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Optical characterization, luminescence properties of Er~(3+) and Er~(3+)/Yb~(3+) co-doped tellurite glasses for broadband amplification

机译:Er〜(3+)和Er〜(3 +)/ Yb〜(3+)共掺杂碲酸盐玻璃的光学表征,发光特性

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In the present paper, optical absorption and emission spectra and luminescence decay lifetimes of different concentrations, 0.1, 0.3, 0.5, 0.7 and 1.0 mol% of Er~(3+) and 0.1Er~(3+)/0.5Yb~(3+) co-doped tellurite glasses (TeO_2-Bi_2O_3-ZnO-Nb_2O_5) were reported. Judd-Ofelt intensity parameters were determined and used to calculate spontaneous radiative transition probabilities (A_(rad)), radiative lifetimes (τ_R), branching ratios (P) and stimulated emission cross-sections (σ_P) for certain emission transitions. NIR emission at 1.5μm and up-conversion spectra of Er~(3+) and Er~(3+)Ab~(3+) co-doped tellurite glasses were measured under excitation wavelength of 980 nm. The absorption, emission and gain cross-sections for ~4I_(13/2)→~4I_(15/2) transition of Er~(3+) are determined. The peak emission cross-section of this transition is found to be higher (9.95×10~(-21) cm~2) for 0.1 mol% of Er~(3+) and lower (6.81×10~(-21) cm~2) for 1.0 mol% of Er~(3+) doped tellurite glasses, which is comparable to other oxide glasses. The larger peak emission cross-section for lower concentration of Er~(3+) is due to the high refractive index of glass matrix (2.1547), relation established from Judd-Ofelt theory. The observed full-widths at half maxima (FWHM) for lower and higher concentrations of Er~(3+) are 64nm and 96 ran respectively. The larger values of FWHM and peak emission cross-sections are potentially useful for optical amplification processes in the design of Erbium doped fiber amplifiers (EDFs). Under 980 nm excitation three strong up-conversion bands were observed at 530nm, 546nm and 665nm. The pump power dependent intensities and mechanisms involved in the up-conversion process have been studied. The luminescence decay profiles for ~4I_(13/2) level were reported for all glass matrices.
机译:本文分别研究了Er〜(3+)和0.1Er〜(3 +)/ 0.5Yb〜(3)浓度为0.1、0.3、0.5、0.7和1.0 mol%时不同浓度的光吸收和发射光谱以及发光衰减寿命。 +)共掺杂碲酸盐玻璃(TeO_2-Bi_2O_3-ZnO-Nb_2O_5)。确定Judd-Ofelt强度参数,并将其用于计算某些发射过渡的自发辐射过渡概率(A_(rad)),辐射寿命(τ_R),分支比(P)和受激发射横截面(σ_P)。在980nm的激发波长下测量了Er〜(3+)和Er〜(3+)Ab〜(3+)共掺杂碲酸盐玻璃在1.5μm处的近红外发射光谱和上转换光谱。确定了Er〜(3+)跃迁〜4I_(13/2)→〜4I_(15/2)的吸收,发射和增益截面。对于0.1mol%的Er〜(3+),此跃迁的发射峰横截面更高(9.95×10〜(-21)cm〜2)而更低(6.81×10〜(-21)cm) 〜2)掺入1.0 mol%的Er〜(3+)碲酸盐玻璃,与其他氧化物玻璃相当。 Er〜(3+)浓度较低时,较大的峰发射截面较大,这是由于玻璃基质的折射率较高(2.1547),这是根据Judd-Ofelt理论建立的。较低和较高浓度的Er〜(3+)的半峰全宽(FWHM)分别为64nm和96nm。 FWHM和峰值发射横截面的较大值可能对掺amplification光纤放大器(EDF)设计中的光学放大过程有用。在980nm激发下,在530nm,546nm和665nm处观察到三个强的上转换带。已经研究了与泵功率有关的强度和上转换过程中涉及的机理。报告了所有玻璃基质在〜4I_(13/2)水平下的发光衰减曲线。

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