Multiharmonic Frequency-Chirped Transducers for Surface-Acoustic-Wave Optomechanics

dc.bibliographicCitation.firstPage014004
dc.bibliographicCitation.issue1
dc.bibliographicCitation.journalTitlePhysical Review Appliedeng
dc.bibliographicCitation.volume9
dc.contributor.authorWeiß, Matthias
dc.contributor.authorHörner, Andreas L.
dc.contributor.authorZallo, Eugenio
dc.contributor.authorAtkinson, Paola
dc.contributor.authorRastelli, Armando
dc.contributor.authorSchmidt, Oliver G.
dc.contributor.authorWixforth, Achim
dc.contributor.authorKrenner, Hubert J.
dc.date.accessioned2023-02-06T10:22:45Z
dc.date.available2023-02-06T10:22:45Z
dc.date.issued2018
dc.description.abstractWide-passband interdigital transducers are employed to establish a stable phase lock between a train of laser pulses emitted by a mode-locked laser and a surface acoustic wave generated electrically by the transducer. The transducer design is based on a multiharmonic split-finger architecture for the excitation of a fundamental surface acoustic wave and a discrete number of its overtones. Simply by introducing a variation of the transducer's periodicity p, a frequency chirp is added. This combination results in wide frequency bands for each harmonic. The transducer's conversion efficiency from the electrical to the acoustic domain is characterized optomechanically using single quantum dots acting as nanoscale pressure sensors. The ability to generate surface acoustic waves over a wide band of frequencies enables advanced acousto-optic spectroscopy using mode-locked lasers with fixed repetition rate. Stable phase locking between the electrically generated acoustic wave and the train of laser pulses is confirmed by performing stroboscopic spectroscopy on a single quantum dot at a frequency of 320 MHz. Finally, the dynamic spectral modulation of the quantum dot is directly monitored in the time domain combining stable phase-locked optical excitation and time-correlated single-photon counting. The demonstrated scheme will be particularly useful for the experimental implementation of surface-acoustic-wave-driven quantum gates of optically addressable qubits or collective quantum states or for multicomponent Fourier synthesis of tailored nanomechanical waveforms.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/11291
dc.identifier.urihttp://dx.doi.org/10.34657/10327
dc.language.isoeng
dc.publisherCollege Park, Md. [u.a.] : American Physical Society
dc.relation.doihttps://doi.org/10.1103/physrevapplied.9.014004
dc.relation.essn2331-7019
dc.rights.licenseCC BY 4.0 Unported
dc.rights.urihttps://creativecommons.org/licenses/by/4.0
dc.subject.ddc530
dc.subject.otherAcoustic spectroscopyeng
dc.subject.otherAcoustic surface wave deviceseng
dc.subject.otherLaser mode lockingeng
dc.subject.otherLaser pulseseng
dc.subject.otherLaserseng
dc.subject.otherLocks (fasteners)eng
dc.subject.otherMode-locked fiber laserseng
dc.subject.otherNanocrystalseng
dc.subject.otherParticle beamseng
dc.subject.otherQuantum dot laserseng
dc.subject.otherQuantum opticseng
dc.subject.otherSemiconductor quantum dotseng
dc.subject.otherTransducerseng
dc.subject.otherUltrasonic transducerseng
dc.titleMultiharmonic Frequency-Chirped Transducers for Surface-Acoustic-Wave Optomechanicseng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccess
wgl.contributorIFWD
wgl.contributorPDI
wgl.subjectPhysikger
wgl.typeZeitschriftenartikelger
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