Hilbert spaces formed by strongly harmonizable stable processes (Q2726706)
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scientific article; zbMATH DE number 1621377
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Hilbert spaces formed by strongly harmonizable stable processes |
scientific article; zbMATH DE number 1621377 |
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19 December 2001
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strongly harmonizable stable process
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time domain
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prediction
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0.89702594
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0.88817227
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0.8828815
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0.87714577
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0.87355185
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Hilbert spaces formed by strongly harmonizable stable processes (English)
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Let \(X= \{X(t), t\in{\mathbf R}\}\) be a strongly harmonizable symmetric \(\alpha\)-stable process which is the Fourier transform of a S\(\alpha X\)S random measure with independent increments \(\Phi\), NEWLINE\[NEWLINEX(t)= \int^\infty_{-\infty} e^{it\lambda}\Phi(d\lambda).NEWLINE\]NEWLINE The closed linear span of \(X(t)\), \(t\in{\mathbf R}\), under the Schilder's norm \(({\mathcal A},\|\cdot\|)_\alpha)\) is the time domain of the process which is a Banach space of jointly S\(\alpha\)S random variables. If \({\mathcal S}_0\) is the linear span of the elements of the set \(\{X(t), t\in{\mathbf R}\}\), a scalar product \(\langle\cdot,\cdot\rangle\) is defined. It is proved that the completion of \(({\mathcal S}_0,\langle\cdot, \cdot\rangle)\) is a Hilbert space, \(({\mathcal S},\langle\cdot,\cdot\rangle_{\mathcal S})\), of jointly symmetric stable random variables with certain properties. Furtheron a moving average representation against a stable random measure \(Z\) exists in \({\mathcal S}\), and \(Z\) has orthogonal increments in \(({\mathcal S},\langle\cdot, \cdot\rangle_{{\mathcal S}})\). The best linear predictor of \(X(t+ T)\) based on \(\{X_s, s\leq t\}\) is given in spectral form and in moving average form.
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