Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field

Sound propagation in the Blume Capel model with quenched diluted single-ion anisotropy is investigated. The sound dispersion relation and an expression for the ultrasonic attenuation are derived with the aid of the method of thermodynamics of irreversible processes. A frequency-dependent dispersion...

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Main Author: Gul Gulpinar
Format: Article
Language:English
Published: Hindawi Limited 2018-01-01
Series:Advances in Condensed Matter Physics
Online Access:http://dx.doi.org/10.1155/2018/3175068
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spelling doaj-b70a5553a44a404dac5a48205f9d307f2020-11-24T22:42:37ZengHindawi LimitedAdvances in Condensed Matter Physics1687-81081687-81242018-01-01201810.1155/2018/31750683175068Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal FieldGul Gulpinar0Department of Physics, Dokuz Eylül University, 35160 Izmir, TurkeySound propagation in the Blume Capel model with quenched diluted single-ion anisotropy is investigated. The sound dispersion relation and an expression for the ultrasonic attenuation are derived with the aid of the method of thermodynamics of irreversible processes. A frequency-dependent dispersion minimum that is shifted to lower temperatures with rising frequency is observed in the ordered region. The thermal and sound frequency (ω) dependencies of the sound attenuation and effect of the Onsager rate coefficient are studied in low- and high-frequency regimes. The results showed that ωτ≪1 and ωτ≫1 are the conditions that describe low- and high-frequency regimes, where τ is the single relaxation time diverging in the vicinity of the critical temperature. In addition, assuming a linear coupling of sound wave with the order parameter fluctuations in the system and ε as the temperature distance from the critical point, we found that the sound attenuation follows the power laws α(ω,ε)~ω2ε-1 and α(ω,ε)~ω0ε1 in the low- and high-frequency regions, while ε→0. Finally, a comparison of the findings of this study with previous theoretical and experimental studies is presented and it is shown that a good agreement is found with our results.http://dx.doi.org/10.1155/2018/3175068
collection DOAJ
language English
format Article
sources DOAJ
author Gul Gulpinar
spellingShingle Gul Gulpinar
Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field
Advances in Condensed Matter Physics
author_facet Gul Gulpinar
author_sort Gul Gulpinar
title Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field
title_short Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field
title_full Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field
title_fullStr Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field
title_full_unstemmed Acoustic Signatures of the Phases and Phase Transitions in the Blume Capel Model with Random Crystal Field
title_sort acoustic signatures of the phases and phase transitions in the blume capel model with random crystal field
publisher Hindawi Limited
series Advances in Condensed Matter Physics
issn 1687-8108
1687-8124
publishDate 2018-01-01
description Sound propagation in the Blume Capel model with quenched diluted single-ion anisotropy is investigated. The sound dispersion relation and an expression for the ultrasonic attenuation are derived with the aid of the method of thermodynamics of irreversible processes. A frequency-dependent dispersion minimum that is shifted to lower temperatures with rising frequency is observed in the ordered region. The thermal and sound frequency (ω) dependencies of the sound attenuation and effect of the Onsager rate coefficient are studied in low- and high-frequency regimes. The results showed that ωτ≪1 and ωτ≫1 are the conditions that describe low- and high-frequency regimes, where τ is the single relaxation time diverging in the vicinity of the critical temperature. In addition, assuming a linear coupling of sound wave with the order parameter fluctuations in the system and ε as the temperature distance from the critical point, we found that the sound attenuation follows the power laws α(ω,ε)~ω2ε-1 and α(ω,ε)~ω0ε1 in the low- and high-frequency regions, while ε→0. Finally, a comparison of the findings of this study with previous theoretical and experimental studies is presented and it is shown that a good agreement is found with our results.
url http://dx.doi.org/10.1155/2018/3175068
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