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Classification of Fractal Antenna Radiation Patterns by the Spectrum Enhancement Algorithm

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Classification of Fractal Antenna Radiation Patterns by the Spectrum Enhancement Algorithm

Giovanni F. Crosta

Inverse Problems & Mathematical Morphology Unit

Department of Environmental Sciences - University of Milan-Bicocca 1, piazza della Scienza - Milan, IT 20126

Giovanni Crosta@uml.edu

Spectrum enhancement. Let g denote a scalar function which is at least continuous on the sur- face T of a torus. Let u ≡ {u

1

, u

2

} denote the spatial frequency vector and G[u] the (distribution- valued) Fourier transform of g. The spectrum enhancement (SE ) algorithm, which was intro- duced a few years ago [e.g., ??] consists of suitable transformations of the function H

(p)

[u] :=

|u|

2β |G[u]||a 2

0,0|2

+ δ[u], where δ is the Dirac measure, a

0,0

is the Fourier amplitude at the origin such that F (g)[0] = a

0,0

δ[u], β ∈ R

+

is the enhancement order and β = 2p. It has been recently shown that SE is related to Fourier transforms of derivatives of g[.], which are of integer order whenever β ∈ N [??] and of fractional order otherwise (β / ∈ N) [??]. Herewith, the role played by the enhancement order β in the fractal analysis of g[.] will be described.

Fractal radiation patterns. Array antennas exhibiting fractal radiation patterns are synthesized by means of generalized Weierstraß functions [??]. For example, in one spatial dimension (x

1

) one has

f [x

1

] :=

X

m=1

η

(D−2)m

h[η

m

x

1

]

where 1 < D < 2, η > 1 and h[.] is a suitably chosen bounded, periodic function of one variable.

It can be shown that the box-counting (B) fractal dimension (dim

B

) of the graph of f [.] (graph[f ]) satisfies dim

B

[graph[f ]] = D. Two-dimensional fractal radiation patterns can be synthesized in a similar way e.g., by separation of variables.

Recognition of fractal radiation patterns. Let simulated or measured radiation patterns be available on the whole surface of the unit sphere or part thereof. Let the pattern dim

B

be un- known or assume the pattern has to be classified by fractal dimension. The SE algorithm can be used to extract features from said patterns and estimate their dim

B

. Moreover, patterns can be classified by a procedure which includes supervised training. Some preliminary classification and recognition results will be provided, based on numerically synthesized fractal radiation patterns.

REFERENCES

[1] G. F. Crosta, C. Urani, L. Fumarola, J. Biomed. Optics, 11 (2), pp. 024020.1 - 024020.18, 2006.

[2] G. F. Crosta, ”Feature Extraction by Differentiation of Fractional Order”, in J. Au Kong et al., Eds., Progr. in Electromag. Res. Symp. 2006 Abstracts, Electromagnetics Academy:

Cambridge, MA, 2006, p 425.

[3] G. F. Crosta, ”Morphological Characterization of Two-dimensional Random Media and Patterns by Fractional Differentiation”, in J. Au Kong et al., Eds., Progr. in Electromag.

Res. Symp. 2008 Abstracts, Electromagnetics Academy: Cambridge, MA, 2008, p 627.

[4] D. H. Werner, P. L. Werner, Radio Science, 30 (1), pp. 29-45, 1995.

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