-
Abstract
This paper is devoted to analyze the class of initial data that can be insensitized for the heat equation.
This issue has been extensively addressed in the literature
both
in the case of complete and approximate insensitization (see [19] and [1], respectively).
But in the context of pure insensitization there are very few results identifying the class of initial data that
can be insensitized. This is a delicate issue which is related to the fact that
insensitization turns out to be equivalent to suitable
observability estimates for a coupled system of heat equations,
one being forward and the other one backward in time.
The existing Carleman inequalities techniques can be applied but they only give interior information of the solutions,
which hardly allows identifying the initial data because of the strong irreversibility of the equations involved in the
system, one of them being an obstruction at the initial time $t=0$ and the other one at the final one $t=T$.
In this article we consider different geometric configurations in which the subdomains to be insensitized and the one in which the external control acts play a key role. We show that, under rather restrictive geometric restrictions, initial data in a
class that can be characterized in terms of a summability condition of their Fourier coefficients with suitable weights, can be
insensitized. But, the main result of the paper, which might seem surprising, shows that this fails to be true in general, so that even the first eigenfunction of the system can not be
insensitized. This result is similar to those obtained in the context of the null controllability of the heat equation in unbounded domains in [14] where it is shown that smooth and compactly supported initial data may not be controlled.
Our proofs combine the existing observability results for heat equations obtained by means of Carleman inequalities, energy and gaussian estimates and Fourier expansions.
Mathematics Subject Classification: Primary: 35K05, 93C20; Secondary: 35B37.
\begin{equation} \\ \end{equation}
-
Access History
-