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| | [No title] (Site not responding. Last check: 2007-10-31) |
 | | We have orthogonal bases, for the full Hilbert space, or just for a (closed) linear subspace of a Hilbert space (non-complete ONS), as the most "beautiful" systems for signal expansions (orthogonal expansions are trivial, however it might be tricky to find a good orthogonal system with certain properties, such as a wavelet basis). |
 | | We can also summarize by saying, that in the frame case, the Hilbert space is the "small" one, and l2(I) is the big one, and conversely, in the case of the Riesz basis, the Hilbert space is the small one. |
 | | In that case we have a symmetric situation, each spaces is identified with a closed subspace of the other, without forcing the two spaces to be "naturally" identified. |
| www.mat.univie.ac.at /~fei/abs/moresymm2.txt (1740 words) |
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