2016
DOI: 10.1021/acsphotonics.6b00707
|View full text |Cite
|
Sign up to set email alerts
|

Impact of Phonons on Dephasing of Individual Excitons in Deterministic Quantum Dot Microlenses

Abstract: Optimized light–matter coupling in semiconductor nanostructures is a key to understand their optical properties and can be enabled by advanced fabrication techniques. Using in situ electron beam lithography combined with a low-temperature cathodoluminescence imaging, we deterministically fabricate microlenses above selected InAs quantum dots (QDs), achieving their efficient coupling to the external light field. This enables performing four-wave mixing microspectroscopy of single QD excitons, revealing the exci… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

2
55
0

Year Published

2017
2017
2022
2022

Publication Types

Select...
9

Relationship

6
3

Authors

Journals

citations
Cited by 41 publications
(57 citation statements)
references
References 43 publications
2
55
0
Order By: Relevance
“…The line broadening has a temperature-dependent shoulder, which cannot be exlained with a white noise model as outlined above. In contrast, the asymmetric lineshape is a direct consequence of the underlying non-Markovian dynamics between the QD and lattice vibrations [24,73,76,93,[121][122][123].…”
Section: A Non-lorentzian Lineshapes (Independent Boson Model)mentioning
confidence: 99%
“…The line broadening has a temperature-dependent shoulder, which cannot be exlained with a white noise model as outlined above. In contrast, the asymmetric lineshape is a direct consequence of the underlying non-Markovian dynamics between the QD and lattice vibrations [24,73,76,93,[121][122][123].…”
Section: A Non-lorentzian Lineshapes (Independent Boson Model)mentioning
confidence: 99%
“…Using the correlation expansion we calculate the dynamics of the phonons created during and immediately after the optical excitation [34,35]. The rapid generation of the exciton leads to the formation of a wave packet leaving the QD region [12,36]. For a spherical QD, the generated wave packet retains the spherical symmetry of the QD.…”
Section: Introductionmentioning
confidence: 99%
“…11) for τ 12 > 0 because of the coherence loss accompanying the emission of a phonon wave packet. 12 The dependence of this effect on the driving pulse areas will be discussed in Sec. V. Because the FWM signal is absent before the second laser pulse and the described drop within a few ps, the FWM amplitude has a maximum at delays τ 12 < 1 ps.…”
Section: A Two-level Systemmentioning
confidence: 99%