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Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction. / Syromyatnikov, A. V.

In: Physical Review B - Condensed Matter and Materials Physics, Vol. 75, 2007, p. 134421.

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Harvard

Syromyatnikov, AV 2007, 'Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction', Physical Review B - Condensed Matter and Materials Physics, vol. 75, pp. 134421.

APA

Syromyatnikov, A. V. (2007). Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction. Physical Review B - Condensed Matter and Materials Physics, 75, 134421.

Vancouver

Syromyatnikov AV. Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction. Physical Review B - Condensed Matter and Materials Physics. 2007;75:134421.

Author

Syromyatnikov, A. V. / Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction. In: Physical Review B - Condensed Matter and Materials Physics. 2007 ; Vol. 75. pp. 134421.

BibTeX

@article{e09d68c331754051bd57effd776c0fa7,
title = "Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction",
abstract = "We discuss Bose-Einstein condensation of magnons (BEC) in magnets with predominant ferromagnetic (FM) interaction in magnetic field $H$ near saturation ($H_c$). Because $H_c$ is independent of FM couplings, magnetic materials of this type can have small $H_c$ that makes them promising candidates for experimental investigation of BEC. Ferromagnets with easy-plane anisotropy and antiferromagnets (AFs) containing weakly coupled FM planes or chains are discussed in detail. We observe small effective interaction between magnons near the QCP in such magnets, in contrast to AFs with strong AF coupling previously discussed. In particular, this smallness allows us to find crossovers in the critical temperature $T_c(H)\propto (H_c-H)^{1/\phi}$ from $\phi=3/2$ to $\phi=1$ in quasi-1D magnets, and from $\phi=3/2$ to $\phi\approx1$ ($T_c\ln T_c\propto H_c-H$) in quasi-2D ones.",
author = "Syromyatnikov, {A. V.}",
year = "2007",
language = "не определен",
volume = "75",
pages = "134421",
journal = "Physical Review B-Condensed Matter",
issn = "1098-0121",
publisher = "American Physical Society",

}

RIS

TY - JOUR

T1 - Bose-Einstein condensation of magnons in magnets with predominant ferromagnetic interaction

AU - Syromyatnikov, A. V.

PY - 2007

Y1 - 2007

N2 - We discuss Bose-Einstein condensation of magnons (BEC) in magnets with predominant ferromagnetic (FM) interaction in magnetic field $H$ near saturation ($H_c$). Because $H_c$ is independent of FM couplings, magnetic materials of this type can have small $H_c$ that makes them promising candidates for experimental investigation of BEC. Ferromagnets with easy-plane anisotropy and antiferromagnets (AFs) containing weakly coupled FM planes or chains are discussed in detail. We observe small effective interaction between magnons near the QCP in such magnets, in contrast to AFs with strong AF coupling previously discussed. In particular, this smallness allows us to find crossovers in the critical temperature $T_c(H)\propto (H_c-H)^{1/\phi}$ from $\phi=3/2$ to $\phi=1$ in quasi-1D magnets, and from $\phi=3/2$ to $\phi\approx1$ ($T_c\ln T_c\propto H_c-H$) in quasi-2D ones.

AB - We discuss Bose-Einstein condensation of magnons (BEC) in magnets with predominant ferromagnetic (FM) interaction in magnetic field $H$ near saturation ($H_c$). Because $H_c$ is independent of FM couplings, magnetic materials of this type can have small $H_c$ that makes them promising candidates for experimental investigation of BEC. Ferromagnets with easy-plane anisotropy and antiferromagnets (AFs) containing weakly coupled FM planes or chains are discussed in detail. We observe small effective interaction between magnons near the QCP in such magnets, in contrast to AFs with strong AF coupling previously discussed. In particular, this smallness allows us to find crossovers in the critical temperature $T_c(H)\propto (H_c-H)^{1/\phi}$ from $\phi=3/2$ to $\phi=1$ in quasi-1D magnets, and from $\phi=3/2$ to $\phi\approx1$ ($T_c\ln T_c\propto H_c-H$) in quasi-2D ones.

M3 - статья

VL - 75

SP - 134421

JO - Physical Review B-Condensed Matter

JF - Physical Review B-Condensed Matter

SN - 1098-0121

ER -

ID: 5083992