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Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides. / Kudrevatykh, N.; Andreev, S. A.; Bartashevich, M. et al.
In: Journal of Magnetism and Magnetic Materials, Vol. 300, No. 1, 2006, p. e448-e451.

Research output: Contribution to journalArticlepeer-review

Harvard

Kudrevatykh, N, Andreev, SA, Bartashevich, M, Bogatkin, A, Milyaev, O, Markin, P, Tereshina, I, Palewski, T & Tereshina, E 2006, 'Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides', Journal of Magnetism and Magnetic Materials, vol. 300, no. 1, pp. e448-e451. https://doi.org/10.1016/j.jmmm.2005.10.189

APA

Kudrevatykh, N., Andreev, S. A., Bartashevich, M., Bogatkin, A., Milyaev, O., Markin, P., Tereshina, I., Palewski, T., & Tereshina, E. (2006). Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides. Journal of Magnetism and Magnetic Materials, 300(1), e448-e451. https://doi.org/10.1016/j.jmmm.2005.10.189

Vancouver

Kudrevatykh N, Andreev SA, Bartashevich M, Bogatkin A, Milyaev O, Markin P et al. Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides. Journal of Magnetism and Magnetic Materials. 2006;300(1):e448-e451. doi: 10.1016/j.jmmm.2005.10.189

Author

Kudrevatykh, N. ; Andreev, S. A. ; Bartashevich, M. et al. / Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides. In: Journal of Magnetism and Magnetic Materials. 2006 ; Vol. 300, No. 1. pp. e448-e451.

BibTeX

@article{16712b388c224180a8ce482490f1db40,
title = "Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides",
abstract = "Ground state spontaneous magnetization study for the Y-2(Fe1-xCox)(14)B and Y2Fe14BHy intermetallic compounds in magnetic fields up to 140 kOe have been performed. Obtained results can be summarized as following: the 3d-ion subsystem magnetization (M-d) does not increase upon the substitution of Co for Fe even for a small Co content, which is unusual for the CoxFe1-x alloys or other similar intermetallic compounds, but agrees well with the 3d-band structure for Y2Fe14B, if the density of states picture for the spin-up and spin-down subbands is not changed upon such substitutions (rigid band model). In Y2Fe14BHy the M-d increases with the hydrogen content increase. This can be explained by the fact that in the Fe-containing compounds, hydrogen atoms produce low-energy electron states. Leaving the 3d-band 3d electrons transit to these states. This is accompanied by the Fermi level displacement to the {"}left'' and increase in the 3d-band splitting, resulting in the M-d rise. (C) 2005 Elsevier B.V. All rights reserved.",
author = "N. Kudrevatykh and Andreev, {S. A.} and M. Bartashevich and A. Bogatkin and O. Milyaev and P. Markin and I. Tereshina and T. Palewski and E. Tereshina",
note = "The work has been supported by CRDF by grant REC-005 and Federal Program on Support of Leading Scientific Schools NSh 205.2003.2.",
year = "2006",
doi = "10.1016/j.jmmm.2005.10.189",
language = "English",
volume = "300",
pages = "e448--e451",
journal = "Journal of Magnetism and Magnetic Materials",
issn = "0304-8853",
publisher = "Elsevier BV",
number = "1",

}

RIS

TY - JOUR

T1 - Magnetization of Y2(Fe1−xCox)B14 intermetallic compound and their hydrides

AU - Kudrevatykh, N.

AU - Andreev, S. A.

AU - Bartashevich, M.

AU - Bogatkin, A.

AU - Milyaev, O.

AU - Markin, P.

AU - Tereshina, I.

AU - Palewski, T.

AU - Tereshina, E.

N1 - The work has been supported by CRDF by grant REC-005 and Federal Program on Support of Leading Scientific Schools NSh 205.2003.2.

PY - 2006

Y1 - 2006

N2 - Ground state spontaneous magnetization study for the Y-2(Fe1-xCox)(14)B and Y2Fe14BHy intermetallic compounds in magnetic fields up to 140 kOe have been performed. Obtained results can be summarized as following: the 3d-ion subsystem magnetization (M-d) does not increase upon the substitution of Co for Fe even for a small Co content, which is unusual for the CoxFe1-x alloys or other similar intermetallic compounds, but agrees well with the 3d-band structure for Y2Fe14B, if the density of states picture for the spin-up and spin-down subbands is not changed upon such substitutions (rigid band model). In Y2Fe14BHy the M-d increases with the hydrogen content increase. This can be explained by the fact that in the Fe-containing compounds, hydrogen atoms produce low-energy electron states. Leaving the 3d-band 3d electrons transit to these states. This is accompanied by the Fermi level displacement to the "left'' and increase in the 3d-band splitting, resulting in the M-d rise. (C) 2005 Elsevier B.V. All rights reserved.

AB - Ground state spontaneous magnetization study for the Y-2(Fe1-xCox)(14)B and Y2Fe14BHy intermetallic compounds in magnetic fields up to 140 kOe have been performed. Obtained results can be summarized as following: the 3d-ion subsystem magnetization (M-d) does not increase upon the substitution of Co for Fe even for a small Co content, which is unusual for the CoxFe1-x alloys or other similar intermetallic compounds, but agrees well with the 3d-band structure for Y2Fe14B, if the density of states picture for the spin-up and spin-down subbands is not changed upon such substitutions (rigid band model). In Y2Fe14BHy the M-d increases with the hydrogen content increase. This can be explained by the fact that in the Fe-containing compounds, hydrogen atoms produce low-energy electron states. Leaving the 3d-band 3d electrons transit to these states. This is accompanied by the Fermi level displacement to the "left'' and increase in the 3d-band splitting, resulting in the M-d rise. (C) 2005 Elsevier B.V. All rights reserved.

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U2 - 10.1016/j.jmmm.2005.10.189

DO - 10.1016/j.jmmm.2005.10.189

M3 - Article

VL - 300

SP - e448-e451

JO - Journal of Magnetism and Magnetic Materials

JF - Journal of Magnetism and Magnetic Materials

SN - 0304-8853

IS - 1

ER -

ID: 42299935