Determining the Parameters of the Jahn–Teller Effect in Impurity Centers from Ultrasonic Experiments: Application to the ZnSe : Ni2+ Crystal
- Authors: Sarychev M.N.1, Zhevstovskikh I.V.1,2, Averkiev N.S.3, Bersuker I.B.4, Gudkov V.V.1, Surikov V.T.5
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Affiliations:
- Ural Federal University Named after the First President of Russia B. N. Yeltsin
- Mikheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences
- Ioffe Institute
- Institute for Theoretical Chemistry, the University of Texas at Austin
- Institute of Solid State Chemistry, Ural Branch, Russian Academy of Sciences
- Issue: Vol 61, No 2 (2019)
- Pages: 180-186
- Section: Impurity Centers
- URL: https://bakhtiniada.ru/1063-7834/article/view/204837
- DOI: https://doi.org/10.1134/S1063783419020240
- ID: 204837
Cite item
Abstract
The earlier developed methodology of ultrasonic investigation for determining the parameters of the Jahn–Teller effect (JTE) in impurity centers in crystals is further developed in application to Ni2+ impurities in ZnSe : Ni2+. For all normal modes propagating along the [110] axis, the temperature dependences of the attenuation of ultrasound are measured in the frequency range 25–165 MHz. At a temperature of about 13 K, for all these modes, attenuation peaks are observed, which indicate the presence of local distortions of both trigonal and tetragonal types. Following the previously developed method, it is shown that these anomalies of attenuation are caused by the relaxation transitions between equivalent local distortions induced by the JTE at the Ni2+ centers. In the tetrahedral environment of selenium, this ion is in the threefold degenerate ground electron state 3T1, in which three types of the JTE can be realized. The data of ultrasonic experiments indicate the realization of the T ⊗ (e + t2) problem, in which the potential energy surface has four equivalent minima of the trigonal type, slightly deformed toward tetragonal saddle points. The trigonal vibronic constants, the stabilization energies of the trigonal minima, and the activation energy of the barriers between them are ev-aluated.
About the authors
M. N. Sarychev
Ural Federal University Named after the First President of Russia B. N. Yeltsin
Email: zhevstovskikh@imp.uran.ru
Russian Federation, Yekaterinburg, 620075
I. V. Zhevstovskikh
Ural Federal University Named after the First President of Russia B. N. Yeltsin; Mikheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences
Author for correspondence.
Email: zhevstovskikh@imp.uran.ru
Russian Federation, Yekaterinburg, 620075; Yekaterinburg, 620108
N. S. Averkiev
Ioffe Institute
Email: zhevstovskikh@imp.uran.ru
Russian Federation, St. Petersburg, 194021
I. B. Bersuker
Institute for Theoretical Chemistry, the University of Texas at Austin
Email: zhevstovskikh@imp.uran.ru
United States, Austin, Texas
V. V. Gudkov
Ural Federal University Named after the First President of Russia B. N. Yeltsin
Email: zhevstovskikh@imp.uran.ru
Russian Federation, Yekaterinburg, 620075
V. T. Surikov
Institute of Solid State Chemistry, Ural Branch, Russian Academy of Sciences
Email: zhevstovskikh@imp.uran.ru
Russian Federation, Yekaterinburg, 620990
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