On a class of stochastic differential equations in a financial network model
|
|
- Emery Edwards
- 6 years ago
- Views:
Transcription
1 1 On a class of stochastic differential equations in a financial network model Tomoyuki Ichiba Department of Statistics & Applied Probability, Center for Financial Mathematics and Actuarial Research, University of California, Santa Barbara Part of research is joint work with Nils Detering & Jean-Pierre Fouque Thira May 217 Thera Stochastics
2 Motivation: On (; F ; (F t ); P) let us consider R N -valued diffusion process (X 1 (t ); : : : ; X N (t )), t < 1 induced by the following random graph structure. Suppose that at time we have a random graph of N vertices f1; : : : ; N g and define the strength of connections between vertices i and j by F -measurable random variable a i ;j (whose distribution may depend on N ) for every 1 i 6= j N and fix a i ;i = for 1 i N. We shall consider dx i (t ) = 1 N NX j=1 for i = 1; : : : ; N, t, a i ;j (X i (t ) X j (t )) dt + db i (t ) ;
3 where (B 1 (t ); : : : ; B N (t )), t is the standard N -dimensional BM, independent of (X 1 (); : : : ; X N ()) and of the random variables (a i ;j ) 1i ;j N. The randomness determined at time affects the diffusion process (X 1 ( ); : : : ; X N ( )). Deterministic A in the context of financial network : Carmona, Fouque, Sun ( 13), Fouque & Ichiba ( 13),... The system is solvable as a linear stochastic system for X ( ) := (X 1 ( ); : : : ; X N ( )). Let A (N) := (a i ;j ) 1i ;j N be the (N N ) random matrix and B ( ) be the (N 1) -vector valued standard Brownian motion.
4 Then the system can be rewritten as dx (t ) = A (N) X (t )dt + db (t ) ; A (N) 1 := N Diag(A(N) 1 1 N ) N A(N) ; where 1 N is the (N 1) vector of ones, and Diag(c) is the diagonal matrix whose diagonal elements are those elements in the vector c. Note that each row sum of elements in the matrix A (N) is zero by definition, i.e., a (N) i ;i = X j 6=i a (N) i ;j for each i = 1; : : : ; N, where a (N) i ;j random matrix A (N). is the (i ; j ) element of the
5 5 The solution to this linear equation is given by X (t ) = e ta(n ) X () + e sa(n ) db (s) ; t : Here we understand e ta(n ) is the (N N ) matrix exponential. Given the initial value X () and A (N), the law of X ( ) is conditionally an N -dimensional Gaussian law with mean e ta(n ) X () and variance covariance matrix Var(X (t )ja (N) ). Q. How to understand the case N! 1 of large network, i.e., what happens if N! 1? For example, if A (N) a :s :! A(1) and N!1
6 if a (1) i ;j = 1 for j = i + 1, a (1) i ;i = 1, a (1) i ;j, o.w., i.e., A (1) := C A ; then how can we solve? dx 1 (t ) = (X 2 (t ) X 1 (t ))dt + dw 1 (t ) ; dx 2 (t ) = (X 3 (t ) X 2 (t ))dt + dw 2 (t ) ; Finite N case: Fernholz & Karatzas ( 8-9) studied flow, filtering and pseudo-brownian motion process in equity markets..
7 7 Example as N! 1 For simplicity let us set X i () =. Given X 2 ( ), we have X 1 (t ) = e (t s) X 2 (s)ds + e (t s) db 1 (s) ; and also, given X 3 ( ), we have X 2 (s) = Z s e (s u) X 3 (u)du + Z s e (s u) db 2 (u) for t, and hence substituting X 2 ( ) into the first one, X 1 (t ) = for t. + e (t s) db 1 (s) + Z s Z e (t s) s e (s u) X 3 (u)du e (t u) db 2 (u)ds
8 By the product rule for semimartingales, we observe Z s e u (s u) k 1 db (u)ds = for k 2 N, t, and hence u (t u)k e db (u) ; k Z s e u db (u)ds = e u (t u)db (u) ; Z sk Z s1 e u db (u)ds 1 ds k = u (t u)k e db (u) k! for k 2 N, t. Thus for the above example we have for t. X 1 (t ) = 1X k= e (t u) (t u)k k! db k+1(u)
9 9 X 1 (t ) = 1X k= e (t u) (t u)k k! is a centered, Gaussian process with covariances E[X 1 (s)x 1 (t )] = e (s+t) 1 X k= Z s Z = e (t s) s e 2v I (2 q db k+1(u) e 2u (k!) 2 (s u)k (t u) k du (t s + v )v )dv for s t, where I ( ) is the modified Bessel function of the first kind with parameter, i.e., I (x ) := for x >, 1. 1X k= x 2 2k+ 1 (k + 1) ( + k + 1)
10 1 In particular, Var(X 1 (t )) = e 2v I (2v )dv = te 2t (I (2t ) + I 1 (2t )) < 1 (it grows as O(t 1=2 ) for large t, also, E[X 1 (s)x 1 (s + t )] = O(e (t 2p (t+s)s) t 1=4 ) :) Thus X 1 ( ) is not stationary. The (marginal) distribution of X k ( ), k 2 N is the same as X 1 ( ), and hence, we may compute (at least numerically) E[X 1 (t )X 2 (u)] = e (t s) E X 2 (s)x 2 (u) ds = e (t s) E X 1 (s)x 1 (u) ds and recursively, E[X 1 (t )X k (u)], k 2 N for t ; u < 1.
11 Sample path of (X 1 ( ); X 2 ( )) generated from the covariance structure. X 1 (t ) = X 1 ( ) X 2 ( ) e (t s) X 2 (s)ds + for t and Law(X 1 ( )) = Law(X 2 ( )). e (t s) db 1 (s) ;
12 Weighted by Poisson probabilities An interpretation of for t : X 1 (t ) = =: 1X k= 1X k= e (t u) (t u)k k! p k (t u)db k+1(u) db k+1(u) Suppose N (s) ; s t is a Poisson process with rate 1, independent of (B k ( ); k 2 N). Then h 1X X 1 (t ) = E k= 1 fn(t u) = kgdb k+1(u) F (t ) where F (t ) := (B k (s); s t ; k 2 N), t. i ;
13 If we replace the Poisson probability by compound Poisson probability, i.e., fn (t ) := N(t) X k=1 k ; where ( k ; k 2 N) are I.I.D. integer-valued R.V. s with P( 1 = i ) = p i, 1 i q, P q i=1 p i = 1 for some q 2 N, independent of N ( ) and (B k ( ); k 2 N), then where fx 1 (t ) := E = ep k (t ) := for k 2 N, t h 1X k= 1X k exp 1 fen(t u) = kg db k+1(u) F (t ) ep k (t u)db k+1(u) ; q X i=1 13 i p i t (z i z 1) = i
14 14 corresponds to the modified matrix A (1) := 1 p 1 p 2 p q 1 p 1 p 2 p q C A ; and dx k (t ) = X k (t ) + qx i=1 p i X i+k (t ) dt + db k (t ) with X k () = for k 2 N, t. In particular, if q = 2, p 1 = p 2 = 1=2, then ep k (t ) = bk X=2c j= e t t k j 2 k j (k 2j )! j! ; t ; k 2 N :
15 15 Another modification: dx 1 (t ) = (X 1 (t ) X 2 (t ))dt + db 1 (t ) ; dx 2 (t ) = (X 2 (t ) X 3 (t ))dt + db 2 (t ) ; We may use the same reasoning in this case to obtain X 1 (t ) = 1X k= e t s ( 1)k (t s) k k! with exponentially growing variance db k+1(s) Var(X 1 (t )) = te 2t (I (2t ) I 1 (2t )) ; t :
16 A formulation of equation with identical distribution Let us consider (; F ; P; ff (t ); t g) on which X ( ) is an adapted stochastic process which is a weak solution to dx (t ) = b(t ; X (t ); X 1 (t ))dt + (t ; X (t ); X 1 (t ))db (t ) ; t ; where r -dimensional standard Brownian motion B ( ) is independent of d -dimensional process X 1 ( ) which has the same distribution as X ( ) on [; T ] i.e., Law(X (s); s T ) = Law(X 1 (s); s T ) ; and also P a.s. X () = x 2 R d and Z T (kb(t ; X (t ); X 1 (t ))k + k i ;j (t ; X (t ); X 1 (t ))k 2 )dt < +1 for 1 i d, 1 j r and T. Here we assume
17 b : R+ R d R d! R d and : R+ R d R d! R d r are Lipschitz continuous with at most linear growth, i.e., there exist a constant K > such that kb(t ; x ; y) b(t ; ex ; ey)k + k(t ; x ; y) (t ; ex ; ey)k K (kx ex k + ky and kb(t ; x ; y)k 2 + k(t ; x ; y)k 2 K 2 (1 + kx k 2 + kyk 2 ) for every (t ; x ; y) 2 R+ R d R d. We also assume that X 1 ( ) is adapted to the filtration ff 1 (t ); t g generated by the Brownian motions (B k (t ); k 1; t ) augmented by the P -null sets. We shall solve this system with distributional identity.
18 When b(t ; x ; y) = x y and (t ; x ; y) = 1, it reduces to the first example X 1 (t ) = e (t s) X 2 (s)ds + e (t s) db 1 (s) ; t : In the linear case we may consider the corresponding A (1) to the example of the block matrix form A (1) = A 1;1 A 1;2 A 1;1 A 1; C A : It looks similar to the nonlinear diffusion dx (t ) = b(x (t ); E[X (t )])dt + (X (t ); E[X (t )])db (t ) ; t of mean-field which appears as Mckean-Vlasov limit of interacting particles (Mckean ( 67), Kac ( 73), Sznitman ( 89), Tanaka ( 84), Shiga & Tanaka ( 85),... ), but is different.
19 Proposition. On some probability space (; F ; P; ff (t ); t g) there is a unique weak solution to dx (t ) = b(t ; X (t ); X 1 (t ))dt + (t ; X (t ); X 1 (t ))db (t ) ; t ; with Law(X 1 (t ); t T ) = Law(X (t ); t T ) and satisfies (t ) = E[ sup kx (s) X 1 (s)k 2 ] ; t st (s)ds + e (t s) Z s (u)du ds c 1 (t ) ; for t T, T >, where := 4K 2 ( 1 + T ), c := 9 max(1; K 2 ( 1 + T )(1 _ T )) ; c 1 := and 1 is a global constant form the Burkholder-Davis-Gundy inequality e(c )T c
20 Idea of proof: Given B ( ) and X 1 ( ), we may construct X ( ) by the method of Picard iteration, i.e., there exists a map : C ([; 1); R d ) C ([; 1); R r )! C ([; 1); R d ) with X (t ) = t (X 1 ; B ) for t. We shall find a fixed point of ( ; B ), i.e., Law(X 1 ( )) = Law( (X 1 ; B )) = Law(X ( )) by evaluating the Wassestein distance W 2;T (; e) := inf E [ sup k(t ) (t e )k 2 ] tt where = Law(( )), e = Law(e ( )) and the infimum is taken over the joint law of (( ); e ( )), and using Banach fixed point theorem.
21 S := n ( ) : (s)ds + e (t s) Z s c 1 (t ) ; t T (u)du ds Note that c >, ( 1 e (c )T ) = ( c ) < 1 and, 1 (t ) := e ct satisfies 1 (s)ds+ e (t s) Z s 1 (u)du ds = c 1 1 (t ) ; t T ; and so, 1 ( ) 2 S and S is non-empty. If f 2 S, then c f 2 S for every positive constant c >. o
22 22 Also, if f ; g 2 S, then a f + (1 a) g 2 S for every a 2 [; 1], and hence, S is convex. Moreover, since ( 1 e (x )T ) = ( x ) is a non-decreasing function of x for x >, 2 (t ) := e c2t with < c 2 c satisfies 2 (s)ds+ e (t s) Z s 2 (u)du ds = 1 e (c2 )T c 2 2 (t ) c 1 2 (t ) ; t T ; and hence 2 ( ) 2 S for every < c 2 c.
23 We may extend to the case of the form dx (t ) = b(t ; X (t ); : : : ; X q (t ))dt +(t ; X (t ); : : : ; X q (t ))db (t ) with Law(X ( )) = Law(X 1 ( )) = = Law(X q ( )) for some q 2 N and with Lipschitz coefficients, where X i ( ) is adapted to the filtration generated by (B k ( ); k i ) for i 2 N.
24 24 Coming back to the diffusions on the graph We say the infinite dimensional matrix x = (x i ;j )(i ;j)2n 2 row-finite if for each i 2 N there is k (i ) 2 N such that x i ;j = for every j k (i ). is We say the infinite dimensional matrix x = (x i ;j )(i ;j)2n 2 is uniformly row-finite, if there is n 2 N such that x i ;j = for every i 2 N and every j with ji j j n. We also say the infinite dimensional matrix (x i ;j )(i ;j)2n 2 (uniformly) column-finite, if its transpose (x i ;j ) (i ;j)2n is 2 (uniformly) row finite. is Let us denote by A the class of uniformly positive definite, bounded, infinite dimensional matrices which are both uniformly row and uniformly column finite.
25 Suppose that there exist u > d > such that all the eigenvalues of A (N) are bounded above by u and below by d for every N, and as N! 1, each (i ; j ) element a (N) i ;j of A (N) converges to an (i ; j ) element a (1) i ;j of fixed matrix A (1) 2 A almost surely for every (i ; j ) 2 N 2, i.e., lim a(n) i ;j = a (1) i ;j : N!1 Assume the first k elements X (k ;N) () = (X 1 (); : : : ; X k ()) of initial random variables X (N) () converges weakly to an R k -valued random vector (k) for every k 2 N. We also assume that sup N E[kX (k ;N) ()k 4 ] < 1 for every k 2 N.
26 26 Then for every k 2 N and T >, as N! 1, the law of the first k elements X (k ;N) ( ) = (X 1 ( ); : : : ; X k ( )) of X (N) ( ) = (X 1 ( ); : : : ; X N ( )) converges weakly in C ([; T ]) to the law of the first k -dimensional stochastic process Y (k) ( ) := (Y 1 ( ); : : : ; Y k ( )) of Y ( ) := (Y i ( )) i2n defined by Y (t ) = e ta(1) Y () + e sa(1) dw (s) ; t ; where Law(Y (k) ()) = Law( (k) ) for every k 2 N and W ( ) is the R 1 -valued standard Brownian motion.
27 Summary Thank you all for your attentions, and Happy Birthday! Examples of linear systems on infinite graph A class of stochastic differential equations with restrictions in their distribution Part of research is supported by grants NSF -DMS and DMS
Some Aspects of Universal Portfolio
1 Some Aspects of Universal Portfolio Tomoyuki Ichiba (UC Santa Barbara) joint work with Marcel Brod (ETH Zurich) Conference on Stochastic Asymptotics & Applications Sixth Western Conference on Mathematical
More informationConvergence at first and second order of some approximations of stochastic integrals
Convergence at first and second order of some approximations of stochastic integrals Bérard Bergery Blandine, Vallois Pierre IECN, Nancy-Université, CNRS, INRIA, Boulevard des Aiguillettes B.P. 239 F-5456
More informationMultilevel Monte Carlo for Stochastic McKean-Vlasov Equations
Multilevel Monte Carlo for Stochastic McKean-Vlasov Equations Lukasz Szpruch School of Mathemtics University of Edinburgh joint work with Shuren Tan and Alvin Tse (Edinburgh) Lukasz Szpruch (University
More informationBrownian 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 informationConvex polytopes, interacting particles, spin glasses, and finance
Convex polytopes, interacting particles, spin glasses, and finance Sourav Chatterjee (UCB) joint work with Soumik Pal (Cornell) Interacting particles Systems of particles governed by joint stochastic differential
More informationBernardo D Auria Stochastic Processes /10. Notes. Abril 13 th, 2010
1 Stochastic Calculus Notes Abril 13 th, 1 As we have seen in previous lessons, the stochastic integral with respect to the Brownian motion shows a behavior different from the classical Riemann-Stieltjes
More informationCompeting Brownian Particles
Competing Brownian Particles Andrey Sarantsev University of California, Santa Barbara February 9, 2018 Andrey Sarantsev California State University, Los Angeles 1 / 16 Brownian Motion A Brownian motion
More informationEULER MARUYAMA APPROXIMATION FOR SDES WITH JUMPS AND NON-LIPSCHITZ COEFFICIENTS
Qiao, H. Osaka J. Math. 51 (14), 47 66 EULER MARUYAMA APPROXIMATION FOR SDES WITH JUMPS AND NON-LIPSCHITZ COEFFICIENTS HUIJIE QIAO (Received May 6, 11, revised May 1, 1) Abstract In this paper we show
More informationStrong Solutions and a Bismut-Elworthy-Li Formula for Mean-F. Formula for Mean-Field SDE s with Irregular Drift
Strong Solutions and a Bismut-Elworthy-Li Formula for Mean-Field SDE s with Irregular Drift Thilo Meyer-Brandis University of Munich joint with M. Bauer, University of Munich Conference for the 1th Anniversary
More informationI forgot to mention last time: in the Ito formula for two standard processes, putting
I forgot to mention last time: in the Ito formula for two standard processes, putting dx t = a t dt + b t db t dy t = α t dt + β t db t, and taking f(x, y = xy, one has f x = y, f y = x, and f xx = f yy
More informationMathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio ( )
Mathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio (2014-2015) Etienne Tanré - Olivier Faugeras INRIA - Team Tosca November 26th, 2014 E. Tanré (INRIA - Team Tosca) Mathematical
More informationWeakly interacting particle systems on graphs: from dense to sparse
Weakly interacting particle systems on graphs: from dense to sparse Ruoyu Wu University of Michigan (Based on joint works with Daniel Lacker and Kavita Ramanan) USC Math Finance Colloquium October 29,
More informationWalsh Diffusions. Andrey Sarantsev. March 27, University of California, Santa Barbara. Andrey Sarantsev University of Washington, Seattle 1 / 1
Walsh Diffusions Andrey Sarantsev University of California, Santa Barbara March 27, 2017 Andrey Sarantsev University of Washington, Seattle 1 / 1 Walsh Brownian Motion on R d Spinning measure µ: probability
More informationSelected Exercises on Expectations and Some Probability Inequalities
Selected Exercises on Expectations and Some Probability Inequalities # If E(X 2 ) = and E X a > 0, then P( X λa) ( λ) 2 a 2 for 0 < λ
More informationBrownian 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 informationOn 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 informationTopics in fractional Brownian motion
Topics in fractional Brownian motion Esko Valkeila Spring School, Jena 25.3. 2011 We plan to discuss the following items during these lectures: Fractional Brownian motion and its properties. Topics in
More informationExercises in stochastic analysis
Exercises in stochastic analysis Franco Flandoli, Mario Maurelli, Dario Trevisan The exercises with a P are those which have been done totally or partially) in the previous lectures; the exercises with
More informationEQUITY MARKET STABILITY
EQUITY MARKET STABILITY Adrian Banner INTECH Investment Technologies LLC, Princeton (Joint work with E. Robert Fernholz, Ioannis Karatzas, Vassilios Papathanakos and Phillip Whitman.) Talk at WCMF6 conference,
More informationPROBABILITY: 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 informationThe concentration of a drug in blood. Exponential decay. Different realizations. Exponential decay with noise. dc(t) dt.
The concentration of a drug in blood Exponential decay C12 concentration 2 4 6 8 1 C12 concentration 2 4 6 8 1 dc(t) dt = µc(t) C(t) = C()e µt 2 4 6 8 1 12 time in minutes 2 4 6 8 1 12 time in minutes
More informationNotes on uniform convergence
Notes on uniform convergence Erik Wahlén erik.wahlen@math.lu.se January 17, 2012 1 Numerical sequences We begin by recalling some properties of numerical sequences. By a numerical sequence we simply mean
More information1. Stochastic Processes and filtrations
1. Stochastic Processes and 1. Stoch. pr., A stochastic process (X t ) t T is a collection of random variables on (Ω, F) with values in a measurable space (S, S), i.e., for all t, In our case X t : Ω S
More informationFormulas for probability theory and linear models SF2941
Formulas for probability theory and linear models SF2941 These pages + Appendix 2 of Gut) are permitted as assistance at the exam. 11 maj 2008 Selected formulae of probability Bivariate probability Transforms
More informationLarge Deviations Principles for McKean-Vlasov SDEs, Skeletons, Supports and the law of iterated logarithm
Large Deviations Principles for McKean-Vlasov SDEs, Skeletons, Supports and the law of iterated logarithm Gonçalo dos Reis University of Edinburgh (UK) & CMA/FCT/UNL (PT) jointly with: W. Salkeld, U. of
More informationELEG 3143 Probability & Stochastic Process Ch. 6 Stochastic Process
Department of Electrical Engineering University of Arkansas ELEG 3143 Probability & Stochastic Process Ch. 6 Stochastic Process Dr. Jingxian Wu wuj@uark.edu OUTLINE 2 Definition of stochastic process (random
More informationA Second-Order Model of the Stock Market
A Second-Order Model of the Stock Market Robert Fernholz INTECH Conference in honor of Ioannis Karatzas Columbia University, New York June 4 8, 2012 This is joint research with T. Ichiba, I. Karatzas.
More informationLOCAL TIMES OF RANKED CONTINUOUS SEMIMARTINGALES
LOCAL TIMES OF RANKED CONTINUOUS SEMIMARTINGALES ADRIAN D. BANNER INTECH One Palmer Square Princeton, NJ 8542, USA adrian@enhanced.com RAOUF GHOMRASNI Fakultät II, Institut für Mathematik Sekr. MA 7-5,
More informationPROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS
PROBABILITY: LIMIT THEOREMS II, SPRING 15. 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 informationProperties of an infinite dimensional EDS system : the Muller s ratchet
Properties of an infinite dimensional EDS system : the Muller s ratchet LATP June 5, 2011 A ratchet source : wikipedia Plan 1 Introduction : The model of Haigh 2 3 Hypothesis (Biological) : The population
More informationFunctional Limit theorems for the quadratic variation of a continuous time random walk and for certain stochastic integrals
Functional Limit theorems for the quadratic variation of a continuous time random walk and for certain stochastic integrals Noèlia Viles Cuadros BCAM- Basque Center of Applied Mathematics with Prof. Enrico
More informationHybrid Atlas Model. of financial equity market. Tomoyuki Ichiba 1 Ioannis Karatzas 2,3 Adrian Banner 3 Vassilios Papathanakos 3 Robert Fernholz 3
Hybrid Atlas Model of financial equity market Tomoyuki Ichiba 1 Ioannis Karatzas 2,3 Adrian Banner 3 Vassilios Papathanakos 3 Robert Fernholz 3 1 University of California, Santa Barbara 2 Columbia University,
More informationOn mean-field approximation of part annihilation and spikes (Probabilit. Citation 数理解析研究所講究録 (2017), 2030:
Title On mean-field approximation of part annihilation and spikes (Probabilit Author(s) Ichiba Tomoyuki Citation 数理解析研究所講究録 (2017) 2030: 28-31 Issue Date 2017-05 URL http://hdlhandlenet/2433/231867 Right
More informationShort-time expansions for close-to-the-money options under a Lévy jump model with stochastic volatility
Short-time expansions for close-to-the-money options under a Lévy jump model with stochastic volatility José Enrique Figueroa-López 1 1 Department of Statistics Purdue University Statistics, Jump Processes,
More informationLecture 21 Representations of Martingales
Lecture 21: Representations of Martingales 1 of 11 Course: Theory of Probability II Term: Spring 215 Instructor: Gordan Zitkovic Lecture 21 Representations of Martingales Right-continuous inverses Let
More informationMonte-Carlo MMD-MA, Université Paris-Dauphine. Xiaolu Tan
Monte-Carlo MMD-MA, Université Paris-Dauphine Xiaolu Tan tan@ceremade.dauphine.fr Septembre 2015 Contents 1 Introduction 1 1.1 The principle.................................. 1 1.2 The error analysis
More informationOn continuous time contract theory
Ecole Polytechnique, France Journée de rentrée du CMAP, 3 octobre, 218 Outline 1 2 Semimartingale measures on the canonical space Random horizon 2nd order backward SDEs (Static) Principal-Agent Problem
More informationJump-type Levy Processes
Jump-type Levy Processes Ernst Eberlein Handbook of Financial Time Series Outline Table of contents Probabilistic Structure of Levy Processes Levy process Levy-Ito decomposition Jump part Probabilistic
More informationWeak solutions of mean-field stochastic differential equations
Weak solutions of mean-field stochastic differential equations Juan Li School of Mathematics and Statistics, Shandong University (Weihai), Weihai 26429, China. Email: juanli@sdu.edu.cn Based on joint works
More informationA 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 informationThe goal of this chapter is to study linear systems of ordinary differential equations: dt,..., dx ) T
1 1 Linear Systems The goal of this chapter is to study linear systems of ordinary differential equations: ẋ = Ax, x(0) = x 0, (1) where x R n, A is an n n matrix and ẋ = dx ( dt = dx1 dt,..., dx ) T n.
More informationExercises with solutions (Set D)
Exercises with solutions Set D. A fair die is rolled at the same time as a fair coin is tossed. Let A be the number on the upper surface of the die and let B describe the outcome of the coin toss, where
More informationNonlinear representation, backward SDEs, and application to the Principal-Agent problem
Nonlinear representation, backward SDEs, and application to the Principal-Agent problem Ecole Polytechnique, France April 4, 218 Outline The Principal-Agent problem Formulation 1 The Principal-Agent problem
More informationBranching Processes II: Convergence of critical branching to Feller s CSB
Chapter 4 Branching Processes II: Convergence of critical branching to Feller s CSB Figure 4.1: Feller 4.1 Birth and Death Processes 4.1.1 Linear birth and death processes Branching processes can be studied
More informationInterest Rate Models:
1/17 Interest Rate Models: from Parametric Statistics to Infinite Dimensional Stochastic Analysis René Carmona Bendheim Center for Finance ORFE & PACM, Princeton University email: rcarmna@princeton.edu
More informationLecture 9. d N(0, 1). Now we fix n and think of a SRW on [0,1]. We take the k th step at time k n. and our increments are ± 1
Random Walks and Brownian Motion Tel Aviv University Spring 011 Lecture date: May 0, 011 Lecture 9 Instructor: Ron Peled Scribe: Jonathan Hermon In today s lecture we present the Brownian motion (BM).
More informationStability of Stochastic Differential Equations
Lyapunov stability theory for ODEs s Stability of Stochastic Differential Equations Part 1: Introduction Department of Mathematics and Statistics University of Strathclyde Glasgow, G1 1XH December 2010
More informationOPTIMAL 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 informationApproximation of BSDEs using least-squares regression and Malliavin weights
Approximation of BSDEs using least-squares regression and Malliavin weights Plamen Turkedjiev (turkedji@math.hu-berlin.de) 3rd July, 2012 Joint work with Prof. Emmanuel Gobet (E cole Polytechnique) Plamen
More informationBrownian survival and Lifshitz tail in perturbed lattice disorder
Brownian survival and Lifshitz tail in perturbed lattice disorder Ryoki Fukushima Kyoto niversity Random Processes and Systems February 16, 2009 6 B T 1. Model ) ({B t t 0, P x : standard Brownian motion
More informationA diamagnetic inequality for semigroup differences
A diamagnetic inequality for semigroup differences (Irvine, November 10 11, 2001) Barry Simon and 100DM 1 The integrated density of states (IDS) Schrödinger operator: H := H(V ) := 1 2 + V ω =: H(0, V
More informationMaximum Likelihood Drift Estimation for Gaussian Process with Stationary Increments
Austrian Journal of Statistics April 27, Volume 46, 67 78. AJS http://www.ajs.or.at/ doi:.773/ajs.v46i3-4.672 Maximum Likelihood Drift Estimation for Gaussian Process with Stationary Increments Yuliya
More informationOn pathwise stochastic integration
On pathwise stochastic integration Rafa l Marcin Lochowski Afican Institute for Mathematical Sciences, Warsaw School of Economics UWC seminar Rafa l Marcin Lochowski (AIMS, WSE) On pathwise stochastic
More informationLarge deviations and averaging for systems of slow fast stochastic reaction diffusion equations.
Large deviations and averaging for systems of slow fast stochastic reaction diffusion equations. Wenqing Hu. 1 (Joint work with Michael Salins 2, Konstantinos Spiliopoulos 3.) 1. Department of Mathematics
More informationBernardo D Auria Stochastic Processes /12. Notes. March 29 th, 2012
1 Stochastic Calculus Notes March 9 th, 1 In 19, Bachelier proposed for the Paris stock exchange a model for the fluctuations affecting the price X(t) of an asset that was given by the Brownian motion.
More information. Find E(V ) and var(v ).
Math 6382/6383: Probability Models and Mathematical Statistics Sample Preliminary Exam Questions 1. A person tosses a fair coin until she obtains 2 heads in a row. She then tosses a fair die the same number
More informationUniformly Uniformly-ergodic Markov chains and BSDEs
Uniformly Uniformly-ergodic Markov chains and BSDEs Samuel N. Cohen Mathematical Institute, University of Oxford (Based on joint work with Ying Hu, Robert Elliott, Lukas Szpruch) Centre Henri Lebesgue,
More informationA class of globally solvable systems of BSDE and applications
A class of globally solvable systems of BSDE and applications Gordan Žitković Department of Mathematics The University of Texas at Austin Thera Stochastics - Wednesday, May 31st, 2017 joint work with Hao
More informationHardy-Stein identity and Square functions
Hardy-Stein identity and Square functions Daesung Kim (joint work with Rodrigo Bañuelos) Department of Mathematics Purdue University March 28, 217 Daesung Kim (Purdue) Hardy-Stein identity UIUC 217 1 /
More informationFourier transforms of measures on the Brownian graph
of measures on the Brownian graph The University of Manchester Joint work with Tuomas Sahlsten (Bristol, UK) and Tuomas Orponen (Helsinki, Finland) ICERM 1th March 216 My co-authors and dimension The Fourier
More informationDiscretization of SDEs: Euler Methods and Beyond
Discretization of SDEs: Euler Methods and Beyond 09-26-2006 / PRisMa 2006 Workshop Outline Introduction 1 Introduction Motivation Stochastic Differential Equations 2 The Time Discretization of SDEs Monte-Carlo
More informationBrownian Motion and Stochastic Calculus
ETHZ, Spring 17 D-MATH Prof Dr Martin Larsson Coordinator A Sepúlveda Brownian Motion and Stochastic Calculus Exercise sheet 6 Please hand in your solutions during exercise class or in your assistant s
More informationMarket environments, stability and equlibria
Market environments, stability and equlibria Gordan Žitković Department of Mathematics University of exas at Austin Austin, Aug 03, 2009 - Summer School in Mathematical Finance he Information Flow two
More informationA 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 informationBranching Brownian motion seen from the tip
Branching Brownian motion seen from the tip J. Berestycki 1 1 Laboratoire de Probabilité et Modèles Aléatoires, UPMC, Paris 09/02/2011 Joint work with Elie Aidekon, Eric Brunet and Zhan Shi J Berestycki
More informationMean-Field optimization problems and non-anticipative optimal transport. Beatrice Acciaio
Mean-Field optimization problems and non-anticipative optimal transport Beatrice Acciaio London School of Economics based on ongoing projects with J. Backhoff, R. Carmona and P. Wang Robust Methods in
More informationAlbert N. Shiryaev Steklov Mathematical Institute. On sharp maximal inequalities for stochastic processes
Albert N. Shiryaev Steklov Mathematical Institute On sharp maximal inequalities for stochastic processes joint work with Yaroslav Lyulko, Higher School of Economics email: albertsh@mi.ras.ru 1 TOPIC I:
More informationECE353: Probability and Random Processes. Lecture 18 - Stochastic Processes
ECE353: Probability and Random Processes Lecture 18 - Stochastic Processes Xiao Fu School of Electrical Engineering and Computer Science Oregon State University E-mail: xiao.fu@oregonstate.edu From RV
More information1 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(B(t i+1 ) B(t i )) 2
ltcc5.tex Week 5 29 October 213 Ch. V. ITÔ (STOCHASTIC) CALCULUS. WEAK CONVERGENCE. 1. Quadratic Variation. A partition π n of [, t] is a finite set of points t ni such that = t n < t n1
More informationfor all f satisfying E[ f(x) ] <.
. Let (Ω, F, P ) be a probability space and D be a sub-σ-algebra of F. An (H, H)-valued random variable X is independent of D if and only if P ({X Γ} D) = P {X Γ}P (D) for all Γ H and D D. Prove that if
More informationStochastic Areas and Applications in Risk Theory
Stochastic Areas and Applications in Risk Theory July 16th, 214 Zhenyu Cui Department of Mathematics Brooklyn College, City University of New York Zhenyu Cui 49th Actuarial Research Conference 1 Outline
More informationWeak 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 informationMean field simulation for Monte Carlo integration. Part II : Feynman-Kac models. P. Del Moral
Mean field simulation for Monte Carlo integration Part II : Feynman-Kac models P. Del Moral INRIA Bordeaux & Inst. Maths. Bordeaux & CMAP Polytechnique Lectures, INLN CNRS & Nice Sophia Antipolis Univ.
More informationRandom Variables and Their Distributions
Chapter 3 Random Variables and Their Distributions A random variable (r.v.) is a function that assigns one and only one numerical value to each simple event in an experiment. We will denote r.vs by capital
More informationHomogenization for chaotic dynamical systems
Homogenization for chaotic dynamical systems David Kelly Ian Melbourne Department of Mathematics / Renci UNC Chapel Hill Mathematics Institute University of Warwick November 3, 2013 Duke/UNC Probability
More informationProperties of the Autocorrelation Function
Properties of the Autocorrelation Function I The autocorrelation function of a (real-valued) random process satisfies the following properties: 1. R X (t, t) 0 2. R X (t, u) =R X (u, t) (symmetry) 3. R
More informationStochastic optimal control with rough paths
Stochastic optimal control with rough paths Paul Gassiat TU Berlin Stochastic processes and their statistics in Finance, Okinawa, October 28, 2013 Joint work with Joscha Diehl and Peter Friz Introduction
More informationGeometry of log-concave Ensembles of random matrices
Geometry of log-concave Ensembles of random matrices Nicole Tomczak-Jaegermann Joint work with Radosław Adamczak, Rafał Latała, Alexander Litvak, Alain Pajor Cortona, June 2011 Nicole Tomczak-Jaegermann
More informationLesson 4: Stationary stochastic processes
Dipartimento di Ingegneria e Scienze dell Informazione e Matematica Università dell Aquila, umberto.triacca@univaq.it Stationary stochastic processes Stationarity is a rather intuitive concept, it means
More informationµ X (A) = P ( X 1 (A) )
1 STOCHASTIC PROCESSES This appendix provides a very basic introduction to the language of probability theory and stochastic processes. We assume the reader is familiar with the general measure and integration
More informationTRANSPORT INEQUALITIES FOR STOCHASTIC
TRANSPORT INEQUALITIES FOR STOCHASTIC PROCESSES Soumik Pal University of Washington, Seattle Jun 6, 2012 INTRODUCTION Three problems about rank-based processes THE ATLAS MODEL Define ranks: x (1) x (2)...
More informationAnalysis of an M/G/1 queue with customer impatience and an adaptive arrival process
Analysis of an M/G/1 queue with customer impatience and an adaptive arrival process O.J. Boxma 1, O. Kella 2, D. Perry 3, and B.J. Prabhu 1,4 1 EURANDOM and Department of Mathematics & Computer Science,
More informationA. Bovier () Branching Brownian motion: extremal process and ergodic theorems
Branching Brownian motion: extremal process and ergodic theorems Anton Bovier with Louis-Pierre Arguin and Nicola Kistler RCS&SM, Venezia, 06.05.2013 Plan 1 BBM 2 Maximum of BBM 3 The Lalley-Sellke conjecture
More informationf (1 0.5)/n Z =
Math 466/566 - Homework 4. We want to test a hypothesis involving a population proportion. The unknown population proportion is p. The null hypothesis is p = / and the alternative hypothesis is p > /.
More informationMan Kyu Im*, Un Cig Ji **, and Jae Hee Kim ***
JOURNAL OF THE CHUNGCHEONG MATHEMATICAL SOCIETY Volume 19, No. 4, December 26 GIRSANOV THEOREM FOR GAUSSIAN PROCESS WITH INDEPENDENT INCREMENTS Man Kyu Im*, Un Cig Ji **, and Jae Hee Kim *** Abstract.
More informationMetric Spaces and Topology
Chapter 2 Metric Spaces and Topology From an engineering perspective, the most important way to construct a topology on a set is to define the topology in terms of a metric on the set. This approach underlies
More informationLecture Notes 3 Convergence (Chapter 5)
Lecture Notes 3 Convergence (Chapter 5) 1 Convergence of Random Variables Let X 1, X 2,... be a sequence of random variables and let X be another random variable. Let F n denote the cdf of X n and let
More informationStrong 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 informationarxiv: v1 [math.pr] 24 Sep 2018
A short note on Anticipative portfolio optimization B. D Auria a,b,1,, J.-A. Salmerón a,1 a Dpto. Estadística, Universidad Carlos III de Madrid. Avda. de la Universidad 3, 8911, Leganés (Madrid Spain b
More informationConvoluted Brownian motions: a class of remarkable Gaussian processes
Convoluted Brownian motions: a class of remarkable Gaussian processes Sylvie Roelly Random models with applications in the natural sciences Bogotá, December 11-15, 217 S. Roelly (Universität Potsdam) 1
More informationStrong approximation for additive functionals of geometrically ergodic Markov chains
Strong approximation for additive functionals of geometrically ergodic Markov chains Florence Merlevède Joint work with E. Rio Université Paris-Est-Marne-La-Vallée (UPEM) Cincinnati Symposium on Probability
More informationKernel Method: Data Analysis with Positive Definite Kernels
Kernel Method: Data Analysis with Positive Definite Kernels 2. Positive Definite Kernel and Reproducing Kernel Hilbert Space Kenji Fukumizu The Institute of Statistical Mathematics. Graduate University
More informationHarnack Inequalities and Applications for Stochastic Equations
p. 1/32 Harnack Inequalities and Applications for Stochastic Equations PhD Thesis Defense Shun-Xiang Ouyang Under the Supervision of Prof. Michael Röckner & Prof. Feng-Yu Wang March 6, 29 p. 2/32 Outline
More informationn E(X t T n = lim X s Tn = X s
Stochastic Calculus Example sheet - Lent 15 Michael Tehranchi Problem 1. Let X be a local martingale. Prove that X is a uniformly integrable martingale if and only X is of class D. Solution 1. If If direction:
More informationMean-Field optimization problems and non-anticipative optimal transport. Beatrice Acciaio
Mean-Field optimization problems and non-anticipative optimal transport Beatrice Acciaio London School of Economics based on ongoing projects with J. Backhoff, R. Carmona and P. Wang Thera Stochastics
More informationExistence and Comparisons for BSDEs in general spaces
Existence and Comparisons for BSDEs in general spaces Samuel N. Cohen and Robert J. Elliott University of Adelaide and University of Calgary BFS 2010 S.N. Cohen, R.J. Elliott (Adelaide, Calgary) BSDEs
More informationVast Volatility Matrix Estimation for High Frequency Data
Vast Volatility Matrix Estimation for High Frequency Data Yazhen Wang National Science Foundation Yale Workshop, May 14-17, 2009 Disclaimer: My opinion, not the views of NSF Y. Wang (at NSF) 1 / 36 Outline
More informationLimit theorems for Hawkes processes
Limit theorems for nearly unstable and Mathieu Rosenbaum Séminaire des doctorants du CMAP Vendredi 18 Octobre 213 Limit theorems for 1 Denition and basic properties Cluster representation of Correlation
More informationEcon Lecture 14. Outline
Econ 204 2010 Lecture 14 Outline 1. Differential Equations and Solutions 2. Existence and Uniqueness of Solutions 3. Autonomous Differential Equations 4. Complex Exponentials 5. Linear Differential Equations
More information