2014
DOI: 10.1002/pssb.201350039
|View full text |Cite
|
Sign up to set email alerts
|

Influence of electron scattering on phonon-plasmon coupled modes dispersion and free-electron absorption in n-doped GaN semiconductors at mid-IR wavelengths

Abstract: The model to calculate the free‐carrier absorption coefficient for polar III–V semiconductors with strong LO phonon–plasmon interaction was generalized by taking into account free‐carrier scattering by defects The following main mechanisms assisting in the photon absorption process, where taken into account: thermal phonon‐like branch and plasmon‐like branch scattering, impurity scattering, and acoustic phonon scattering. To calculate the contributions of phonon–plasmon coupled modes into the absorption coeffi… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
3
0
1

Year Published

2016
2016
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 9 publications
(4 citation statements)
references
References 30 publications
0
3
0
1
Order By: Relevance
“…If ωр and ω LO are close then the independent plasmons and longitudinal optical phonons which existed earlier are replaced by coupled plasmon-phonon modes [13][14][15][16][17][18][19][20][21][22][23][24][25][26] whose frequencies (where ω + is the high-frequency one and ωis the low-frequency one) can easily be calculated using the following formula (plasmon and LO phonon damping is disregarded):…”
Section: Methodsmentioning
confidence: 99%
“…If ωр and ω LO are close then the independent plasmons and longitudinal optical phonons which existed earlier are replaced by coupled plasmon-phonon modes [13][14][15][16][17][18][19][20][21][22][23][24][25][26] whose frequencies (where ω + is the high-frequency one and ωis the low-frequency one) can easily be calculated using the following formula (plasmon and LO phonon damping is disregarded):…”
Section: Methodsmentioning
confidence: 99%
“…The lower intensity of reflectivity can be found in Figure 3(b), where nanostructured film tends to have greater volume fraction of air. In the meantime, the spectra revealed a dip at approximately 620 cm -1 corresponds to the coupled phonon-plasmon mode arising from the impurity scattering happened at the lateral surface [22,23]. The obtained value was shifted from the reported longitudinal-optical (LO) phonon mode 590 cm -1 towards higher frequency.…”
Section: Resultsmentioning
confidence: 75%
“…N opt was calculated from far IR reflection spectra (plasma resonance) [2][3][4][5][6] taking into account the interaction of plasma oscillations with longitudinal optical phonons (the plasmon-phonon coupling) [7][8][9][10][11][12][13][14][15][16][17]. The wavenumber dependence of the reflection spectrum R(n) was recorded in the 340-1000 cm -1 spectral range with a Tensor-27 Fourier spectrometer.…”
Section: Methodsmentioning
confidence: 99%