2014
DOI: 10.1063/1.4838059
|View full text |Cite
|
Sign up to set email alerts
|

Phonons and defects in semiconductors and nanostructures: Phonon trapping, phonon scattering, and heat flow at heterojunctions

Abstract: Defects in semiconductors introduce vibrational modes that are distinct from bulk modes because they are spatially localized in the vicinity of the defect. Light impurities produce high-frequency modes often visible by Fourier-transform infrared absorption or Raman spectroscopy. Their vibrational lifetimes vary by orders of magnitude and sometimes exhibit unexpectedly large isotope effects. Heavy impurities introduce low-frequency modes sometimes visible as phonon replicas in photoluminescence bands. But other… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
35
0

Year Published

2015
2015
2024
2024

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 41 publications
(36 citation statements)
references
References 35 publications
1
35
0
Order By: Relevance
“…The pure dephasing time between the VBM, the CBM, and the defect states for different systems. References (61)(62)(63)(64)(65)(66)(67)(68)(69)…”
Section: Supplementary Materialsmentioning
confidence: 99%
“…The pure dephasing time between the VBM, the CBM, and the defect states for different systems. References (61)(62)(63)(64)(65)(66)(67)(68)(69)…”
Section: Supplementary Materialsmentioning
confidence: 99%
“…The different behavior of phonons within structures with dislocations might be related with different spatially localized modes associate with the different types of dislocations [27]. It is not on the scope of the current study, but it will be interesting to investigate the dynamic properties of defects as the vibrational lifetimes of phonons trapped in each kind of dislocations [26,27,28,65].…”
Section: Temperature Dependence Of the Thermal Conductivitymentioning
confidence: 99%
“…It is known that doping impurities in semiconductors will induce IPMs, which mainly couples with the impurity bands and may scatter and couple with bulk phonon modes . These modes can be determined by calculating the phonon spatial localization (labeled as L ) . The localization of the phonon mode s on the (group of) atom(s) α is Lαs=J=x,y,zIαeIJs2, where eIJs is the eigenvector of the dynamical matrix corresponds to the phonon mode s .…”
Section: Electron–hole Recombination In Doped Semiconductormentioning
confidence: 99%