2016
DOI: 10.1103/physrevb.94.014301
|View full text |Cite
|
Sign up to set email alerts
|

Dynamics of charge carriers on hexagonal nanoribbons with vacancy defects

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

1
34
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 23 publications
(35 citation statements)
references
References 35 publications
1
34
0
Order By: Relevance
“…Note that the response time, which is roughly the same in both cases, is due to the fact that the field was adiabatically introduced in the system. After a simulated time of approximately 30 fs, the carrier follows the direction of the applied field and its dynamics is consistent to what was previously reported in the literature 23,26 . The importance of the SO consideration can be better appreciated by the comparison between the two situations, rather than in the description of the process itself.…”
Section: Resultssupporting
confidence: 87%
See 3 more Smart Citations
“…Note that the response time, which is roughly the same in both cases, is due to the fact that the field was adiabatically introduced in the system. After a simulated time of approximately 30 fs, the carrier follows the direction of the applied field and its dynamics is consistent to what was previously reported in the literature 23,26 . The importance of the SO consideration can be better appreciated by the comparison between the two situations, rather than in the description of the process itself.…”
Section: Resultssupporting
confidence: 87%
“…Note that, in order to restrict edge effects, periodic boundary conditions were considered in the nanoribbon’s length, just as in ref. 23 . The electric field strength is settled to be 1.5 mV/Å for all cases and is oriented along the nanoribbon’s length.…”
Section: Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…From Fig. 1(a) one can realize that, during the first 100 fs, the strength of the electric field is turned on quasi-adiabatically – following the procedure established in refs 36,37 – to preserve numerical stability. After this transient period, the bipolarons are accelerated and reach their saturation velocity at around 400 fs.…”
Section: Resultsmentioning
confidence: 99%