2016
DOI: 10.1103/physrevb.93.195316
|View full text |Cite
|
Sign up to set email alerts
|

Overcoming power broadening of the quantum dot emission in a pure wurtzite nanowire

Abstract: Vous avez des questions? Nous pouvons vous aider. Pour communiquer directement avec un auteur, consultez la première page de la revue dans laquelle son article a été publié afin de trouver ses coordonnées. Si vous n'arrivez pas à les repérer, communiquez avec nous à PublicationsArchive-ArchivesPublications@nrc-cnrc.gc.ca. Questions? Contact the NRC Publications Archive team atPublicationsArchive-ArchivesPublications@nrc-cnrc.gc.ca. If you wish to email the authors directly, please see the first page of the pub… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
91
0

Year Published

2016
2016
2023
2023

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 82 publications
(93 citation statements)
references
References 47 publications
2
91
0
Order By: Relevance
“…This technique has been demonstrated to yield defect-free, pure wurtzite nanowires, which is essential to obtain long single-photon coherence27. Figure 1a shows a scanning electron microscopy (SEM) image of a tapered InP nanowire waveguide containing an InAsP segment, 200 nm from the nanowire base, defining the optically active quantum dot that we study.…”
Section: Resultsmentioning
confidence: 99%
“…This technique has been demonstrated to yield defect-free, pure wurtzite nanowires, which is essential to obtain long single-photon coherence27. Figure 1a shows a scanning electron microscopy (SEM) image of a tapered InP nanowire waveguide containing an InAsP segment, 200 nm from the nanowire base, defining the optically active quantum dot that we study.…”
Section: Resultsmentioning
confidence: 99%
“…The meaning of c e and c h in our calculations is that of an average occupation of charge traps55 in QD and CL, respectively, changing from less than one to two electron-hole pairs per QD volume as P is increased. In our understanding, there is probably an important contribution of trap-state filling effect to the emission blue-shift with pumping in type-II.…”
Section: Methodsmentioning
confidence: 96%
“…The resulting interacting SQD -multifunctional LMUs in turn provide the hierarchical building blocks that can be readily interconnected in architectures designed to provide circuit-and system-level functionality. To date, approaches to integrated SQD-LMU structures have been based on either micropillar 7-10 / nanowire [11][12][13][14] or 2D photonic crystal 1,[15][16][17][18][19][20] platforms, the former inherently well-suited to architectures exploiting vertical emission of photons while the latter to horizontal emission. Great progress has been achieved using vertical micropillar / nanowire architecture in realizing single photon emission rate enhancement [7][8][9][10] , purity 8,10,11,13,14 , indistinguishability 9,10,14 and photon collection efficiency control [9][10][11][12][13][14] , all important figures of merit for SPSs.…”
Section: Introductionmentioning
confidence: 99%
“…The large spectral non-uniformity makes it difficult to spectrally match QD with the light manipulating elements within the tuning range of the well-established spectral tuning technique 19,21 . Another class of SPS is based on QDs in nanowire [12][13][14][48][49][50] structures typically grown via the metal nanoparticle seeded vapor-liquid-solid (VLS) growth mechanism. The nanowire diameter is controlled by the seed particle diameter and in turn the QD lateral size is controlled by the nanowire diameter 48,49 .…”
Section: Introductionmentioning
confidence: 99%