Vacancies in zinc selenide crystal investigated in ultrasonic experiment
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AVERKIEV, Nikita, BERSUKER, Isaac, GUDKOV, V., BARYSHNIKOV, Kirill, KOLIBABA, Gleb, ZHEVSTOVSKIKH, Irina, MAYAKIN, V., MONAKHOV, Andrey, NEDEOGLO, Dumitru, SARYCHEV, M., SURIKOV, V.. Vacancies in zinc selenide crystal investigated in ultrasonic experiment. In: Materials Science and Condensed Matter Physics, Ed. 7, 16-19 septembrie 2014, Chișinău. Chișinău, Republica Moldova: Institutul de Fizică Aplicată, 2014, Editia 7, p. 85.
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Materials Science and Condensed Matter Physics
Editia 7, 2014
Conferința "Materials Science and Condensed Matter Physics"
7, Chișinău, Moldova, 16-19 septembrie 2014

Vacancies in zinc selenide crystal investigated in ultrasonic experiment


Pag. 85-85

Averkiev Nikita1, Bersuker Isaac2, Gudkov V.34, Baryshnikov Kirill1, Kolibaba Gleb5, Zhevstovskikh Irina3, Mayakin V.3, Monakhov Andrey1, Nedeoglo Dumitru5, Sarychev M.3, Surikov V.6
 
1 Ioffe Physical-Technical Institute, RAS,
2 University of Texas at Austin,
3 Ural Federal University,
4 Russian Vocational Pedagogical University, Ekaterinburg,
5 Moldova State University,
6 Institute of Solid State Chemistry, Urals Branch of the Russian Academy of Sciences, Ekaterinburg
 
 
Disponibil în IBN: 26 februarie 2019


Rezumat

Anomalies in temperature dependences of attenuation and velocity of ultrasound have been found in ZnSe c1ystal made by the seeded physical vapor-transpo1i method in vacuum. The character of anomalies has been similar to ones observed in 3d impurity c1ystals in which the Jahn-Teller (IT) effect (JTE) [1] takes place. Our investigation has indicated the trigonal symmetiy of the local vibronic mode, meaning that the JT centers subject to T R e + t2 JTE problem. To detennine the impurity responsible for the anomalies, we have caITied out mass specti·oscopic investigation using an ELAN 9000 ICP-MS quadrnpole-based insti11ment (Perkin-Elmer SCIEX). It proved to be that detected 3d impurities that could lead to the JTE have much smaller concenti·ations to be studied in an ulti·asonic experiment. Therefore, we have considered vacancies VZn as the JT centers in this c1ystal. We have simulated the background attenuation ab = 0.0138xT 2 + 0.0126xT 4.