Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals

<p>Ge-doped Cd<sub>1-x</sub>Mn<sub>x</sub>Te (x = 0.02, 0.04, 0.08) crystals were grown by the Bridgman method. Carried out electrical measurements in the temperature range 280-420 K have found that the crystals’ hole conductivity is controlled by the deep compensated a...

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Main Authors: S. Solodin, Ye. Nikoniuk, G. Rarenko, P. Fochuk
Format: Article
Language:English
Published: Vasyl Stefanyk Precarpathian National University 2019-07-01
Series:Фізика і хімія твердого тіла
Subjects:
Online Access:http://journals.pu.if.ua/index.php/pcss/article/view/3832
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author S. Solodin
Ye. Nikoniuk
G. Rarenko
P. Fochuk
author_facet S. Solodin
Ye. Nikoniuk
G. Rarenko
P. Fochuk
author_sort S. Solodin
collection DOAJ
description <p>Ge-doped Cd<sub>1-x</sub>Mn<sub>x</sub>Te (x = 0.02, 0.04, 0.08) crystals were grown by the Bridgman method. Carried out electrical measurements in the temperature range 280-420 K have found that the crystals’ hole conductivity is controlled by the deep compensated acceptors, whose ionization energy (ε<sub>A</sub>) was increased with the content Mn (x) according to the relation ε<sub>A</sub> = 0.6 (1 + 2х) eV. At 300 K: ρ = (10<sup>8</sup>-10<sup>9</sup>) (Ohm´cm), R<sub>H</sub> = (5×10<sup>9</sup>-5×10<sup>10</sup>) cm<sup>3</sup>/C; mobility of current carriers ~ 50 cm<sup>2</sup>/(V´s).</p>
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spelling doaj.art-f6270d5335184e059c241eecb05dff302022-12-22T03:15:03ZengVasyl Stefanyk Precarpathian National UniversityФізика і хімія твердого тіла1729-44282309-85892019-07-0120214414810.15330/pcss.20.2.144-1483213Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystalsS. Solodin0Ye. Nikoniuk1G. Rarenko2P. Fochuk3Чернівецький національний університет ім. Юрія ФедьковичаNational University of Water Management and Nature ResourcesЧернівецький національний університет ім. Юрія ФедьковичаЧернівецький національний університет ім. Юрія Федьковича<p>Ge-doped Cd<sub>1-x</sub>Mn<sub>x</sub>Te (x = 0.02, 0.04, 0.08) crystals were grown by the Bridgman method. Carried out electrical measurements in the temperature range 280-420 K have found that the crystals’ hole conductivity is controlled by the deep compensated acceptors, whose ionization energy (ε<sub>A</sub>) was increased with the content Mn (x) according to the relation ε<sub>A</sub> = 0.6 (1 + 2х) eV. At 300 K: ρ = (10<sup>8</sup>-10<sup>9</sup>) (Ohm´cm), R<sub>H</sub> = (5×10<sup>9</sup>-5×10<sup>10</sup>) cm<sup>3</sup>/C; mobility of current carriers ~ 50 cm<sup>2</sup>/(V´s).</p>http://journals.pu.if.ua/index.php/pcss/article/view/3832cd1-xmnxteтверді розчиниелектричні властивостіефект холлагерманій
spellingShingle S. Solodin
Ye. Nikoniuk
G. Rarenko
P. Fochuk
Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals
Фізика і хімія твердого тіла
cd1-xmnxte
тверді розчини
електричні властивості
ефект холла
германій
title Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals
title_full Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals
title_fullStr Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals
title_full_unstemmed Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals
title_short Electro-physical properties of Ge-doped Cd1-xMnxTe (x <0,1) crystals
title_sort electro physical properties of ge doped cd1 xmnxte x 0 1 crystals
topic cd1-xmnxte
тверді розчини
електричні властивості
ефект холла
германій
url http://journals.pu.if.ua/index.php/pcss/article/view/3832
work_keys_str_mv AT ssolodin electrophysicalpropertiesofgedopedcd1xmnxtex01crystals
AT yenikoniuk electrophysicalpropertiesofgedopedcd1xmnxtex01crystals
AT grarenko electrophysicalpropertiesofgedopedcd1xmnxtex01crystals
AT pfochuk electrophysicalpropertiesofgedopedcd1xmnxtex01crystals