scholarly journals Independent Control Over Size and Surface Density of Droplet Epitaxial Nanostructures Using Ultra-Low Arsenic Fluxes

Nanomaterials ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 1184
Author(s):  
Sergey V. Balakirev ◽  
Natalia E. Chernenko ◽  
Mikhail M. Eremenko ◽  
Oleg A. Ageev ◽  
Maxim S. Solodovnik

Modern and future nanoelectronic and nanophotonic applications require precise control of the size, shape and density of III-V quantum dots in order to predefine the characteristics of devices based on them. In this paper, we propose a new approach to control the size of nanostructures formed by droplet epitaxy. We reveal that it is possible to reduce the droplet volume independently of the growth temperature and deposition amount by exposing droplets to ultra-low group-V flux. We carry out a thorough study of the effect of arsenic pressure on the droplet characteristics and demonstrate that indium droplets with a large initial size (>100 nm) and a low surface density (<108 cm−2) are able to shrink to dimensions appropriate for quantum dot applications. Small droplets are found to be unstable and difficult to control, while larger droplets are more resistive to arsenic flux and can be reduced to stable, small-sized nanostructures (~30 nm). We demonstrate the growth conditions under which droplets transform into dots, ring and holes and describe a mechanism of this transformation depending on the ultra-low arsenic flux. Thus, we observe phenomena which significantly expand the capabilities of droplet epitaxy.

2021 ◽  
Vol 2086 (1) ◽  
pp. 012017
Author(s):  
D V Kirichenko ◽  
S V Balakirev ◽  
N E Chernenko ◽  
M M Eremenko ◽  
M S Solodovnik

Abstract In this paper, we present the results of an experimental study of the influence of the ultra-low arsenic flux on the parameters of In nanodroplets obtained by droplet epitaxy on the GaAs substrate. We demonstrate that the arsenic flux can be used to alter the size of droplets without changing their surface density. An increase in the arsenic flux leads to a reduction of the nanostructure size or their complete decay. However, we demonstrate that certain growth conditions allow providing saturation of the size of nanostructures (∼30 nm) which ensures good reproducibility of the process. The mechanism of ring and hole formation at various arsenic fluxes is also discussed.


Author(s):  
Takaaki Mano ◽  
Akihiro Ohtake ◽  
Neul Ha ◽  
Takeshi Noda ◽  
Yoshiki Sakuma ◽  
...  

RSC Advances ◽  
2015 ◽  
Vol 5 (49) ◽  
pp. 38810-38817 ◽  
Author(s):  
Yeping Li ◽  
Jingbo Xu ◽  
Yun Xu ◽  
Liying Huang ◽  
Junli Wang ◽  
...  

The objective of the study is to describe a new approach of combining quantum dots into chitosan as an anti-cancer drug carrier.


1998 ◽  
Vol 37 (Part 1, No. 12B) ◽  
pp. 7158-7160 ◽  
Author(s):  
Chae-Deok Lee ◽  
Chanro Park ◽  
Hwack Joo Lee ◽  
Kyu-Seok Lee ◽  
Seong-Ju Park ◽  
...  

2010 ◽  
Vol 8 (2) ◽  
pp. 275-277 ◽  
Author(s):  
T. Kawazu ◽  
T. Noda ◽  
T. Mano ◽  
M. Ohmori ◽  
Y. Akiyama ◽  
...  
Keyword(s):  

1998 ◽  
Vol 51 (1-3) ◽  
pp. 127-131 ◽  
Author(s):  
B.P Zhang ◽  
T Yasuda ◽  
W.X Wang ◽  
Y Segawa ◽  
K Edamatsu ◽  
...  
Keyword(s):  

2002 ◽  
Vol 722 ◽  
Author(s):  
S. Kiravittaya ◽  
R. Songmuang ◽  
O. G. Schmidt

AbstractEnsembles of homogeneous self-assembled quantum dots (QDs) and nanoholes are fabricated using molecular beam epitaxy in combination with atomically precise in situ etching. Self-assembled InAs QDs with height fluctuations of ±5% were grown using a very low indium growth rate on GaAs (001) substrate. If these dots are capped with GaAs at low temperature, strong room temperature emission at 1.3 νm with a linewidth of 21 meV from the islands is observed. Subsequently, we fabricate homogeneous arrays of nanoholes by in situ etching the GaAs surface of the capped InAs QDs with AsBr3. The depths of the nanoholes can be tuned over a range of 1-6 nm depending on the nominal etching depth and the initial capping layer thickness. We appoint the formation of nanoholes to a pronounced selectivity of the AsBr3 to local strain fields. The holes can be filled with InAs again such that an atomically flat surface is recovered. QDs in the second layer preferentially form at those sites, where the holes were initially created. Growth conditions for the second InAs layer can be chosen in such a way that lateral QD molecules form on a flat surface.


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