2025-02-23T03:25:48-05:00 DEBUG: VuFindSearch\Backend\Solr\Connector: Query fl=%2A&wt=json&json.nl=arrarr&q=id%3A%22irk-123456789-175250%22&qt=morelikethis&rows=5
2025-02-23T03:25:48-05:00 DEBUG: VuFindSearch\Backend\Solr\Connector: => GET http://localhost:8983/solr/biblio/select?fl=%2A&wt=json&json.nl=arrarr&q=id%3A%22irk-123456789-175250%22&qt=morelikethis&rows=5
2025-02-23T03:25:48-05:00 DEBUG: VuFindSearch\Backend\Solr\Connector: <= 200 OK
2025-02-23T03:25:48-05:00 DEBUG: Deserialized SOLR response

High-field magnetoelasticity of Tm₂Co₁₇ and comparison with Er₂Co₁₇

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...

Full description

Saved in:
Bibliographic Details
Main Authors: Andreev, A.V., Zvyagin, A.A., Skourski, Y., Yasin, S., Zherlitsyn, S.
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2017
Series:Физика низких температур
Subjects:
Online Access:http://dspace.nbuv.gov.ua/handle/123456789/175250
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary: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 larger magnitude (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 the magnetoacoustics and magnetostriction are rather different in Tm₂Co₁₇ and Er₂Co₁₇. This supports different nature of the field-induced transitions in these compounds.