2013
DOI: 10.1103/physrevb.87.241302
|View full text |Cite
|
Sign up to set email alerts
|

Postselected indistinguishable single-photon emission from the Mollow triplet sidebands of a resonantly excited quantum dot

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
12
0

Year Published

2014
2014
2025
2025

Publication Types

Select...
6
3

Relationship

1
8

Authors

Journals

citations
Cited by 18 publications
(12 citation statements)
references
References 33 publications
0
12
0
Order By: Relevance
“…2(f). Frequency-resolved correlations for this system have been theoretically investigated in the past [16,[41][42][43][44] and were even measured [13,45,46] before the concept of the 2PS was put forward. But in both theoretical and …”
Section: Valleys Of Accessible Correlationsmentioning
confidence: 99%
“…2(f). Frequency-resolved correlations for this system have been theoretically investigated in the past [16,[41][42][43][44] and were even measured [13,45,46] before the concept of the 2PS was put forward. But in both theoretical and …”
Section: Valleys Of Accessible Correlationsmentioning
confidence: 99%
“…At this point it is worth emphasizing first that both HFS values are of comparable magnitude to or even significantly larger than the observed emission line widths ∆ν of the Mollow triplet components of QD 1 (see Fig. 1(d) According to the theory of dressed state emission [9,11], the frequencies of the triplet [16].…”
mentioning
confidence: 73%
“…The resulting spectrum, arising from strong resonant pumping, is composed of three lines: a central line, called Rayleigh (R), and two symmetric sidebands called respectively fluorescence (F) and three-photon (T) lines18. The photons emitted in the F and T sidebands have been demonstrated to be highly indistinguishable19, and can also be emitted in a cascaded manner if the QD is specifically pumped20. The splitting of the QD sidebands can be spectrally aligned to the atomic transitions of the Cs hyper fine splitting (that is 9.2 GHz) and their spectral position can be controlled precisely by adjusting the laser power or the QD-to-laser detuning.…”
Section: Resultsmentioning
confidence: 99%