Loss of martingality in asset price models with lognormal stochastic volatility

Size: px
Start display at page:

Download "Loss of martingality in asset price models with lognormal stochastic volatility"

Transcription

1 Loss of maringaliy in asse price models wih lognormal sochasic volailiy BJourdain July 7, 4 Absrac In his noe, we prove ha in asse price models wih lognormal sochasic volailiy, when he correlaion coefficien beween he Brownian moion driving he volailiy and he one driving he acualized asse price is posiive, his price is no a maringale Inroducion On a filered probabiliy space Ω, F, F, P, we consider he following risk-neural model for he acualized asse price X : dx = σ X ρ db + 1 ρ dw, X = x σ = e Y 1 dy = db + µd γy d, Y = y where B, W is a wo-dimensional F -Brownian moion, y, µ and γ belong o R, x and are posiive consans and he correlaion coefficien ρ beween he Brownian moion ρ B + 1 ρ W driving he asse price and he Brownian moion B driving he volailiy belongs o [ 1, 1] In his model, firs inroduced by Sco [7] p46, he volailiy σ is he exponenial of he Ornsein-Uhlenbeck process Y When he elasiciy coefficien γ is zero, σ evolves according o he Black-Scholes Sochasic Differenial Equaion dσ = σ db + µ + /d, and 1 is he model inroduced by Hull&Whie [3] and a special case of he very popular SABR model [1] Since X = x E e Ys ρ db s + 1 ρ dw s, where E sands for Dooleans-Dade exponenial, his process is a non-negaive F local maringale and herefore a super-maringale his leads o he following naural quesion : is X a ENPC-CERMICS, 6-8 av Blaise Pascal, Cié Descares, Champs sur Marne, Marne-la-Vallée Cedex, France and MAHFI projec - jourdain@cermicsenpcfr 1

2 rue maringale? he answer urns ou o be affirmaive if and only if he correlaion coefficien ρ is non-posiive see heorem 1 below In addiion, when ρ >, i is possible o check ha EX is decreasing see Proposiion 4 As a consequence, he Call-Pu pariy relaion does no hold whaever he mauriy and srike of he opions he exisence of such arbirage opporuniies invalidaes he model For ρ, X is a maringale and we invesigae he inegrabiliy of X δ for > and δ > 1 his quesion is imporan for numerical consideraions : for insance, inegrabiliy of X is necessary o ensure ha he convergence of a Mone-Carlo esimaor of EX K + is ruled by he cenral limi heorem Basically, we obain ha X δ is inegrable when δ < 1/1 ρ and ha EX δ is infinie when δ > 1/1 ρ 1 Sudy of maringale propery Our main resul is he following one : heorem 1 Process X is a maringale if and only if ρ Remark he fac ha X is no a maringale when ρ > is no so bad since in order o modelize he increase of volailiy in krach siuaions, ρ is generally chosen non-posiive For >, by Jensen inequaliy and since Y sds is a Gaussian random variable wih posiive variance, E 1 exp e Ys ds E exp e Ysds = + herefore we canno rely on Novikov crierion and corollaries see [5] p198 o prove ha X is a maringale in case ρ In conras, in he models proposed eiher in [7] p41, [8] where he sochasic volailiy σ in he firs line of 1 solves or in [4], [] where dσ = µ γσ d + db σ = Y for Y = y + one easily checks ha µ γy s ds + >, c >, sup E e c σ < + Ys db s wih µ, y As a consequence if 1 < and 1 c, hen by Jensen inequaliy, E e 1 σ d 1 1 E e 1 σ d < By [5] Corollary 514 p199, one concludes ha X is always a maringale in such models

3 In order o deal wih he general SABR model [1], le us consider X solving dx = e Y X β ρdb + 1 ρ dw, X = x wih β, 1 and Y like in 1 Inroducing τ n = inf{, X > n}, one has EX τ n = x + E τn x + x + E e Ys X β s ds e Ys/1 β 1 β EX s τn β ds E e Ys/1 β 1 β 1 + EX s τn ds Remarking ha s E e Ys/1 β is locally bounded, using Gronwall s Lemma, and leing n +, one obains ha E ds is locally bounded which ensures ha eys Xs β X is a maringale In conclusion, in he SABR model, he acualized asse price may fail o be a maringale only in he limi case β = 1 Proof : As X is a super-maringale, i is enough o check ha he non-increasing funcion EX /x is no consan if and only if ρ > Using he independence of W and B and he fac ha Y is adaped o he naural filraion of B, one obains EX = x E E ρ = x E E ρ 1 e Ys db s E E ρ e Ys dw s B s, s e Ys db s In case ρ =, one concludes ha EX = x for any posiive ime o deal wih he case ρ, we are firs going o use Girsanov heorem in order o be able o apply Exercice 1 p 354 [6] his way, EX /x urns ou o be equal o he probabiliy for he explosion ime of a well-chosen sochasic differenial equaion o be greaer han We will finally analyse wheher his explosion ime is finie wih posiive probabiliy hanks o Feller s es for explosions [5] p Le us inroduce he probabiliy measure Q such ha dq γy µ dp = E F According o Girsanov heorem, B = B + For any, y + B = y + B γ γy µ + γb s db s + γb s ds is a Brownian moion under Q y + B s ds + µ As rajecorial uniqueness holds for he Ornsein-Uhlenbeck Sochasic Differenial Equaion, by Yamada Waanabe heorem, he law of B, y + B under probabiliy measure Q is he 3

4 same as he law of B, Y under probabiliy measure P As a consequence, EX ] = E [E ρ expy + B s d x B s = E [E ρ ] = E [E bb s db s expy + B s db s exp ρ γy µ expy + B s E γy µ + γb s ds + γb s db s ] where bz = ρ expy + z + µ γy γz Le us briefly recall he link made in [6] Exercice 1 p354 beween he las expecaion and he probabiliy for he explosion ime of he Sochasic Differenial Equaion Z = B + 3 bz s ds 4 o be greaer han Since funcion b is locally Lipschiz coninuous, for any n N, here exiss a bounded and globally Lipschiz coninuous funcion b n which coincides wih b on inerval [ n, n] We denoe by Z n he soluion of he equaion similar o 4 wih b replaced by b n and inroduce τ n = inf{ : Z n > n} hen Z = n 1 {τn 1 <τ n}z n convenion : τ = solves 4 on ime-inerval [, τ where τ = lim n + τ n Le us also define σ n = inf{ : B > n} By Girsanov heorem and since b n coincides wih b on inerval [ n, n], Pτ n > = E 1 {σn>}e b n B s db s = E 1 {σn>}e Leing n + hen using 3, we conclude ha Pτ > = E E bb s db s = EX x bb s db s In order o analyse he explosion ime τ of he sochasic differenial equaion 4 hanks o Feller s es for explosions, we inroduce consans ρ = ρe y / and η = µ γy / so ha he drif coefficien of his equaion wries bz = ρ expz/ + η/ γz Noice ha he sign of ρ is he same as he one of ρ Funcion z pz = e ρ exp γx ηx ρe x dx 5 4

5 is a scale funcion According o [5] heorem 59 p348, Pτ = + = 1 is equivalen o v+ = v = + where funcion v is given by vz = = z z p x p y dydx exp γx ηx ρe x exp γy + ηy + ρe y dydx 6 o conclude he proof, we are going o check ha v+ < + if ρ > and ha v+ = v = + if ρ < Case ρ > ie ρ > : le > be such ha y, γy + η + ρe y > By inegraion by pars, one has for x, exp γy + ηy + ρe y dy = exp γx + ηx + ρe x γx + η + ρe x exp γx 1 + η + ρe γ + η + ρe + ρey γ exp γy + ηy + ρe y γy + η + ρe y dy One may choose large enough o ensure ha y, ρ e y γ 1 γy + η + ρey hen for any x, exp γy + ηy + ρe y dy exp γx + ηx + ρe x γx + η + ρe x and one easily concludes ha v+ < + Case ρ < ie ρ < : hen p+ = + which implies v+ = + according o [5] Problem 57 p348 If γ >, hen p = and herefore v = + I only remains o check ha v = + in case γ Since for non posiive y, exp ρe y belongs o [exp ρ, 1, v = + is equivalen o w = where wz = z If γ =, hen η = µ/ and expγx ηx exp γy + ηydydx wz = { z if µ = µ z + µ e µz/ 1 if µ which ensures w = + If γ <, seing < η/γ, one obains by inegraion by pars ha for x exp γy + ηydy = exp γx + ηx η γx exp γx + ηx η γx exp γ + η η γ exp γ + η η γ γ exp γy + ηy η γy dy 5

6 Hence for any x, one has exp γy + ηydy exp γx + ηx η γx + C, where he consan C does no depend on x One deduces ha w = + Remark 3 he argumen given a he end of he previous proof o check ha v = + in case ρ < also leads o he same conclusion in case ρ > When he correlaion coefficien ρ is posiive, he non-increasing and non-negaive funcion EX is no consan I is naural o wonder wheher his funcion is decreasing and wheher i ends o as + he nex proposiion answers boh quesions : Proposiion 4 Assume ha ρ > hen EX is decreasing In addiion, EX ends o as ends o + if and only if eiher γ > or γ = and µ Remark 5 As a consequence, when ρ >,, K >, EX K + EK X + < x K ie he Call-Pu pariy relaion does no hold Proof : Le us firs deal wih he limi of EX = x Pτ > as ends o + One easily checks ha he scale funcion pz defined by 5 saisfies p = if and only if eiher γ > or γ = and η Because η = µ γy /, he laer condiion is equivalen o γ = and µ Since v+ is finie according o he proof of heorem 1 and v = + according o Remark 3, by [5] Proposiion 53 p35, one concludes ha Pτ < + = 1 and equivalenly lim + EX = if and only if γ > or γ = and µ Le us now check ha EX is decreasing As we need o emphasize he dependence on he iniial condiions, we denoe X x,y, Y y he soluion of 1 One has, x >, y R, EX x,y = x EX 1,y Le us firs check ha for any posiive, he se A = {y R : EX 1,y < 1} has posiive Lebesgue measure Indeed if > is such ha he Lebesgue measure of A is zero, remarking ha by he Markov propery, EX 1,y = E EX 1,y F = E EX x,y x,y=x 1,y,Y y = E X 1,y EX 1,y y=y y, and ha since he law of Y y is absoluely coninuous wih respec o he Lebesgue measure PY y A =, we obain EX 1,y = EX1,y herefore A = A By inducion, for any n N, A n = A and for y R \ A, X 1,y is a maringale, which conradics heorem 1 Le now s < Again by he Markov Propery, EX 1,y = E X 1,y +s/ E X s/ 1,y y=y y +s/ 6

7 Since he law of Y y +s/ is equivalen o he Lebesgue measure, P Y y +s/ A s/ > One deduces ha EX 1,y < EX 1,y +s/ As he righ-hand-side is no greaer han EX 1,y s, one concludes ha EX 1,y is decreasing Inegrabiliy of X δ for δ > 1 Proposiion 6 Le > and δ > 1 If ρ = hen EX δ = + If ρ <, hen EX δ < + if and only if one of he following condiions is saisfied : δ < 1/1 ρ δ = 1/1 ρ and γ > δ = 1/1 ρ, γ = and µ + Proof : Le us compue X o he power δ wih δ > 1 : X δ = x δ exp δ ρ e Ys db s + 1 δ1 ρ 1 e Ys ds E δ 1 ρ herefore, reasoning like in, one obains [ EX δ = x δ E exp δ ρ e Ys db s + 1 δ1 ρ 1 e Ys dw s ] e Ys ds 7 In case ρ =, by Jensen inequaliy and since Y sds is a Gaussian variable wih posiive variance, δδ 1 EX δ = xδ [exp E ] [ δδ 1 e Ys ds x δ E exp e Le us now deal wih he case ρ < According o 1 and Iô s formula, e Y e y = e Ys db s + µ + / γy s e Ys ds Ysds ] = + Insering in 7 he expression of eys db s obained from his formula, one obains ρ EX δ = xδ [exp E δ ey e y ρ + γy s µ / + 1 ] δ1 ρ 1e Ys e Ys ds Under any of he hree condiions saed in he Proposiion, funcion ρ y R γy µ / + 1 δ1 ρ 1e y e y is bounded from above by a finie consan C As a consequence, ρ δ ey e y ρ + γy s µ / + 1 δ1 ρ 1e Ys e Ys ds δc ρe y / 7

8 and for any >, sup EX δ xδ exp δc ρey / [, ] Le us now suppose ha none of he hree condiions saed in he Proposiion is saisfied hen here is a posiive consan ε such ha funcion ρ y R γy µ / + 1 δ1 ρ 1e y e y εe y is bounded from below by a finie consan As a consequence here is a posiive consan C such as [ ρ ] EX δ CE exp δ ey + ε e Ys ds By Jensen inequaliy, EX δ CE [exp δ ρ ey + εe 1 Ysds] [ = CE exp δρe Y / E exp δεe 1 Since he covariance marix of he Gaussian vecor Y, Y sds is non-degenerae, E exp δεe 1 Ysds Y = + almos surely and one concludes ha EX δ = + Ysds ] Y Remark 7 For ρ >, when one of he following condiion is saisfied δ > 1/1 ρ δ = 1/1 ρ and γ > δ = 1/1 ρ and γ = and µ +, hen funcion y R ρ γy µ / + 1 δ1 ρ 1e y e y is bounded from below herefore EX δ CEexpδρeY / = + when > Bu i does no seem easy o analyse wheher EX δ is finie when none of he previous condiions holds References [1] PS Hagan, D Kumar, AS Lesniewski, and DE Woodward Managing Smile Risk Preprin, [] SL Heson A Closed-Form Soluion for Opions wih Sochasic Volailiy wih Applicaions o Bond and Currency Opions he Review of Financial Sudies, 6:37 343, 1993 [3] J Hull and A Whie he Pricing of Opions on Asses wih Sochasic Volailiies he Journal of Finance, XLII:81 3, june 1987 [4] J Hull and A Whie An analysis of he bias in opion pricing caused by a sochasic volailiy Advances in Fuures and Opions Research, 3:9 61,

9 [5] I Karazas and SE Shreve Brownian Moion and Sochasic Calculus Springer-Verlag, 1988 [6] D Revuz and M Yor Coninuous maringales and Brownian moion Springer-Verlag, 1991 [7] L Sco Opion pricing when he variance changes randomly : heory, esimaion and an applicaion Journal of Financial and Quaniaive Analysis, : , 1987 [8] EM Sein and JC Sein Sock Price Disribuions wih Sochasic Volailiy: An Analyic Approach he Review of Financial Sudies, 44:77 75,

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

On a Fractional Stochastic Landau-Ginzburg Equation

On a Fractional Stochastic Landau-Ginzburg Equation Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn

More information

Stochastic Modelling in Finance - Solutions to sheet 8

Stochastic Modelling in Finance - Solutions to sheet 8 Sochasic Modelling in Finance - Soluions o shee 8 8.1 The price of a defaulable asse can be modeled as ds S = µ d + σ dw dn where µ, σ are consans, (W ) is a sandard Brownian moion and (N ) is a one jump

More information

Homework 10 (Stats 620, Winter 2017) Due Tuesday April 18, in class Questions are derived from problems in Stochastic Processes by S. Ross.

Homework 10 (Stats 620, Winter 2017) Due Tuesday April 18, in class Questions are derived from problems in Stochastic Processes by S. Ross. Homework (Sas 6, Winer 7 Due Tuesday April 8, in class Quesions are derived from problems in Sochasic Processes by S. Ross.. A sochasic process {X(, } is said o be saionary if X(,..., X( n has he same

More information

f(s)dw Solution 1. Approximate f by piece-wise constant left-continuous non-random functions f n such that (f(s) f n (s)) 2 ds 0.

f(s)dw Solution 1. Approximate f by piece-wise constant left-continuous non-random functions f n such that (f(s) f n (s)) 2 ds 0. Advanced Financial Models Example shee 3 - Michaelmas 217 Michael Tehranchi Problem 1. Le f : [, R be a coninuous (non-random funcion and W a Brownian moion, and le σ 2 = f(s 2 ds and assume σ 2

More information

arxiv: v1 [math.pr] 21 May 2010

arxiv: v1 [math.pr] 21 May 2010 ON SCHRÖDINGER S EQUATION, 3-DIMENSIONAL BESSEL BRIDGES, AND PASSAGE TIME PROBLEMS arxiv:15.498v1 [mah.pr 21 May 21 GERARDO HERNÁNDEZ-DEL-VALLE Absrac. In his work we relae he densiy of he firs-passage

More information

Lecture #31, 32: The Ornstein-Uhlenbeck Process as a Model of Volatility

Lecture #31, 32: The Ornstein-Uhlenbeck Process as a Model of Volatility Saisics 441 (Fall 214) November 19, 21, 214 Prof Michael Kozdron Lecure #31, 32: The Ornsein-Uhlenbeck Process as a Model of Volailiy The Ornsein-Uhlenbeck process is a di usion process ha was inroduced

More information

Utility maximization in incomplete markets

Utility maximization in incomplete markets Uiliy maximizaion in incomplee markes Marcel Ladkau 27.1.29 Conens 1 Inroducion and general seings 2 1.1 Marke model....................................... 2 1.2 Trading sraegy.....................................

More information

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation: M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno

More information

6. Stochastic calculus with jump processes

6. Stochastic calculus with jump processes A) Trading sraegies (1/3) Marke wih d asses S = (S 1,, S d ) A rading sraegy can be modelled wih a vecor φ describing he quaniies invesed in each asse a each insan : φ = (φ 1,, φ d ) The value a of a porfolio

More information

What Ties Return Volatilities to Price Valuations and Fundamentals? On-Line Appendix

What Ties Return Volatilities to Price Valuations and Fundamentals? On-Line Appendix Wha Ties Reurn Volailiies o Price Valuaions and Fundamenals? On-Line Appendix Alexander David Haskayne School of Business, Universiy of Calgary Piero Veronesi Universiy of Chicago Booh School of Business,

More information

Lecture 4: Processes with independent increments

Lecture 4: Processes with independent increments Lecure 4: Processes wih independen incremens 1. A Wienner process 1.1 Definiion of a Wienner process 1.2 Reflecion principle 1.3 Exponenial Brownian moion 1.4 Exchange of measure (Girsanov heorem) 1.5

More information

4 Sequences of measurable functions

4 Sequences of measurable functions 4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences

More information

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite American Journal of Operaions Research, 08, 8, 8-9 hp://wwwscirporg/journal/ajor ISSN Online: 60-8849 ISSN Prin: 60-8830 The Opimal Sopping Time for Selling an Asse When I Is Uncerain Wheher he Price Process

More information

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance. 1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard

More information

Essential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems

Essential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems Essenial Microeconomics -- 6.5: OPIMAL CONROL Consider he following class of opimizaion problems Max{ U( k, x) + U+ ( k+ ) k+ k F( k, x)}. { x, k+ } = In he language of conrol heory, he vecor k is he vecor

More information

Uniqueness of solutions to quadratic BSDEs. BSDEs with convex generators and unbounded terminal conditions

Uniqueness of solutions to quadratic BSDEs. BSDEs with convex generators and unbounded terminal conditions Recalls and basic resuls on BSDEs Uniqueness resul Links wih PDEs On he uniqueness of soluions o quadraic BSDEs wih convex generaors and unbounded erminal condiions IRMAR, Universié Rennes 1 Châeau de

More information

Option pricing and implied volatilities in a 2-hypergeometric stochastic volatility model

Option pricing and implied volatilities in a 2-hypergeometric stochastic volatility model Opion pricing and implied volailiies in a 2-hypergeomeric sochasic volailiy model Nicolas Privaul Qihao She Division of Mahemaical Sciences School of Physical and Mahemaical Sciences Nanyang Technological

More information

Chapter 14 Wiener Processes and Itô s Lemma. Options, Futures, and Other Derivatives, 9th Edition, Copyright John C. Hull

Chapter 14 Wiener Processes and Itô s Lemma. Options, Futures, and Other Derivatives, 9th Edition, Copyright John C. Hull Chaper 14 Wiener Processes and Iô s Lemma Copyrigh John C. Hull 014 1 Sochasic Processes! Describes he way in which a variable such as a sock price, exchange rae or ineres rae changes hrough ime! Incorporaes

More information

A proof of Ito's formula using a di Title formula. Author(s) Fujita, Takahiko; Kawanishi, Yasuhi. Studia scientiarum mathematicarum H Citation

A proof of Ito's formula using a di Title formula. Author(s) Fujita, Takahiko; Kawanishi, Yasuhi. Studia scientiarum mathematicarum H Citation A proof of Io's formula using a di Tile formula Auhor(s) Fujia, Takahiko; Kawanishi, Yasuhi Sudia scieniarum mahemaicarum H Ciaion 15-134 Issue 8-3 Dae Type Journal Aricle Tex Version auhor URL hp://hdl.handle.ne/186/15878

More information

arxiv: v1 [math.pr] 19 Feb 2011

arxiv: v1 [math.pr] 19 Feb 2011 A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of

More information

arxiv: v1 [math.ca] 15 Nov 2016

arxiv: v1 [math.ca] 15 Nov 2016 arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy

More information

Generalized Snell envelope and BSDE With Two general Reflecting Barriers

Generalized Snell envelope and BSDE With Two general Reflecting Barriers 1/22 Generalized Snell envelope and BSDE Wih Two general Reflecing Barriers EL HASSAN ESSAKY Cadi ayyad Universiy Poly-disciplinary Faculy Safi Work in progress wih : M. Hassani and Y. Ouknine Iasi, July

More information

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

More information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL: Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS

More information

Example on p. 157

Example on p. 157 Example 2.5.3. Le where BV [, 1] = Example 2.5.3. on p. 157 { g : [, 1] C g() =, g() = g( + ) [, 1), var (g) = sup g( j+1 ) g( j ) he supremum is aken over all he pariions of [, 1] (1) : = < 1 < < n =

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

Algorithmic Trading: Optimal Control PIMS Summer School

Algorithmic Trading: Optimal Control PIMS Summer School Algorihmic Trading: Opimal Conrol PIMS Summer School Sebasian Jaimungal, U. Torono Álvaro Carea,U. Oxford many hanks o José Penalva,(U. Carlos III) Luhui Gan (U. Torono) Ryan Donnelly (Swiss Finance Insiue,

More information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

Existence and uniqueness of solution for multidimensional BSDE with local conditions on the coefficient

Existence and uniqueness of solution for multidimensional BSDE with local conditions on the coefficient 1/34 Exisence and uniqueness of soluion for mulidimensional BSDE wih local condiions on he coefficien EL HASSAN ESSAKY Cadi Ayyad Universiy Mulidisciplinary Faculy Safi, Morocco ITN Roscof, March 18-23,

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

arxiv: v1 [math.pr] 6 Oct 2008

arxiv: v1 [math.pr] 6 Oct 2008 MEASURIN THE NON-STOPPIN TIMENESS OF ENDS OF PREVISIBLE SETS arxiv:8.59v [mah.pr] 6 Oc 8 JU-YI YEN ),) AND MARC YOR 3),4) Absrac. In his paper, we propose several measuremens of he nonsopping imeness of

More information

LECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS

LECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS LECTURE : GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS We will work wih a coninuous ime reversible Markov chain X on a finie conneced sae space, wih generaor Lf(x = y q x,yf(y. (Recall ha q

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE Topics MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES 2-6 3. FUNCTION OF A RANDOM VARIABLE 3.2 PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE 3.3 EXPECTATION AND MOMENTS

More information

Local Strict Comparison Theorem and Converse Comparison Theorems for Reflected Backward Stochastic Differential Equations

Local Strict Comparison Theorem and Converse Comparison Theorems for Reflected Backward Stochastic Differential Equations arxiv:mah/07002v [mah.pr] 3 Dec 2006 Local Sric Comparison Theorem and Converse Comparison Theorems for Refleced Backward Sochasic Differenial Equaions Juan Li and Shanjian Tang Absrac A local sric comparison

More information

On Gronwall s Type Integral Inequalities with Singular Kernels

On Gronwall s Type Integral Inequalities with Singular Kernels Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies

More information

On R d -valued peacocks

On R d -valued peacocks On R d -valued peacocks Francis HIRSCH 1), Bernard ROYNETTE 2) July 26, 211 1) Laboraoire d Analyse e Probabiliés, Universié d Évry - Val d Essonne, Boulevard F. Mierrand, F-9125 Évry Cedex e-mail: francis.hirsch@univ-evry.fr

More information

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his

More information

14 Autoregressive Moving Average Models

14 Autoregressive Moving Average Models 14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class

More information

Dynamics of a stochastic predator-prey model with Beddington DeAngelis functional response

Dynamics of a stochastic predator-prey model with Beddington DeAngelis functional response SCIENTIA Series A: Mahemaical Sciences, Vol. 22 22, 75 84 Universidad Técnica Federico Sana María Valparaíso, Chile ISSN 76-8446 c Universidad Técnica Federico Sana María 22 Dynamics of a sochasic predaor-prey

More information

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial

More information

Unit Root Time Series. Univariate random walk

Unit Root Time Series. Univariate random walk Uni Roo ime Series Univariae random walk Consider he regression y y where ~ iid N 0, he leas squares esimae of is: ˆ yy y y yy Now wha if = If y y hen le y 0 =0 so ha y j j If ~ iid N 0, hen y ~ N 0, he

More information

Math 334 Fall 2011 Homework 11 Solutions

Math 334 Fall 2011 Homework 11 Solutions Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then

More information

CH Sean Han QF, NTHU, Taiwan BFS2010. (Joint work with T.-Y. Chen and W.-H. Liu)

CH Sean Han QF, NTHU, Taiwan BFS2010. (Joint work with T.-Y. Chen and W.-H. Liu) CH Sean Han QF, NTHU, Taiwan BFS2010 (Join work wih T.-Y. Chen and W.-H. Liu) Risk Managemen in Pracice: Value a Risk (VaR) / Condiional Value a Risk (CVaR) Volailiy Esimaion: Correced Fourier Transform

More information

DISCRETE GRONWALL LEMMA AND APPLICATIONS

DISCRETE GRONWALL LEMMA AND APPLICATIONS DISCRETE GRONWALL LEMMA AND APPLICATIONS JOHN M. HOLTE MAA NORTH CENTRAL SECTION MEETING AT UND 24 OCTOBER 29 Gronwall s lemma saes an inequaliy ha is useful in he heory of differenial equaions. Here is

More information

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,

More information

Stochastic Model for Cancer Cell Growth through Single Forward Mutation

Stochastic Model for Cancer Cell Growth through Single Forward Mutation Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com

More information

Backward stochastic dynamics on a filtered probability space

Backward stochastic dynamics on a filtered probability space Backward sochasic dynamics on a filered probabiliy space Gechun Liang Oxford-Man Insiue, Universiy of Oxford based on join work wih Terry Lyons and Zhongmin Qian Page 1 of 15 gliang@oxford-man.ox.ac.uk

More information

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions MA 14 Calculus IV (Spring 016) Secion Homework Assignmen 1 Soluions 1 Boyce and DiPrima, p 40, Problem 10 (c) Soluion: In sandard form he given firs-order linear ODE is: An inegraing facor is given by

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

Time discretization of quadratic and superquadratic Markovian BSDEs with unbounded terminal conditions

Time discretization of quadratic and superquadratic Markovian BSDEs with unbounded terminal conditions Time discreizaion of quadraic and superquadraic Markovian BSDEs wih unbounded erminal condiions Adrien Richou Universié Bordeaux 1, INRIA équipe ALEA Oxford framework Le (Ω, F, P) be a probabiliy space,

More information

On Oscillation of a Generalized Logistic Equation with Several Delays

On Oscillation of a Generalized Logistic Equation with Several Delays Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid

More information

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004 ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS TO THE BACKWARD STOCHASTIC LORENZ SYSTEM

EXISTENCE AND UNIQUENESS OF SOLUTIONS TO THE BACKWARD STOCHASTIC LORENZ SYSTEM Communicaions on Sochasic Analysis Vol. 1, No. 3 (27) 473-483 EXISTENCE AND UNIQUENESS OF SOLUTIONS TO THE BACKWARD STOCHASTIC LORENZ SYSTEM P. SUNDAR AND HONG YIN Absrac. The backward sochasic Lorenz

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

Couplage du principe des grandes déviations et de l homogénisation dans le cas des EDP paraboliques: (le cas constant)

Couplage du principe des grandes déviations et de l homogénisation dans le cas des EDP paraboliques: (le cas constant) Couplage du principe des grandes déviaions e de l homogénisaion dans le cas des EDP paraboliques: (le cas consan) Alioune COULIBALY U.F.R Sciences e Technologie Universié Assane SECK de Ziguinchor Probabilié

More information

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS Elecronic Journal of Differenial Equaions, Vol. 217 217, No. 118, pp. 1 14. ISSN: 172-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS

More information

arxiv: v1 [math.pr] 2 Oct 2017

arxiv: v1 [math.pr] 2 Oct 2017 An Exension of Clark-Haussman Formula and Applicaions arxiv:171.939v1 [mah.pr] 2 Oc 217 Traian A. Pirvu 1 and Ulrich G. Haussmann 2 1 Deparmen of Mahemaics and Saisics, McMaser Universiy 128 Main Sree

More information

Quasi-sure Stochastic Analysis through Aggregation

Quasi-sure Stochastic Analysis through Aggregation E l e c r o n i c J o u r n a l o f P r o b a b i l i y Vol. 16 (211), Paper no. 67, pages 1844 1879. Journal URL hp://www.mah.washingon.edu/~ejpecp/ Quasi-sure Sochasic Analysis hrough Aggregaion H. Mee

More information

Notes for Lecture 17-18

Notes for Lecture 17-18 U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up

More information

The Strong Law of Large Numbers

The Strong Law of Large Numbers Lecure 9 The Srong Law of Large Numbers Reading: Grimme-Sirzaker 7.2; David Williams Probabiliy wih Maringales 7.2 Furher reading: Grimme-Sirzaker 7.1, 7.3-7.5 Wih he Convergence Theorem (Theorem 54) and

More information

Representation of Stochastic Process by Means of Stochastic Integrals

Representation of Stochastic Process by Means of Stochastic Integrals Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of

More information

Optimal Investment under Dynamic Risk Constraints and Partial Information

Optimal Investment under Dynamic Risk Constraints and Partial Information Opimal Invesmen under Dynamic Risk Consrains and Parial Informaion Wolfgang Puschögl Johann Radon Insiue for Compuaional and Applied Mahemaics (RICAM) Ausrian Academy of Sciences www.ricam.oeaw.ac.a 2

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,

More information

13.3 Term structure models

13.3 Term structure models 13.3 Term srucure models 13.3.1 Expecaions hypohesis model - Simples "model" a) shor rae b) expecaions o ge oher prices Resul: y () = 1 h +1 δ = φ( δ)+ε +1 f () = E (y +1) (1) =δ + φ( δ) f (3) = E (y +)

More information

EMS SCM joint meeting. On stochastic partial differential equations of parabolic type

EMS SCM joint meeting. On stochastic partial differential equations of parabolic type EMS SCM join meeing Barcelona, May 28-30, 2015 On sochasic parial differenial equaions of parabolic ype Isván Gyöngy School of Mahemaics and Maxwell Insiue Edinburgh Universiy 1 I. Filering problem II.

More information

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

On the Timing Option in a Futures Contract

On the Timing Option in a Futures Contract On he Timing Opion in a Fuures Conrac Francesca Biagini, Mahemaics Insiue Universiy of Munich Theresiensr. 39 D-80333 Munich, Germany phone: +39-051-2094459 Francesca.Biagini@mahemaik.uni-muenchen.de Tomas

More information

The expectation value of the field operator.

The expectation value of the field operator. The expecaion value of he field operaor. Dan Solomon Universiy of Illinois Chicago, IL dsolom@uic.edu June, 04 Absrac. Much of he mahemaical developmen of quanum field heory has been in suppor of deermining

More information

Differential Equations

Differential Equations Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Y 0.4Y 0.45Y Y to a proper ARMA specification. HG Jan 04 ECON 50 Exercises II - 0 Feb 04 (wih answers Exercise. Read secion 8 in lecure noes 3 (LN3 on he common facor problem in ARMA-processes. Consider he following process Y 0.4Y 0.45Y 0.5 ( where

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Lecture 2 April 04, 2018

Lecture 2 April 04, 2018 Sas 300C: Theory of Saisics Spring 208 Lecure 2 April 04, 208 Prof. Emmanuel Candes Scribe: Paulo Orensein; edied by Sephen Baes, XY Han Ouline Agenda: Global esing. Needle in a Haysack Problem 2. Threshold

More information

Martingales versus PDEs in Finance: An Equivalence Result with Examples

Martingales versus PDEs in Finance: An Equivalence Result with Examples Maringales versus PDEs in Finance: An Equivalence Resul wih Examples David Heah Universiy of Technology, Sydney PO Box 23 Broadway, NSW 2007 Ausralia and Marin Schweizer Technische Universiä Berlin Fachbereich

More information

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018 MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren

More information

Explicit construction of a dynamic Bessel bridge of dimension 3

Explicit construction of a dynamic Bessel bridge of dimension 3 Explici consrucion of a dynamic Bessel bridge of dimension 3 Luciano Campi Umu Çein Albina Danilova February 25, 23 Absrac Given a deerminisically ime-changed Brownian moion Z saring from, whose imechange

More information

Existence of multiple positive periodic solutions for functional differential equations

Existence of multiple positive periodic solutions for functional differential equations J. Mah. Anal. Appl. 325 (27) 1378 1389 www.elsevier.com/locae/jmaa Exisence of muliple posiive periodic soluions for funcional differenial equaions Zhijun Zeng a,b,,libi a, Meng Fan a a School of Mahemaics

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

Undetermined coefficients for local fractional differential equations

Undetermined coefficients for local fractional differential equations Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani

More information

12: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME. Σ j =

12: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME. Σ j = 1: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME Moving Averages Recall ha a whie noise process is a series { } = having variance σ. The whie noise process has specral densiy f (λ) = of

More information

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures.

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures. HOMEWORK # 2: MATH 2, SPRING 25 TJ HITCHMAN Noe: This is he las soluion se where I will describe he MATLAB I used o make my picures.. Exercises from he ex.. Chaper 2.. Problem 6. We are o show ha y() =

More information

Most Probable Phase Portraits of Stochastic Differential Equations and Its Numerical Simulation

Most Probable Phase Portraits of Stochastic Differential Equations and Its Numerical Simulation Mos Probable Phase Porrais of Sochasic Differenial Equaions and Is Numerical Simulaion Bing Yang, Zhu Zeng and Ling Wang 3 School of Mahemaics and Saisics, Huazhong Universiy of Science and Technology,

More information

Optimal Investment, Consumption and Retirement Decision with Disutility and Borrowing Constraints

Optimal Investment, Consumption and Retirement Decision with Disutility and Borrowing Constraints Opimal Invesmen, Consumpion and Reiremen Decision wih Disuiliy and Borrowing Consrains Yong Hyun Shin Join Work wih Byung Hwa Lim(KAIST) June 29 July 3, 29 Yong Hyun Shin (KIAS) Workshop on Sochasic Analysis

More information

Simulation of BSDEs and. Wiener Chaos Expansions

Simulation of BSDEs and. Wiener Chaos Expansions Simulaion of BSDEs and Wiener Chaos Expansions Philippe Briand Céline Labar LAMA UMR 5127, Universié de Savoie, France hp://www.lama.univ-savoie.fr/ Workshop on BSDEs Rennes, May 22-24, 213 Inroducion

More information

Introduction to SLE Lecture Notes

Introduction to SLE Lecture Notes Inroducion o SLE Lecure Noe May 13, 16 - The goal of hi ecion i o find a ufficien condiion of λ for he hull K o be generaed by a imple cure. I urn ou if λ 1 < 4 hen K i generaed by a imple curve. We will

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar

More information

Fractional Method of Characteristics for Fractional Partial Differential Equations

Fractional Method of Characteristics for Fractional Partial Differential Equations Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics

More information

Heat kernel and Harnack inequality on Riemannian manifolds

Heat kernel and Harnack inequality on Riemannian manifolds Hea kernel and Harnack inequaliy on Riemannian manifolds Alexander Grigor yan UHK 11/02/2014 onens 1 Laplace operaor and hea kernel 1 2 Uniform Faber-Krahn inequaliy 3 3 Gaussian upper bounds 4 4 ean-value

More information

Hamilton Jacobi equations

Hamilton Jacobi equations Hamilon Jacobi equaions Inoducion o PDE The rigorous suff from Evans, mosly. We discuss firs u + H( u = 0, (1 where H(p is convex, and superlinear a infiniy, H(p lim p p = + This by comes by inegraion

More information

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning

More information

A FAMILY OF MARTINGALES GENERATED BY A PROCESS WITH INDEPENDENT INCREMENTS

A FAMILY OF MARTINGALES GENERATED BY A PROCESS WITH INDEPENDENT INCREMENTS Theory of Sochasic Processes Vol. 14 3), no. 2, 28, pp. 139 144 UDC 519.21 JOSEP LLUÍS SOLÉ AND FREDERIC UTZET A FAMILY OF MARTINGALES GENERATED BY A PROCESS WITH INDEPENDENT INCREMENTS An explici procedure

More information

Homogenization of random Hamilton Jacobi Bellman Equations

Homogenization of random Hamilton Jacobi Bellman Equations Probabiliy, Geomery and Inegrable Sysems MSRI Publicaions Volume 55, 28 Homogenizaion of random Hamilon Jacobi Bellman Equaions S. R. SRINIVASA VARADHAN ABSTRACT. We consider nonlinear parabolic equaions

More information

SOLUTIONS TO ASSIGNMENT 2 - MATH 355. with c > 3. m(n c ) < δ. f(t) t. g(x)dx =

SOLUTIONS TO ASSIGNMENT 2 - MATH 355. with c > 3. m(n c ) < δ. f(t) t. g(x)dx = SOLUTIONS TO ASSIGNMENT 2 - MATH 355 Problem. ecall ha, B n {ω [, ] : S n (ω) > nɛ n }, and S n (ω) N {ω [, ] : lim }, n n m(b n ) 3 n 2 ɛ 4. We wan o show ha m(n c ). Le δ >. We can pick ɛ 4 n c n wih

More information