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Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds. / Bykov, A. A.; Chetverikov, Yu O.; Moskvin, E. V.; Pirogov, A. N.; Grigoriev, S. V.

в: Journal of Magnetism and Magnetic Materials, Том 424, 15.02.2017, стр. 347-351.

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

Harvard

Bykov, AA, Chetverikov, YO, Moskvin, EV, Pirogov, AN & Grigoriev, SV 2017, 'Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds', Journal of Magnetism and Magnetic Materials, Том. 424, стр. 347-351. https://doi.org/10.1016/j.jmmm.2016.10.037

APA

Bykov, A. A., Chetverikov, Y. O., Moskvin, E. V., Pirogov, A. N., & Grigoriev, S. V. (2017). Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds. Journal of Magnetism and Magnetic Materials, 424, 347-351. https://doi.org/10.1016/j.jmmm.2016.10.037

Vancouver

Bykov AA, Chetverikov YO, Moskvin EV, Pirogov AN, Grigoriev SV. Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds. Journal of Magnetism and Magnetic Materials. 2017 Февр. 15;424:347-351. https://doi.org/10.1016/j.jmmm.2016.10.037

Author

Bykov, A. A. ; Chetverikov, Yu O. ; Moskvin, E. V. ; Pirogov, A. N. ; Grigoriev, S. V. / Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds. в: Journal of Magnetism and Magnetic Materials. 2017 ; Том 424. стр. 347-351.

BibTeX

@article{8c3f86bf80fc4b98bb6bfa42ed0fa093,
title = "Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds",
abstract = "The Y1−xTbxMn6Sn6 compounds (x=0, 0.175, 0.2, 0.225, 0.25) were studied by small angle neutron scattering (SANS) and paramagnetic neutron spin echo. The YMn6Sn6 compound is found to be a helimagnet in the whole temperature range below TN=310 K. Close to TN an additional peak of a Lorenz shape was observed at Q=0. The peak is thought to have originated from the ferromagnetic fluctuations of the magnetic Mn moment in the ab-plane of the hexagonal crystal structure. Compounds, in which Y is replaced by Tb, change their magnetic order with the increase of temperature: from easy cone ferromagnetic phase at low T through the helicoidal phase to the ferromagnetic fluctuation close to TN. Temperature-concentration phase diagram of Y1−xTbxMn6Sn6 is built on the basis of the obtained data.",
author = "Bykov, {A. A.} and Chetverikov, {Yu O.} and Moskvin, {E. V.} and Pirogov, {A. N.} and Grigoriev, {S. V.}",
note = "Publisher Copyright: {\textcopyright} 2016 Elsevier B.V.",
year = "2017",
month = feb,
day = "15",
doi = "10.1016/j.jmmm.2016.10.037",
language = "English",
volume = "424",
pages = "347--351",
journal = "Journal of Magnetism and Magnetic Materials",
issn = "0304-8853",
publisher = "Elsevier",

}

RIS

TY - JOUR

T1 - Magnetic phase diagram of Y1−xTbxMn6Sn6 compounds

AU - Bykov, A. A.

AU - Chetverikov, Yu O.

AU - Moskvin, E. V.

AU - Pirogov, A. N.

AU - Grigoriev, S. V.

N1 - Publisher Copyright: © 2016 Elsevier B.V.

PY - 2017/2/15

Y1 - 2017/2/15

N2 - The Y1−xTbxMn6Sn6 compounds (x=0, 0.175, 0.2, 0.225, 0.25) were studied by small angle neutron scattering (SANS) and paramagnetic neutron spin echo. The YMn6Sn6 compound is found to be a helimagnet in the whole temperature range below TN=310 K. Close to TN an additional peak of a Lorenz shape was observed at Q=0. The peak is thought to have originated from the ferromagnetic fluctuations of the magnetic Mn moment in the ab-plane of the hexagonal crystal structure. Compounds, in which Y is replaced by Tb, change their magnetic order with the increase of temperature: from easy cone ferromagnetic phase at low T through the helicoidal phase to the ferromagnetic fluctuation close to TN. Temperature-concentration phase diagram of Y1−xTbxMn6Sn6 is built on the basis of the obtained data.

AB - The Y1−xTbxMn6Sn6 compounds (x=0, 0.175, 0.2, 0.225, 0.25) were studied by small angle neutron scattering (SANS) and paramagnetic neutron spin echo. The YMn6Sn6 compound is found to be a helimagnet in the whole temperature range below TN=310 K. Close to TN an additional peak of a Lorenz shape was observed at Q=0. The peak is thought to have originated from the ferromagnetic fluctuations of the magnetic Mn moment in the ab-plane of the hexagonal crystal structure. Compounds, in which Y is replaced by Tb, change their magnetic order with the increase of temperature: from easy cone ferromagnetic phase at low T through the helicoidal phase to the ferromagnetic fluctuation close to TN. Temperature-concentration phase diagram of Y1−xTbxMn6Sn6 is built on the basis of the obtained data.

UR - http://www.scopus.com/inward/record.url?scp=84992560909&partnerID=8YFLogxK

U2 - 10.1016/j.jmmm.2016.10.037

DO - 10.1016/j.jmmm.2016.10.037

M3 - Article

AN - SCOPUS:84992560909

VL - 424

SP - 347

EP - 351

JO - Journal of Magnetism and Magnetic Materials

JF - Journal of Magnetism and Magnetic Materials

SN - 0304-8853

ER -

ID: 86427839