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Optical studies of Cr$^{3+}$-Cr$^{2+}$ pair center in KZnF$_{3}$ crystal

机译:Cr $ ^ {3 +} $ - Cr $ ^ {2 +} $对中心的光学研究KZnF $ _ {3} $ crystal

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摘要

Optical absorption spectra of Cr$^{3+}$-Cr$^{2+}$ pair center inKZnF$_{3}$:Cr$^{3+}$,Cr$^{2+}$ crystal were investigated in wide temperaturerange. Broad band at 30800 cm$^{-1}$ is attributed to cation-cation(e_g)-electron transfer transition. Narrow lines with maxima at 16720 cm$^{-1}$and 19880 cm$^{-1}$ have been assigned to purely electronic exchange-inducedelectric-dipole transitions from the ground(Cr$^{3+}$,(^4A_{2g});Cr$^{2+}$,(^5E_g)) state to excited(Cr$^{3+}$,(^4A_{2g});Cr$^{2+}$,(^3E_g^a)) and(Cr$^{3+}$,(^4A_{2g});Cr$^{2+}$,(^3E_g^b)) states, respectively. It's vibronicsatellites corresponding to (a_{1g}) local mode of Cr$^{3+}$ fluorineoctahedron of the pair are also observed. Energy of the local mode for theground and mentioned excited states are 580, 540 and 530 cm$^{-1}$. Instead ofexpected double exchange for mixed valence pair ferromagnetic superexchange forCr$^{3+}$-Cr$^{2+}$ pair in KZnF$_{3}$ crystal is realized. Exchange integral(J=-14.9\pm0.4) cm$^{-1}$ and Jahn-Teller splitting (\Delta_{JT}=340\pm40)cm$^{-1}$ for the ground state of the pair were obtained by analysis of thetemperature dependence of absorption lines. Important features of the crossoverdouble exchange - ferromagnetic superexchange are discussed.
机译:Cr $ ^ {3 +} $-Cr $ ^ {2 +} $对中心在KZnF $ _ {3} $:Cr $ ^ {3 +} $,Cr $ ^ {2 +} $晶体中的光吸收光谱为在宽温度范围内进行了调查。 30800 cm $ ^ {-1} $的宽带归因于阳离子-阳离子(e_g)-电子转移跃迁。最大值为16720 cm $ ^ {-1} $和19880 cm $ ^ {-1} $的细线已分配给纯电子交换诱发的从地面起的电偶极跃迁(Cr $ ^ {3 +} $,( ^ 4A_ {2g}); Cr $ ^ {2 +} $,(^ 5E_g))状态为激发(Cr $ ^ {3 +} $,(^ 4A_ {2g}); Cr $ ^ {2 +} $ ,((^ 3E_g ^ a))和(Cr $ ^ {3 +} $,(^ 4A_ {2g}); Cr $ ^ {2 +} $,(^ 3E_g ^ b))状态。还观察到了与一对成对的Cr $ ^ {3 +} $氟八面体的(a_ {1g})局域模相对应的振动卫星。地面和提到的激发态的局部模式能量分别为580、540和530 cm $ ^ {-1} $。代替混合价对的预期双交换,实现了在KZnF $ _ {3} $晶体中对Cr $ ^ {3 +} $-Cr $ ^ {2 +} $对的铁磁超交换。将积分(J = -14.9 \ pm0.4)cm $ ^ {-1} $和Jahn-Teller分裂(\ Delta_ {JT} = 340 \ pm40)cm $ ^ {-1} $交换为基态通过分析吸收线对温度的依赖性获得了该对。讨论了交叉双交换的重要特征-铁磁超交换。

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