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The multiphoton ultraviolet and visible upconversion luminescence of ZBLAN material

机译:Zblan材料的多光子紫外和可见升高发光

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The multiphoton ultraviolet and visible upconversion luminescence of Tm~(3+)Yb~(3+) codoped ZBLAN fluoride glass as excited by a 975nm diode laser was studied. Two typical ultraviolet 290.6nm ~1I_6 → ~3H_6 and 362.0nm ~1D_2 → ~3H_6 upconversion luminescence lines were found. The careful measurement of the variation of upconversion luminescence intensity F as a function of the 975nm pumping laser power P has proven that the 290.6nm ~1I_6 → ~3H_6 and 362.0nm ~1D_2 →~3H_6 upconversion luminescences are a six-photon and a five-photon upconversion luminescence respectively. Several visible upconversion luminescence lines at 450.5nm, 473.9nm, 648.5nm, (687.3nm, 696.2nm) and (793.5nm, 800.7nm) were found also, which result from the fluorescence transitions of ~1D_2 →~3F_4, ~1G_4→~3H_6,~1G_4→~3F_4,~3F_3→~3H_6 and ~3H_4→~3H_6 of Tm~(3+) ion respectively. It has been proved that the upconversion luminescence of ~1G_4 state is a three-photon upconversion process, while that of ~3F_3 or~ 3H_4 state is a two-photon upconversion process. The theoretical analysis suggests that the upconversion mechanism of the 362.0nm ~1D_2→~3H_6 upconversion luminescence is the cross energy transfer of {~3H_4(Tm~(3+))→~3F_4(Tm~(3+)), ~1G_4(Tm~(3+))→~1D_2(Tm~(3+))} and {~1G_4(Tm~(3+))→~3F_4(Tm~(3+)), ~3H_4(Tm~(3+))→~1D_2(Tm~(3+))} between Tm~(3+) ions, whereas the mechanism of the 290.6nm ~1I_6→~ 3H_6 upconversion luminescence is the sequential energy transfer of {~2F_(5/2)(Yb~(3+))→~2F_(7/2)(Yb~(3+)), ~1D_2(Tm~(3+))→~3P_1(Tm~(3+))} and {~2F_(5/2)(Yb~(3+))→~2F(7/2)(Yb~(3+)), ~1D_2(Tm~(3+))→~3P_2(Tm~(3+))} from Yb~(3+) ions to Tm~(3+) ions. In addition, the upconversion luminescence of ~1G_4 and ~3H_4 state also results from the sequential energy transfer {~2F_(5/2)(Yb~(3+))→~2F_(7/2)(Yb~(3+)), ~3H_4(Tm~(3+))-VG_4(Tm~(3+))} and {~2F_(5/2)(Yb~(3+))→~2F_(7/2)(Yb~(3+)),~3F_4(Tm~(3+))→~3F_2(Tm~(3+))} from Yb~(3+) ions to Tm~(3+) ions respectively.
机译:研究了由975nm二极管激光器激发的Tm〜(3+)Yb〜(3+)Copoped Zblan氟化物玻璃的多光子紫外和可见升高发光。两个典型的紫外线290.6nm〜1i_6→〜3h_6和362.0nm〜1d_2→〜3h_6上转换发光线。仔细测量升高发光强度F的变化作为975nm泵浦激光功率P的函数已经证明了290.6nm〜1i_6→〜3h_6和362.0nm〜1d_2→〜3h_6上变发光是六光子和五个-photon上变频发光分别。还发现在450.5nm,473.9nm,648.5nm,(687.3nm,696.2nm)和(793.5nm,800.7nm)几个可见上转换发光线,其中从〜1D_2→〜3F_4,〜1G_4的荧光跃迁导致→ 〜3H_6,〜1G_4→〜3F_4,〜3F_3→〜3H_6和〜3H_4→〜3H_6的TM〜(3+)离子。已经证明,〜1G_4状态的上变频发光是三光子上升过程,而〜3F_3或〜3H_4状态的状态是双光子上升过程。理论分析表明,362.0nm〜1d_2→〜3h_6上变化发光的上变化机制是{〜3h_4(tm〜(3 +))→〜3f_4(tm〜(3+)),〜1g_4的交叉能量转移(tm〜(3 +))→〜1d_2(tm〜(3+))}和{〜1g_4(tm〜(3 +))→〜3f_4(tm〜(3+)),〜3h_4(tm〜( 3 +))→〜1d_2(tm〜(3+))} Tm〜(3+)离子之间,而290.6nm〜1i_6→〜3h_6的机制是{〜2f_的顺序能量转移(5 / 2)(Yb〜(3 +))→〜2f_(7/2)(Yb〜(3+)),〜1d_2(tm〜(3 +))→〜3p_1(tm〜(3+))}和{〜2f_(5/2)(Yb〜(3 +))→〜2f(7/2)(Yb〜(3+)),〜1d_2(tm〜(3 +))→〜3p_2(tm〜 (3 +))}从Yb〜(3+)离子到Tm〜(3+)离子。此外,〜1g_4和〜3H_4状态的上变发光也来自连续能量转移{〜2f_(5/2)(Yb〜(3 +))→〜2f_(7/2)(YB〜(3+ )),〜3H_4(TM〜(3 +)) - VG_4(TM〜(3+))}和{〜2F_(5/2)(YB〜(3 +))→〜2f_(7/2)( YB〜(3 +)),〜3F_4(TM〜(3 +))→〜3F_2(TM〜(3+))}从Yb〜(3+)离子分别为TM〜(3+)离子。

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