Okay, so welcome everyone. We have Professor Tia Lizzi from the University of Paris-Dauphin
and today he will be speaking about non-contrability results for the half heat equation on the
low line based on the called the Ferro Dal wave function and applications of question
equations. We are looking forward to you also, Dizzy.
Okay, thank you very much for the introduction and also thank you very much Marius and Enrique
for giving me the opportunity to present my work here in this seminar. So as you told,
the main subject of this talk will be two results of non-contrability and so in fact
the results in themselves are not very impressive but what is interesting here is rather the method
I used which is quite original and I hope that it can be maybe extended to many other situations.
Okay, so this is the outline of the talk. So first of all I will give some general facts
about linear control theory to be sure that everybody has the case to understand the rest
of the talk and then I will define and give some properties of the main tool I will use here,
meaning what I call the Prolique Solidar wave function. Then I will present the non-contrability
result on the half heat equation and to finish I will explain how to use this previous result
on the half heat equation on the Grushin equation and give a conclusion. Okay, so
first of all maybe I would like to explain a little bit what is the main, what is in fact
the main goals of control theory. So the general goal is to act on dynamical system, so you take
some dynamical system y prime is equal to f of y u, so y is the state of a physical or biological
system and u is a parameter that you can choose which is called the control and you can choose it
in order to ensure a certain number of properties. So roughly speaking you can decompose the
problem into three subclasses. The first type of problems would be what I recall the controllability
problem, so meaning that you take an initial condition in some class in some state space
and you would like to find a control such that at some given time capital T you can reach a
prescribed target set. So it is what we call an open loop system meaning that the control will
depend only on the initial condition and not at the evolution of the state over time. So this is
rather a theoretical question and it has many links notably with inverse problems or unique
continuation properties. A second issue is the question of stabilization, so in this case you
would like, so you take a typical system which is unstable and you would like to make it stable
by choosing a control which depends itself on the state y and you would like to ensure that at
infinite time for example you go to an equilibrium zero for example, so it has many implications in
robotics, electronics, fluid mechanics. And the last issue would be optimal control, so in this case
your goal will be to find some control use such that you minimize some cost functional depending
on y and u. So in this case contrary to the controllability problem you cannot really reach
some target state but your goal is to minimize some cost functionals. And here what I will focus
on in this talk is the first problem, so the problem of controllability.
Okay so the general framework is the following, so you take some linear operators for example
on Hilbert spaces you take and you consider a dynamical system of the form y prime is equal
to a1 plus bu, so y is the state of the system, b is what is called the control operator and you
have some parameter u which is the control, so this is the parameter that you can choose
in order to reach some goal as we will see afterwards. So the situation
so you can think about is the following, so you take a to be the Dirichlet Laplace operator
and bounded domain capital omega of rd for example and capital b will be for example the
the characteristic function of subsets little omega, so this is called distributed control,
so you have a control which is localized localized somewhere and you would like to act on the whole
whole domain thanks to this control localized on little omega. So here we will be interested in
what we call the the null controllability property, so what does it mean? It means that
for any initial condition in a state space you would like to find a control such that
you reach the equilibrium capital T, the equilibrium zero at time capital T and so of course
as soon as you have reached this equilibrium zero you can switch off the control and you will stay
at zero forever. So here it is a problem of existence, it means you have to find a control.
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01:08:36 Min
Aufnahmedatum
2021-03-05
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2021-03-05 16:36:38
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