Szczegóły publikacji
Opis bibliograficzny
Characterization of magnetic properties, including magnetocaloric effect, of $RE_{5}Pt_{2}In_{4}$ (RE = Gd-Tm) compounds / Altifani Rizky Hayyu, Stanisław Baran, Andrzej Szytuła, Katarzyna BERENT, Aleksandra Deptuch // Journal of Alloys and Compounds ; ISSN 0925-8388 . — 2024 — vol. 1001 art. no. 175054, s. 1–14. — Bibliogr. s. 12–14, Abstr. — Publikacja dostępna online od: 2024-06-07
Autorzy (5)
- Hayyu Altifani Rizky
- Baran Stanisław
- Szytuła Andrzej
- AGHBerent Katarzyna
- Deptuch Aleksandra
Słowa kluczowe
Dane bibliometryczne
| ID BaDAP | 153872 |
|---|---|
| Data dodania do BaDAP | 2024-06-21 |
| Tekst źródłowy | URL |
| DOI | 10.1016/j.jallcom.2024.175054 |
| Rok publikacji | 2024 |
| Typ publikacji | artykuł w czasopiśmie |
| Otwarty dostęp |  |
| Czasopismo/seria | Journal of Alloys and Compounds |
Abstract
The RE5Pt2In4 (RE = Gd-Tm) rare earth compounds have been investigated by means of X-ray diffraction (XRD) as well as by DC and AC magnetometric measurements. The compounds crystallize in an orthorhombic crystal structure of the Lu5Ni2In4-type (Pbam space group, No. 55). With decreasing temperature, the intermetallics undergo a transition from para- to ferro-/ferri- (RE = Gd, Tb, Ho, Er) or antiferromagnetic state (RE = Tm). In case of Dy5Pt2In4, the ferromagnetic state is reached through an intermediate antiferromagnetic order present in a limited temperature range. The critical temperatures of magnetic ordering range from 4.1 K (RE = Tm) up to 108 K (RE = Tb). For the majority of investigated compounds, a cascade of additional magnetic transitions is found below the respective critical temperatures of magnetic ordering. The magnetic moments are found solely on the rare earth atoms, while the moments of the remaining Pt and In atoms are absent or are too small to be detected while accompanied by the strong rare earth’s moments. The magnetocaloric (MCE) performance of RE5T2In4 (RE = Gd-Tm) is found quite good, especially while taking into account the compounds with RE = Ho and Er. Maximum magnetic entropy change (-Delta Smax/M) reaches 11.8 (RE = Ho) or 11.4 J ⋅ kg−1 ⋅ K−1 (RE = Er) under magnetic flux density change of 0–9 T. Under the same conditions, the relative cooling power (RCP) and refrigerant capacity (RC) equal 607 and 495 J ⋅ kg−1 (RE = Ho) or 434 and 341 J ⋅ kg−1 (RE = Er).
