Magneto-crystalline anisotropy of NdFe0.9Mn0.1O3 single crystal

Kód výsledku v IS VaVaI

<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216305%3A26620%2F18%3APU135546" target="_blank" >RIV/00216305:26620/18:PU135546 - isvavai.cz</a>

Nalezeny alternativní kódy

RIV/68081723:_____/18:00495432 RIV/00216208:11320/18:10380464

Výsledek na webu

<a href="https://www.sciencedirect.com/science/article/pii/S0921452617308608?via%3Dihub" target="_blank" >https://www.sciencedirect.com/science/article/pii/S0921452617308608?via%3Dihub</a>

DOI - Digital Object Identifier

<a href="http://dx.doi.org/10.1016/j.physb.2017.10.121" target="_blank" >10.1016/j.physb.2017.10.121</a>

Jazyk výsledku

angličtina

Název v původním jazyce

Magneto-crystalline anisotropy of NdFe0.9Mn0.1O3 single crystal

Popis výsledku v původním jazyce

Our present study on oriented single crystal revealed huge magneto-crystalline anisotropy with respect to principal crystallographic axes, even several magnetic transitions were observed below T-N = 748 K (c-axis) at 700 K (a-axis) as well 657 K (b-axis). The spin reorientation of magnetic moment takes place in very narrow temperature range between 135 K and 125 K and is attributed to vanishing of ferromagnetic component aligned along b-axis. Measurements of magnetic isotherms trace the development of ferromagnetic component and revealed the intermediate temperature range between 120 K and 20 K which is characterised by zero ferromagnetic components in any principal crystal direction. The ferromagnetic component develops consecutive at low temperature below 20 K along a-axis. Our study indicates completely different magnetic structure of NdFe0.9Mn0.1O3 below 135 K in comparison with NdFeO3.

Název v anglickém jazyce

Magneto-crystalline anisotropy of NdFe0.9Mn0.1O3 single crystal

Popis výsledku anglicky

Our present study on oriented single crystal revealed huge magneto-crystalline anisotropy with respect to principal crystallographic axes, even several magnetic transitions were observed below T-N = 748 K (c-axis) at 700 K (a-axis) as well 657 K (b-axis). The spin reorientation of magnetic moment takes place in very narrow temperature range between 135 K and 125 K and is attributed to vanishing of ferromagnetic component aligned along b-axis. Measurements of magnetic isotherms trace the development of ferromagnetic component and revealed the intermediate temperature range between 120 K and 20 K which is characterised by zero ferromagnetic components in any principal crystal direction. The ferromagnetic component develops consecutive at low temperature below 20 K along a-axis. Our study indicates completely different magnetic structure of NdFe0.9Mn0.1O3 below 135 K in comparison with NdFeO3.

Druh

J_imp - Článek v periodiku v databázi Web of Science

CEP obor

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OECD FORD obor

10302 - Condensed matter physics (including formerly solid state physics, supercond.)

Projekt

—

Návaznosti

I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace

Rok uplatnění

2018

Kód důvěrnosti údajů

S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Název periodika

PHYSICA B-CONDENSED MATTER

ISSN

0921-4526

e-ISSN

1873-2135

Svazek periodika

536

Číslo periodika v rámci svazku

1

Stát vydavatele periodika

NL - Nizozemsko

Počet stran výsledku

4

Strana od-do

89-92

Kód UT WoS článku

000431075600023

EID výsledku v databázi Scopus

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