High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇

Acoustic properties (ultrasound velocity and attenuation) and magnetostriction were measured in pulsed fields up to 60 T applied along the c axis of Tm₂Co₁₇ single crystal. Similar to Er₂Co₁₇, the transition in Tm₂Co₁₇ is accompanied by clear anomalies in the sound velocity. The observed 0.3% jump o...

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Дата:2018
Автори: Andreev, A.V., Zvyagin, A.A., Skourski, Y., Yasin, S., Zherlitsyn, S.
Формат: Стаття
Мова:English
Опубліковано: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2018
Назва видання:Физика низких температур
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Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/176230
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:High-field magnetoelasticity of Tm₂Co₁₇ and comparison with Er₂Co₁₇ / A.V. Andreev, A.A. Zvyagin, Y. Skourski, S. Yasin, S. Zherlitsyn // Физика низких температур. — 2018. — Т. 44, № 11. — С. 1575-1580. — Бібліогр.: 16 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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spelling irk-123456789-1762302021-02-05T01:26:06Z High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇ Andreev, A.V. Zvyagin, A.A. Skourski, Y. Yasin, S. Zherlitsyn, S. Специальный выпуск К 80-летию со дня рождения А.И. Звягина Acoustic properties (ultrasound velocity and attenuation) and magnetostriction were measured in pulsed fields up to 60 T applied along the c axis of Tm₂Co₁₇ single crystal. Similar to Er₂Co₁₇, the transition in Tm₂Co₁₇ is accompanied by clear anomalies in the sound velocity. The observed 0.3% jump of the sound velocity at the transition is negative in Tm₂Co₁₇, whereas it is positive in Er₂Co₁₇. The magnetostriction at the transition also differs very much from that in Er₂Co₁₇. In Tm₂Co₁₇, the transition is accompanied by a smooth minimum of 0.15·10–4 in longitudinal magnetostriction whereas in Er₂Co₁₇ by a very sharp expansion of much largermagnitude (1.2·10–4). In the transverse mode, the effect in Tm₂Co₁₇ looks as very broad minimum of low amplitude (< 0.1·10–4) whereas in Er₂Co₁₇ as very sharp and large shrinkage (2.6·10–4). Thus, both themagnetoacoustics and magnetostriction are rather different in Tm₂Co₁₇ and Er₂Co₁₇. This supports different nature of the field-induced transitions in these compounds. 2018 Article High-field magnetoelasticity of Tm₂Co₁₇ and comparison with Er₂Co₁₇ / A.V. Andreev, A.A. Zvyagin, Y. Skourski, S. Yasin, S. Zherlitsyn // Физика низких температур. — 2018. — Т. 44, № 11. — С. 1575-1580. — Бібліогр.: 16 назв. — англ. 0132-6414 PACS: 62.65.+k, 75.47.Np, 75.80.+q http://dspace.nbuv.gov.ua/handle/123456789/176230 en Физика низких температур Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Специальный выпуск К 80-летию со дня рождения А.И. Звягина
Специальный выпуск К 80-летию со дня рождения А.И. Звягина
spellingShingle Специальный выпуск К 80-летию со дня рождения А.И. Звягина
Специальный выпуск К 80-летию со дня рождения А.И. Звягина
Andreev, A.V.
Zvyagin, A.A.
Skourski, Y.
Yasin, S.
Zherlitsyn, S.
High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇
Физика низких температур
description Acoustic properties (ultrasound velocity and attenuation) and magnetostriction were measured in pulsed fields up to 60 T applied along the c axis of Tm₂Co₁₇ single crystal. Similar to Er₂Co₁₇, the transition in Tm₂Co₁₇ is accompanied by clear anomalies in the sound velocity. The observed 0.3% jump of the sound velocity at the transition is negative in Tm₂Co₁₇, whereas it is positive in Er₂Co₁₇. The magnetostriction at the transition also differs very much from that in Er₂Co₁₇. In Tm₂Co₁₇, the transition is accompanied by a smooth minimum of 0.15·10–4 in longitudinal magnetostriction whereas in Er₂Co₁₇ by a very sharp expansion of much largermagnitude (1.2·10–4). In the transverse mode, the effect in Tm₂Co₁₇ looks as very broad minimum of low amplitude (< 0.1·10–4) whereas in Er₂Co₁₇ as very sharp and large shrinkage (2.6·10–4). Thus, both themagnetoacoustics and magnetostriction are rather different in Tm₂Co₁₇ and Er₂Co₁₇. This supports different nature of the field-induced transitions in these compounds.
format Article
author Andreev, A.V.
Zvyagin, A.A.
Skourski, Y.
Yasin, S.
Zherlitsyn, S.
author_facet Andreev, A.V.
Zvyagin, A.A.
Skourski, Y.
Yasin, S.
Zherlitsyn, S.
author_sort Andreev, A.V.
title High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇
title_short High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇
title_full High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇
title_fullStr High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇
title_full_unstemmed High-field magnetoelasticity of Tm₂Co₁₇ and comparison with E₂Co₁₇
title_sort high-field magnetoelasticity of tm₂co₁₇ and comparison with e₂co₁₇
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2018
topic_facet Специальный выпуск К 80-летию со дня рождения А.И. Звягина
url http://dspace.nbuv.gov.ua/handle/123456789/176230
citation_txt High-field magnetoelasticity of Tm₂Co₁₇ and comparison with Er₂Co₁₇ / A.V. Andreev, A.A. Zvyagin, Y. Skourski, S. Yasin, S. Zherlitsyn // Физика низких температур. — 2018. — Т. 44, № 11. — С. 1575-1580. — Бібліогр.: 16 назв. — англ.
series Физика низких температур
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