2005
DOI: 10.1103/physrevb.72.035416
|View full text |Cite
|
Sign up to set email alerts
|

Continuum modeling of sputter erosion under normal incidence: Interplay between nonlocality and nonlinearity

Abstract: Under specific experimental circumstances, sputter erosion on semiconductor materials exhibits highly ordered hexagonal dot-like nanostructures. In a recent attempt to theoretically understand this pattern forming process, Facsko et al. [Phys. Rev. B 69, 153412 (2004)] suggested a nonlocal, damped Kuramoto-Sivashinsky equation as a potential candidate for an adequate continuum model of this self-organizing process. In this study we theoretically investigate this proposal by (i) formally deriving such a nonloca… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
37
0

Year Published

2006
2006
2015
2015

Publication Types

Select...
5
3

Relationship

2
6

Authors

Journals

citations
Cited by 32 publications
(38 citation statements)
references
References 22 publications
0
37
0
Order By: Relevance
“…Modeling stochastic fluctuations in the sputtering process by Gaussian white noise with covariance 2D, the general form of a balance equation reads ‫ץ‬ t H = ١ · J H + F + . In our former contributions 19,24 we expanded the detachment contribution F to lowest order in linear and nonlinear terms. From a systematic point of view, it is more stringent to expand the linear terms up to fourth order in ١, since ١ · J H is of order four in ١.…”
Section: ͑3͒mentioning
confidence: 99%
See 1 more Smart Citation
“…Modeling stochastic fluctuations in the sputtering process by Gaussian white noise with covariance 2D, the general form of a balance equation reads ‫ץ‬ t H = ١ · J H + F + . In our former contributions 19,24 we expanded the detachment contribution F to lowest order in linear and nonlinear terms. From a systematic point of view, it is more stringent to expand the linear terms up to fourth order in ١, since ١ · J H is of order four in ١.…”
Section: ͑3͒mentioning
confidence: 99%
“…͑1͒, i.e., with a 0 =0,a 1x = a 1y , a 3x = a 3y , has already been successfully employed to describe pattern formation under normal incidence of the ion beam. [23][24][25] In a shifted frame of reference, Eq. ͑1͒ becomes local and reads in dimensionless variables ‫ץ‬ t h = − ͑␥ + ‫ץ‬ x 2 + ‫ץ␣‬ y 2 + ٌ 4 ͒h + ‫ץ͑‬ x h͒ 2 + ‫ץ͑␤‬ y h͒ 2 + .…”
mentioning
confidence: 99%
“…As a consequence of [15,16] Possible anisotropies stemming from ion-induced surface diffusion are at this stage neglected.…”
mentioning
confidence: 99%
“…R into the model leads to a vast number of coefficients in combination with the Kuramoto-Sivashinsky equation by what it cannot be considered as minimal model anymore. However, the derivation of the Kuramoto-Sivashinsky equation as erosion model is typically achieved by a systematic expansion in terms compatible with the symmetries to the lowest order [22,38,59]. If F app.…”
Section: Using the Relationsmentioning
confidence: 99%
“…To that end, a variety of generalizations of equation (1) have been proposed and investigated [32][33][34][35][36][37][38][39][40][41][42][43]. The outcome can be concluded as follows: in order to reproduce hexagonally arranged dots with a generalized Kuramoto-Sivashinsky equation, one either has to incorporate a non-local term or couple in an additional surface composition equation [36,37].…”
Section: Introductionmentioning
confidence: 99%