Difference between revisions of "Rosinger nowhere-dense generalized function algebra"
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+ | In the general framework of [[Generalized function algebras|generalized function algebras]] developed by E.E. Rosinger [[#References|[a3]]], [[#References|[a4]]], [[#References|[a5]]], [[#References|[a6]]], a distinguished role is played by ideals in the sequence algebra $\mathcal{C} ^ { \infty } ( \Omega ) ^ { \text{N} }$, $\Omega$ an open subset of ${\bf R} ^ { n }$, which are defined by vanishing properties. Given a family $S$ of subsets of $\Omega$, stable under finite unions, one considers the ideal $\mathcal{I} _ { S }$ in $\mathcal{C} ^ { \infty } ( \Omega ) ^ { \text{N} }$ determined by those $( u_j )_{ j \in \mathbf{N}}$ for which there is a $\Gamma \in S$ such that for all $x \in \Omega \backslash \Gamma$, $( u_j )_{ j \in \mathbf{N}}$ vanishes near $x$ eventually, that is, there are a $j _0$ and a neighbourhood $V \subset \Omega \backslash \Gamma$ of $x$ such that $u _ { j } | _ { V } \equiv 0$ for $j \geq j_0$. The nowhere-dense generalized function algebra $\mathcal{R} _ { \text{nd} } ( \Omega ) = \mathcal{C} ^ { \infty } ( \Omega ) ^ { \text{N} } / \mathcal{I} _ { \text{nd} }$ is obtained when $S$ is the class of nowhere-dense, closed subsets of $\Omega$. The space $\mathcal{R} _ { \text{nd} } ( \Omega )$ contains $\mathcal{C} ^ { \infty } ( \Omega )$ via the constant imbedding. It has two distinguishing features. First, the family $\{ \mathcal{R} _ { \text{nd} } ( \Omega ) : \Omega \, \text{open} \}$ forms a [[Flabby sheaf|flabby sheaf]], and in a certain sense the smallest flabby sheaf containing $\mathcal{C} ^ { \infty } ( \Omega )$, see [[#References|[a2]]]. Secondly, the algebra $C _ { \text{nd} } ^ { \infty } ( \Omega )$ of (equivalence classes of) smooth functions defined off some nowhere-dense, closed subset of $\Omega$ can be imbedded into $\mathcal{R} _ { \text{nd} } ( \Omega )$. | ||
− | Replacing the single differential algebra | + | In particular, solutions to partial differential equations defined piecewise off nowhere-dense closed sets $\Gamma$ (no growth restrictions near $\Gamma$) can be interpreted as global solutions in $\mathcal{R} _ { \text{nd} } ( \Omega )$ by means of a suitable regularization method. The space of distributions $\mathcal{D} ^ { \prime } ( \Omega )$ (cf. also [[Generalized functions, space of|Generalized functions, space of]]) is imbedded in any algebra of the form $\mathcal{C} ^ { \infty } ( \Omega ) / \mathcal{I} _ { S }$ by a general procedure [[#References|[a4]]] using an algebraic basis. |
+ | |||
+ | Further generalizations of the ideal $\mathcal{I} _ {\operatorname{nd} }$ to include larger exceptional sets as well as applications to non-smooth differential geometry can be found in [[#References|[a1]]]; non-linear Lie group actions on generalized functions using the framework of $\mathcal{R} _ { \text{nd} } ( \Omega )$ are studied in [[#References|[a7]]]. | ||
+ | |||
+ | Replacing the single differential algebra ${\cal R = C} ^ { \infty } ( \Omega ) / {\cal I} _ { S }$ with chains of algebras $\mathcal{R} ^ { \infty } \rightarrow \ldots \rightarrow \mathcal{R} ^ { m } \rightarrow \ldots \rightarrow \mathcal{R} ^ { 0 }$ using the spaces $\mathcal{C} ^ { m } ( \Omega )$ in the place of $\mathcal{C} ^ { \infty } ( \Omega )$ at each level, allows one to achieve consistency of the multiplication and derivation with the pointwise product of $\mathcal{C} ^ { m }$-functions as well as the derivative of $\mathcal{C} ^ { m + 1 } \rightarrow \mathcal{C} ^ { m }$ at each fixed level $m$. | ||
See also [[Generalized function algebras|Generalized function algebras]]. | See also [[Generalized function algebras|Generalized function algebras]]. | ||
====References==== | ====References==== | ||
− | <table>< | + | <table><tr><td valign="top">[a1]</td> <td valign="top"> A. Mallios, E.E. Rosinger, "Space-time foam dense singularities and de Rham cohomology" ''Acta Applic. Math.'' (to appear) {{MR|1847884}} {{ZBL|1005.46020}} </td></tr><tr><td valign="top">[a2]</td> <td valign="top"> M. Oberguggenberger, E.E. Rosinger, "Solution of continuous nonlinear PDEs through order completion" , North-Holland (1994) {{MR|1286940}} {{ZBL|0821.35001}} </td></tr><tr><td valign="top">[a3]</td> <td valign="top"> E.E. Rosinger, "Distributions and nonlinear partial differential equations" , Springer (1978) {{MR|0514014}} {{ZBL|0469.35001}} </td></tr><tr><td valign="top">[a4]</td> <td valign="top"> E.E. Rosinger, "Nonlinear partial differential equations. Sequential and weak solutions" , North-Holland (1980) {{MR|0590891}} {{ZBL|0447.35001}} </td></tr><tr><td valign="top">[a5]</td> <td valign="top"> E.E. Rosinger, "Generalized solutions of nonlinear partial differential equations" , North-Holland (1987) {{MR|0918145}} {{ZBL|0635.46033}} </td></tr><tr><td valign="top">[a6]</td> <td valign="top"> E.E. Rosinger, "Nonlinear partial differential equations, an algebraic view of generalized solutions" , North-Holland (1990) {{MR|}} {{ZBL|0717.35001}} </td></tr><tr><td valign="top">[a7]</td> <td valign="top"> E.E. Rosinger, "Parametric Lie group actions on global generalized solutions of nonlinear PDEs. Including a solution to Hilbert's fifth problem" , Kluwer Acad. Publ. (1998)</td></tr></table> |
Latest revision as of 16:56, 1 July 2020
In the general framework of generalized function algebras developed by E.E. Rosinger [a3], [a4], [a5], [a6], a distinguished role is played by ideals in the sequence algebra $\mathcal{C} ^ { \infty } ( \Omega ) ^ { \text{N} }$, $\Omega$ an open subset of ${\bf R} ^ { n }$, which are defined by vanishing properties. Given a family $S$ of subsets of $\Omega$, stable under finite unions, one considers the ideal $\mathcal{I} _ { S }$ in $\mathcal{C} ^ { \infty } ( \Omega ) ^ { \text{N} }$ determined by those $( u_j )_{ j \in \mathbf{N}}$ for which there is a $\Gamma \in S$ such that for all $x \in \Omega \backslash \Gamma$, $( u_j )_{ j \in \mathbf{N}}$ vanishes near $x$ eventually, that is, there are a $j _0$ and a neighbourhood $V \subset \Omega \backslash \Gamma$ of $x$ such that $u _ { j } | _ { V } \equiv 0$ for $j \geq j_0$. The nowhere-dense generalized function algebra $\mathcal{R} _ { \text{nd} } ( \Omega ) = \mathcal{C} ^ { \infty } ( \Omega ) ^ { \text{N} } / \mathcal{I} _ { \text{nd} }$ is obtained when $S$ is the class of nowhere-dense, closed subsets of $\Omega$. The space $\mathcal{R} _ { \text{nd} } ( \Omega )$ contains $\mathcal{C} ^ { \infty } ( \Omega )$ via the constant imbedding. It has two distinguishing features. First, the family $\{ \mathcal{R} _ { \text{nd} } ( \Omega ) : \Omega \, \text{open} \}$ forms a flabby sheaf, and in a certain sense the smallest flabby sheaf containing $\mathcal{C} ^ { \infty } ( \Omega )$, see [a2]. Secondly, the algebra $C _ { \text{nd} } ^ { \infty } ( \Omega )$ of (equivalence classes of) smooth functions defined off some nowhere-dense, closed subset of $\Omega$ can be imbedded into $\mathcal{R} _ { \text{nd} } ( \Omega )$.
In particular, solutions to partial differential equations defined piecewise off nowhere-dense closed sets $\Gamma$ (no growth restrictions near $\Gamma$) can be interpreted as global solutions in $\mathcal{R} _ { \text{nd} } ( \Omega )$ by means of a suitable regularization method. The space of distributions $\mathcal{D} ^ { \prime } ( \Omega )$ (cf. also Generalized functions, space of) is imbedded in any algebra of the form $\mathcal{C} ^ { \infty } ( \Omega ) / \mathcal{I} _ { S }$ by a general procedure [a4] using an algebraic basis.
Further generalizations of the ideal $\mathcal{I} _ {\operatorname{nd} }$ to include larger exceptional sets as well as applications to non-smooth differential geometry can be found in [a1]; non-linear Lie group actions on generalized functions using the framework of $\mathcal{R} _ { \text{nd} } ( \Omega )$ are studied in [a7].
Replacing the single differential algebra ${\cal R = C} ^ { \infty } ( \Omega ) / {\cal I} _ { S }$ with chains of algebras $\mathcal{R} ^ { \infty } \rightarrow \ldots \rightarrow \mathcal{R} ^ { m } \rightarrow \ldots \rightarrow \mathcal{R} ^ { 0 }$ using the spaces $\mathcal{C} ^ { m } ( \Omega )$ in the place of $\mathcal{C} ^ { \infty } ( \Omega )$ at each level, allows one to achieve consistency of the multiplication and derivation with the pointwise product of $\mathcal{C} ^ { m }$-functions as well as the derivative of $\mathcal{C} ^ { m + 1 } \rightarrow \mathcal{C} ^ { m }$ at each fixed level $m$.
See also Generalized function algebras.
References
[a1] | A. Mallios, E.E. Rosinger, "Space-time foam dense singularities and de Rham cohomology" Acta Applic. Math. (to appear) MR1847884 Zbl 1005.46020 |
[a2] | M. Oberguggenberger, E.E. Rosinger, "Solution of continuous nonlinear PDEs through order completion" , North-Holland (1994) MR1286940 Zbl 0821.35001 |
[a3] | E.E. Rosinger, "Distributions and nonlinear partial differential equations" , Springer (1978) MR0514014 Zbl 0469.35001 |
[a4] | E.E. Rosinger, "Nonlinear partial differential equations. Sequential and weak solutions" , North-Holland (1980) MR0590891 Zbl 0447.35001 |
[a5] | E.E. Rosinger, "Generalized solutions of nonlinear partial differential equations" , North-Holland (1987) MR0918145 Zbl 0635.46033 |
[a6] | E.E. Rosinger, "Nonlinear partial differential equations, an algebraic view of generalized solutions" , North-Holland (1990) Zbl 0717.35001 |
[a7] | E.E. Rosinger, "Parametric Lie group actions on global generalized solutions of nonlinear PDEs. Including a solution to Hilbert's fifth problem" , Kluwer Acad. Publ. (1998) |
Rosinger nowhere-dense generalized function algebra. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Rosinger_nowhere-dense_generalized_function_algebra&oldid=50121