Critical-cone characterization of directional solution derivatives in Asplund spaces
Establish, in the infinite-dimensional Asplund-space setting of Theorem 3.1, that the direction \(\bar v(\bar y)\) associated with directional \(V\)-flatness belongs to the critical cone \(C(\bar x,\bar y;\bar u)\), rather than only to the linearization cone \(\mathbb L(\bar x,\bar y;\bar u)\).
References
In the finite-dimensional framework established in Theorem 3.1, the direction \bar{v}(\bar{y}) is shown to belong to the critical cone C(\bar{x}, \bar{y}; \bar{u}). However, in Theorem~\ref{thm: directional subdifferential of V}, we can only guarantee that \bar{v}(\bar{y}) \in \mathbb{L}(\bar{x}, \bar{y}; \bar{u}). This discrepancy arises because, in the infinite-dimensional setting, we cannot guarantee the existence of a sequence y_k \in S(x_k) satisfying \frac{y_k - \bar{y}{t_k} \to \bar{v}(\bar{y}). Consequently, we are unable to establish the following sequence of estimates: