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The structural and optical properties of neodymium doped lithium niobate and yttrium aluminum garnet single crystals

机译:掺钕铌酸锂和钇铝石榴石单晶的结构和光学性质

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摘要

A Neodymium doped Lithium Niobate (LiNbO3) single crystal of composition (48.6 - y) Li2CO3 + (51.4) Nb2O5 + (y) Nd2O3, (y = 0.5, y = 1.0) and a Neodymium doped Yttrium Aluminum Garnet (YAG) single crystal of composition (31 - y) Y2O3 + (69.0) Al2O3+ (y) Nd2O3, (y = 0.5, y = 1.0) were prepared by using Czochralski technique. The structural and optical properties of the crystals along the boule were investigated. The dopant concentration is varied along the crystal boule. The FTIR spectra of the Nd: LiNbO3 crystals show that there are slight to the peaks at peaks of 3243 cm-1 - 3251 cm-1 when the content of Nd2O3 is increased and this shows the existence of OH bond stretching. In addition, the presence of the IR band in the range of 3567 cm-1 - 3572 cm-1 shows that the OH bond is due to the defect of the crystals while fundamental stretching of OH groups can be assigned to a band in the range of 3846 cm-1 - 3866 cm-1. As for the Nd: YAG crystals, sharp peaks are observed at 698 cm-1 and 748 cm-1 which can be assigned to Y – O symmetrical stretching and Y – O asymmetrical stretching, respectively. The first peak shifts slightly from 698 cm-1- 699 cm-1 and the second peak from 748 cm-1 - 751 cm-1 as the content of Nd2O3 in the system is increased. In addition, a band in the range of 801 cm-1 - 803 cm-1 is assigned to Y – O bonds which have strong metal-oxygen stretching vibrations in tetrahedral arrangement. The IR peaks at 3290 cm-1 - 3369 cm-1 show the fundamental stretching of OH groups. The UV–Vis–NIR spectroscopy of Nd: LiNbO3 crystals show that the values of indirect optical band gaps lie between 2.78 eV to 2.57 eV and those of the direct optical band gaps are between 3.82 eV to 3.71 eV. The Urbach energy for the Nd: LiNbO3 crystal decreases from 0.69 eV to 0.48 eV. The UV–Vis–NIR spectroscopy of Nd: YAG crystals show that the values of indirect optical band gaps lie between 1.99 eV to 2.10 eV and those of the direct optical band gaps lie between 4.83 eV to 4.85 eV. The Urbach energy for the Nd: YAG crystal decreases from 2.44 eV to 2.09 eV. The change in band gaps is associated with the structural change occurring after the addition of Nd2O3 as the dopant in the crystal system. Luminescence spectra of Nd: LiNbO3 crystals show that there is a 2G9/2 ?4I9/2 transition corresponding to a green emission at 492 nm and a 2H11/2 ?4I9/2 transition corresponding to an orange emission at 621 nm. As for Nd: YAG crystals, there is a 2G11/2 ?4I9/2 transition corresponding to a blue emission at 449 nm and a 2G9/2 ?4I9/2 transition corresponding to a cyan emission at 490 nm. As a conclusion, the two crystal systems show that the increase of Nd2O3 dopant from 0.5% mol to 1.0% mol will contribute to the decrease of crystal defects.
机译:组成为(48.6-y)Li2CO3 +(51.4)Nb2O5 +(y)Nd2O3(y = 0.5,y = 1.0)的掺钕铌酸锂(LiNbO3)单晶和掺钕钇铝石榴石(YAG)单晶用Czochralski技术制备(31-y)Y 2 O 3 +(69.0)Al 2 O 3 +(y)Nd 2 O 3(y = 0.5,y = 1.0)。研究了沿晶块的晶体的结构和光学性质。掺杂剂浓度沿晶锭变化。 Nd:LiNbO3晶体的FTIR光谱表明,当Nd2O3的含量增加时,在3243 cm-1-3251 cm-1的峰处有轻微的峰,这表明存在OH键拉伸。此外,IR波段在3567 cm-1-3572 cm-1范围内的存在表明OH键是由于晶体缺陷造成的,而OH基团的基本拉伸可被指定为该范围内的波段。 3846 cm-1-3866 cm-1。对于Nd:YAG晶体,在698 cm-1和748 cm-1处观察到尖锐的峰,可以分别指定为Y-O对称拉伸和Y-O非对称拉伸。随着系统中Nd2O3含量的增加,第一个峰从698 cm-1- 699 cm-1发生微小变化,第二个峰从748 cm-1-751 cm-1发生变化。另外,在Y – O键上分配了801 cm-1-803 cm-1范围内的一个带,这些键在四面体排列中具有很强的金属-氧拉伸振动。 3290 cm-1-3369 cm-1处的IR峰显示了OH基团的基本伸展。 Nd:LiNbO3晶体的UV-Vis-NIR光谱表明,间接光学带隙的值在2.78 eV至2.57 eV之间,而直接光学带隙的值在3.82 eV至3.71 eV之间。 Nd:LiNbO3晶体的Urbach能量从0.69 eV降低到0.48 eV。 Nd:YAG晶体的UV-Vis-NIR光谱表明,间接光学带隙的值在1.99 eV至2.10 eV之间,而直接光学带隙的值在4.83 eV至4.85 eV之间。 Nd:YAG晶体的Urbach能量从2.44 eV降低到2.09 eV。带隙的变化与在晶体系统中添加Nd2O3作为掺杂剂后发生的结构变化有关。 Nd:LiNbO 3晶体的发光光谱表明,存在对应于492nm的绿色发射的2G9 / 2→4I9 / 2跃迁和对应于621nm的橙色发射的2H11 / 2→4I9 / 2跃迁。对于Nd:YAG晶体,存在对应于449nm的蓝色发射的2G11 /2λ4I9/ 2跃迁和对应于490nm的蓝绿色发射的2G9 /2λ4I9/ 2跃迁。综上所述,两种晶体体系均表明,Nd2O3掺杂剂从0.5%mol增加到1.0%mol将有助于减少晶体缺陷。

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