2017
DOI: 10.1103/physreva.96.043805
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Collective enhancements in many-emitter phonon lasing

Abstract: We investigate theoretically the many-emitter phonon laser based on optically driven semiconductor quantum dots within an acoustic nanocavity. We map the phonon laser Hamiltonian to a Tavis-Cummings type interaction with an unexpected additional many-emitter energy shift. This many-emitter interaction with the cavity mode results in a variety of resonances dependent on the number of participating emitters. We show that the many-emitter phonon laser also includes the single emitter resonance besides these colle… Show more

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Cited by 13 publications
(9 citation statements)
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“…In example/ex4a we implement the phonon laser/laser cooling master equation from refs 74 , 75 , which represents a set of two-level systems coupled to a phonon mode and driven by an external laser, usually at the Stokes or anti-Stokes resonances Here is the detuning of the two-level systems from the driving laser. For positive detuning near the Stokes resonance this corresponds to laser cooling and for negative detuning at the anti-Stokes resonance this corresponds to phonon lasing.…”
Section: Building Arbitrary Liouvilliansmentioning
confidence: 99%
“…In example/ex4a we implement the phonon laser/laser cooling master equation from refs 74 , 75 , which represents a set of two-level systems coupled to a phonon mode and driven by an external laser, usually at the Stokes or anti-Stokes resonances Here is the detuning of the two-level systems from the driving laser. For positive detuning near the Stokes resonance this corresponds to laser cooling and for negative detuning at the anti-Stokes resonance this corresponds to phonon lasing.…”
Section: Building Arbitrary Liouvilliansmentioning
confidence: 99%
“…Because of the tensor product structure of the Hilbert space of composite quantum systems, the complexity increases exponentially with increasing N , which provides strong limitations on the analytical and numerical feasibility. Therefore, additional restrictions of the model are necessary, which can be: (i) a limitation to very small numbers N [25][26][27], (ii) a limitation to small excitation intensities (i.e., small numbers of photons compared to the number of QEs) [28,29],or (iii) assuming ensembles consisting of N QEs with identical [30] or a small number of distinct [31] frequencies. Here we will rely on the assumption of an ensemble with identical frequencies, which is further motivated by our finding in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…Due to the interaction with the solid state environment (via, e.g., acoustic phonons), these processes cannot be completely eliminated, but the idea of controlling them has motivated theoretical investigations to turn this drawback into a useful and essential feature. In recent proposals a dissipative interaction is used to induce phonon-lasing [20], ground-state cooling [21,22], or even stabilization of the dynamics [18,23,24] in the strong coupling regime. Nevertheless, for efficient reservoir engineering, a more general theoretical framework is needed to understand, describe, and control a wide variety of different systems and structured reservoirs at finite temperatures.…”
Section: Introductionmentioning
confidence: 99%