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  <title>DSpace Collection:</title>
  <link rel="alternate" href="http://www.openstarts.units.it:80/dspace/handle/10077/4388" />
  <subtitle />
  <id>http://www.openstarts.units.it:80/dspace/handle/10077/4388</id>
  <updated>2013-05-21T15:05:38Z</updated>
  <dc:date>2013-05-21T15:05:38Z</dc:date>
  <entry>
    <title>A noncooperative mixed parabolic-elliptic system and positivity</title>
    <link rel="alternate" href="http://www.openstarts.units.it:80/dspace/handle/10077/4659" />
    <author>
      <name>Sweers, Guido</name>
    </author>
    <id>http://www.openstarts.units.it:80/dspace/handle/10077/4659</id>
    <updated>2012-11-21T08:43:05Z</updated>
    <published>1994-01-01T00:00:00Z</published>
    <summary type="text">Title: A noncooperative mixed parabolic-elliptic system and positivity
Authors: Sweers, Guido
Abstract: Per quanto concerne la positività, i sistemi cooperativi ellittici e parabolici si comportano come le corrispondenti equazioni: una sorgente positiva implica che la soluzione è positiva. I sistemi con accoppiamento non cooperativo presentano invece un diverso comportamento. Per i sistemi ellittici non cooperativi sussiste un risultato limitato ma uniforme di positività mentre per i sistemi parabolici non cooperativi non esiste alcun risultato di positività. In questo lavoro si esaminano condizioni che assicurino la positività di un sistema intermedio di tipo misto parabolico-ellittico.; Concerning positivity, cooperative elliptic and parabolic systems behave like the corresponding equations: a positive source implies that the solution is positive. Systems with a noncooperative coupling do not yield such type of behaviour. For noncoopemtive elliptic systems there is a restricted but uniform, positivity result and for the noncoopemtive parabolic system there is no positivity result at all. Here we address positivity presenting properties of an intermediate mixed parabolic-elliptic system.
Type: Articolo</summary>
    <dc:date>1994-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Limits of Dirichlet problems in perforated domains: a new formulation</title>
    <link rel="alternate" href="http://www.openstarts.units.it:80/dspace/handle/10077/4658" />
    <author>
      <name>Dal Maso, G.</name>
    </author>
    <author>
      <name>Toader, R.</name>
    </author>
    <id>http://www.openstarts.units.it:80/dspace/handle/10077/4658</id>
    <updated>2012-11-21T11:30:05Z</updated>
    <published>1994-01-01T00:00:00Z</published>
    <summary type="text">Title: Limits of Dirichlet problems in perforated domains: a new formulation
Authors: Dal Maso, G.; Toader, R.
Abstract: Sia A un operatore ellittico lineare del secondo ordine con coefficienti&#xD;
misurabili e limitati su un aperto limitato $\Omega$ di $\mathbf{R}^{\textrm{n}}$&#xD;
, sia &#xD;
\[&#xD;
K*=\{w*\epsilon H_{0}^{1}\left(\Omega\right):A*w*\leq1\, in\,\mathcal{D}'\left(\Omega\right)\qquad,&#xD;
\]&#xD;
\[&#xD;
e,\, w*\geq0\, a.e.\, in\,\Omega\}\qquad,&#xD;
\]&#xD;
 e sia $\Omega_{h}$ un'arbitraria successione di sottoinsiemi aperti&#xD;
di $\Omega$. Dimostriamo il seguente risultato di compattezza: esistono&#xD;
una sottosuccessione, che indichiamo ancora con $\Omega_{h}$ ed una&#xD;
funzione w{*} $\epsilon$ K{*} tali che, per ogni f $\epsilon L^{\infty}\left(\Omega\right)$&#xD;
, le soluzioni u$_{h}\epsilon H_{0}^{1}\left(\Omega_{h}\right)$ delle&#xD;
equazioni Au$_{h}$ = f in $\Omega_{h}$ , estese a zero su $\Omega/\Omega_{h}$,&#xD;
convergano debolmente in $H_{0}^{1}\left(\Omega\right)$ all'unica&#xD;
soluzione u del problema.&#xD;
\[&#xD;
\left(*\right)\begin{cases}&#xD;
\begin{array}{c}&#xD;
u\epsilon H_{0}^{1}\left(\Omega\right)\cap L^{\infty}\left(\Omega\right)\\&#xD;
\left\langle Au,\, w*\varphi\right\rangle -\left\langle A*w*,\, u\varphi\right\rangle +\left\langle 1,u\varphi\right\rangle =\left\langle f,w*\varphi\right\rangle \:\forall\varphi\epsilon C_{0}^{\infty}\left(\Omega\right)&#xD;
\end{array}\end{cases}&#xD;
\]&#xD;
 Studiamo inoltre in maniera sistematica le proprietà delle soluzioni&#xD;
di tale equazione. Dimostriamo infine il seguente risultato di densità:&#xD;
per ogni w{*}$\epsilon$K{*} esiste una successione $\Omega_{h}$&#xD;
di sottoinsiemi aperti di $\Omega$ tali che per ogni f $\epsilon L^{\infty}\left(\Omega\right)$&#xD;
le soluzioni u$_{h}\epsilon H_{0}^{1}\left(\Omega_{h}\right)$ dell'equazione&#xD;
Au$_{h}$=f in $\Omega_{h}$, estese a zero $\Omega/\Omega_{h}$ convergano&#xD;
debolmente in $H_{0}^{1}\left(\Omega\right)$alla soluzione di ({*}).; Let A be a linear elliptic operator of the second order with bounded&#xD;
measurable coefficients on a bounded open set $\Omega$ of $\mathbf{R}^{\textrm{n}}$&#xD;
, let &#xD;
\[&#xD;
K*=\{w*\epsilon H_{0}^{1}\left(\Omega\right):A*w*\leq1\, in\,\mathcal{D}'\left(\Omega\right)\qquad,&#xD;
\]&#xD;
\[&#xD;
e,\, w*\geq0\, a.e.\, in\,\Omega\}\qquad,&#xD;
\]&#xD;
 and let $\Omega_{h}$ be an arbitrary sequence of open subsets of&#xD;
$\Omega$. We prove the following compactness result: there exist&#xD;
a subsequence, still denoted by $\Omega_{h}$ and a function w{*}&#xD;
$\epsilon$ K{*} such that, for every f $\epsilon L^{\infty}\left(\Omega\right)$&#xD;
, the solutions u$_{h}\epsilon H_{0}^{1}\left(\Omega_{h}\right)$&#xD;
of the equation Au$_{h}$ = f in $\Omega_{h}$ , extended by zero&#xD;
on $\Omega/\Omega_{h}$, converge weakly in $H_{0}^{1}\left(\Omega\right)$&#xD;
to the unique solution u of the problem.&#xD;
\[&#xD;
\left(*\right)\begin{cases}&#xD;
\begin{array}{c}&#xD;
u\epsilon H_{0}^{1}\left(\Omega\right)\cap L^{\infty}\left(\Omega\right)\\&#xD;
\left\langle Au,\, w*\varphi\right\rangle -\left\langle A*w*,\, u\varphi\right\rangle +\left\langle 1,u\varphi\right\rangle =\left\langle f,w*\varphi\right\rangle \:\forall\varphi\epsilon C_{0}^{\infty}\left(\Omega\right)&#xD;
\end{array}\end{cases}&#xD;
\]&#xD;
 We provide a self-contained study of the properties of the solutions&#xD;
of ({*}). We prove also the following density result: for any w{*}$\epsilon$K{*}&#xD;
there exists a sequence $\Omega_{h}$ of open subsets of $\Omega$&#xD;
such that for every f $\epsilon L^{\infty}\left(\Omega\right)$ the&#xD;
solutions u$_{h}\epsilon H_{0}^{1}\left(\Omega_{h}\right)$ of the&#xD;
equation Au$_{h}$=f in $\Omega_{h}$, extended by zero on $\Omega/\Omega_{h}$&#xD;
converge weakly in $H_{0}^{1}\left(\Omega\right)$to the solution&#xD;
of ({*}).
Type: Articolo</summary>
    <dc:date>1994-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>On the commutativity of s-unital rings and periodical rings</title>
    <link rel="alternate" href="http://www.openstarts.units.it:80/dspace/handle/10077/4657" />
    <author>
      <name>Giri, R. D.</name>
    </author>
    <author>
      <name>Tiwari, Shraddha</name>
    </author>
    <id>http://www.openstarts.units.it:80/dspace/handle/10077/4657</id>
    <updated>2012-11-21T11:44:29Z</updated>
    <published>1994-01-01T00:00:00Z</published>
    <summary type="text">Title: On the commutativity of s-unital rings and periodical rings
Authors: Giri, R. D.; Tiwari, Shraddha
Abstract: In questo lavoro vengono provati due teoremi relativi alla commutatività di anelli s-unitali e di anelli periodici.; In this paper two theorems have been proved for the commutativity of s-unital rings and periodic rings respectively.
Type: Articolo</summary>
    <dc:date>1994-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Constant obstacle problem and rearrangements</title>
    <link rel="alternate" href="http://www.openstarts.units.it:80/dspace/handle/10077/4655" />
    <author>
      <name>Ravaglia, Carlo</name>
    </author>
    <id>http://www.openstarts.units.it:80/dspace/handle/10077/4655</id>
    <updated>2012-11-21T08:54:48Z</updated>
    <published>1994-01-01T00:00:00Z</published>
    <summary type="text">Title: Constant obstacle problem and rearrangements
Authors: Ravaglia, Carlo
Abstract: Problema con ostacolo costante e riordinamenti. Si dà una maggiorazione della misura dell'insieme di contatto della soluzione di una disequazione variazionale con ostacolo costante, con un operatore ellittico del secondo ordine contenente i termini di ordine inferiore.; We give an upper bound for the measure of the coincidence set of the solution of a variational inequality with constant obstacle, related to an elliptic second order operator with lower-order terms.
Type: Articolo</summary>
    <dc:date>1994-01-01T00:00:00Z</dc:date>
  </entry>
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