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| | [No title] |
 | | Similarly, a {\it spectral measure} of a half-line problem is, by definition, a measure $\rho$ for which $U$ is an isometry from $L_2(0,N)$ to $L_2(\mathbb R, d\rho)$ for all $N>0$. |
 | | In the limit circle case, the measures from the Weyl circle construction are again spectral measures in this wider sense, but there are many other spectral measures. |
 | | The measures from $\mathcal{M}_N$ are sometimes also called spectral measures of the problem on $[0,N]$ (for example in \cite{Mar,RemdB}), but here it is better to avoid this usage of the term, in order to avoid confusion with the spectral measures $\rho_{\beta}$, $\beta\in [0,\pi)$, introduced above, which form a (small) subset of $\mathcal{M}_N$. |
| www.ma.utexas.edu /mp_arc/papers/02-394 (3070 words) |
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