<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>The hyperbolic/elliptic transition in the multi-dimensional Riemann problem</dc:title>
<dc:creator>Heinrich Freistuehler</dc:creator><dc:creator>D. Serre</dc:creator>
<dc:subject>35L67</dc:subject><dc:subject>35L65</dc:subject><dc:subject>conservation laws</dc:subject><dc:subject>rarefaction waves</dc:subject><dc:subject>Riemann problem</dc:subject>
<dc:description>For a continuous self-similar solution to a system of conservation laws, genuine nonlinearity yields Lipschitz continuity at points where the type of the governing system changes. This is a well-known fact in one space dimension, where a constant state $\bar{u}$ bifurcates towards a rarefaction wave at a point $x/t$ that equals an eigenvalue $\lambda_j(\bar{u})$. We extend this observation to several space dimensions. The result generalizes a calculation that Bae, Chen, and Feldman [\textit{Regularity of solutions to regular shock reflection for potential flow}, Invent. Math. \textbf{175} (2009), no. 3, 505--543] carried out in their paper (see their Theorem 4.2) in two space dimensions for an irrotational gas. 

As a corollary, we find the astonishing fact that a genuinely $3$D rarefaction wave matches a constant state in a $C^1$-way, rather than a Lipschitz-way.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2013</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2013.62.4918</dc:identifier>
<dc:source>10.1512/iumj.2013.62.4918</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 62 (2013) 465 - 485</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>