<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>Pointwise convergence of solutions to the nonelliptic Schrodinger equation</dc:title>
<dc:creator>Keith Rogers</dc:creator><dc:creator>Ana Vargas</dc:creator><dc:creator>Luis Vega</dc:creator>
<dc:subject>35Q55</dc:subject><dc:subject>42B25</dc:subject><dc:subject>Schr\&quot;odinger equation</dc:subject><dc:subject>pointwise convergence</dc:subject>
<dc:description>It is conjectured that the solution to the Schr\&quot;odinger equation in $\mathbb{R}^{n+1}$ converges almost everywhere to its initial datum $f$, for all $f \in H^{s}(\mathbb{R}^n)$, if and only if $s \ge \frac{1}{4}$. It is known that there is an $s &lt; \frac{1}{2}$ for which the solution converges for all $f \in H^{s}(\mathbb{R}^{2})$. We show that the solution to the nonelliptic Schr\&quot;odinger equation, $i\partial_{t}u + (\partial^{2}_{x} - \partial^{2}_{y})u = 0$, converges to its initial datum $f$, for all $f \in H^{s}(\mathbb{R}^{2})$, if and only if $s \ge \frac{1}{2}$. Thus the pointwise behaviour is worse than that of the standard Schr\&quot;odinger equation. In higher dimensions, we have similar results with the loss of the endpoint.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2006</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2006.55.2827</dc:identifier>
<dc:source>10.1512/iumj.2006.55.2827</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 55 (2006) 1893 - 1906</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>