Quadrupolar susceptibility of LiTmF4 crystal and the nature of forbidden 3H6(Γ2)-3F2(Γ2) transition

N. Altshuler, A. L. Larionov, M. P. Rodionova, A. Stolov
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Abstract

The narrow low intensity line with maximum at (lambda) -1 equals 15104 cm-1 and width (delta) equals 0.7 cm-1 at T equals 4.2 K have been detected in absorption spectrum of regular LiTmF4 crystal. The observed line belongs to transition form ground state 3H6((Gamma) 2) to lowest level (Gamma) 2 of 3F2 term of Tm3+(4f12) ion. The perturbation, which induces (Gamma) 2 - (Gamma) 2 transition, does not break S4 symmetry of Tm3+ sites. The perturbation of this kind is the interaction of Tm3+ 4f-electrons with electric field, created by quadrupolar moments of lattice ions, which are induced, int urn, by incident electromagnetic wave. To calculate the components of the quadrupolar moment tensors for ions in LiTmF4 single crystal, we have formulated and solved the system of self-consistent linear equations. We take into account interactions between all induced dipolar and quadrupolar moments and their interactions with electric fields of incident wave. The calculated transition probailities per second are in qualitative accordance with experimental data.
LiTmF4晶体的四极磁化率及禁止3H6(Γ2)-3F2(Γ2)转变的性质
在常规LiTmF4晶体的吸收光谱中,发现了在T = 4.2 K处最大λ = 1 = 15104 cm-1,宽度δ = 0.7 cm-1的窄弱谱线。观测线属于Tm3+(4f12)离子3F2项从基态3H6((Gamma) 2)到最低能级(Gamma) 2的跃迁。引起(Gamma) 2 - (Gamma) 2跃迁的扰动不会破坏Tm3+位的S4对称性。这种扰动是Tm3+ 4f电子与电场的相互作用,电场是由晶格离子的四极矩产生的,而晶格离子又由入射电磁波引起。为了计算litmt4单晶中离子的四极矩张量的分量,我们建立并求解了自洽线性方程组。我们考虑了所有感应偶极矩和四极矩之间的相互作用以及它们与入射波电场的相互作用。计算得到的每秒跃迁概率与实验数据基本一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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