Cores for generators of some Markov semigroups

Size: px
Start display at page:

Download "Cores for generators of some Markov semigroups"

Transcription

1 Cores for generators of some Markov semigroups Giuseppe Da Prato, Scuola Normale Superiore di Pisa, Italy and Michael Röckner Faculty of Mathematics, University of Bielefeld, Germany and Department of Statistics, Purdue University, W. Lafayette, 4796, IN, U. S. A. Abstract We consider a stochastic differential equation on R d with Lipschitz coefficients. We find a core for the infinitesimal generator of the corresponding Markov process. Some applications, in particular, to well-posedness of Fokker Planck equations are given. 2 Mathematics Subject Classification AMS: 61, 6J35, 47D7. Key words: stochastic differential equation, Markov process, transition semigroup, core. 1 Introduction We are here concerned with a stochastic differential equation in := R d, dx = b(x)dt + σ(x)dw (t), (1.1) X() = x, Research supported by the DFG through CRC 71 and the I. Newton Institute, Cambridge, UK. 1

2 where b : and σ : L() are Lipschitz continuous. It is well known that equation (1.1) has a unique solution X(, x). Moreover, the transition semigroup P t ϕ(x) = E[ϕ(X(t, x))], ϕ C b (), (1.2) is Feller. (C b () is the Banach space of all mappings ϕ : R which are uniformly continuous and bounded, endowed with the norm ϕ := sup x ϕ(x).) If b and σ are not bounded P t, t, is not strongly continuous in C b () but only pointwise continuous. We call it a π-semigroup, see later for a precise definition. Though the ille Yosida theory cannot be applied to P t, one can define an infinitesimal generator K following [1] or [5]. Then the problem arises to show the relationship between K and the Kolmogorov operator where K ϕ := 1 2 Tr [a(x)d2 ϕ] + b(x), Dϕ(x), ϕ C 2 b (), (1.3) a(x) = σ(x)σ (x), x. The main result of this paper is that if in addition b and σ are of class C 2 with bounded second derivatives, then K ϕ = K ϕ, ϕ C 2 b () and the space Cb 2 () is a core for K. This result seems to be new when a is not uniformly elliptic, see the monograph [3] and references therein for the case of uniformly elliptic a. 2 Notations and preliminaries Let us precise our assumptions. ypothesis 2.1 (i) b : and there is K 1 > such that b(x) b(y) K 1 x y, x. (2.1) (ii) σ : L() and there is K 2 > such that σ(x) σ(y) S K 2 x y, x, (2.2) where the sub-index S means the ilbert Schmidt norm. 2

3 We note that by (2.1) and (2.2) it follows that and b(x) K 1 x + b(), x, (2.3) σ(x) S K 2 x + σ() S, x, (2.4) respectively. Sometimes we shall need the following more stringent assumptions. ypothesis 2.2 (i) b and σ are of class C 2 and fulfill ypothesis 2.1. (ii) There is K 3 > such that b (x) + σ (x) S K 3, x. (2.5) The following two propositions are well known. Proposition 2.3 Assume that ypothesis 2.1 is fulfilled. Then for any x and any T > there is a unique solution X(, x) L 2 W (Ω; C([, T ]; )) of equation (1.1). Moreover, for all m N, X(, x) L m W (Ω; C([, T ]; )) and there is C T,m > such that E ( X(t, x) m ) C T,m (1 + x m ), x, t [, T ]. (2.6) Finally, there is C T > such that E X(t, x) X(t, y) C T x y, x, y, t [, T ]. (2.7) By L m W (Ω; C([, T ]; )) we mean the space of all adapted continuous stochastic processes F such that ( E ) sup F (t) m < +. t [,T ] Proposition 2.4 Assume that ypothesis 2.2 is fulfilled and let X(, x) be the solution to (1.1). Then the following statements hold. (i) X(t, x) is continuously differentiable in any direction h and setting η h (t, x) = X x (t, x) h we have dη h = b (X)η h dt + σ (X)(η h, dw (t)), (2.8) η h () = h. Moreover, there exists ω 1 R such that E η h (t, x) 2 e 2ω 1t h 2, h, t >. (2.9) 3

4 (ii) X(t, x) is twice continuously differentiable in any couple of directions h, k and setting ζ h,k (t, x) = X x (t, x)(h, k) we have dζ h,k = b (X)ζ h,k dt + b (X)(η h, η k )dt +σ (X)(ζ h,k, dw (t)) + σ (X)(η h, η k, dw (t)), (2.1) ζ h,k () =. Moreover, there exists ω 2 R and C 2 > such that E ζ h,k (t, x) 2 C 2 e 2ω 2t h 2 k 2, h, k, t >. (2.11) 2.1 Transition semigroup Let us introduce some notations. For any k N by Cb k () we denote the space of all mappings ϕ : R which are uniformly continuous and bounded together with their derivatives of order lesser than k. Cb k (), endowed with the norm ϕ k := ϕ + k D j ϕ, is a Banach space. Moreover, for any m N by C b,m () we denote the space of all mappings ϕ : R such that the mapping j=1 R, x ϕ(x) 1 + x m belongs to C b (). C b,m (), endowed with the norm ϕ(x) ϕ b,m := sup x 1 + x, m is a Banach space. Taking into account (2.6) we can define the transition semigroup P t ϕ(x) = E[ϕ(X(t, x))], ϕ C b,m (). (2.12) We know that P t ϕ C b () for all t and all ϕ C b (). It follows from (2.6) that also P t ϕ C b,m () for all ϕ C b,m (). Furthermore, P t, t, is a semigroup. 4

5 Proposition 2.5 Assume that ypothesis 2.2 is fulfilled. Then Cb 1 () and Cb 2() are stable for P t, t. Moreover there exist positive constants K 1 and K 2 such that P t ϕ j K j ϕ j, ϕ C j b (), j = 1, 2, t, (2.13) where j denotes the norm in C j b (). Proof. The assertions follow from Propositions 2.4 and the identities and DP t ϕ(x), h = E[ Dϕ(X(t, x)), η h (t, x) ], t, h, x, D 2 P t ϕ(x)h, k = E[ Dϕ(X(t, x)), ζ h,k (t, x) ] 2.2 Itô s formula +E[D 2 ϕ(x(t, x))(η h (t, x), η k (t, x))], t, h, k, x. Let us consider the Kolmogorov operator (1.3). By ypothesis 2.1 it follows that there exists M > such that for all ϕ Cb 2 () we have K ϕ(x) M(1 + x 2 ), x, (2.14) so that K ϕ C b,2 (). Proposition 2.6 (Itô s formula) Assume that ypothesis 2.1 is fulfilled. Then for all ϕ Cb 2 () we have E[ϕ(X(t, x))] = ϕ(x) + Proof. Write X(t, x) = x + t By (2.3) and (2.6) we see that t E[K ϕ(x(s, x))]ds. (2.15) b(x(s, x))ds + t σ(x(s, x))dw (s). E b(x(t, x)) C T,1 K 1 (1 + x ) + b(). so that b(x(, x)) C W ([, T ]; L 1 (Ω, R d )). 5

6 Moreover, by (2.4) and (2.6) so that, E σ(x(t, x)) 2 S 2K 2 (1 + x ) σ() 2 S, σ(x(, x)) C W ([, T ]; L 2 (Ω, R d )). Then we may apply Itô s formula and the conclusion follows. Note that if ϕ C 2 b () we have K ϕ C b,2 () by (2.14). Therefore, d dt P tϕ = P t K ϕ, ϕ C 2 b (). (2.16) Proposition 2.7 Assume that ypothesis 2.2 is fulfilled. Then d dt P tϕ = K P t ϕ, ϕ C 2 b (). (2.17) Proof. By the semigroup property, Proposition 2.5 and (2.16) we have for all ϕ C 2 b () d dt P tϕ = d dɛ P t+ɛϕ ɛ= = d dɛ P ɛ(p t ϕ) ɛ= = K P t ϕ 3 The infinitesimal generator of P t Let us introduce some notations. Given a sequence (ϕ n ) C b () and ϕ C b (), we say that (ϕ n ) is π-convergent to ϕ and write ϕ π n ϕ, if the following conditions are fulfilled. (i) For each x we have (ii) sup ϕ n < +. n N lim ϕ n(x) = ϕ(x). n Proposition 3.1 Assume that ypothesis 2.1 is fulfilled and let (ϕ n ) C b (), ϕ C b () such that ϕ n π ϕ. Then for all t we have P t ϕ n π P t ϕ. 6

7 We say that P t is a π-semigroup. Proof of Proposition 3.1. For any x we have lim P tϕ n (x) = lim E[ϕ n (X(t, x))] = P t ϕ(x), n n thank s to the dominated convergence theorem. Moreover P t ϕ n ϕ n sup ϕ n <. n N We follow here [5]. Definition 3.2 We say that ϕ belongs to the domain of the infinitesimal generator K of P t in C b () if (i) For each x there exists the limit (ii) and K ϕ C b (). 1 sup ɛ (,1] ɛ P ɛϕ ϕ < +. 1 lim ɛ ɛ (P ɛϕ(x) ϕ(x)) =: K ϕ(x) K is called the infinitesimal generator of P t. In the following we set ɛ := 1 ɛ (P ɛ 1). Proposition 3.3 Let ϕ D(K ) and let t. Then P t ϕ K and we have K P t ϕ(x) = P t K ϕ(x), x. (3.1) Moreover, P t ϕ(x) is differentiable in t and d dt P tϕ(x) = K P t ϕ(x) = P t K ϕ(x), x. (3.2) Proof. Let ϕ K. Then we have ɛ P t ϕ(x) = P t ɛ ϕ(x). 7

8 Since ɛ ϕ π K ϕ, by Proposition 3.1 it follows that ɛ P t ϕ π P t K ϕ. So, P t ϕ D(K ) and K P t ϕ = P t K ϕ. On the other hand, D + P t ϕ(x) = lim ɛ P t ɛ ϕ(x) = P t K ϕ(x) and (3.1) follows because K ϕ is continuous. We shall denote by ρ(k ) the resolvent set of K and by R(λ, K ) its resolvent. The following result is proved in [5] under slightly different assumptions. We sketch here the proof for the reader s convenience. Proposition 3.4 ρ(k ) (, + ). f C b () we have Moreover, for any λ > and any Proof. Set R(λ, K )f(x) = e λt P t f(x)dt, x. (3.3) ɛ := 1 ɛ (P ɛ 1). Let f C b () and for any λ >, x set F (λ)f(x) = + e λt P t f(x)dt. Then it is not difficult to see that F (λ)f C b (). Let us show that λ ρ(k ). Since ɛ F (λ)f(x) = 1 [ ] ɛ eλɛ e λt P t f(x)dt e λt P t f(x)dt = 1 ɛ (eλɛ 1) ɛ we easily deduce that F (λ)f D(K ) and Therefore ɛ e λt P t f(x)dt 1 ɛ ɛ eλɛ e λt P t f(x)dt, lim ɛ F (λ)f(x) = λf (λ)f(x) f(x). (3.4) ɛ K F (λ)f = λf (λ) f. (3.5) 8

9 It remains to show that F (λ)(λ K )ϕ = ϕ, ϕ D(K ). (3.6) This will complete the proof that λ ρ(k ). To prove (3.6) choose ϕ D(K ), then, taking into account Proposition 3.3, we have e λt P t K ϕ(x)dt = = ϕ(x) + λf (λ)ϕ(x), x. which implies (3.6). Remark 3.5 By (3.3) it follows that e λt d dt P tϕ(x)dt R(λ, K )f 1 λ f, f C b (). Therefore K is m dissipative in C b (). We are going to investigate the relationship between K and K. Proposition 3.6 Assume that ypothesis 2.1 is fulfilled. If ϕ D(K ) C 2 b () then K ϕ = K ϕ. Proof. By Proposition 2.6 we have As t we find Now we show that 1 t (P tϕ(x) ϕ(x)) = t E[K ϕ(x(s, x))]ds. K ϕ(x) = K ϕ(x), x. D := {ϕ C 2 b () : K ϕ C b ()}, is a core for K. Let us first show that D D(K ). Proposition 3.7 Assume that ypothesis 2.1 is fulfilled and let ϕ D. Then ϕ D(K ) and we have K ϕ = K ϕ. 9

10 Proof. Let ϕ D. By Itô s formula (2.15) we have Therefore, 1 t (P tϕ(x) ϕ(x)) = t E[K ϕ(x(s, x))]ds. 1 lim t t (P tϕ(x) ϕ(x)) = K ϕ(x), x, and 1 t (P tϕ ϕ) K ϕ, which implies that ϕ D(K ) and K ϕ = K ϕ. Theorem 3.8 Assume that ypothesis 2.2 is fulfilled. Then D is a core for K, that is, for any ϕ D(K ) there exists a sequence (ϕ n ) D such that ϕ n ϕ, K ϕ n K ϕ, in C b (). Proof. Let ϕ D(K ). Fix λ > and set f := λϕ K ϕ. Since Cb 2 () is dense in C b () there exists a sequence (f n ) Cb 2() such that f n f in C b (). Set ϕ n := (λ K ) 1 f n, n N. By Proposition 3.4 it is clear that ϕ n D(K ) and lim ϕ n = ϕ, n lim K ϕ n = K ϕ, n in C b (). It remains to show that ϕ n D for any n N. In fact, taking into account Proposition 2.5, we see that ϕ n D(K ) Cb 2 (), so that by Proposition 3.6 we have K ϕ n = K ϕ n C b (), and hence ϕ n D for any n N. So, D is a core as claimed. Remark 3.9 The above result can be generalized. In fact ypothesis 2.2 and also the global Lipschitz assumption in ypothesis 2.1 are too strong. E. g. assumptions as ypotheses 1.1 and 1.2 in [2] are sufficient. Details will be the subject of future work. 4 Applications We start with an important identity K (ϕ 2 ) = 2ϕK ϕ + σ Dϕ 2, ϕ C 2 b (), (4.1) whose proof is straightforward. 1

11 Proposition 4.1 Assume, besides ypothesis 2.2, that σ is bounded. Then for any ϕ D we have ϕ 2 D and K (ϕ 2 ) = 2ϕK ϕ + σ Dϕ 2. (4.2) Proof. Let ϕ D. Then ϕ 2 C 2 b () and by (4.1) it follows that K (ϕ 2 ) C b (). Corollary 4.2 Let ϕ D. Given λ > set f = λϕ K ϕ. Then we have ϕ 2 = (2λ K ) 1 (2ϕf σ Dϕ 2 ). (4.3) 4.1 Invariant measures In this subsection we assume that ypothesis 2.2 holds. Let µ P(). We say that µ is invariant if P t ϕdµ = ϕdµ, ϕ C b (). (4.4) Proposition 4.3 µ is invariant for P t if and only if K ϕdµ =, ϕ D. (4.5) Proof. Since the only if part is obvious, let us show the if part. Assume that (4.5) is fulfilled. Then K ϕdµ =, ϕ D(K ). Then if ϕ D(K ) we have by Proposition 3.3, that P s ϕ D(K ), for all s and P t ϕ(x) ϕ(x) = t K P s ϕ(x)ds. Integrating with respect to µ, yields (P t ϕ ϕ)dµ =, ϕ D(K ). Therefore, µ is invariant. 11

12 Proposition 4.4 Assume that µ is an invariant measure for P t such that x 2 µ(dx) < +. (4.6) Then we have ϕk ϕdµ = 1 2 σ Dϕ 2 dµ, ϕ C 2 b (). (4.7) Proof. Step 1 We have K ϕdµ =, ϕ Cb 2 (). (4.8) The proof follows by (2.14), (2.17), (4.6) and Lebesgues dominated convergence theorem Step 2 Conclusion. By (4.1) we have = K (ϕ 2 )dµ = 2 so, the conclusion follows. ϕk ϕdµ Application to Fokker Planck σ Dϕ 2 dµ, ϕ C 2 b (), In this subsection we assume that ypothesis 2.2 holds. Let B() be the Borel σ-algebra of. We recall that a measure µ(dt, dx) = µ t (dx)dt on B([, T ]) B(), where µ t are probability measures on B(), measurable in t [, T ], is called a solution to the Fokker Planck equation for (K, D) if t ϕ dµ t = ϕ dµ + K ϕ dµ s ds, a.e. t, ϕ D. (4.9) Theorem 4.5 For every probability measure ζ on B() there exists a unique measure µ(dt, dx) = µ t (dx)dt (as above) solving (4.9) with µ = ζ. Proof. Existence is trivial. Just define the measure µ t by ϕ(x) µ t (dx) := E[ϕ(X(t, x))]ζ(dx), a.e. t, ϕ : R +, B()-measurable. Then (4.9) follows by Proposition 2.6 (i.e., by Itô s formula). To show uniqueness we note that Theorem 3.8 implies that (4.9) with µ = ζ holds for all ϕ K. ence uniqueness follows from [4, Theorem 2.12]. 12

13 References [1] S. Cerrai, A ille-yosida theorem for weakly continuous semigroups, Semigroup Forum, 49, , [2] S. Cerrai, Second order PDE s in finite and infinite dimensions. A probabilistic approach, Lecture Notes in Mathematics, 1762, Springer-Verlag, 21. [3] L. Lorenzi and M. Bertoldi, Analytical methods for Markov semigroups, Chapman & ill/crc, 26. [4] L. Manca, Kolmogorov operators in spaces of continuous functions and equations for measures. Theses of Scuola Normale Superiore di Pisa (New Series)], 1. Edizioni della Normale, Pisa, 28. [5] E. Priola, On a class of Markov type semigroups in spaces of uniformly continuous and bounded functions, Studia Math., 136, ,

Kolmogorov equations in Hilbert spaces IV

Kolmogorov equations in Hilbert spaces IV March 26, 2010 Other types of equations Let us consider the Burgers equation in = L 2 (0, 1) dx(t) = (AX(t) + b(x(t))dt + dw (t) X(0) = x, (19) where A = ξ 2, D(A) = 2 (0, 1) 0 1 (0, 1), b(x) = ξ 2 (x

More information

Kolmogorov equations for stochastic PDE s with multiplicative noise

Kolmogorov equations for stochastic PDE s with multiplicative noise Kolmogorov equations for stochastic PDE s with multiplicative noise Giuseppe Da Prato 1 Scuola Normale Superiore, Pisa, Italy 1 Introduction We are here concerned with the following stochastic differential

More information

13 The martingale problem

13 The martingale problem 19-3-2012 Notations Ω complete metric space of all continuous functions from [0, + ) to R d endowed with the distance d(ω 1, ω 2 ) = k=1 ω 1 ω 2 C([0,k];H) 2 k (1 + ω 1 ω 2 C([0,k];H) ), ω 1, ω 2 Ω. F

More information

Strong uniqueness for stochastic evolution equations with possibly unbounded measurable drift term

Strong uniqueness for stochastic evolution equations with possibly unbounded measurable drift term 1 Strong uniqueness for stochastic evolution equations with possibly unbounded measurable drift term Enrico Priola Torino (Italy) Joint work with G. Da Prato, F. Flandoli and M. Röckner Stochastic Processes

More information

Stochastic Invariance and Degenerate Elliptic Operators. P. Cannarsa G. Da Prato H. Frankowska

Stochastic Invariance and Degenerate Elliptic Operators. P. Cannarsa G. Da Prato H. Frankowska Stochastic Invariance and Degenerate Elliptic Operators P. Cannarsa G. Da Prato H. Frankowska Preprint di Matematica N. 1 Maggio 2008 Stochastic Invariance and Degenerate Elliptic Operators P. Cannarsa,

More information

Fonctions on bounded variations in Hilbert spaces

Fonctions on bounded variations in Hilbert spaces Fonctions on bounded variations in ilbert spaces Newton Institute, March 31, 2010 Introduction We recall that a function u : R n R is said to be of bounded variation (BV) if there exists an n-dimensional

More information

b i (µ, x, s) ei ϕ(x) µ s (dx) ds (2) i=1

b i (µ, x, s) ei ϕ(x) µ s (dx) ds (2) i=1 NONLINEAR EVOLTION EQATIONS FOR MEASRES ON INFINITE DIMENSIONAL SPACES V.I. Bogachev 1, G. Da Prato 2, M. Röckner 3, S.V. Shaposhnikov 1 The goal of this work is to prove the existence of a solution to

More information

Elliptic Operators with Unbounded Coefficients

Elliptic Operators with Unbounded Coefficients Elliptic Operators with Unbounded Coefficients Federica Gregorio Universitá degli Studi di Salerno 8th June 2018 joint work with S.E. Boutiah, A. Rhandi, C. Tacelli Motivation Consider the Stochastic Differential

More information

Notions such as convergent sequence and Cauchy sequence make sense for any metric space. Convergent Sequences are Cauchy

Notions such as convergent sequence and Cauchy sequence make sense for any metric space. Convergent Sequences are Cauchy Banach Spaces These notes provide an introduction to Banach spaces, which are complete normed vector spaces. For the purposes of these notes, all vector spaces are assumed to be over the real numbers.

More information

L -uniqueness of Schrödinger operators on a Riemannian manifold

L -uniqueness of Schrödinger operators on a Riemannian manifold L -uniqueness of Schrödinger operators on a Riemannian manifold Ludovic Dan Lemle Abstract. The main purpose of this paper is to study L -uniqueness of Schrödinger operators and generalized Schrödinger

More information

Introduction to Random Diffusions

Introduction to Random Diffusions Introduction to Random Diffusions The main reason to study random diffusions is that this class of processes combines two key features of modern probability theory. On the one hand they are semi-martingales

More information

A NOTE ON STOCHASTIC INTEGRALS AS L 2 -CURVES

A NOTE ON STOCHASTIC INTEGRALS AS L 2 -CURVES A NOTE ON STOCHASTIC INTEGRALS AS L 2 -CURVES STEFAN TAPPE Abstract. In a work of van Gaans (25a) stochastic integrals are regarded as L 2 -curves. In Filipović and Tappe (28) we have shown the connection

More information

Lecture 12. F o s, (1.1) F t := s>t

Lecture 12. F o s, (1.1) F t := s>t Lecture 12 1 Brownian motion: the Markov property Let C := C(0, ), R) be the space of continuous functions mapping from 0, ) to R, in which a Brownian motion (B t ) t 0 almost surely takes its value. Let

More information

SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS

SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS C O L L O Q U I U M M A T H E M A T I C U M VOL. LXIII 1992 FASC. 2 SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS BY JACEK D Z I U B A Ń S K I (WROC

More information

Semigroups and Linear Partial Differential Equations with Delay

Semigroups and Linear Partial Differential Equations with Delay Journal of Mathematical Analysis and Applications 264, 1 2 (21 doi:1.16/jmaa.21.675, available online at http://www.idealibrary.com on Semigroups and Linear Partial Differential Equations with Delay András

More information

Feller Processes and Semigroups

Feller Processes and Semigroups Stat25B: Probability Theory (Spring 23) Lecture: 27 Feller Processes and Semigroups Lecturer: Rui Dong Scribe: Rui Dong ruidong@stat.berkeley.edu For convenience, we can have a look at the list of materials

More information

{σ x >t}p x. (σ x >t)=e at.

{σ x >t}p x. (σ x >t)=e at. 3.11. EXERCISES 121 3.11 Exercises Exercise 3.1 Consider the Ornstein Uhlenbeck process in example 3.1.7(B). Show that the defined process is a Markov process which converges in distribution to an N(0,σ

More information

Invariant Measures Associated to Degenerate Elliptic Operators

Invariant Measures Associated to Degenerate Elliptic Operators Invariant Measures Associated to Degenerate Elliptic Operators P. Cannarsa, G. Da Prato, H. Frankowska August 6, 2009 Abstract This paper is devoted to the study of the existence and uniqueness of the

More information

Regularization by noise in infinite dimensions

Regularization by noise in infinite dimensions Regularization by noise in infinite dimensions Franco Flandoli, University of Pisa King s College 2017 Franco Flandoli, University of Pisa () Regularization by noise King s College 2017 1 / 33 Plan of

More information

Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach

Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach Alberto Bressan Department of Mathematics, Penn State University University Park, Pa 1682, USA e-mail: bressan@mathpsuedu

More information

Some Properties of NSFDEs

Some Properties of NSFDEs Chenggui Yuan (Swansea University) Some Properties of NSFDEs 1 / 41 Some Properties of NSFDEs Chenggui Yuan Swansea University Chenggui Yuan (Swansea University) Some Properties of NSFDEs 2 / 41 Outline

More information

OPERATOR SEMIGROUPS. Lecture 3. Stéphane ATTAL

OPERATOR SEMIGROUPS. Lecture 3. Stéphane ATTAL Lecture 3 OPRATOR SMIGROUPS Stéphane ATTAL Abstract This lecture is an introduction to the theory of Operator Semigroups and its main ingredients: different types of continuity, associated generator, dual

More information

Classical and quantum Markov semigroups

Classical and quantum Markov semigroups Classical and quantum Markov semigroups Alexander Belton Department of Mathematics and Statistics Lancaster University United Kingdom http://www.maths.lancs.ac.uk/~belton/ a.belton@lancaster.ac.uk Young

More information

A Concise Course on Stochastic Partial Differential Equations

A Concise Course on Stochastic Partial Differential Equations A Concise Course on Stochastic Partial Differential Equations Michael Röckner Reference: C. Prevot, M. Röckner: Springer LN in Math. 1905, Berlin (2007) And see the references therein for the original

More information

Infinite-dimensional calculus under weak spatial regularity of the processes

Infinite-dimensional calculus under weak spatial regularity of the processes Infinite-dimensional calculus under weak spatial regularity of the processes Franco Flandoli1, Francesco Russo2, Giovanni Zanco3 November 8, 215 Abstract Two generalizations of Itô formula to infinite-dimensional

More information

PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS

PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS Annales Academiæ Scientiarum Fennicæ Mathematica Volumen 28, 2003, 207 222 PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS Fumi-Yuki Maeda and Takayori Ono Hiroshima Institute of Technology, Miyake,

More information

ON THE FRACTIONAL CAUCHY PROBLEM ASSOCIATED WITH A FELLER SEMIGROUP

ON THE FRACTIONAL CAUCHY PROBLEM ASSOCIATED WITH A FELLER SEMIGROUP Dedicated to Professor Gheorghe Bucur on the occasion of his 7th birthday ON THE FRACTIONAL CAUCHY PROBLEM ASSOCIATED WITH A FELLER SEMIGROUP EMIL POPESCU Starting from the usual Cauchy problem, we give

More information

ON THE FAVARD CLASSES OF SEMIGROUPS ASSOCIATED WITH PSEUDO-RESOLVENTS

ON THE FAVARD CLASSES OF SEMIGROUPS ASSOCIATED WITH PSEUDO-RESOLVENTS ON THE FAVARD CLASSES OF SEMIGROUPS ASSOCIATED WITH PSEUDO-RESOLVENTS WOJCIECH CHOJNACKI AND JAN KISYŃSKI ABSTRACT. A pseudo-resolvent on a Banach space, indexed by positive numbers and tempered at infinity,

More information

BIHARMONIC WAVE MAPS INTO SPHERES

BIHARMONIC WAVE MAPS INTO SPHERES BIHARMONIC WAVE MAPS INTO SPHERES SEBASTIAN HERR, TOBIAS LAMM, AND ROLAND SCHNAUBELT Abstract. A global weak solution of the biharmonic wave map equation in the energy space for spherical targets is constructed.

More information

16 1 Basic Facts from Functional Analysis and Banach Lattices

16 1 Basic Facts from Functional Analysis and Banach Lattices 16 1 Basic Facts from Functional Analysis and Banach Lattices 1.2.3 Banach Steinhaus Theorem Another fundamental theorem of functional analysis is the Banach Steinhaus theorem, or the Uniform Boundedness

More information

at time t, in dimension d. The index i varies in a countable set I. We call configuration the family, denoted generically by Φ: U (x i (t) x j (t))

at time t, in dimension d. The index i varies in a countable set I. We call configuration the family, denoted generically by Φ: U (x i (t) x j (t)) Notations In this chapter we investigate infinite systems of interacting particles subject to Newtonian dynamics Each particle is characterized by its position an velocity x i t, v i t R d R d at time

More information

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 21, 2003, 211 226 SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS Massimo Grosi Filomena Pacella S.

More information

The Wiener Itô Chaos Expansion

The Wiener Itô Chaos Expansion 1 The Wiener Itô Chaos Expansion The celebrated Wiener Itô chaos expansion is fundamental in stochastic analysis. In particular, it plays a crucial role in the Malliavin calculus as it is presented in

More information

MATHS 730 FC Lecture Notes March 5, Introduction

MATHS 730 FC Lecture Notes March 5, Introduction 1 INTRODUCTION MATHS 730 FC Lecture Notes March 5, 2014 1 Introduction Definition. If A, B are sets and there exists a bijection A B, they have the same cardinality, which we write as A, #A. If there exists

More information

Problem Set 5: Solutions Math 201A: Fall 2016

Problem Set 5: Solutions Math 201A: Fall 2016 Problem Set 5: s Math 21A: Fall 216 Problem 1. Define f : [1, ) [1, ) by f(x) = x + 1/x. Show that f(x) f(y) < x y for all x, y [1, ) with x y, but f has no fixed point. Why doesn t this example contradict

More information

Homogenization with stochastic differential equations

Homogenization with stochastic differential equations Homogenization with stochastic differential equations Scott Hottovy shottovy@math.arizona.edu University of Arizona Program in Applied Mathematics October 12, 2011 Modeling with SDE Use SDE to model system

More information

The stochastic obstacle problem for the harmonic oscillator with damping

The stochastic obstacle problem for the harmonic oscillator with damping Preprint di Matematica - n. 9 Novembre 2005 The stochastic obstacle problem for the harmonic oscillator with damping Viorel Barbu Giuseppe a Prato SCUOLA NORMALE SUPERIORE PISA The stochastic obstacle

More information

Some SDEs with distributional drift Part I : General calculus. Flandoli, Franco; Russo, Francesco; Wolf, Jochen

Some SDEs with distributional drift Part I : General calculus. Flandoli, Franco; Russo, Francesco; Wolf, Jochen Title Author(s) Some SDEs with distributional drift Part I : General calculus Flandoli, Franco; Russo, Francesco; Wolf, Jochen Citation Osaka Journal of Mathematics. 4() P.493-P.54 Issue Date 3-6 Text

More information

Probability and Measure

Probability and Measure Part II Year 2018 2017 2016 2015 2014 2013 2012 2011 2010 2009 2008 2007 2006 2005 2018 84 Paper 4, Section II 26J Let (X, A) be a measurable space. Let T : X X be a measurable map, and µ a probability

More information

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011 LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS S. G. Bobkov and F. L. Nazarov September 25, 20 Abstract We study large deviations of linear functionals on an isotropic

More information

SMSTC (2007/08) Probability.

SMSTC (2007/08) Probability. SMSTC (27/8) Probability www.smstc.ac.uk Contents 12 Markov chains in continuous time 12 1 12.1 Markov property and the Kolmogorov equations.................... 12 2 12.1.1 Finite state space.................................

More information

On lower bounds for C 0 -semigroups

On lower bounds for C 0 -semigroups On lower bounds for C 0 -semigroups Yuri Tomilov IM PAN, Warsaw Chemnitz, August, 2017 Yuri Tomilov (IM PAN, Warsaw) On lower bounds for C 0 -semigroups Chemnitz, August, 2017 1 / 17 Trivial bounds For

More information

ON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS

ON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS PORTUGALIAE MATHEMATICA Vol. 55 Fasc. 4 1998 ON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS C. Sonoc Abstract: A sufficient condition for uniqueness of solutions of ordinary

More information

Absolutely convergent Fourier series and classical function classes FERENC MÓRICZ

Absolutely convergent Fourier series and classical function classes FERENC MÓRICZ Absolutely convergent Fourier series and classical function classes FERENC MÓRICZ Bolyai Institute, University of Szeged, Aradi vértanúk tere 1, Szeged 6720, Hungary, e-mail: moricz@math.u-szeged.hu Abstract.

More information

We denote the space of distributions on Ω by D ( Ω) 2.

We denote the space of distributions on Ω by D ( Ω) 2. Sep. 1 0, 008 Distributions Distributions are generalized functions. Some familiarity with the theory of distributions helps understanding of various function spaces which play important roles in the study

More information

Weak convergence and large deviation theory

Weak convergence and large deviation theory First Prev Next Go To Go Back Full Screen Close Quit 1 Weak convergence and large deviation theory Large deviation principle Convergence in distribution The Bryc-Varadhan theorem Tightness and Prohorov

More information

L p Spaces and Convexity

L p Spaces and Convexity L p Spaces and Convexity These notes largely follow the treatments in Royden, Real Analysis, and Rudin, Real & Complex Analysis. 1. Convex functions Let I R be an interval. For I open, we say a function

More information

ON THE POLICY IMPROVEMENT ALGORITHM IN CONTINUOUS TIME

ON THE POLICY IMPROVEMENT ALGORITHM IN CONTINUOUS TIME ON THE POLICY IMPROVEMENT ALGORITHM IN CONTINUOUS TIME SAUL D. JACKA AND ALEKSANDAR MIJATOVIĆ Abstract. We develop a general approach to the Policy Improvement Algorithm (PIA) for stochastic control problems

More information

On some weighted fractional porous media equations

On some weighted fractional porous media equations On some weighted fractional porous media equations Gabriele Grillo Politecnico di Milano September 16 th, 2015 Anacapri Joint works with M. Muratori and F. Punzo Gabriele Grillo Weighted Fractional PME

More information

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS Fixed Point Theory, Volume 9, No. 1, 28, 3-16 http://www.math.ubbcluj.ro/ nodeacj/sfptcj.html NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS GIOVANNI ANELLO Department of Mathematics University

More information

Measure Theory on Topological Spaces. Course: Prof. Tony Dorlas 2010 Typset: Cathal Ormond

Measure Theory on Topological Spaces. Course: Prof. Tony Dorlas 2010 Typset: Cathal Ormond Measure Theory on Topological Spaces Course: Prof. Tony Dorlas 2010 Typset: Cathal Ormond May 22, 2011 Contents 1 Introduction 2 1.1 The Riemann Integral........................................ 2 1.2 Measurable..............................................

More information

A n (T )f = 1 n 1. T i f. i=0

A n (T )f = 1 n 1. T i f. i=0 REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Volumen 46, Número 1, 2005, Páginas 47 51 A NOTE ON THE L 1 -MEAN ERGODIC THEOREM Abstract. Let T be a positive contraction on L 1 of a σ-finite measure space.

More information

Your first day at work MATH 806 (Fall 2015)

Your first day at work MATH 806 (Fall 2015) Your first day at work MATH 806 (Fall 2015) 1. Let X be a set (with no particular algebraic structure). A function d : X X R is called a metric on X (and then X is called a metric space) when d satisfies

More information

The Smoluchowski-Kramers Approximation: What model describes a Brownian particle?

The Smoluchowski-Kramers Approximation: What model describes a Brownian particle? The Smoluchowski-Kramers Approximation: What model describes a Brownian particle? Scott Hottovy shottovy@math.arizona.edu University of Arizona Applied Mathematics October 7, 2011 Brown observes a particle

More information

ON SECOND ORDER DERIVATIVES OF CONVEX FUNCTIONS ON INFINITE DIMENSIONAL SPACES WITH MEASURES

ON SECOND ORDER DERIVATIVES OF CONVEX FUNCTIONS ON INFINITE DIMENSIONAL SPACES WITH MEASURES ON SECOND ORDER DERIVATIVES OF CONVEX FUNCTIONS ON INFINITE DIMENSIONAL SPACES WITH MEASURES VLADIMIR I. BOGACHEV AND BEN GOLDYS Abstract. We consider convex functions on infinite dimensional spaces equipped

More information

On the martingales obtained by an extension due to Saisho, Tanemura and Yor of Pitman s theorem

On the martingales obtained by an extension due to Saisho, Tanemura and Yor of Pitman s theorem On the martingales obtained by an extension due to Saisho, Tanemura and Yor of Pitman s theorem Koichiro TAKAOKA Dept of Applied Physics, Tokyo Institute of Technology Abstract M Yor constructed a family

More information

GIOVANNI COMI AND MONICA TORRES

GIOVANNI COMI AND MONICA TORRES ONE-SIDED APPROXIMATION OF SETS OF FINITE PERIMETER GIOVANNI COMI AND MONICA TORRES Abstract. In this note we present a new proof of a one-sided approximation of sets of finite perimeter introduced in

More information

A scaling limit from Euler to Navier-Stokes equations with random perturbation

A scaling limit from Euler to Navier-Stokes equations with random perturbation A scaling limit from Euler to Navier-Stokes equations with random perturbation Franco Flandoli, Scuola Normale Superiore of Pisa Newton Institute, October 208 Newton Institute, October 208 / Subject of

More information

Convergence of Feller Processes

Convergence of Feller Processes Chapter 15 Convergence of Feller Processes This chapter looks at the convergence of sequences of Feller processes to a iting process. Section 15.1 lays some ground work concerning weak convergence of processes

More information

1 Brownian Local Time

1 Brownian Local Time 1 Brownian Local Time We first begin by defining the space and variables for Brownian local time. Let W t be a standard 1-D Wiener process. We know that for the set, {t : W t = } P (µ{t : W t = } = ) =

More information

Brownian Motion. 1 Definition Brownian Motion Wiener measure... 3

Brownian Motion. 1 Definition Brownian Motion Wiener measure... 3 Brownian Motion Contents 1 Definition 2 1.1 Brownian Motion................................. 2 1.2 Wiener measure.................................. 3 2 Construction 4 2.1 Gaussian process.................................

More information

Introduction to Semigroup Theory

Introduction to Semigroup Theory Introduction to Semigroup Theory Franz X. Gmeineder LMU München, U Firenze Bruck am Ziller / Dec 15th 2012 Franz X. Gmeineder Introduction to Semigroup Theory 1/25 The Way Up: Opening The prototype of

More information

13. Examples of measure-preserving tranformations: rotations of a torus, the doubling map

13. Examples of measure-preserving tranformations: rotations of a torus, the doubling map 3. Examples of measure-preserving tranformations: rotations of a torus, the doubling map 3. Rotations of a torus, the doubling map In this lecture we give two methods by which one can show that a given

More information

EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM. Saeid Shokooh and Ghasem A. Afrouzi. 1. Introduction

EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM. Saeid Shokooh and Ghasem A. Afrouzi. 1. Introduction MATEMATIČKI VESNIK MATEMATIQKI VESNIK 69 4 (217 271 28 December 217 research paper originalni nauqni rad EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM Saeid Shokooh and Ghasem A.

More information

Spaces with Ricci curvature bounded from below

Spaces with Ricci curvature bounded from below Spaces with Ricci curvature bounded from below Nicola Gigli February 23, 2015 Topics 1) On the definition of spaces with Ricci curvature bounded from below 2) Analytic properties of RCD(K, N) spaces 3)

More information

Errata Applied Analysis

Errata Applied Analysis Errata Applied Analysis p. 9: line 2 from the bottom: 2 instead of 2. p. 10: Last sentence should read: The lim sup of a sequence whose terms are bounded from above is finite or, and the lim inf of a sequence

More information

c 2001 Society for Industrial and Applied Mathematics

c 2001 Society for Industrial and Applied Mathematics SIAM J. CONTROL OPTIM. Vol. 4, No. 3, pp. 824 852 c 21 Society for Industrial and Applied Mathematics STATIONARY HAMILTON JACOBI EQUATIONS IN HILBERT SPACES AND APPLICATIONS TO A STOCHASTIC OPTIMAL CONTROL

More information

L p Functions. Given a measure space (X, µ) and a real number p [1, ), recall that the L p -norm of a measurable function f : X R is defined by

L p Functions. Given a measure space (X, µ) and a real number p [1, ), recall that the L p -norm of a measurable function f : X R is defined by L p Functions Given a measure space (, µ) and a real number p [, ), recall that the L p -norm of a measurable function f : R is defined by f p = ( ) /p f p dµ Note that the L p -norm of a function f may

More information

LOCAL FIXED POINT THEORY INVOLVING THREE OPERATORS IN BANACH ALGEBRAS. B. C. Dhage. 1. Introduction

LOCAL FIXED POINT THEORY INVOLVING THREE OPERATORS IN BANACH ALGEBRAS. B. C. Dhage. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 24, 24, 377 386 LOCAL FIXED POINT THEORY INVOLVING THREE OPERATORS IN BANACH ALGEBRAS B. C. Dhage Abstract. The present

More information

p 1 ( Y p dp) 1/p ( X p dp) 1 1 p

p 1 ( Y p dp) 1/p ( X p dp) 1 1 p Doob s inequality Let X(t) be a right continuous submartingale with respect to F(t), t 1 P(sup s t X(s) λ) 1 λ {sup s t X(s) λ} X + (t)dp 2 For 1 < p

More information

Math 328 Course Notes

Math 328 Course Notes Math 328 Course Notes Ian Robertson March 3, 2006 3 Properties of C[0, 1]: Sup-norm and Completeness In this chapter we are going to examine the vector space of all continuous functions defined on the

More information

MATH MEASURE THEORY AND FOURIER ANALYSIS. Contents

MATH MEASURE THEORY AND FOURIER ANALYSIS. Contents MATH 3969 - MEASURE THEORY AND FOURIER ANALYSIS ANDREW TULLOCH Contents 1. Measure Theory 2 1.1. Properties of Measures 3 1.2. Constructing σ-algebras and measures 3 1.3. Properties of the Lebesgue measure

More information

Brownian motion. Samy Tindel. Purdue University. Probability Theory 2 - MA 539

Brownian motion. Samy Tindel. Purdue University. Probability Theory 2 - MA 539 Brownian motion Samy Tindel Purdue University Probability Theory 2 - MA 539 Mostly taken from Brownian Motion and Stochastic Calculus by I. Karatzas and S. Shreve Samy T. Brownian motion Probability Theory

More information

An invariance result for Hammersley s process with sources and sinks

An invariance result for Hammersley s process with sources and sinks An invariance result for Hammersley s process with sources and sinks Piet Groeneboom Delft University of Technology, Vrije Universiteit, Amsterdam, and University of Washington, Seattle March 31, 26 Abstract

More information

OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS

OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS APPLICATIONES MATHEMATICAE 29,4 (22), pp. 387 398 Mariusz Michta (Zielona Góra) OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS Abstract. A martingale problem approach is used first to analyze

More information

Your first day at work MATH 806 (Fall 2015)

Your first day at work MATH 806 (Fall 2015) Your first day at work MATH 806 (Fall 2015) 1. Let X be a set (with no particular algebraic structure). A function d : X X R is called a metric on X (and then X is called a metric space) when d satisfies

More information

Continuous Functions on Metric Spaces

Continuous Functions on Metric Spaces Continuous Functions on Metric Spaces Math 201A, Fall 2016 1 Continuous functions Definition 1. Let (X, d X ) and (Y, d Y ) be metric spaces. A function f : X Y is continuous at a X if for every ɛ > 0

More information

STOCHASTIC DIFFERENTIAL EQUATIONS DRIVEN BY PROCESSES WITH INDEPENDENT INCREMENTS

STOCHASTIC DIFFERENTIAL EQUATIONS DRIVEN BY PROCESSES WITH INDEPENDENT INCREMENTS STOCHASTIC DIFFERENTIAL EQUATIONS DRIVEN BY PROCESSES WITH INDEPENDENT INCREMENTS DAMIR FILIPOVIĆ AND STEFAN TAPPE Abstract. This article considers infinite dimensional stochastic differential equations

More information

Reminder Notes for the Course on Measures on Topological Spaces

Reminder Notes for the Course on Measures on Topological Spaces Reminder Notes for the Course on Measures on Topological Spaces T. C. Dorlas Dublin Institute for Advanced Studies School of Theoretical Physics 10 Burlington Road, Dublin 4, Ireland. Email: dorlas@stp.dias.ie

More information

SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT

SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT Abstract. These are the letcure notes prepared for the workshop on Functional Analysis and Operator Algebras to be held at NIT-Karnataka,

More information

Measure and Integration: Solutions of CW2

Measure and Integration: Solutions of CW2 Measure and Integration: s of CW2 Fall 206 [G. Holzegel] December 9, 206 Problem of Sheet 5 a) Left (f n ) and (g n ) be sequences of integrable functions with f n (x) f (x) and g n (x) g (x) for almost

More information

arxiv: v1 [math.pr] 1 May 2014

arxiv: v1 [math.pr] 1 May 2014 Submitted to the Brazilian Journal of Probability and Statistics A note on space-time Hölder regularity of mild solutions to stochastic Cauchy problems in L p -spaces arxiv:145.75v1 [math.pr] 1 May 214

More information

ON THE REGULARITY OF ONE PARAMETER TRANSFORMATION GROUPS IN BARRELED LOCALLY CONVEX TOPOLOGICAL VECTOR SPACES

ON THE REGULARITY OF ONE PARAMETER TRANSFORMATION GROUPS IN BARRELED LOCALLY CONVEX TOPOLOGICAL VECTOR SPACES Communications on Stochastic Analysis Vol. 9, No. 3 (2015) 413-418 Serials Publications www.serialspublications.com ON THE REGULARITY OF ONE PARAMETER TRANSFORMATION GROUPS IN BARRELED LOCALLY CONVEX TOPOLOGICAL

More information

ON MARKOV AND KOLMOGOROV MATRICES AND THEIR RELATIONSHIP WITH ANALYTIC OPERATORS. N. Katilova (Received February 2004)

ON MARKOV AND KOLMOGOROV MATRICES AND THEIR RELATIONSHIP WITH ANALYTIC OPERATORS. N. Katilova (Received February 2004) NEW ZEALAND JOURNAL OF MATHEMATICS Volume 34 (2005), 43 60 ON MARKOV AND KOLMOGOROV MATRICES AND THEIR RELATIONSHIP WITH ANALYTIC OPERATORS N. Katilova (Received February 2004) Abstract. In this article,

More information

Real Analysis Problems

Real Analysis Problems Real Analysis Problems Cristian E. Gutiérrez September 14, 29 1 1 CONTINUITY 1 Continuity Problem 1.1 Let r n be the sequence of rational numbers and Prove that f(x) = 1. f is continuous on the irrationals.

More information

Fast-slow systems with chaotic noise

Fast-slow systems with chaotic noise Fast-slow systems with chaotic noise David Kelly Ian Melbourne Courant Institute New York University New York NY www.dtbkelly.com May 1, 216 Statistical properties of dynamical systems, ESI Vienna. David

More information

New York Journal of Mathematics. A Refinement of Ball s Theorem on Young Measures

New York Journal of Mathematics. A Refinement of Ball s Theorem on Young Measures New York Journal of Mathematics New York J. Math. 3 (1997) 48 53. A Refinement of Ball s Theorem on Young Measures Norbert Hungerbühler Abstract. For a sequence u j : R n R m generating the Young measure

More information

PREDICTABLE REPRESENTATION PROPERTY OF SOME HILBERTIAN MARTINGALES. 1. Introduction.

PREDICTABLE REPRESENTATION PROPERTY OF SOME HILBERTIAN MARTINGALES. 1. Introduction. Acta Math. Univ. Comenianae Vol. LXXVII, 1(28), pp. 123 128 123 PREDICTABLE REPRESENTATION PROPERTY OF SOME HILBERTIAN MARTINGALES M. EL KADIRI Abstract. We prove as for the real case that a martingale

More information

Uniqueness of Fokker-Planck equations for spin lattice systems (I): compact case

Uniqueness of Fokker-Planck equations for spin lattice systems (I): compact case Semigroup Forum (213) 86:583 591 DOI 1.17/s233-12-945-y RESEARCH ARTICLE Uniqueness of Fokker-Planck equations for spin lattice systems (I): compact case Ludovic Dan Lemle Ran Wang Liming Wu Received:

More information

2 A Model, Harmonic Map, Problem

2 A Model, Harmonic Map, Problem ELLIPTIC SYSTEMS JOHN E. HUTCHINSON Department of Mathematics School of Mathematical Sciences, A.N.U. 1 Introduction Elliptic equations model the behaviour of scalar quantities u, such as temperature or

More information

Trace Class Operators and Lidskii s Theorem

Trace Class Operators and Lidskii s Theorem Trace Class Operators and Lidskii s Theorem Tom Phelan Semester 2 2009 1 Introduction The purpose of this paper is to provide the reader with a self-contained derivation of the celebrated Lidskii Trace

More information

Random Process Lecture 1. Fundamentals of Probability

Random Process Lecture 1. Fundamentals of Probability Random Process Lecture 1. Fundamentals of Probability Husheng Li Min Kao Department of Electrical Engineering and Computer Science University of Tennessee, Knoxville Spring, 2016 1/43 Outline 2/43 1 Syllabus

More information

Solutions: Problem Set 4 Math 201B, Winter 2007

Solutions: Problem Set 4 Math 201B, Winter 2007 Solutions: Problem Set 4 Math 2B, Winter 27 Problem. (a Define f : by { x /2 if < x

More information

CESARO OPERATORS ON THE HARDY SPACES OF THE HALF-PLANE

CESARO OPERATORS ON THE HARDY SPACES OF THE HALF-PLANE CESARO OPERATORS ON THE HARDY SPACES OF THE HALF-PLANE ATHANASIOS G. ARVANITIDIS AND ARISTOMENIS G. SISKAKIS Abstract. In this article we study the Cesàro operator C(f)() = d, and its companion operator

More information

On Semigroups Of Linear Operators

On Semigroups Of Linear Operators On Semigroups Of Linear Operators Elona Fetahu Submitted to Central European University Department of Mathematics and its Applications In partial fulfillment of the requirements for the degree of Master

More information

Annalee Gomm Math 714: Assignment #2

Annalee Gomm Math 714: Assignment #2 Annalee Gomm Math 714: Assignment #2 3.32. Verify that if A M, λ(a = 0, and B A, then B M and λ(b = 0. Suppose that A M with λ(a = 0, and let B be any subset of A. By the nonnegativity and monotonicity

More information

MATH 418: Lectures on Conditional Expectation

MATH 418: Lectures on Conditional Expectation MATH 418: Lectures on Conditional Expectation Instructor: r. Ed Perkins, Notes taken by Adrian She Conditional expectation is one of the most useful tools of probability. The Radon-Nikodym theorem enables

More information

René Bartsch and Harry Poppe (Received 4 July, 2015)

René Bartsch and Harry Poppe (Received 4 July, 2015) NEW ZEALAND JOURNAL OF MATHEMATICS Volume 46 2016, 1-8 AN ABSTRACT ALGEBRAIC-TOPOLOGICAL APPROACH TO THE NOTIONS OF A FIRST AND A SECOND DUAL SPACE III René Bartsch and Harry Poppe Received 4 July, 2015

More information

PROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS

PROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS PROBABILITY: LIMIT THEOREMS II, SPRING 218. HOMEWORK PROBLEMS PROF. YURI BAKHTIN Instructions. You are allowed to work on solutions in groups, but you are required to write up solutions on your own. Please

More information

2 Lebesgue integration

2 Lebesgue integration 2 Lebesgue integration 1. Let (, A, µ) be a measure space. We will always assume that µ is complete, otherwise we first take its completion. The example to have in mind is the Lebesgue measure on R n,

More information