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    <dc:date>2013-05-25T02:13:23Z</dc:date>
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    <title>In front of the sea</title>
    <link>http://hdl.handle.net/2117/10512</link>
    <description>Title: In front of the sea
Authors: Bru Bistuer, Eduard</description>
    <dc:date>2010-12-09T16:49:35Z</dc:date>
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  <item rdf:about="http://hdl.handle.net/2117/10511">
    <title>Universitat Politècnica de Catalunya: Escola Tècnica Superior d’Arquitectura de Barcelona</title>
    <link>http://hdl.handle.net/2117/10511</link>
    <description>Title: Universitat Politècnica de Catalunya: Escola Tècnica Superior d’Arquitectura de Barcelona
Authors: Bru Bistuer, Eduard</description>
    <dc:date>2010-12-09T16:33:22Z</dc:date>
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  <item rdf:about="http://hdl.handle.net/2117/792">
    <title>Canonical Homotopy Operators for @ in the Ball with Respect to the Bergman Metric</title>
    <link>http://hdl.handle.net/2117/792</link>
    <description>Title: Canonical Homotopy Operators for @ in the Ball with Respect to the Bergman Metric
Authors: Andersson, Mats; Ortega Cerdà, Joaquim
Abstract: We notice that some well-known homotopy operators due to Skoda et. al. for&#xD;
the $\bar\partial$-complex in the ball actually give the boundary values&#xD;
of the canonical homotopy operators with respect to certain weighted&#xD;
Bergman metrics. We provide explicit formulas even for the interior values&#xD;
of these operators. The construction is based on a technique of&#xD;
representing a $\bar\partial$-equation as a $\bar\partial_b$-equation on the&#xD;
boundary of the ball in a higher dimension. The kernel corresponding to&#xD;
the operator that is canonical with respect to the Euclidean metric was&#xD;
previously found by Harvey and Polking. Contrary to the Euclidean case,&#xD;
any form which is smooth up to the boundary belongs to the domain of the&#xD;
corresponding operator $\bar\partial^*$, with respect to the metrics we&#xD;
consider. We also discuss the corresponding $\bar\square$-operator and its&#xD;
canonical solution operator. &#xD;
&#xD;
Moreover, our homotopy operators satisfy a certain commutation rule with&#xD;
the Lie derivative with respect to the vector fields&#xD;
$\partial/\partial\zeta_k$, which makes it possible to construct homotopy&#xD;
formulas even for the $\partial\bar\partial$-operator.</description>
    <dc:date>2007-04-27T18:30:39Z</dc:date>
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