Standard

Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states. / Podgornykh, S. m.; Kazantsev, V. a.; Myakon’kikh, V. i. et al.
In: Journal of Experimental and Theoretical Physics, Vol. 105, No. 1, 01.07.2007, p. 62-64.

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

Harvard

Podgornykh, SM, Kazantsev, VA, Myakon’kikh, VI, Shcherbakova, EV & Ermakov, AA 2007, 'Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states', Journal of Experimental and Theoretical Physics, vol. 105, no. 1, pp. 62-64. https://doi.org/10.1134/S106377610707014X

APA

Podgornykh, S. M., Kazantsev, V. A., Myakon’kikh, V. I., Shcherbakova, E. V., & Ermakov, A. A. (2007). Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states. Journal of Experimental and Theoretical Physics, 105(1), 62-64. https://doi.org/10.1134/S106377610707014X

Vancouver

Podgornykh SM, Kazantsev VA, Myakon’kikh VI, Shcherbakova EV, Ermakov AA. Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states. Journal of Experimental and Theoretical Physics. 2007 Jul 1;105(1):62-64. doi: 10.1134/S106377610707014X

Author

Podgornykh, S. m. ; Kazantsev, V. a. ; Myakon’kikh, V. i. et al. / Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states. In: Journal of Experimental and Theoretical Physics. 2007 ; Vol. 105, No. 1. pp. 62-64.

BibTeX

@article{10705c248c6c4d579620c5dc3a70d431,
title = "Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states",
abstract = "The low-temperature specific heat C p of La(Fe 0.873Co0.007Al0.12)13 compound has been measured in two states: (i) antiferromagnetic (AFM) with a N{\'e}el temperature of T N = 192 K and (ii) ferromagnetic (FM). The FM order appears at T = 4.2 K in a sample exposed to an external magnetic field with induction B C 2.5 T and is retained for a long time in a zero field at temperatures up to T*C = 23 K. The coefficient γFM in the low-temperature specific heat C = γT + βT 3 in the FM state differs quite insignificantly from that (γAFM) in the AFM state. Contributions to the low-temperature specific heat, which are related to a change in the elastic and magnetoelastic energy caused by magnetostrictive deformations, are considered.",
author = "Podgornykh, {S. m.} and Kazantsev, {V. a.} and Myakon{\textquoteright}kikh, {V. i.} and Shcherbakova, {E. v.} and Ermakov, {A. a.}",
year = "2007",
month = jul,
day = "1",
doi = "10.1134/S106377610707014X",
language = "English",
volume = "105",
pages = "62--64",
journal = "Journal of Experimental and Theoretical Physics",
issn = "1063-7761",
publisher = "American Institute of Physics Publising LLC",
number = "1",

}

RIS

TY - JOUR

T1 - Specific heat of La(Fe0.873Co0.007Al0.12)13 compound in antiferromagnetic and ferromagnetic states

AU - Podgornykh, S. m.

AU - Kazantsev, V. a.

AU - Myakon’kikh, V. i.

AU - Shcherbakova, E. v.

AU - Ermakov, A. a.

PY - 2007/7/1

Y1 - 2007/7/1

N2 - The low-temperature specific heat C p of La(Fe 0.873Co0.007Al0.12)13 compound has been measured in two states: (i) antiferromagnetic (AFM) with a Néel temperature of T N = 192 K and (ii) ferromagnetic (FM). The FM order appears at T = 4.2 K in a sample exposed to an external magnetic field with induction B C 2.5 T and is retained for a long time in a zero field at temperatures up to T*C = 23 K. The coefficient γFM in the low-temperature specific heat C = γT + βT 3 in the FM state differs quite insignificantly from that (γAFM) in the AFM state. Contributions to the low-temperature specific heat, which are related to a change in the elastic and magnetoelastic energy caused by magnetostrictive deformations, are considered.

AB - The low-temperature specific heat C p of La(Fe 0.873Co0.007Al0.12)13 compound has been measured in two states: (i) antiferromagnetic (AFM) with a Néel temperature of T N = 192 K and (ii) ferromagnetic (FM). The FM order appears at T = 4.2 K in a sample exposed to an external magnetic field with induction B C 2.5 T and is retained for a long time in a zero field at temperatures up to T*C = 23 K. The coefficient γFM in the low-temperature specific heat C = γT + βT 3 in the FM state differs quite insignificantly from that (γAFM) in the AFM state. Contributions to the low-temperature specific heat, which are related to a change in the elastic and magnetoelastic energy caused by magnetostrictive deformations, are considered.

UR - https://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=tsmetrics&SrcApp=tsm_test&DestApp=WOS_CPL&DestLinkType=FullRecord&KeyUT=000248825500014

UR - http://www.scopus.com/inward/record.url?partnerID=8YFLogxK&scp=36048991469

U2 - 10.1134/S106377610707014X

DO - 10.1134/S106377610707014X

M3 - Article

VL - 105

SP - 62

EP - 64

JO - Journal of Experimental and Theoretical Physics

JF - Journal of Experimental and Theoretical Physics

SN - 1063-7761

IS - 1

ER -

ID: 41289003