Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves

We present the concept on coherence that, in finite-size systems, free induction decay time is controllable through appropriately designing frequency dispersion curves as function of wave vector. We confirmed the present concept from numerical calculation of free induction decay time of coherent fol...

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Main Author: Hideo Takeuchi
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:Journal of Physics Communications
Subjects:
Online Access:https://doi.org/10.1088/2399-6528/adb53a
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author Hideo Takeuchi
author_facet Hideo Takeuchi
author_sort Hideo Takeuchi
collection DOAJ
description We present the concept on coherence that, in finite-size systems, free induction decay time is controllable through appropriately designing frequency dispersion curves as function of wave vector. We confirmed the present concept from numerical calculation of free induction decay time of coherent folded longitudinal acoustic (LA) phonons that are generated through impulsive stimulated Raman scattering processes in fine-size GaAs/AlAs superlattices. It is well-known that, in finite-size superlattices, the wave-vector (momentum) conservation is relaxed; therefore, the width of the folded LA phonon Raman band is broadened. This is the preset focusing viewpoint. We found that a ratio of GaAs-thickness to AlAs-layer thickness, which governs the line shape of the phonon dispersion curve, influences the free induction decay time of the coherent folded LA phonon. The above-mentioned ratio also causes a change in the zone-centre gap frequency of the folded LA phonon dispersion. The zone-centre gap relates to the free induction decay time. The coherent folded LA phonon is an ensemble of the in-phase oscillating folded LA phonons. Since the finite-effect causes the relaxation of the wave-vector conservation, the ensemble of the in-phase oscillating folded LA phonons are composed of the phonons with various frequencies. The variety in frequency of the constituent folded LA phonons results in the appearance of the free induction decay depending on the zone-centre gap frequency depending on the phonon dispersion curve.
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spelling doaj.art-71bf207440624f6d805b0a5987847b382025-02-20T12:47:31ZengIOP PublishingJournal of Physics Communications2399-65282025-01-019202500410.1088/2399-6528/adb53aFree induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curvesHideo Takeuchi0https://orcid.org/0000-0002-8073-3233Department of Physics and Electronics, Graduate School of Engineering, Osaka Metropolitan University (formerly Osaka City University) , 1-1 Gakuen, Naka, Sakai, Osaka 599-8531, Japan; Faculty of Science and Technology, Sophia University Yotsuya Campus , 7-1 Kioi, Chiyoda, Tokyo 102-8554, JapanWe present the concept on coherence that, in finite-size systems, free induction decay time is controllable through appropriately designing frequency dispersion curves as function of wave vector. We confirmed the present concept from numerical calculation of free induction decay time of coherent folded longitudinal acoustic (LA) phonons that are generated through impulsive stimulated Raman scattering processes in fine-size GaAs/AlAs superlattices. It is well-known that, in finite-size superlattices, the wave-vector (momentum) conservation is relaxed; therefore, the width of the folded LA phonon Raman band is broadened. This is the preset focusing viewpoint. We found that a ratio of GaAs-thickness to AlAs-layer thickness, which governs the line shape of the phonon dispersion curve, influences the free induction decay time of the coherent folded LA phonon. The above-mentioned ratio also causes a change in the zone-centre gap frequency of the folded LA phonon dispersion. The zone-centre gap relates to the free induction decay time. The coherent folded LA phonon is an ensemble of the in-phase oscillating folded LA phonons. Since the finite-effect causes the relaxation of the wave-vector conservation, the ensemble of the in-phase oscillating folded LA phonons are composed of the phonons with various frequencies. The variety in frequency of the constituent folded LA phonons results in the appearance of the free induction decay depending on the zone-centre gap frequency depending on the phonon dispersion curve.https://doi.org/10.1088/2399-6528/adb53acoherence timefree induction decayfinite-size effectscoherent folded LA phononphonon dispersion curveultrafast optical phenomena
spellingShingle Hideo Takeuchi
Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves
Journal of Physics Communications
coherence time
free induction decay
finite-size effects
coherent folded LA phonon
phonon dispersion curve
ultrafast optical phenomena
title Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves
title_full Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves
title_fullStr Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves
title_full_unstemmed Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves
title_short Free induction decay processes of coherent folded longitudinal acoustic phonons in GaAs/AlAs finite size superlattices: control through the design of phonon dispersion curves
title_sort free induction decay processes of coherent folded longitudinal acoustic phonons in gaas alas finite size superlattices control through the design of phonon dispersion curves
topic coherence time
free induction decay
finite-size effects
coherent folded LA phonon
phonon dispersion curve
ultrafast optical phenomena
url https://doi.org/10.1088/2399-6528/adb53a
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