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Temperature behavior of the local magnetization vectors in ferromagnetic inverted opal-like structures. / Shishkin, I. S.; Mistonov, A. A.; Grigoryeva, N. A.; Menzel, D.; Grigoriev, S. V.

в: Journal of Surface Investigation, Том 10, № 1, 01.01.2016, стр. 156-168.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

Harvard

Shishkin, IS, Mistonov, AA, Grigoryeva, NA, Menzel, D & Grigoriev, SV 2016, 'Temperature behavior of the local magnetization vectors in ferromagnetic inverted opal-like structures', Journal of Surface Investigation, Том. 10, № 1, стр. 156-168. https://doi.org/10.1134/S102745101601033X

APA

Vancouver

Author

Shishkin, I. S. ; Mistonov, A. A. ; Grigoryeva, N. A. ; Menzel, D. ; Grigoriev, S. V. / Temperature behavior of the local magnetization vectors in ferromagnetic inverted opal-like structures. в: Journal of Surface Investigation. 2016 ; Том 10, № 1. стр. 156-168.

BibTeX

@article{007503af970843e4ac7d6c8b3ad7f2fb,
title = "Temperature behavior of the local magnetization vectors in ferromagnetic inverted opal-like structures",
abstract = "The behavior of magnetization in films of ferromagnetic inverted opal-like nanostructures based on cobalt and nickel is studied. The remagnetization curves M(H) and temperature dependences M(T) in the ranges of H from–50000 to +50000 Oe and T = 5–350 K are measured by magnetometry using a superconducting quantum interference device (SQUID-magnetometry). It is demonstrated that at T > 70 K, the total magnetization of the inverted nanostructures is composed of four local magnetizations, the vectors of which are oriented along the 〈111〉 anisotropy axes of a spatial opal-like structure. At low temperatures, the anisotropy of the film is found to make an additional significant contribution. The critical magnetic fields corresponding to reorientation of the local magnetization vectors along the 〈111〉 anisotropy axes are determined from the M(H) experimental curves. The data obtained for ferromagnetic inverted opal-like nanostructures are compared with the behavior of magnetization in continuous nickel and cobalt films.",
keywords = "inverted opal-like nanostructures, model of critical fields, SQUID-magnetometry",
author = "Shishkin, {I. S.} and Mistonov, {A. A.} and Grigoryeva, {N. A.} and D. Menzel and Grigoriev, {S. V.}",
year = "2016",
month = jan,
day = "1",
doi = "10.1134/S102745101601033X",
language = "English",
volume = "10",
pages = "156--168",
journal = "ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ",
issn = "1027-4510",
publisher = "МАИК {"}Наука/Интерпериодика{"}",
number = "1",

}

RIS

TY - JOUR

T1 - Temperature behavior of the local magnetization vectors in ferromagnetic inverted opal-like structures

AU - Shishkin, I. S.

AU - Mistonov, A. A.

AU - Grigoryeva, N. A.

AU - Menzel, D.

AU - Grigoriev, S. V.

PY - 2016/1/1

Y1 - 2016/1/1

N2 - The behavior of magnetization in films of ferromagnetic inverted opal-like nanostructures based on cobalt and nickel is studied. The remagnetization curves M(H) and temperature dependences M(T) in the ranges of H from–50000 to +50000 Oe and T = 5–350 K are measured by magnetometry using a superconducting quantum interference device (SQUID-magnetometry). It is demonstrated that at T > 70 K, the total magnetization of the inverted nanostructures is composed of four local magnetizations, the vectors of which are oriented along the 〈111〉 anisotropy axes of a spatial opal-like structure. At low temperatures, the anisotropy of the film is found to make an additional significant contribution. The critical magnetic fields corresponding to reorientation of the local magnetization vectors along the 〈111〉 anisotropy axes are determined from the M(H) experimental curves. The data obtained for ferromagnetic inverted opal-like nanostructures are compared with the behavior of magnetization in continuous nickel and cobalt films.

AB - The behavior of magnetization in films of ferromagnetic inverted opal-like nanostructures based on cobalt and nickel is studied. The remagnetization curves M(H) and temperature dependences M(T) in the ranges of H from–50000 to +50000 Oe and T = 5–350 K are measured by magnetometry using a superconducting quantum interference device (SQUID-magnetometry). It is demonstrated that at T > 70 K, the total magnetization of the inverted nanostructures is composed of four local magnetizations, the vectors of which are oriented along the 〈111〉 anisotropy axes of a spatial opal-like structure. At low temperatures, the anisotropy of the film is found to make an additional significant contribution. The critical magnetic fields corresponding to reorientation of the local magnetization vectors along the 〈111〉 anisotropy axes are determined from the M(H) experimental curves. The data obtained for ferromagnetic inverted opal-like nanostructures are compared with the behavior of magnetization in continuous nickel and cobalt films.

KW - inverted opal-like nanostructures

KW - model of critical fields

KW - SQUID-magnetometry

UR - http://www.scopus.com/inward/record.url?scp=84958764420&partnerID=8YFLogxK

U2 - 10.1134/S102745101601033X

DO - 10.1134/S102745101601033X

M3 - Article

AN - SCOPUS:84958764420

VL - 10

SP - 156

EP - 168

JO - ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ

JF - ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ

SN - 1027-4510

IS - 1

ER -

ID: 11973597