystal

1INTRODUCTIONThelasersoperatedataround2mmwavelengthhavegainedmuchinterestbecauseofvariousappli-cations,e.g.(1)groundorspaceremotesensingforLIDARandmetrology,(2)medicalapplicationssinceliquidwaterhasastrongabsorptionbandnear2mm,and(3)eyesafelaser[1,2].The2…     

Investigation of thermal stability and spectroscopic properties in Er3+/Yb3+ co-doped niobic tungsten tellurite glasses

A series of novel Er3+/Yb3+ co-doped 75TeO2-(25-x)Nb2O5-xWO3 (TNW: x=0, 3, 6, 9, 12, and 15 mol%) glasses have been prepared. Effect of WO3 on the thermal stability and spectroscopic properties of Er3+/Yb3+ co-doped niobic tellurite glasses have been investigated. With WO3 content increasing from 0 to 15 mol%, the fluorescence full width at half maximum (FWHM), the peak of stimulated emission cross-section (sigmaepeak), the measured lifetime (taum), and quantum efficiency (eta) change from 71 nm, 8.47x10(-21) cm2, 2.86 ms, 84.1% to 76 nm, 7.22x10(-21) cm2, 3.14 ms, 88.9%, respectively. The FWHM and sigmaepeak of Er3+ ions in different glass hosts were compared; the obtained data reveals that this new TNW4 glass may be a potentially useful candidate material host for broadband amplifiers.     

Spectral Parameters of Nd^3＋ inthe Nd^3＋：GdMgB5O10 Crystal

1 INTRODUCTION With the development of diode-pumped solid-statelasers, the search of more efficient materials for diode-pumped solid-state lasers is becoming more and moreimportant. The good laser materials should have thefeatures of large absorption coefficient and large ab-sorption line widths, as well as large emission crosssection at the emission wavelength. In the past years,a number of Nd3 -doped crystals, such as Nd3 :YVO4 , Nd3 :YAG[2], Nd3 :KLW[3] and Nd3 : [1]YAP…     

Growth and Spectral Characteristics of Yb3＋-doped LiGd（MoO4）2 Crystal

The Yb3+-doped LiGd(MoO4)2 crystal with the size up to Φ20×30 mm3 has been grown by Czochralski technique.The polarized room temperature absorption and emission spectra have been investigated.This crystal exhibits a broad absorption band centered at 975 nm with an FWHM of 43 and 59 nm for π-and σ-polarization,respectively,and the corresponding maximal absorption cross-sections are 3.36 and 2.42×10-20 cm2.The emission broadband has an FWHM of 47 and 54 nm for π-and σ-polarization,respectively,with the corresponding emission cross sections of 3.92 and 3.34 × 10-20 cm2 at 1020 nm.The measured fluorescence lifetime is 287 μs.     

Optical transitions of Er3+/Yb3+ codoped TeO2-WO3-Bi2O3 glass

Optical absorption and emission properties of the Er3+/Yb3+ codoped TeO2-WO3-Bi2O3 (TWB) glass has been investigated. The transition probabilities, excited state lifetimes, and the branching ratios have been predicted for Er3+ based on the Judd-Ofelt theory. The broad 1.5 microm fluorescence was observed under 970 nm excitation, and its full width at half maximum (FWHM) is 77 nm. The emission cross-section is calculated using the McCumber theory, and the peak emission cross-section is 1.03 x 10(-21) cm2 at 1.531 microm. This value is much larger than those of the silicate and phosphate glasses. Efficient green and weak red upconversion luminescence from Er3+ centers in the glass sample was observed at room temperature, and the upconversion excitation processes have been analyzed.     

Investigation of thermal stability and spectroscopic properties in Er3+/Yb3+-codoped TeO2-Li2O-B2O3-GeO2 glasses

The new Er3+/Yb3+ co-doped 70TeO2-5Li2O-(25-x)B2O3-xGeO2 (x = 0, 5, 10, 15 fand 20 mol.%) glasses were prepared. The thermal stability, absorption spectra, emission spectra and lifetime of the 4I(13/2) level of Er3+ ions were measured and studied. The FT-IR spectra were carried out in order to investigate the structure of local arrangements in glasses. It is found that the thermal stability, absorption cross-section of Yb3+, emission intensity and lifetime of the 4I(13/2) level of Er3+ increase with increasing GeO2 content in the glass composition, while the fluorescence width at half maximum (FWHM) at 1.5 um of Er3+ is about 70 nm. The obtained data suggest that this system glass can be used as a candidate host material for potential broadband optical amplifiers.     

Growth and Spectral Properties of Yb^3＋-doped Ba3Gd（BO3）3 Crystal

Crystal of Yb3+-doped Ba3Gd(BO3)3 has been grown by the Czochralski method. The spectroscopic characterizations have been investigated at room temperature. The Yb3+:Ba3Gd(BO3)3 crystal exhibits broad absorption at 976nm with FWHM of 7nm and large overall spitting of 2F7/2 manifold (823cm-1). The absorption and emission cross sections are 5.09×10-21cm2 at 976nm and 0.97×10-21cm2 at 1040nm,respectively. The fluorescence lifetime is 2.84 ms.     

Study of luminescence properties of novel Er3+ single-doped and Er3+/Yb3+ co-doped tellurite glasses

The novel Er(3+) single-doped and Er(3+)/Yb(3+) co-doped tellurite glasses were prepared. The effect of Yb(2)O(3) concentration on absorption spectra, emission spectra and upconversion spectra of glasses were measured and investigated. The emission intensity, fluorescence full width at half maximum (FWHM) and upconversion luminescence of Er(3+) go up with the increasing concentration of Yb(3+) ions. The maximum FWHM of (4)I(13/2) --> (4)I(15/2) transition of Er(3+) is approximate 77 nm for 1.41 x 10(21)ions/cm(3) concentration of Yb(3+)-doped glass. The visible upconversion emissions at about 532, 546 and 659 nm, corresponding to the (2)H(11/2) --> (4)I(15/2), (4)S(3/2) --> (4)I(15/2) and (4)F(9/2) --> (4)I(15/2) transitions of Er(3+), respectively, were simultaneously observed under the excitation at 970 nm. Subsequently, the possible upconversion mechanisms and important role of Yb(3+) on the green and red emissions were discussed and compared. The results demonstrate that this kind of tellurite glass may be a potentially useful material for developing potential amplifiers and upconversion optical devices.     

Spectral properties of Nd-doped BiB_3O_6 crystal

Transparent Nd : BiB3O6 crystal has been grown by top-seeded method. The refraction indices of the crystal were measured and the parameters of chromatic dispersion were fitted. The room temperature absorption spectra of the crystal have been measured and compared with that of 0.2 mol/L NdCI3 solution. According to Judd-Ofelt (JO) theory, the spectral strength parameters Ω2 = 0.1776×10-20 cm2, Ω4 = 0.1282×10-20 cm2 and Ω6 = 0.1357×10-20 cm2 of Nd3+ ion were fitted. The radiative transition probabilities AJ,(?), oscillator strengths fJ,(?), radiative lifetime T and the branching ratio β(?) have all been calculated. Based on these parameters, the properties and application perspective are discussed.