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Master Thesis - Department of Computer Science

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(a) (b)<br />

Figure A.6: Frequency images (after filtering) <strong>of</strong> two input fingerprints shown in<br />

Fig. A.2.<br />

where φ is the orientation <strong>of</strong> the Gabor filter, f is the frequency <strong>of</strong> a sinusoidal plane<br />

wave, and δx and δy are the space constants <strong>of</strong> the Gaussian envelope along x and y<br />

axes, respectively. The modulation transfer function (MTF) <strong>of</strong> the Gabor filter can<br />

be represented as,<br />

H(u, v : φ, f) =<br />

�<br />

2πδxδyexp − 1<br />

�<br />

(uφ − u0)<br />

2<br />

2<br />

δ2 +<br />

u<br />

(vφ − v0) 2<br />

δ2 +<br />

��<br />

v<br />

�<br />

2πδxδyexp −<br />

(A.22)<br />

1<br />

�<br />

(uφ + u0)<br />

2<br />

2<br />

δ2 +<br />

u<br />

(vφ + v0) 2<br />

δ2 ��<br />

,<br />

v<br />

(A.23)<br />

uφ = u cos φ + v sin φ, (A.24)<br />

vφ = −u sin φ + v cos φ, (A.25)<br />

u0 =<br />

2π cos φ<br />

,<br />

f<br />

(A.26)<br />

v0 =<br />

2π sin φ<br />

.<br />

f<br />

(A.27)<br />

where δu = 1/2πδx and δv = 1/2πδy. To apply Gabor filters to an image, three<br />

parameters must be specified:<br />

• The frequency, f,<br />

• The filter orientation φ, and<br />

• The standard deviations <strong>of</strong> the Gaussian envelope, δx and δy.<br />

In this case, the frequency <strong>of</strong> the filter is given by local ridge frequency and the<br />

orientation by local ridge orientation. The selection <strong>of</strong> the values <strong>of</strong> δx and δy involves<br />

130

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