Definition 14.6.1 (Arens Extension).label Let $E, F, G$ be normed vector spaces over $K \in \RC$ and $\lambda \in L^{2}(E, F; G)$ be a continuous bilinear mapping, then there exists a unique bilinear mapping $\Lambda_{1}: E^{**}\times F^{**}\to G^{**}$ such that:

  1. (1)

    For each $(x, y) \in E \times F$, $\Lambda_{1}(x, y) = \lambda(x, y)$.

  2. (2)

    For each $x \in E$, $\Lambda_{1}(x, \cdot)$ is weak*-continuous.

  3. (3)

    For each $y \in F^{**}$, $\Lambda_{1}(\cdot, y)$ is weak*-continuous.

Similarly, there exists a unique bilinear mapping $\Lambda_{2}: E^{**}\times F^{**}\to G^{**}$ such that:

  1. (1)

    For each $(x, y) \in E \times F$, $\Lambda_{2}(x, y) = \lambda(x, y)$.

  2. (2’)

    For each $x \in E^{**}$, $\Lambda_{2}(x, \cdot)$ is weak*-continuous.

  3. (3’)

    For each $y \in F$, $\Lambda_{2}(\cdot, y)$ is weak*-continuous.

The mappings $\Lambda_{1}, \Lambda_{2}: E^{**}\times F^{**}\to G^{**}$ are the first and second Arens extensions of $\lambda$, respectively.

Proof, [Section 1, Theorem 3.2, Are51]. For each $x \in E$, the mapping $\lambda(x, \cdot) \in L(F; G)$ admits an adjoint $\lambda^{*}(x, \cdot) \in L(G^{*}; F^{*})$, which induces an adjoint of the bilinear map as follows

\[\lambda^{*}: E \times G^{*} \to F^{*} \quad \dpn{y, \lambda^*(x, \phi)}{F}= \dpn{\lambda(x, y), \phi}{G}\]

Applying the above operation again yields a second adjoint

\[\lambda^{**}: F^{**}\times G^{*} \to E^{*} \quad \dpn{x, \lambda^{**}(y, \phi)}{E}= \dpn{\lambda^*(x, \phi), y}{F^*}\]

and finally, applying the adjoint operation a third time gives

\[\Lambda_{1} = \lambda^{***}: E^{**}\times F^{**}\to G^{**}\quad \dpn{\phi, \lambda^{***}(x, y)}{G^*}= \dpn{\lambda^{**}(y, \phi), x}{E^*}\]

(1): Let $(x, y) \in E \times F$, then for each $\phi \in G^{*}$,

\[\dpn{\phi, \Lambda_1(x, y)}{G^*}= \dpn{\lambda^{**}(y, \phi), x}{E^*}= \dpn{\lambda^*(x, \phi), y}{F^*}= \dpn{\lambda(x, y), \phi}{G}\]

By the Hahn-Banach Theorem, $\Lambda_{1}$ is an extension of $\lambda$.

(2): Fix $x \in E$ and $\phi \in G^{*}$, then for each $y \in F^{**}$,

\begin{align*}\dpn{\phi, \Lambda_1(x, y)}{G^*}&= \dpn{\lambda^{**}(y, \phi), x}{E^*}= \dpn{x, \lambda^{**}(y, \phi)}{E}\\&= \dpn{\lambda^*(x, \phi), y}{F^*}\end{align*}

Since $\lambda^{*}(x, \phi) \in F^{*}$, $\Lambda_{1}(x, \cdot)$ is weak*-continuous.

(3): Fix $y \in F^{**}$ and $\phi \in G^{*}$, then for each $x \in E^{**}$, $\dpn{\phi, \Lambda_1(x, y)}{G^*}= \dpn{\lambda^{**}(y, \phi), x}{E^*}$. Since $\lambda^{**}(y, \phi) \in E^{*}$, $\Lambda_{1}(\cdot, y)$ is weak*-continuous.

(Uniqueness): By Goldstine’s Theorem, $E$ is weak*-dense in $E^{**}$, and $F$ is weak*-dense in $F^{**}$, so the extension is uniquely determined.$\square$

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