2016
DOI: 10.1103/physrevb.94.195411
|View full text |Cite
|
Sign up to set email alerts
|

Carrier-density-dependent recombination dynamics of excitons and electron-hole plasma in m -plane InGaN/GaN quantum wells

Abstract: We study the carrier-density-dependent recombination dynamics in m-plane InGaN/GaN multiple quantum wells in the presence of n-type background doping by time-resolved photoluminescence. Based on Fermi's golden rule and Saha's equation, we decompose the radiative recombination channel into an excitonic and an electron-hole pair contribution, and extract the injected carrier-density-dependent bimolecular recombination coefficients. Contrary to the standard electron-hole picture, our results confirm the strong in… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

2
36
0

Year Published

2018
2018
2023
2023

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 44 publications
(39 citation statements)
references
References 38 publications
2
36
0
Order By: Relevance
“…12,13 While excitons in GaN-based nanostructures have relatively high binding energies and small Bohr radii 21 (as compared to GaAs-based structures) and thus could exhibit quantum properties at higher temperatures, 22 the additional challenges that must be faced to achieve such degree of control are numerous. These may include nonradiative losses, 23 megavolt per centimeter-strong built-in electric fields, 24 an exponential dependence of the lifetime on the exciton density under high excitation conditions, [25][26][27] and the guided-and-scattered light that must be distinguished from the exciton photoluminescence (PL). 17,28 In this letter we overcome those challenges and report on the realization of ∼ 10 µm ×50 µm-size thermalized exciton fluid, trapped in the plane of a GaN/(GaAl)N quantum well grown on a free-standing GaN substrate.…”
mentioning
confidence: 99%
“…12,13 While excitons in GaN-based nanostructures have relatively high binding energies and small Bohr radii 21 (as compared to GaAs-based structures) and thus could exhibit quantum properties at higher temperatures, 22 the additional challenges that must be faced to achieve such degree of control are numerous. These may include nonradiative losses, 23 megavolt per centimeter-strong built-in electric fields, 24 an exponential dependence of the lifetime on the exciton density under high excitation conditions, [25][26][27] and the guided-and-scattered light that must be distinguished from the exciton photoluminescence (PL). 17,28 In this letter we overcome those challenges and report on the realization of ∼ 10 µm ×50 µm-size thermalized exciton fluid, trapped in the plane of a GaN/(GaAl)N quantum well grown on a free-standing GaN substrate.…”
mentioning
confidence: 99%
“…The fits for the LD, MD, and HD samples are presented in Section S4 in the Supporting Information. The strong dependence of the time constants on the pump fluence points to recombination processes like Auger recombination, which is typical for semiconductors with large carrier densities …”
Section: Resultsmentioning
confidence: 99%
“…20,21 Given the large exciton binding energy in InGaN quantum wells due to a strong quantum confinement effect, 22 the presence of both free carriers and excitons should be considered in density dependent carrier dynamics studies, which has recently been suggested. 12,23,24 Even at room temperature, a rapid formation of excitons results in a significant exciton fraction in the total carrier population in InGaN quantum wells, as quantitatively calculated by Hangleiter et al 24 Blancon et al recently 25 proposed that the lower energy states at the layer edges/surface area of perovskite nanoplatelets could directly facilitate exciton dissociation.…”
Section: Introductionmentioning
confidence: 90%
“…6,[9][10][11] However, detailed analyses of carrier dynamics are still unable to explain the change in luminescence properties of MQW nanorods over planar layers with respect to their carrier density dependence. [12][13][14][15] In particular, the impact of the significant increase of surface states in nanorods is not fully understood. A significant enhancement in the PL efficiency of nanorods is in contrast to the fact that enhanced non-radiative recombinationexpected in nanorods due to surface damage is actually detrimental to the radiative efficiency.…”
Section: Introductionmentioning
confidence: 99%