<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:title>Unconditional convergence of spectral decompositions of 1D Dirac operators with regular boundary conditions</dc:title>
<dc:creator>Plamen Djakov</dc:creator><dc:creator>Boris Mityagin</dc:creator>
<dc:subject>47E05</dc:subject><dc:subject>34L40</dc:subject><dc:subject>34L10</dc:subject><dc:subject>Dirac operators</dc:subject><dc:subject>Riesz bases</dc:subject><dc:subject>regular boundary conditions</dc:subject>
<dc:description>One-dimensional Dirac operators
\[
L_{bc}(v)y = i\begin{pmatrix}1&amp;\hfill 0\0&amp;-1\end{pmatrix}\frac{\mathrm{d}y}{\mathrm{d}x}+v(x)y,\quad y=\begin{pmatrix}y_1\y_2\end{pmatrix}, x\in[0,\pi],
\]
considered with $L^2$-potentials $v(x) = \left(\begin{smallmatrix}0&amp;P(x)\\Q(x)&amp;0\end{smallmatrix}\right)$ and subject to regular boundary conditions ($bc$), have discrete spectrum.

For strictly regular $bc$, it is shown that every eigenvalue of the free operator $L^0_{bc}$ is simple and has the form $\lambda_{k,\alpha}^0 = k+\tau_{\alpha}$, where $\alpha\in\{1,2\}$, $k\in 2\mathbb{Z}$ and $\tau_{\alpha} = \tau_{\alpha}(bc)$; if $|k| &gt; N(v,bc)$, each of the discs $D_k^{\alpha} = \{z : |z-\lambda_{k,\alpha}^0| &lt; ho = \rho(bc)\}$, $\alpha\in\{1,2\}$, contains exactly one simple eigenvalue $\lambda_{k,\alpha}$ of $L_{bc}(v)$ and $(\lambda_{k,\alpha}-\lambda_{k,\alpha}^0)_{k\in 2\mathbb{Z}}$ is an $\ell^2$-sequence. Moreover, it is proven that the root projections $P_{n,\alpha} = 1/(2\pi i)\int_{\partial D^{\alpha}_n}(z-L_{bc}(v))^{-1}\mathrm{d}z$ satisfy the Bari-Markus condition
\[
\sum_{|n| &gt; N}\|P_{n,\alpha}-P_{n,\alpha}^0\|^2 &lt; \infty,\quad n\in 2\mathbb{Z},
\]
where $P_n^0$ are the root projections of the free operator $L^0_{bc}$. Hence, for strictly regular $bc$, there is a Riesz basis consisting of root functions (all but finitely many being eigenfunctions). Similar results are obtained for regular but not strictly regular $bc$---then in general there is no Riesz basis consisting of root functions, but we prove that the corresponding system of two-dimensional root projections is a Riesz basis of projections.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2012</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2012.61.4531</dc:identifier>
<dc:source>10.1512/iumj.2012.61.4531</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 61 (2012) 359 - 398</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>