Maximal monotone operators on hilbert spaces and applications
Table Of Contents
- Abstract i
Acknowledgment ii
Dedication iii
Table of Contents v
Introduction vi
1 Hilbert Spaces and Sobolev Spaces 1
- 1.1Hilbert spaces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.
- 1.1Examples . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
- 1.2Function Spaces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
1.
- 2.1Lp Spaces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
1.
- 2.2Test functions . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
1.
- 2.3Distributions . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
- 1.3Sobolev spaces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
2 Maximal Monotone Operators on Hilbert spaces 8
- 2.1Examples of maximal monotone operators . . . . . . . . . . . . . . . 11
- 2.2Yosida Approximation of a maximal monotone operator . . . . . . . . 14
- 2.3Self adjoint Operators . . . . . . . . . . . . . . . . . . . . . . . . . . 27
- 2.4Application . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 32
iv
Bibliography 35
Thesis Abstract
Let H be a real Hilbert space and A D(A) H ! H be an unbounded, linear,
self-adjoint, and maximal monotone operator. The aim of this thesis is to solve
u0(t) + Au(t) = 0, when A is linear but not bounded. The classical theory of
differential linear systems cannot be applied here because the exponential formula
exp(tA) does not make sense, since A is not continuous. Here we assume A is
maximal monotone on a real Hilbert space, then we use the Yosida approximation
to solve. Also, we provide many results on regularity of solutions. To illustrate the
basic theory of the thesis, we propose to solve the heat equation in L2(
). In order
to do that, we use many important properties from Sobolev spaces, Green’s formula
and Lax-Milgram’s theorem.
Thesis Overview
<p>
</p><p>Hilbert Spaces and Sobolev Spaces<br>The aim of this chapter is to recall some results on Lp spaces, distributions and<br>Sobolev spaces that we use in the next chapter.<br>1.1 Hilbert spaces<br>A normed vector space is closed under vector addition and scalar multiplication.<br>The norm defined on such a space generalises the elementary concept of the length<br>of a vector. However, it is not always possible to obtain an analogue of the dot<br>product, namely<br>a:b = a1b1 + a2b2 + a3b3<br>which yields<br>jaj =<br>p<br>a:a<br>which is an important tool in many applications. Hence, the question arises whether<br>the dot product can be generalised to arbitrary vectors spaces. In fact, this can be<br>done and leads to inner product spaces and complete inner product spaces, called<br>Hilbert spaces.<br>Definition 1.1. Let H be a linear space. An inner product on H is a function<br>h:; :i : H H ! R<br>1<br>defined on H H with values in R such that the following conditions are satisfied.<br>For x; y; z 2 H; ; 2 R<br>a) hx; xi 0 and hx; xi = 0 if and only if x = 0<br>b) hx; yi = hy; xi<br>c) hx + y; zi = hx; zi + hy; zi<br>The pair (H; h:; :i) is called an inner product space. A Hilbert space, H is a complete<br>inner product space ( complete in the metric defined by the inner product ).<br>1.1.1 Examples<br>1. Euclidean space Rn.<br>The space Rn is a Hilbert space with inner product defined by<br>hx; yi =<br>Xn<br>i=0<br>xiyi<br>where,<br>x = (x1; x2; :::; xn) and y = (y1; y2; :::; yn)<br>We obtain<br>jjxjj =<br>p<br>hx; xi = (<br>Xn<br>i=0<br>x2i<br>)<br>1<br>2<br>2. Space L2(<br>):<br>L2(<br>) := ff :<br>! R : f is measurable and<br>R</p><p>f2dx < 1g, where<br>is an open<br>set in Rn; is a Hilbert space with the inner product defined<br>hf; gi =<br>Z</p><p>f(x)g(x)dx<br>and<br>jjfjj = (<br>Z</p><p>jf(x)jdx)<br>1<br>2<br>3. Hilbert sequence space l2.<br>l2 := f(xn)n0 R :<br>1P<br>i=0<br>jxij2 < 1g is a Hilbert space with inner product<br>defined by<br>hx; yi =<br>X1<br>i=0<br>xiyi<br>2<br>Convergence of this series follows from Cauchy-Schwar’z inequality and the fact that<br>x; y 2 l2, by assumption.<br>The norm is defined by<br>jjxjj = (<br>X1<br>i=0<br>jxij2)<br>1<br>2<br>An inner product on H defines a norm on H given by<br>jjxjj =<br>p<br>hx; xi<br>and a metric on H given by<br>d(x; y) = jjx ô€€€ yjj =<br>p<br>hx ô€€€ y; x ô€€€ yi<br>Hence, inner products are normed spaces and Hilbert spaces are Banach space.<br>A norm on an inner product space satisfies the important parallelogram equality<br>jjx + yjj2 + jjx ô€€€ yjj2 = 2(jjxjj2 + jjyjj2) for all x; y 2 H<br>Not all normed spaces are inner product spaces.<br>4. Space lp.<br>Let 1 p < 1 be a fixed real number, we define lp space as<br>lp = f(xn)n0 R :<br>X1<br>i=0<br>jxijp < 1g:<br>When p 6= 2, lp is not a Hilbert space.<br>5. Space C([a; b];R).<br>The space C([a; b];R) provided with supremum norm is not a Hilbert space.<br>Proposition 1.2. Let (H; h:; :i) be an inner product space. Then, for all x; y 2 H<br>a. jhx; yij jjxjjjjyjj (Schwar0z inequality) where the equality holds if and<br>only if x,y are linearly dependent.<br>b. jjx + yjj jjxjj + jjyjj (triangle inequality) where the equality holds if<br>and only if x=cy (c 0)<br>Proposition 1.3. (Continuity of inner product). Let (xn)n0; (yn)n0 be sequences<br>in H, such that xn ! x and yn ! y, then<br>hxn; yni ! hx; yi:<br>3<br>1.2 Function Spaces<br>Here, we recall the definitions of functions spaces used in this thesis.<br>1.2.1 Lp Spaces<br>Definition 1.4. Let<br>be a nonempty open set in Rn, for 1 p < 1, we define<br>Lp(<br>) := ff :<br>! R : f is measurable and<br>Z</p><p>jf(x)jpdx < 1g<br>Remark 1.5. We say two functions f and g are equivalent if f = g almost everywhere.<br>Then we define Lp(<br>) spaces as the equivalent classes for this relationship.<br>The space Lp(<br>) can be seen as a space of functions. We do however, need to be<br>careful sometimes. For example, saying that f 2 Lp(<br>) is continuous means that f<br>is equivalent to a continuous function. Now, for f 2 Lp(<br>), we define<br>jjfjjp = (<br>Z</p><p>jf(x)jpdx)<br>1<br>p ; 1 p < 1<br>The Lp(<br>) is a Banach space.<br>1.2.2 Test functions<br>Definition 1.6. Let f :<br>! R be a continuous function. The support is<br>supp(f) := fx 2<br>: f(x) 6= 0g<br>The function is said to be of compact support on<br>if the support is a compact set<br>contained inside<br>.<br>Definition 1.7. The space of test functions in<br>, denoted by D(<br>) is the space of<br>all C1 functions defined on<br>which have compact supports in<br>.<br>C1(<br>) denotes the space of all real-valued functions on<br>of class C1.<br>= (1; 2; :::; n) 2 Nn is called multi-index with length jj =<br>Pn<br>i=1<br>i.<br>Let x = (x1; x2; :::; xn) 2 Rn. We write D = @jj<br>@<br>1<br>x1 :::@n<br>xn<br>and it acts on the space<br>C1(<br>). Thus, for f 2 C1(<br>), Df = @jjf<br>@<br>1<br>x1 :::@n<br>xn<br>is it partial derivatives of order jj.<br>Definition 1.8. Let f ngn0 be a sequence in D(<br>) and 2 D(<br>).<br>n ! in D(<br>) if<br>1. 9 a compact set K<br>: supp( ); supp( n) K; for all n 1<br>2. D n ! D uniformly on K; 8 2 Nn:<br>4<br>1.2.3 Distributions<br>Definition 1.9. A distribution on<br>is any continuous linear mapping T : D(<br>) !<br>R. The set of all distributions is denoted by D0(<br>).<br>Remark 1.10. By linearity, to show that T is continuous, it is enough to show that,<br>if n ! 0 in D(<br>), then it is enough to show that (T; n) ! 0 in R:<br>Definition 1.11. A function f :<br>! R is locally integrable if for any compact set,<br>K<br>, we have that Z<br>K<br>jf(x))jdx < 1<br>The collection of all locally integrable functionals on<br>is denoted by L1l<br>oc(<br>)<br>If f 2 C(<br>), then f 2 L1l<br>oc(<br>). For any f 2 L1l<br>oc(<br>), f gives a distribution Tf defined<br>by<br>(Tf ; ) =<br>Z</p><p>f(x) (x)dx; for all 2 D(<br>)<br>Definition 1.12. If T 2 D0(<br>) is a distribution on an open set<br>Rn, and if<br>is any multi-index, we define the distribution DT by<br>(DT; ) = (ô€€€1)jj(T;D ) (1.1)<br>and it is the th partial derivative of T.<br>So, the map D : D0(<br>) ! D0(<br>) defined in (1.1) is linear and continuous.<br>1.3 Sobolev spaces<br>Sobolev spaces are based on the concept of weak (distributional) derivatives. It gives<br>us a modern approach to the study of differential equations.<br>Definition 1.13. Let 1 p < 1 and k be a non-negative integer. Then, Sobolev<br>space Wk;p(<br>) is defined by<br>Wk;p(<br>) := fu 2 LP (<br>) : Du 2 Lp(<br>); 8 0 jj kg<br>The space is equipped with the norm<br>jjujjWk;p(<br>) := (<br>X<br>0jjk<br>jjDujjp<br>LP (<br>))<br>1<br>p<br>5<br>WK;p<br>0 (<br>) = D(<br>)</p><p>Wk;p(<br>) i.e., WK;p<br>0 (<br>) is the closure of D(<br>) with respect to the<br>norm jj:jjWk;p(<br>).<br>When p=2, we write Hk(<br>) = Wk;2(<br>) and Hk<br>0 (<br>) = Wk;2<br>0 (<br>) and these are real<br>Hilbert spaces with the following inner product<br>hu; viHk(<br>) =<br>X<br>0jjk<br>Z</p><p>DuDvdx<br>and the norm<br>jjujjHk(<br>) = (<br>X<br>0jjk<br>jjDujj2<br>L2(<br>))<br>1<br>2<br>For, k=0,<br>W0;p(<br>) = LP (<br>):<br>Wk;p(<br>) are Banach spaces.<br>Given that<br>is smooth, then:<br>Wk;p<br>0 (<br>) := fu 2 Wk;p(<br>) : u = Du = ::: = Dkô€€€1u = 0 on @<br>g:<br>For p=2, we have<br>Wk;2<br>0 (<br>) := fu 2 Wk;2(<br>) : u = Du = ::: = Dkô€€€1u = 0 on @<br>g<br>For p=2,and k=1 , we have<br>W1;2<br>0 (<br>) := fu 2 W1;2(<br>) = H1(<br>) : u = 0 on @<br>g<br>and we denote it by H1<br>0(<br>)<br>For p=2, k=2, we write<br>W2;2(<br>) = H2(<br>):<br>Theorem 1.14. Let<br>be smooth and u 2 L2(<br>) such that u 2 L2(<br>). Then<br>u 2 H2(<br>):<br>6<br>Green’s Formula<br>Theorem 1.15. Let<br>be bounded and smooth. Let u 2 H2(<br>) and v 2 H1(<br>),<br>then Z</p><p>ru:rvdx =<br>Z<br>@</p><p>v<br>@u<br>@n<br>ds ô€€€<br>Z</p><p>vudx<br>where @u<br>@n denotes the normal derivative defined by @u<br>@n = ru:ô€€€!n<br>:<br>where ô€€€!n<br>denotes the normal vector.<br>if u = v, then<br>Z</p><p>jjrujj2dx =<br>Z<br>@</p><p>u<br>@u<br>@n<br>ds ô€€€<br>Z</p><p>uuds<br>=<br>Z<br>@</p><p>u<br>@u<br>@n<br>ds +<br>Z</p><p>u(ô€€€u)ds<br>Then,<br>Z</p><p>(ô€€€u)udx =<br>Z</p><p>jjrujj2dx ô€€€<br>Z<br>@</p><p>u<br>@u<br>@n<br>ds<br>Theorem 1.16. (Lax-Milgram). Let a : V V ! R be a bilinear, continuous,<br>and coercive functional. Then, for each f 2 V 9! u 2 V :<br>a(u; v) = (f; v); for all v 2 V<br>Proposition 1.17. (Poincaré’s inequality). Suppose<br>is a bounded set. Then<br>there exists a constant C(<br>) > 0 such that<br>jjujjL2(<br>) C(<br>)jjrujjL2(<br>); for all u 2 W1;2<br>0 (<br>):</p><p> </p>
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