2005
DOI: 10.1103/physrevb.71.075324
|View full text |Cite
|
Sign up to set email alerts
|

Hot-phonon effect on power dissipation in a biasedAlxGa1xNAlN

Abstract: The Monte Carlo simulation of hot-electron energy dissipation is carried out for a biased AlGaN / AlN / GaN channel. The conduction band profile and electron wave functions are calculated through self-consistent solution of Poisson and Schrödinger equations. Nonelastic scattering of electrons on acoustic phonons and nonequilibrium longitudinal optical ͑LO͒ phonons is included. The nonequilibrium LO phonons are treated in terms of hot-phonon lifetime. The dependence of electron temperature and dissipated power … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

6
87
0

Year Published

2006
2006
2023
2023

Publication Types

Select...
9
1

Relationship

3
7

Authors

Journals

citations
Cited by 80 publications
(93 citation statements)
references
References 27 publications
(24 reference statements)
6
87
0
Order By: Relevance
“…The estimated electron number in the channel is N e = 4.9·10 7 . The electron volume density is around n ∼ 10 19 cm −3 : the effective quantum well width is not known, and the value d = 4.8 nm is assumed (this value is available from calculations for a similar 2DEG channel [11]). The contact resistance is taken into account when the applied electric field and the noise temperature are estimated.…”
Section: Samplementioning
confidence: 99%
“…The estimated electron number in the channel is N e = 4.9·10 7 . The electron volume density is around n ∼ 10 19 cm −3 : the effective quantum well width is not known, and the value d = 4.8 nm is assumed (this value is available from calculations for a similar 2DEG channel [11]). The contact resistance is taken into account when the applied electric field and the noise temperature are estimated.…”
Section: Samplementioning
confidence: 99%
“…2. The profile was considered to be similar to that calculated for the same type heterostructure [7]. A strong (of the order of tens of kv/cm) electric field parallel to the heterointerfaces was applied to the samples.…”
Section: Sample Characterizationmentioning
confidence: 99%
“…Hot phonons complicate the problem further on: the LOphonon distribution differs from the equilibrium one. Fortunately, at a high density of electron gas present in a 2D channel, the hot-electron temperature approximation holds [23,24]. Moreover, a quasi-equilibrium hot subsystem forms because of intense electron-LOphonon scattering [19].…”
Section: Fluctuation Techniquementioning
confidence: 99%