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Transform coding techniques for lossy hyperspectral data compression

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IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING (SUBMITTED DEC. 2005) 11<br />

akin to per<strong>for</strong>ming a 3D rate-distortion optimization, which is known to provide significantly better<br />

results than band-by-band optimization [16].<br />

The per<strong>for</strong>mance evaluation is carried out on 16-bit radiance AVIRIS <strong>data</strong> cubes. AVIRIS scenes<br />

have 224 bands and 614 × 512 pixels resolution, but each scene has been cropped to 256 × 256 × 224<br />

pixels. Scene 4 of Cuprite and scene 3 of Jasper Ridge have been employed; <strong>for</strong> brevity, we only<br />

report the set of results <strong>for</strong> Cuprite.<br />

B. Energy compaction results<br />

For clarity, in Tab. I we summarize the acronyms used in the figures to identify the eight 3D<br />

trans<strong>for</strong>ms that have been evaluated.<br />

TABLE I<br />

ACRONYMS OF THE EVALUATED TRANSFORMS<br />

Acronym<br />

DWT3D<br />

DWP3D<br />

DWT1D2D<br />

DWP1D-DWT2D<br />

DWP1D-DWP2D<br />

DWT1D-DWP2D<br />

DCT1D-DWT2D<br />

KLT1D-DWT2D<br />

Sect.<br />

II.E.1<br />

II.E.2<br />

II.E.3<br />

II.E.4<br />

II.E.5<br />

II.E.6<br />

II.E.7<br />

II.E.8<br />

We anticipate that, not surprisingly, we have found that the spectral correlation plays a crucial role<br />

<strong>for</strong> <strong>compression</strong>, since the trans<strong>for</strong>ms that are better able to capture this correlation are those that<br />

rank best <strong>for</strong> <strong>compression</strong>. It is already known <strong>for</strong> lossless <strong>compression</strong> (see e.g. [25]) that large<br />

bit-rate reductions can be achieved by employing an efficient model of the spectral correlation. As<br />

will be seen, exploiting this correlation in the <strong>lossy</strong> case calls <strong>for</strong> the use of separate spectral and<br />

spatial trans<strong>for</strong>ms.<br />

In Fig. 5 we compare the DWT3D and DWP3D trans<strong>for</strong>ms. Neither trans<strong>for</strong>m is computed<br />

separately in the spectral dimension. As can be seen, the rate-distortion curve of the DWP3D trans<strong>for</strong>m<br />

is significantly better than that of the DWT3D. This is due to the fact that the 3D square wavelet<br />

trans<strong>for</strong>m is isotropic in all three dimension. This may not be the most appropriate correlation model<br />

of a <strong>hyperspectral</strong> <strong>data</strong>set, since the subband decomposition in the spectral dimension is not as fine as<br />

it could be. Hence, because of the rather rough tessellation of 3D frequency space, the DWT3D turns

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