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Examination of Commensurate Magnetic Structures in the Dy/Y multilayer system under applied magnetic field. / Grigoriev, S. V.; Tarnavich, V. V.; Chetverikov, Yu O.; Lott, D.; Schreyer, A.

в: Journal of Surface Investigation, Том 9, № 5, 01.09.2015, стр. 974-979.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Grigoriev, SV, Tarnavich, VV, Chetverikov, YO, Lott, D & Schreyer, A 2015, 'Examination of Commensurate Magnetic Structures in the Dy/Y multilayer system under applied magnetic field', Journal of Surface Investigation, Том. 9, № 5, стр. 974-979. https://doi.org/10.1134/S1027451015050298

APA

Vancouver

Author

Grigoriev, S. V. ; Tarnavich, V. V. ; Chetverikov, Yu O. ; Lott, D. ; Schreyer, A. / Examination of Commensurate Magnetic Structures in the Dy/Y multilayer system under applied magnetic field. в: Journal of Surface Investigation. 2015 ; Том 9, № 5. стр. 974-979.

BibTeX

@article{f17cf1a9ec5d4c068b5eb42e3385e36c,
title = "Examination of Commensurate Magnetic Structures in the Dy/Y multilayer system under applied magnetic field",
abstract = "In zero magnetic field, the magnetic system of a Dy/Y multilayer superstructure represents a spin spiral with a coherence length many times exceeding the Y/Dy bilayer thickness. When the magnetic spiral period does not coincide with the Dy-layer thickness, each structural layer is characterized by an average uncompensated magnetic moment. In an applied magnetic field, magnetic layers tend to order ferromagnetically. Along with ferromagnetic order coaxial to the magnetic field, fourfold commensurate spin structure similar to a spiral and twofold commensurate spin structure similar to antiferromagnetic spin-flop ordering are formed. The fourfold structure is observed at temperatures close to the critical N{\'e}el temperature at dS > dDy (TN = 160 K) in relatively weak magnetic fields. The twofold structure of an antiferromagnet is characteristic of relatively strong fields. This phenomenon is explained in terms of the competition between the Ruderman–Kittel–Kasuya–Yoshida and Zeeman interactions.",
keywords = "antiferromagnets, commensurate magnetic structures, giant magnetoresistance effect, multilayer superstructures, spin spiral structure",
author = "Grigoriev, {S. V.} and Tarnavich, {V. V.} and Chetverikov, {Yu O.} and D. Lott and A. Schreyer",
note = "Publisher Copyright: {\textcopyright} 2015, Pleiades Publishing, Ltd.",
year = "2015",
month = sep,
day = "1",
doi = "10.1134/S1027451015050298",
language = "English",
volume = "9",
pages = "974--979",
journal = "ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ",
issn = "1027-4510",
publisher = "МАИК {"}Наука/Интерпериодика{"}",
number = "5",

}

RIS

TY - JOUR

T1 - Examination of Commensurate Magnetic Structures in the Dy/Y multilayer system under applied magnetic field

AU - Grigoriev, S. V.

AU - Tarnavich, V. V.

AU - Chetverikov, Yu O.

AU - Lott, D.

AU - Schreyer, A.

N1 - Publisher Copyright: © 2015, Pleiades Publishing, Ltd.

PY - 2015/9/1

Y1 - 2015/9/1

N2 - In zero magnetic field, the magnetic system of a Dy/Y multilayer superstructure represents a spin spiral with a coherence length many times exceeding the Y/Dy bilayer thickness. When the magnetic spiral period does not coincide with the Dy-layer thickness, each structural layer is characterized by an average uncompensated magnetic moment. In an applied magnetic field, magnetic layers tend to order ferromagnetically. Along with ferromagnetic order coaxial to the magnetic field, fourfold commensurate spin structure similar to a spiral and twofold commensurate spin structure similar to antiferromagnetic spin-flop ordering are formed. The fourfold structure is observed at temperatures close to the critical Néel temperature at dS > dDy (TN = 160 K) in relatively weak magnetic fields. The twofold structure of an antiferromagnet is characteristic of relatively strong fields. This phenomenon is explained in terms of the competition between the Ruderman–Kittel–Kasuya–Yoshida and Zeeman interactions.

AB - In zero magnetic field, the magnetic system of a Dy/Y multilayer superstructure represents a spin spiral with a coherence length many times exceeding the Y/Dy bilayer thickness. When the magnetic spiral period does not coincide with the Dy-layer thickness, each structural layer is characterized by an average uncompensated magnetic moment. In an applied magnetic field, magnetic layers tend to order ferromagnetically. Along with ferromagnetic order coaxial to the magnetic field, fourfold commensurate spin structure similar to a spiral and twofold commensurate spin structure similar to antiferromagnetic spin-flop ordering are formed. The fourfold structure is observed at temperatures close to the critical Néel temperature at dS > dDy (TN = 160 K) in relatively weak magnetic fields. The twofold structure of an antiferromagnet is characteristic of relatively strong fields. This phenomenon is explained in terms of the competition between the Ruderman–Kittel–Kasuya–Yoshida and Zeeman interactions.

KW - antiferromagnets

KW - commensurate magnetic structures

KW - giant magnetoresistance effect

KW - multilayer superstructures

KW - spin spiral structure

UR - http://www.scopus.com/inward/record.url?scp=84944218490&partnerID=8YFLogxK

U2 - 10.1134/S1027451015050298

DO - 10.1134/S1027451015050298

M3 - Article

AN - SCOPUS:84944218490

VL - 9

SP - 974

EP - 979

JO - ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ

JF - ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ

SN - 1027-4510

IS - 5

ER -

ID: 86428361