Cr^3＋：LiCaA1F6晶体的缺陷

观察并分析了Ｃｒ＾３＋：ＬｉＣａＡ１Ｆ６晶体的缺陷,发现其中主要包括组分过冷、不定形固体颗粒和异相微晶颗粒等三类包裹体。此外,缺陷的宏观分布与生长方向有关。最后,讨论了缺陷的产生机理和消除途径。     

Sr_3Ga_2Ge_4O_（14）晶体中Cr~（3＋）和Cr~（4＋）吸收光谱

采用提拉法生长了掺Ｃｒ的Ｓｒ３Ｇａ２Ｇｅ４Ｏ１４低温石榴石结构型单晶，测量了它的吸收光谱及其偏振特性，系统描述了该晶体在可见和近红外波段各吸收带的特征，指出Ｃｒ在此晶体晶格中主要存在两种价态Ｃｒ３＋和Ｃｒ４＋，Ｃｒ４＋在近红外的吸收将影响到Ｃｒ３＋的发光。     

YAG晶体中Cr~（3＋）→Tm~（3＋），Er~（3＋）→Tm~（3＋）的能量

研究了加入敏化离子Ｃｒ３＋和Ｅｒ３＋的Ｔｍ：ＹＡＧ晶体的吸收谱和荧光谱，计算了Ｃｒ３＋、Ｅｒ３＋、Ｔｍ３＋离子的２Ｅ、４Ｉ１３／２、３Ｆ４能态的平均寿命及能量；转移效率、转移速率．得出Ｃｒ３＋→Ｔｍ３＋转移效率为８０％，转移速率为２．１×１０３ｓ－１．由（Ｅｒ，Ｔｍ）：ＹＡＧ的荧光谱可见存在Ｅｒ３＋→Ｔｍ３＋的有效的能量转移．讨论了Ｃｒ３＋→Ｔｍ３＋和Ｅｒ３＋→Ｔｍ３＋能量转移的不同．     

Er：YLF晶体中Er^3＋离子的光谱特征

利用居地－奥非脱（Ｊｕｄｄ－Ｏｆｅｌｔ）理论计算了Ｅｒ＾３＋离了在氟化钇锂（ＬｉＹＦ４简写为ＹＬＦ）晶体中的辐射跃迁几率Ａｊｊ无辐射跃迁几率ωＪＪ及激发态荧光寿命τ，并根据荧光动力学方程计算出各激发态布居数ＮＪ与掺杂浓度ｘ的关系，对２．７μｍ激光（＾４Ｉ１１／２→＾４Ｉ１３／２）来说，掺杂浓度要大于～３ａｔ％，才能实现布居数反转，对波长为１．７３μｍ的＾４Ｉ１３／２→＾４Ｉ１５／２跃迁，存在荧光强     

Cr,Ca：YAG晶体中四价Cr^4＋中心的晶场特性

综合分析了铬钙离子共掺钇铝石榴石晶体可见光－近红外区的室温吸收光谱,其中四配位和六配位的四价Ｃｒ＾２＋离子光谱成分是共存的,拟合得到的晶场参数符合光谱学的理论和实验规律,并且这两类Ｃｒ＾４＋中心的晶声性质均受到晶体中二价补偿离子Ｃａ＾２＋的影响。     

Cr^4＋：YAG晶体的激光态吸收研究

对Cr^4 ,YAG晶体作为1064nm激光的可饱和吸收体进行了研究,利用速率方程,描述了强激光下晶体的激光发态吸收（ESA）的动力学过程。用实验验证了所导出的光强与透过率的理论曲线,并因此论述了可以利用晶体的激发态吸收进行激光调Q,并对其进行优化。     

掺镁铌酸锂晶体的缺陷结构及其结晶化学分析

根据铌酸锂晶体本征缺陷的Ｌｉ空位模型,提出了掺镁铌酸锂晶体的缺陷结构模型;计算出了掺镁铌酸锂晶体中Ｌｉ_２Ｏ,Ｎｂ_２Ｏ₅的含量、［Ｌｉ］／［Ｎｂ］比以及晶体的密度随掺镁浓度的变化关系．计算结果与文献中报道的实验结果相符合关键词：     

LiNbO3晶体中Eu^3＋激发态的无辐射跃迁

测量了ＬｉＮｂＯ３：Ｅｕ＾３＋晶体的吸收、激发和发射光谱，较全面地确定了Ｅｕ＾３＋的能级位置，观测了该晶体的荧光发射强度随温度的变化，确定了Ｅｕ＾３＋在ＬｉＮｂＯ３晶体中的无辐射跃迁机理。     

高掺镁LiNbO3晶体折射率温度系数的表示式

推导了掺５ｍｏｌ％ＭｇＯ的ＬｉＮｂＯ３晶体折射率温度系数的表示式。利用这些表示式可以计算２９３～４２８Ｋ温度和０．５３９８μｍ～１．３４１４μｍ波长范围内的折射率温度系度，结果表明：计算值和实验值的最大相对偏差是１２％，用具有最大相对偏差的折射率温度系数的计算值，计算１．０７９５μｍ波长的非临界相位匹配温度，其值为３８２．４Ｋ，它与实验值仅差６Ｋ。因此，本文得到的表示式，对于采用这种晶体，设计在上     

Electronic structure and spectrum of Cr3+ in LiCaAlF6

The electronic structure and spectrum of Cr³⁺ in LiCaAlF₆ are investigated by using the discrete variatitional-local density functional (DV-LDF) method with embedded cluster model. The clusters (CrF₆)^3– withC ₃,D _3d andO _h point group symmetries embedded in the crystal are treated. The one-electron energy levels, densities of states, orbital populations, spin polarization splittings and energies of some terms are calculated. The results show that the relaxation of F^– ions around the Cr³⁺ impurity is inevitable, and that theD _3d andO _h (CrF₆)^3– clusters, with an extended bond-lengthR(Cr–F) chosen to be equal to 1.88 Å can represent this relaxation in a much better way. All the ligand-field transition energies, which are obtained from the transition-state energy and the Griffith parameters, as yielded by a restricted one-electron DV-LDF calculation, compare well with the experimental ones.     

Photoluminescence and Optical Absorption of Cs2NaScF6:Cr3+

The main objective of this paper is the characterization of the spectroscopic properties of new materials that are prospective laser media. This approach allows for the comparison of the properties of the Cr³⁺ in different environments. Here, we have studied the photoluminescence and optical absorption of Cs₂NaScF₆:Cr³⁺ single crystals. On the basis of near-infrared luminescence measurements at 2, 77, and 300 K the observed lines originated from the Cr³⁺-centres were associated with the transition and the lifetimes were obtained. In spite of the quenching observed as a function of temperature at least 10% of the 2 K emission intensity for Cs₂NaScF₆ doped with 1% of Cr³⁺ remains at room temperature. Besides, the 2 K emission broad band could be well described in terms of normal modes of the octahedral complex [CrF₆]³⁻, and the Racah and crystal-field parameters calculated.     

复合氟化物中缺陷对Eu2+光谱的影响

用传统的高温固相法及近几年兴起的温和水热法合成了KMgF3:Fu多晶粉末,同时用BridgmanStockbarger法生长了KMgF3:Eu单晶体。对三种方法合成的样品进行比较发现：水热和单晶样品中,除了Eu^2 的f→f锐线发射外,还观察到420nm处的宽带发射;这些发射带主要应归属于晶体中存在的色心和氧中心。而且与高温样品相比,Eu^2 在360nm处的线发射强度明显减小,原因是发生了Eu^2 到色心的能量传递。     

Time-resolved spectroscopy in LiCaAlF6 doped with Cr3+ as a function of pressure and temperature: Excited-state crossover and phase-transition effects

This work investigates phase transition (PT) and excited-state-crossover (ESCO) effects on the photoluminescence (PL) properties of LiCaAlF₆: Cr³⁺. The structural requirements for changing the Cr³⁺ PL behavior from a broad-band emission at 1.59 eV (781 nm) at ambient conditions, to ruby-like narrow-line emission at 1.87 eV (663 nm) are analyzed in the 0–35 GPa range. We report a PL study on LiCaAlF₆: Cr³⁺ by means of time-resolved emission as a function of pressure and temperature. In particular we focus on the PL variations occurring around the pressure-induced trigonal-to-monoclinic first-order PT in LiCaAlF₆ at 7 GPa.     

Er3+:Yb3+共掺杂氟氧混合物玻璃的上转换发光研究

制备了化学配方为 (5 0 -x)GeO2 ·PbF2 ·WO3·(6 +x)CdF2 ·1 4Yb2 O3·0 6Er2 O3(x =10 ,2 0 ,30 )氟氧混合物玻璃。研究了 930nm发光二极管激发下Er3+ :Yb3+ 共掺杂情形下的Er3+ 离子的上转换发光特性 ,观测到了Er3+ 离子中心波长位于 5 4 3,5 5 0和 6 5 5nm处的三个强荧光发射带。通过对样品的反斯托克斯喇曼光谱的测量 ,确定了基质的最大声子能量 ,在此基础上分析了上转换荧光的产生机制。利用基质的平均电负性差和平均阳离子场强这两个参数 ,讨论了基质材料中GeO2 和CdF2 含量的调整对上转换发光的影响。     

Flashlamp-pumped laser performance of LiCaAIF6:Cr3+

The results of flashlamp pumping of the LiCaAIF₆:Cr³⁺ (Cr:LiCAF) laser crystal are reported. We have so far obtained slope efficiencies as high as 1.55% in a close-coupled, diffusely reflecting cavity. Based on the measured insertion loss of the presently available material, we predict that an efficiency of about 4% will be obtained when low-loss material becomes available. This extrapolated efficiency is comparable with the performance of a high-quality alexandrite laser rod in the same apparatus.     

Vibrational Analysis of the Elpasolites Cs2NaAlF6 and Cs2NaGaF6 Doped with Cr3+ Ions by Fluorescence Spectroscopy

Interest in 3d transition metal impurities in ionic crystals has increased due to their important role in the laser activity of these materials. Moreover, recent advances in tunable solid-state lasers and high-power semiconductor laser diode arrays have generated a strong interest in investigating new compounds that emit in the visible and near-infrared spectral regions. In particular, many optical studies have been devoted to Cr³⁺-doped fluoride crystals as a consequence of the high quality of some Cr³⁺-based laser materials. In the present investigation, the low-temperature emission spectra of Cr³⁺ ions in the hexagonal elpasolites Cs₂NaAlF₆ and Cs₂NaGaF₆ have been measured. Each compound has two crystallographically inequivalent octahedral sites for the Al³⁺ and Ga³⁺ ions that can be occupied by Cr³⁺ ions. For both materials, the luminescence spectrum presents two zero-phonon lines accompanied by a well-defined vibrational structure. The different peaks of the emission broad band are described in terms of phonons of the lattice and normal modes of the octahedral complex [CrF₆]^3–. A detailed analysis of the vibrational structure observed leads to the conclusion that the ²E and ⁴T₂ excited states of the [CrF₆]^3– ion are displaced along the e_g and a_1g and probably the t_2g coordinates.     

YAG∶Cr3+ 晶体精细光谱结构研究

采用不同的晶体畸变模型，利用CDM(complete diagonalization method)方法对YAG∶Cr3+ 晶体的EPR参量进行了系统研究.通过计算结果对晶格畸变模型进行了分析.结果表明,在三角对称下，对杂质离子电荷与中心离子电荷相等的情况，不适合用杂质离子沿C3轴位移的模型来研究晶体的局域结构，而且由于基态和第一激发态的零场分裂都对局域结构微变非常敏感，因此仅由基态零场分裂来确定晶格局域结构是不可靠的.同时结果表明，Cr3+ 离子进入YAG晶体后，产生了Δθ=1.88°的三角畸变.从而成功统一地解释了YAG∶Cr3+ 晶体的EPR参量和精细光谱结构.     

Cr3+:GdAl3(BO3)4晶体生长和光谱特性的研究

采用顶部籽晶法从K2 Mo3 O10 B2 O3 助熔剂体系生长出尺寸为 30mm的Cr3 :GAB晶体 ,吸收谱测试表明 :Cr3 离子在晶体中有两个宽且强的吸收带及一个微弱的吸收线 ,两宽带中心的波长为 4 2 0和 5 95nm ,对应于 4A2 →4T1和4A2 →4T2 两个具有相同的总自旋能级之间的跃迁 ,在4A2 →4T2 吸收宽带的长波边缘处有个很小的吸收峰 ,其波长为 6 81nm ,对应于 4A2 → 2 E(R线 )的跃迁。荧光测试表明 :Cr3 :GdAl3 (BO3 ) 4(CGAB)晶体荧光宽带和一个较弱的荧光线峰并存 ,宽带范围为 6 5 0～ 85 0nm ,峰值波长为 72 3nm ,对应于4T2 → 2 E ,4A2 的联合能级跃迁 ,荧光线峰波长约为 70 0nm ,其强度较弱。计算了晶场强度和Racah参数 ,其中Dq/B =2 371,晶体属于中阶场介质。研究表明 ,CGAB晶体具备可调谐激光晶体的基本光谱要求 ,且有良好的物化性能 ,可以实现宽频带可调谐激光输出。它又具有较大的倍频系数 ,有望实现 35 0nm附近紫外的自倍频激光输出。     

Tb掺杂氟化铅晶体的发光特征

用非真空Bridgman方法制备了掺有Tb杂质的氟化铅（PbF2:Tb)晶体,闯杂浓度从0.008at.%至0.6at.%。在室温下测量了该晶体的吸收和发射光谱,发现该晶体在X－射线和紫外线激发下均能够发出比较强的荧光。FbF2:Tb晶体的光吸收起源于Tb^3 离子的4f-4f跃迁,而其光发射则源于Tb^3 离子的电子分别从其激发态^5D3和^5D4能级路迁到基态^7Fj(J=6,5,4,3,2)。 荧光强度随掺杂浓度的提高而提高,当Tb^3 离子浓度较低时,以^5D3→^7FJ跃迁发射为主,当Tb^3 离子浓度较高时,则以^5D4→^7FJ跃迁发射为主。在同一晶体中,发光强度随中心所占晶格位置的改变而改变,反映出Tb^3 离子在PbF2晶体中的分布具有分凝系数大于1的特征。推测Tb^3 离子在PbF2晶体中占据Pb格位,同时产生间隙F^-离子缺陷来平衡电价。