projected dynamical systems on hilbert sps
TRANSCRIPT
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PROJECTED DYNAMICAL SYSTEMS ON HILBERT SPACES
THESIS ABSTRACT
MONICA-GABRIELA COJOCARU
1. Introduction
The notion of projected dynamical systems is relatively new, being introduced in themathematical literature in the last decade. In this thesis we present the generalization of
this notion from Euclidean space to Hilbert spaces of arbitrary dimensions.
These systems are non-smooth dynamical systems and are dened as the solutions to a
class of ordinary differential equations with a discontinuous right-hand side. We refer to
this class of equations as projected differential equations . The word projected indicates
the use of a specic operator in dening a projected differential equation. This operator
restrains the whole Hilbert space X onto a non-empty, closed and convex subset K X .
The motivation for studying a projected dynamical system is that it can be used in thestudy of dynamics of perturbed steady states of problems arising from Economic Theory,
Physics and Engineering.
This study can be conducted via the theory of variational inequalities, a theory closely
related to calculus of variations and free boundary problems. It is the case that the crit-
ical points of a projected differential equation coincide with the solutions to a variational
inequality problem. The solvability of variational inequalities is a question that has been
answered positively in many contexts (see for example [B-C], [C-Y], [Is1], [Is2], [Is3], [Is4],
[Is5], [Is-C2], [Is-C3], [K-S], [Lu], [M2], [H-P], [Is7] and the references therein). In the thesis
we use the notion of exceptional family of elements to assert the solvability of variational
inequality problems on closed, convex and unbounded subsets of a Hilbert space.
Through a projected dynamics we can show, under suitable conditions, whether or not
equilibria have stability and/or attracting properties. In short, we can show if and how the
equilibria will be reached.1
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2 MONICA-GABRIELA COJOCARU
The main results of this thesis consist of proving the existence of projected dynamical
systems on Hilbert spaces of any dimension (that is, proving that the discontinuous differ-
ential equation has unique solutions) and proving results about the dynamics of perturbed
equilibria (critical points of a projected differential equation). We will present below the
main results and outline the ideas and approaches for their proofs.
2. Projected differential equations and projected dynamical systems
Let X be a Hilbert space of arbitrary dimension and K X a non-empty, closed and
convex subset. Let · , · be the inner product on X . For any z X , there exists an unique
element in K , denoted by P K (z), such that ||P K (z) − z || = inf y K
|| y − z || . P K is called the
projection operator of the space X onto the subset K . In [K-S] Chapter I, Theorems2.3 and Corollary 2.4 it is shown that for a Hilbert space X and K X a non-empty closed
convex subset, P K is Lipschitz continuous with constant 1.
DEFINITION 2.1. For x K , the set T K (x ) = h> 0
1h (K − x ) is called the tangent cone
to K at the point x. The cone T K (x ) is a closed convex cone. The normal cone to the set
K at the point x is the polar cone of T K (x ) and it is given by N K (x ) := { p X | p, x − x ≥
0, x K }. The normal cone is also a closed, convex cone. According to [A-C], Chapter
5, Section 1, Proposition 2 we have that N K (x ) = T K (x )− and also T K (x ) = N K (x )− .
Now we introduce the directional derivative of the projection operator P K .
PROPOSITION 2.1. For any x K and any element v X the limit
ΠK (x, v ) := limδ→ 0+
P K (x + δv) − xδ
exists and ΠK (x, v ) = P T K (x ) (v).
A proof of this result can be found in [Z] Lemma 4.6 or [S].
REMARK 2.1. Let ΠK : K × X → X be the operator given by ( x, v ) → ΠK (x, v ). Thenwhenever v T K (x ), ΠK (x, v ) = v. The operator Π K is discontinuous on the boundary of
the set. The following result can be found in [I-R], Theorem 2.23.
THEOREM 2.1 (Moreau) . If C X is a closed convex cone, C − its polar cone and
x ,y,z X , then the following statements are equivalent:
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PROJECTED DYNAMICAL SYSTEMS ON HILBERT SPACES THESIS ABSTRACT 3
1). z = x + y, x C , y C − and x, y = 0 ;
2). x = P C (z) and y = P C − (z).
The operator Π K plays a crucial role in the context of this thesis. Π K can be characterized
by the following theorem, which is our generalization of a similar result in [Du]:
THEOREM 2.2. Let X be an innite dimensional Hilbert space and K X be a non-
empty closed, convex subset. Then
(i) ΠK (x, v ) = v, if x intK .
(ii) ΠK (x, v ) = v, if x ∂K and supn N K (x )
v, n ≤ 0.
(iii) ΠK (x, v ) = v − v, n n , if x ∂K , supn N K (x )
v, n > 0 and n achieves that supremum.
In the thesis we use a simpler characterization of Π K .
PROPOSITION 2.2. Let X be an arbitrary Hilbert space and K X a closed and convex
subset. Then there exists n N K (x ) such that
ΠK (x, v ) = v − n, for each x K and v X,
and ||ΠK (x, v )|| ≤ || v|| .
Proof. The proof is immediate by Moreau’s theorem.
DEFINITION 2.2. Let X be a Hilbert space of arbitrary dimension and K X be a
non-empty, closed and convex subset. Let F : K → X be a vector eld. Then the ordinary
differential equation
(1) dx(t )
dt = Π K (x (t ), − F (x (t )))
is called the projected differential equation associated with F and K .
The projected differential equation is present in [A-C], [CO] and [He] if one considers the
case of single-valued mappings from K to X . However, the rst formulation of equation(1) in the form above occurred in 1990 in the paper [D-I] and then in [D-N] in Euclidean
space, for convex polyhedral subsets K R n .
DEFINITION 2.3. A point x K is called a critical point or an equilibrium for the
equation (1) if ΠK (x , − F (x )) = 0 .
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4 MONICA-GABRIELA COJOCARU
There is a fundamental relation between a projected dynamical system and a variational
inequality problem.
THEOREM 2.3. Let X be a Hilbert space and K X be a non-empty, closed and convex
subset. Let F : K → X be a vector eld. Consider the variational inequality problem:
(2) nd x K such that F (x ), y − x ≥ 0, y K.
Then the solutions to problem (2) coincide with the critical points of the projected differential
equation (1).
Proof. The proof is simple, using Moreau’s theorem.
REMARK 2.2. A rst proof of this result can be found in [D-I] Section 5.3 for the case of X a Euclidean space and K a convex polyhedral subset.
Consider the initial value problem
(3) dx (t )
dt = Π K (x (t ), − F (x (t ))) , x(0) = x 0 K.
An absolutely continuous function x : [0, l ] R → X such that x(t ) K for all t [0, l]
and dx(t )
dt = Π K (x (t ), − F (x (t ))), for almost all t [0, l ], is called a solution to the initial
value problem (3). If solutions to problem (3) exist on R+ and are unique starting at each
point x0, then we can associate to this initial value problem a dynamical system:
DEFINITION 2.4. A projected dynamical system is given by a mapping
Φ : K × R + → K which solves the initial value problem:
Φx (t ) = Π K (Φx (t ), − F (Φx (t ))) , Φx (0) = x.
We make the convention Φ x (·) := x(·).
3. Existence of projected dynamical systems on H-spaces
In the paper Existence of solutions to projected differential equations on Hilbert spaces
[C-J], we show that problem (3) has solutions in the general context of a Hilbert space of
innite dimension, and for any non-empty, closed, convex subset K X and any Lipschitz
continuous vector eld F : K → X . The paper is attached .
We give here the statement of the main theorem followed by the theorem about the
extension of solutions from an interval in R to R+ .
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PROJECTED DYNAMICAL SYSTEMS ON HILBERT SPACES THESIS ABSTRACT 5
THEOREM 3.1. Let X be a Hilbert space of arbitrary dimension and K X a non-
empty, closed and convex subset. Let F : K → X be a Lipschitz continuous vector eld
with Lipschitz constant b. Let x0 K and L > 0 so that ||x 0 || ≤ L . Then the initial value
problem dx (t )
dt = Π K (x (t ), − F (x (t )) , x(0) = x 0 has a unique solution on the interval [0, l ],
where l := L
|| F (x 0)|| + bL.
THEOREM 3.2. Consider the initial value problem
(4) dx (t )
dt = Π K (x (t ), − F (x (t ))) , x(0) = x 0
in the hypothesis of Theorem 3.1. Then the solutions can be extended to [0, ∞ ).
Proof. From Theorem 6.1 we can assert the existence of a solution to problem (6) on an
interval [0 , l ], where l = L
|| F (x 0)|| + bL, with b > 0 xed and L > 0 arbitrary.
We note that we can choose L such that l ≥ 11 + b
in the following way: if ||F (x 0) || = 0
we let L = 1 and if ||F (x 0)|| = 0, then we let L ≥ || F (x 0) || . In both cases we obtain
l ≥ 11 + b
. Therefore beginning at each initial point x0 K problem (6) has a solution on
an interval of length at least [0 , 11 + b
]. Now if we consider problem (6) with x(0) = x ( 11 + b
)
and applying again Theorem 6.1, we obtain an extension of the solution on an interval of
length at least 1
1 + b. By continuing this solution we obtain a solution on [0 , ∞ ).
4. Dynamics of perturbed steady-states
In this section we exploit the fundamental relation between a variational inequality prob-
lem dened by the vector eld F on the subset K , and a projected dynamical system,
involving the vector eld − F (Theorem 2.2). Namely, we show that under supplementary
conditions on F , the equilibria of this system, hence the solutions to a variational inequal-
ity, display stability and attracting properties. These supplementary conditions consist of
pseudo- and quasi-monotonicity.
The notion of monotonicity is the natural generalization of the notion of an increasing
real valued function of one variable. There exist generalizations of this notion to various
larger classes of mappings (pseudo-monotone and quasi-monotone), (see [Ka]). We will limit
ourselves in this abstract to a few illustrations.
Let X be a Hilbert space and K X a non-empty subset. A mapping F : K → X is called
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6 MONICA-GABRIELA COJOCARU
monotone if for all x, y K , F (y) − F (x ), y − x ≥ 0. Monotone mappings are used in
the theory of variational inequalities, in Optimization, in Nonlinear Analysis, in the theory
of nonlinear differential equations as can be seen in [A-C], [B-C], [Hk], [K-S], [K-Z], [La],
[M2], [Na6], [P], [R-W], [Z],[Da2].
DEFINITION 4.1. (i) A map F is called pseudo-monotone on K if, for every pair of
distinct points x, y , we have
y − x, F (x ) ≥ 0 = y − x, F (y) ≥ 0.
(iii) A map F is strongly pseudo-monotone on K if, there exists η > 0 such that, for
every pair of distinct points x, y , we have
y − x, F (x ) ≥ 0 = y − x, F (y) ≥ η|| y − x || 2.
(iv) A map F is quasi-monotone on K if for every distinct pair x, y we have
y − x, F (x ) > 0 = y − x, F (y) ≥ 0.
These classes of mappings are distinct (see [Ka]). We now present the dynamics results for
equilibria of projected systems under pseudo- and quasi-monotonicity conditions. First we
use the notion of monotone attractor. This notion is different than the one of an attractor,
as used in the classical theory of dynamical systems. We recall that a compact set D X iscalled an attractor for the projected dynamical system (3) if there exists a neighbourhood
V of the set D and T > 0 such that x (T ) V , for each x V and x(t ) → D , as t → ∞ for
each x V .
DEFINITION 4.2. An equilibrium x of (3) is a monotone attractor if δ > 0 such
that, x B (x , δ ) and x(t ) the unique solution of (3) starting at the point x, the function
d(x, t ) := ||x (t ) − x || is non-increasing as a function of t. The point x is a global
monotone attractor if all the above is true for any x K .
REMARK 4.1. Denition 4.2 is used in [Is-C1], [Is-C3], [Na6], [Na7] and [P] as well. We
note that an equilibrium x may be a monotone attractor, but not necessarily an attractor.
The rst result characterizes the behaviour of equilibria of (3), located both in the interior
of the set and on the boundary. It is easy to see that a strict equilibrium (see the denition
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PROJECTED DYNAMICAL SYSTEMS ON HILBERT SPACES THESIS ABSTRACT 7
below) can only exist on ∂K , but it is interesting to notice that under different conditions
they display the same behaviour:
THEOREM 4.1. Let x be an equilibrium of (3).
(i) If F is pseudo-monotone on K, then x is a global monotone attractor.
(ii) If F is quasi-monotone on K and x is a strict equilibrium (i.e. F (x , y − x > 0) ,
then x is a global monotone attractor.
This is proved by studying the function D (t ) := 12
|| x (t ) − x || 2, with x(0) K .
Another formulation for a variational inequality problem (VIP), was introduced by G.
Minty. Given a closed, convex subset K in a Hilbert space X and a mapping F : K → X ,
a variational inequality problem in the sense of Minty (MVIP) is to nd x K such thatF (y), x − y ≤ 0 for all y K . There exists a relation between VIP and MVIP.
THEOREM 4.2. (i) If F is continuous on nite dimensional subspaces and x is a solution
to the MVIP, then it is a solution to the VIP.
(ii) If F is pseudo-monotone and x is a solution to the VIP, then it is a solution to the
MVIP.
Proof. A proof of this result can be found in [K-S] Chapter III, Lemma 1.5.
We can characterize the set of solutions to MVIP.
THEOREM 4.3. The set of global monotone attractors for the projected system (3) coin-
cides with the set of solutions of the MVIP associated to the same system.
Proof. We use the same idea as in the theorem above, i.e. we use the fact that
D (t ) := ddt (
12
|| x (t ) − x || 2) ≤ 0, with x(0) K .
DEFINITION 4.3. Let x K be an equilibrium of the system (3) and let x(t ) denote
the solution with x(0) = x K .
(i) The point x is exponentially stable if there exists δ > 0 and B > 0, µ > 0 constants
such that x B (x , δ ) and t ≥ 0 we have ||x (t ) − x || ≤ B || x − x || e− tµ .
(ii) The point x is a nite-time attractor if there exists δ > 0 such that for any x
B (x , δ ), there exists some moment of time T := T (x ) < ∞ such that x(t ) = x for any
t ≥ T (x ).
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8 MONICA-GABRIELA COJOCARU
(iii) The point x is globally exponentially stable or globally nite-time attractor
if (i) or, respectively (ii), takes place for any x K .
We nally state other two results, their proof being based on the same idea as before.
THEOREM 4.4. Suppose that x is an equilibrium of the system (3). If F is strongly
pseudo-monotone on K , then x is globally exponentially stable and is therefore a global
attractor.
DEFINITION 4.4. A map F is called strongly pseudo-monotone with degree α on
K if, there exists η > 0 such that, for every pair of distinct points x, y , we have
y − x, F (x ) ≥ 0 = y − x, F (y) ≥ η|| y − x || α .
THEOREM 4.5. Suppose that x is an equilibrium of (3). If F is strongly pseudo-
monotone with degree α < 2 on K , then x is a globally nite-time attractor.
5. Summary and future work
We presented here in brief the development of the theory of projected dynamical systems,
from Euclidean space to arbitrary Hilbert spaces. We used elements from various areas of Mathematics (Set-valued Mappings, Differential Inclusions, Functional and Convex Analy-
sis) to obtain results about equilibria of some applied problems. We showed the existence
of equilibria through the theory of variational inequalities, we showed the existence of pro-
jected systems on Hilbert spaces and we studied the dynamics of the problems around these
equilibrium points through the projected dynamical systems theory.
This thesis is intended to be a starting point for future work on projected dynamical
systems. There are a few directions that can be followed and explored, based on the
research developed in this thesis. One such direction could consist of studying applications
to this theory and nding relevant interpretations of the mathematical results.
The theory of projected dynamics was born as a result of applied problems and it has
its roots and motivation in Applied Mathematics. However, it is our opinion that a pro-
jected dynamical system is a very rich topic in Pure Mathematics as well, considering the
interesting blend of mathematical notions involved in proving its existence.
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PROJECTED DYNAMICAL SYSTEMS ON HILBERT SPACES THESIS ABSTRACT 9
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Department of Mathematics and Statistics, Jeffery Hall, room 229, Queen’s University,
Kingston, Ontario, Canada
E-mail address : [email protected]