2020
DOI: 10.1103/physrevb.102.235303
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Optical signatures of electron-phonon decoupling due to strong light-matter interactions

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Cited by 24 publications
(36 citation statements)
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“…[ 54 ] Because we neglect the non‐Markovian effects, we also do not describe the acoustic phonon sideband, which in GaAs dots is about three orders of magnitudes below the Mollow triplet peaks. [ 58,59 ] Also for more evolved photon properties [ 60,61 ] or entangled photons, [ 62,63 ] the rate equations might fail depending on the parameter regime. Nonetheless, to describe the quantum dynamics of the electronic states in a QD, rate equations capture the essential features given that a non‐monotoneous phonon spectral density is taken into account and by their simplicity offer beautiful insight in the underlying physics.…”
Section: Dynamicsmentioning
confidence: 99%
“…[ 54 ] Because we neglect the non‐Markovian effects, we also do not describe the acoustic phonon sideband, which in GaAs dots is about three orders of magnitudes below the Mollow triplet peaks. [ 58,59 ] Also for more evolved photon properties [ 60,61 ] or entangled photons, [ 62,63 ] the rate equations might fail depending on the parameter regime. Nonetheless, to describe the quantum dynamics of the electronic states in a QD, rate equations capture the essential features given that a non‐monotoneous phonon spectral density is taken into account and by their simplicity offer beautiful insight in the underlying physics.…”
Section: Dynamicsmentioning
confidence: 99%
“…In this section, we present the underlying unitary transformations and derive the corresponding master equations. The unitary transformations considered are the identity transformation, the standard polaron transformation [38,44,[47][48][49], a variationally optimized polaron transformation [14,[50][51][52][53], and a polariton-polaron transformation. An illustration of the exciton-cavity-phonon system together with the effects of the variational polaron transformation and polariton-polaron transformation can be seen in Fig.…”
Section: Perturbative Master Equationsmentioning
confidence: 99%
“…Here, the strong emitter-cavity interaction can significantly influence and, in some cases, decouple the vibrational dynamics [11][12][13]. In this regime, the optical emission spectrum exhibits two distinct polariton peaks which are both dressed * mabuni1998@gmail.com with a distinct vibrational sideband [14,15]. On the other hand, resonant phonon-induced transitions between the polariton states is a dominating effect in the intermediate regime, where the polariton splitting is comparable with the typical environmental phonon frequency.…”
Section: Introductionmentioning
confidence: 99%
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