2007
DOI: 10.1103/physrevlett.98.265501
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Selective Optical Generation of Coherent Acoustic Nanocavity Modes

Abstract: Femtosecond pump-probe experiments on a Ga0.85In0.15As nanocavity enclosed by two Ga(0.85)In(0.15)As/AlAs phonon Bragg mirrors reveal selective generation of terahertz confined acoustic modes and regular folded phonons. Selective generation of the confined modes alone is achievable for laser excitation at certain energies below the mirror absorption edges, corresponding to electronic transitions within the cavity layer only. Calculations based on the photoelastic effect explain the experimental results. Decay … Show more

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Cited by 58 publications
(23 citation statements)
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“…This gradual transition from real to virtual excitation has strong consequences regarding the selectivity of the optically generated coherent phonons. 13,[23][24][25] This conceptually explains the abrupt sign change of the electronic contribution to DR=R observed between 150 K and 100 K [see Fig. 3(a)], and the change in the acoustic components in Fig.…”
Section: -3mentioning
confidence: 69%
See 1 more Smart Citation
“…This gradual transition from real to virtual excitation has strong consequences regarding the selectivity of the optically generated coherent phonons. 13,[23][24][25] This conceptually explains the abrupt sign change of the electronic contribution to DR=R observed between 150 K and 100 K [see Fig. 3(a)], and the change in the acoustic components in Fig.…”
Section: -3mentioning
confidence: 69%
“…4(b)], i.e., when the detection mechanism occurs due to the coupling to real carriers in the absorbing range to a regime where the sample is more transparent and the coupling is more virtual. 13,[23][24][25] In fact, the curve corresponding to k …”
Section: -3mentioning
confidence: 99%
“…In these cases, the excitation laser should be resonant with the excitonic transition of the acoustic spacer, as described in Refs. [13,40].…”
Section: Interface Modes Through Materials Composition Tuningmentioning
confidence: 99%
“…The mass density and the speed of sound are usually condensed into a single parameter, the acoustic impedance (Z = ρv) [11,12]. Acoustic cavities have been used to study fundamental phenomena such as the confinement of acoustic phonons [10,13,14], their lifetimes [15] to control phonon propagation dynamics [10], and as efficient coherent phonon generators [13,16,17]. By coupling several acoustic resonators, it is furthermore possible to generate effective phononic potentials and to study, e.g., Bloch oscillations of acoustic phonons [12,18,19].…”
Section: Introductionmentioning
confidence: 99%
“…Elastic waves in solids could also endure a periodic Young modulus and/or a periodic density. Studies on such systems are currently numerous 5,6,7 and lead to a new field of physics namely Phononics 8,9 .…”
Section: Introductionmentioning
confidence: 99%