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Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах. / Shishkin, I.S.; Mistonov, A.A.; Grigoryeva, N.A.; Menzel, D.; Grigoriev, S.V.

In: ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ, Vol. 10, No. 1, 2016, p. 161–173.

Research output: Contribution to journal › Article › peer-review

Harvard

Shishkin, IS, Mistonov, AA, Grigoryeva, NA, Menzel, D & Grigoriev, SV 2016, 'Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах', ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ, vol. 10, no. 1, pp. 161–173. https://doi.org/10.7868/S020735281602013X

APA

Shishkin, I. S., Mistonov, A. A., Grigoryeva, N. A., Menzel, D., & Grigoriev, S. V. (2016). Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах. ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ, 10(1), 161–173. https://doi.org/10.7868/S020735281602013X

Vancouver

Shishkin IS, Mistonov AA, Grigoryeva NA, Menzel D, Grigoriev SV. Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах. ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ. 2016;10(1):161–173. https://doi.org/10.7868/S020735281602013X

Author

Shishkin, I.S. ; Mistonov, A.A. ; Grigoryeva, N.A. ; Menzel, D. ; Grigoriev, S.V. / Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах. In: ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ. 2016 ; Vol. 10, No. 1. pp. 161–173.

BibTeX

@article{a9e175a2d4414e58af941d077db8c377,
title = "Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах",
abstract = "he behavior of magnetization in films of ferromagnetic inverted opallike nanostructures basedon cobalt and nickel is studied. The remagnetization curves M(H) and temperature dependences M(T) in theranges of H from –50 000 to +50 000 Oe and T = 5–350 K are measured by magnetometry using a superconducting quantum interference device (SQUIDmagnetometry). It is demonstrated that at T > 70 K, the totalmagnetization of the inverted nanostructures is composed of four local magnetizations, the vectors of whichare oriented along the [111] anisotropy axes of a spatial opallike 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 determinedfrom the M(H) experimental curves. The data obtained for ferromagnetic inverted opallike nanostructuresare compared with the behavior of magnetization in continuous nickel and cobalt films",
keywords = "inverse opals, SQUID-magnetometry, artificial spin ice",
author = "I.S. Shishkin and A.A. Mistonov and N.A. Grigoryeva and D. Menzel and S.V. Grigoriev",
year = "2016",
doi = "10.7868/S020735281602013X",
language = "русский",
volume = "10",
pages = "161–173",
journal = "ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ",
issn = "1027-4510",
publisher = "МАИК {"}Наука/Интерпериодика{"}",
number = "1",

}

RIS

TY - JOUR

T1 - Температурное поведение вектора локальной намагниченности в ферромагнитных опалоподобных структурах

AU - Shishkin, I.S.

AU - Mistonov, A.A.

AU - Grigoryeva, N.A.

AU - Menzel, D.

AU - Grigoriev, S.V.

PY - 2016

Y1 - 2016

N2 - he behavior of magnetization in films of ferromagnetic inverted opallike nanostructures basedon cobalt and nickel is studied. The remagnetization curves M(H) and temperature dependences M(T) in theranges of H from –50 000 to +50 000 Oe and T = 5–350 K are measured by magnetometry using a superconducting quantum interference device (SQUIDmagnetometry). It is demonstrated that at T > 70 K, the totalmagnetization of the inverted nanostructures is composed of four local magnetizations, the vectors of whichare oriented along the [111] anisotropy axes of a spatial opallike 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 determinedfrom the M(H) experimental curves. The data obtained for ferromagnetic inverted opallike nanostructuresare compared with the behavior of magnetization in continuous nickel and cobalt films

AB - he behavior of magnetization in films of ferromagnetic inverted opallike nanostructures basedon cobalt and nickel is studied. The remagnetization curves M(H) and temperature dependences M(T) in theranges of H from –50 000 to +50 000 Oe and T = 5–350 K are measured by magnetometry using a superconducting quantum interference device (SQUIDmagnetometry). It is demonstrated that at T > 70 K, the totalmagnetization of the inverted nanostructures is composed of four local magnetizations, the vectors of whichare oriented along the [111] anisotropy axes of a spatial opallike 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 determinedfrom the M(H) experimental curves. The data obtained for ferromagnetic inverted opallike nanostructuresare compared with the behavior of magnetization in continuous nickel and cobalt films

KW - inverse opals

KW - SQUID-magnetometry

KW - artificial spin ice

U2 - 10.7868/S020735281602013X

DO - 10.7868/S020735281602013X

M3 - статья

VL - 10

SP - 161

EP - 173

JO - ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ

JF - ПОВЕРХНОСТЬ. РЕНТГЕНОВСКИЕ, СИНХРОТРОННЫЕ И НЕЙТРОННЫЕ ИССЛЕДОВАНИЯ

SN - 1027-4510

IS - 1

ER -

ID: 7550241