Rough Paths and its Applications in Machine Learning
|
|
- Brandon Arthur Morris
- 5 years ago
- Views:
Transcription
1 Pah ignaure Machine learning applicaion Rough Pah and i Applicaion in Machine Learning July 20, 2017 Rough Pah and i Applicaion in Machine Learning
2 Pah ignaure Machine learning applicaion Hiory and moivaion Terry Lyon (1998), Differenial equaion driven by rough ignal, Rev. Ma. Iberoamericana 14. Originally formulaed o udy ochaic differenial equaion in a pah-wie manner. Rough pah heory heory of regulariy rucure Soluion o KPZ equaion (Marin Hairer, Field medal 2014). Now begin applied o oher hard problem in aiical phyic. Recenly, rough pah heory i finding applicaion in machine learning. Rough Pah and i Applicaion in Machine Learning
3 Pah ignaure Machine learning applicaion Conrolled differenial equaion Conider he following differenial equaion: y = V (y ) x Fir-order approximaion o he oluion: For, [0, T ], y y = V (y ) V (y r ) x r dr x r dr = V (y ) (x x ) Rough Pah and i Applicaion in Machine Learning
4 Pah ignaure Machine learning applicaion Second-order approximaion y y = V (y r1 ) x r 1 dr 1 ( r1 V (y ) + ) = V (y r2 ) y r 2 dr 2 x r 1 dr 1 [ ] = V (y ) x r 1 dr 1 + ( r1 ) V (y r2 )V (y r2 ) x r 2 dr 2 x r 1 dr 1 [ ] V (y ) dx r1 [ + V (y )V (y ) ( r1 ) ] dx r2 dx r1 Rough Pah and i Applicaion in Machine Learning
5 Pah ignaure Machine learning applicaion Separaing ignal from vecor field In one dimenion: In d dimenion: y y V (y ) [x x ] + V (y )V (y ) [ ] 1 2 (x x ) 2 y y V (y ) [x x ] d ( + V (y )V (y ) r1 i,j=1 ) dx r (i) 2 dx r (j) 1 e i e j Rough Pah and i Applicaion in Machine Learning
6 Pah ignaure Machine learning applicaion 2-dimenional cae ( Given y = ( ) y (1) y (2) ) = [ V (1) 1 (y ) V (1) V (2) 1 (y ) V (2) 2 (y ) ] ) 2 (y ) (x (1) ( ), x (2) we have y y [ V (1) 1 (y ) V (1) 2 (y ) V (2) 1 (y ) V (2) 2 (y ) + V (y )V (y ) ] [ ([ ] x (1) x (1) x (2) x (2) r1 dx (1) r 2 dx r (1) 1 r1 dx (2) r 2 dx r (1) 1 r1 dx (1) r 2 dx r (2) 1 r1 dx (2) r 2 dx r (2) 1 ]). Rough Pah and i Applicaion in Machine Learning
7 Pah ignaure Machine learning applicaion 2-dimenional cae con. where [ r1 dx (1) r 2 dx r (1) 1 r1 dx (2) r 2 dx r (1) 1 x (k), r1 dx (1) r 2 dx r (2) 1 r1 dx (2) r 2 dx r (2) 1 ( = 1 2 and he Lévy-area i given by A = r1 x (1), x (2), x (1), ] ) 2 x (1), x (2), ) 2 x (2), ( } {{ } ymmeric par := x (k) x (k), k = 1, 2, dx r (1) 2 dx r (2) 1 r1 + 1 [ ] 0 A 2 A 0 }{{} ani ymmeric par dx (2) r 2 dx (1) r 1. Rough Pah and i Applicaion in Machine Learning
8 Pah ignaure Machine learning applicaion Green heorem A = 1 x (2) dx (1) + x (1) dx (2) 2 C Rough Pah and i Applicaion in Machine Learning
9 Pah ignaure Machine learning applicaion Signaure of a pah For all 0 T, S n (x), := ( 1, x,, x 2,,..., x n ), R R d ( R d R d) ( R d) n, where x k, i he convenional k-h ieraed inegral of he pah x over he inerval [, ]: d ( x k, = j 1,...,j k =1 <r 1< <r k < dx (j1) r 1 dx (j k ) r k ) e j1 e jk. Rough Pah and i Applicaion in Machine Learning
10 Pah ignaure Machine learning applicaion Chen Ideniy The ignaure i an elemen of a Lie group called he ep-n nilpoen group wih d generaor. I aifie S n (x), = S n (x),u S n (x) u,, u, [0, T ], u, where given a = ( 1, a 1,..., a n), b = ( 1, b 1,..., b n), group muliplicaion i performed by a b := ( 1, c 1,..., c n), c k = k a i b k i, 1 k n. E.g. (1, a 1, a 2 ) (1, b 1, b 2 ) = (1, a 1 + b 1, a 2 + b 2 + a 1 b 1 ). i=0 Rough Pah and i Applicaion in Machine Learning
11 Pah ignaure Machine learning applicaion Fracional Brownian moion: W H (i) Hur parameer: H (0, 1) (ii) Coninuou pah, no differeniable a.e. (iii) W W N (0, 2H ) (iv) Covariance funcion: R(, ) = 1 2 ( 2H + 2H 2H) (v) H = 1 2 : Sandard Brownian moion, R(, ) =. (vi) H > 1 2 : Incremen along dijoin inerval are poiively correlaed. (vii) H < 1 2 : Incremen along dijoin inerval are negaively correlaed. (viii) Neiher a Markov proce nor a maringale (unle H = 1 2 ) Rough Pah and i Applicaion in Machine Learning
12 Pah ignaure Machine learning applicaion Sample pah Rough Pah and i Applicaion in Machine Learning
13 Pah ignaure Machine learning applicaion Hölder coninuiy and rough pah Definiion A funcion f i aid o be α-hölder coninuou on an inerval [0, T ] if f () f () C α,, [0, T ]. Hölder coninuiy meaure how rough a funcion i. Fac: Fracional Brownian moion wih Hur parameer H i almo urely (H ε)-hölder coninuou for any ε > 0. Definiion Given 1 3 < α 1 2, X = ( 1, X,, X 2,) i an α-hölder rough pah if i aifie Chen ideniy, X i α-hölder coninuou and X 2 i 2α-Hölder coninuou. Rough Pah and i Applicaion in Machine Learning
14 Pah ignaure Machine learning applicaion Ió inegraion a rough pah inegraion T 0 Y dw = lim π 0 i Y i W i, i+1, where he limi i aken in L 2 (Ω) and no almo urely pah-wie becaue he pah are no regular enough. Even o, convergence in L 2 (Ω) relie on he fac W i a maringale, and ha Y i adaped o he filraion of W. Define W, Io := ( ( 1, A 1,, A 2 ) ), = 1, W,, W,r1 dw r1 Then given a Gubinelli derivaive Y, T 0 almo urely. Y dw = T 0 Y dw Io = lim π 0 Y i A 1 i, i+1 + Y A 2 i, i+1 Rough Pah and i Applicaion in Machine Learning
15 Pah ignaure Machine learning applicaion Properie of he ignaure The ignaure ha more or le a one-o-one relaion wih i pah (ee T. Lyon and B. Hambly, Uniquene for he ignaure of a pah of bounded variaion and he reduced pah group, 2010). I i a graded ummary of he daa ream encoded in he pah. Ieraed inegral capure non-linear apec of he pah. Form a naural bai for funcional on daa ream. I provide a rich e of feaure ha can be ued in a machine learning pipeline. Rough Pah and i Applicaion in Machine Learning
16 Pah ignaure Machine learning applicaion Applicaion Finance: J. Field, L. Gyurkó, M. Konkowki and T. Lyon (2014), Exracing informaion from he ignaure of a financial daa ream, arxiv: v2. Sound compreion: T. Lyon and N. Sidorova (2005), Sound compreion: a rough pah approach, In Proceeding of he 4h inernaional ympoium on Informaion and communicaion. Idenifying paern in MEG can ec. I. Chevyrev and A. Kormilizin (2016), A Primer on he Signaure Mehod in Machine Learning, arxiv: v1. Rough Pah and i Applicaion in Machine Learning
17 Pah ignaure Machine learning applicaion Chinee handwriing recogniion SCUT gpen: Online Chinee handwriing recogniion ofware Began a a collaboraion beween Terry Lyon and Ben Graham (Univeriy of Warwick) App developed by HCII-Lab in Souh China Univeriy of Technology Sae of he ar: Won fir place in ICDAR2013 compeiion wih an error rae of 2.61% (Second place: 3.13%, Human error: 4.81%). Combine rough pah heory and a deep convoluional neural nework. Ue fir 3 level of he ignaure of he pah. Ben Graham (2013), Spare array of ignaure for online characer recogniion, arxiv: v2. Rough Pah and i Applicaion in Machine Learning
18 Pah ignaure Machine learning applicaion Concluion and rambling Texbook: Peer Friz and Marin Hairer (2014), A Coure on Rough Pah, Springer. Terry Lyon, M. Caruana, and T. Lévy (2007), Differenial equaion driven by Rough Pah, Springer. Fuure direcion: Applicaion o ochaic conrol and reinforcemen learning: (i) Exend conrol heory o dynamical yem perurbed by coloured noie. (ii) Find efficien Mone-Carlo cheme o compue opimal pah and conrol rajecorie. Rough Pah and i Applicaion in Machine Learning
Fractional Ornstein-Uhlenbeck Bridge
WDS'1 Proceeding of Conribued Paper, Par I, 21 26, 21. ISBN 978-8-7378-139-2 MATFYZPRESS Fracional Ornein-Uhlenbeck Bridge J. Janák Charle Univeriy, Faculy of Mahemaic and Phyic, Prague, Czech Republic.
More information6. 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 informationOn 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 informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual
More informationExplicit form of global solution to stochastic logistic differential equation and related topics
SAISICS, OPIMIZAION AND INFOMAION COMPUING Sa., Opim. Inf. Compu., Vol. 5, March 17, pp 58 64. Publihed online in Inernaional Academic Pre (www.iapre.org) Explici form of global oluion o ochaic logiic
More informationESTIMATES FOR THE DERIVATIVE OF DIFFUSION SEMIGROUPS
Elec. Comm. in Probab. 3 (998) 65 74 ELECTRONIC COMMUNICATIONS in PROBABILITY ESTIMATES FOR THE DERIVATIVE OF DIFFUSION SEMIGROUPS L.A. RINCON Deparmen of Mahemaic Univeriy of Wale Swanea Singleon Par
More informationarxiv: 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 informationChapter 6. Laplace Transforms
Chaper 6. Laplace Tranform Kreyzig by YHLee;45; 6- An ODE i reduced o an algebraic problem by operaional calculu. The equaion i olved by algebraic manipulaion. The reul i ranformed back for he oluion of
More informationA 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, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max
ecure 8 7. Sabiliy Analyi For an n dimenional vecor R n, he and he vecor norm are defined a: = T = i n i (7.) I i eay o how ha hee wo norm aify he following relaion: n (7.) If a vecor i ime-dependen, hen
More informationAn 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 informationFractional 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 informationBackward 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 informationExample 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 information6.8 Laplace Transform: General Formulas
48 HAP. 6 Laplace Tranform 6.8 Laplace Tranform: General Formula Formula Name, ommen Sec. F() l{ f ()} e f () d f () l {F()} Definiion of Tranform Invere Tranform 6. l{af () bg()} al{f ()} bl{g()} Lineariy
More informationChapter 6. Laplace Transforms
6- Chaper 6. Laplace Tranform 6.4 Shor Impule. Dirac Dela Funcion. Parial Fracion 6.5 Convoluion. Inegral Equaion 6.6 Differeniaion and Inegraion of Tranform 6.7 Syem of ODE 6.4 Shor Impule. Dirac Dela
More information18.03SC Unit 3 Practice Exam and Solutions
Sudy Guide on Sep, Dela, Convoluion, Laplace You can hink of he ep funcion u() a any nice mooh funcion which i for < a and for > a, where a i a poiive number which i much maller han any ime cale we care
More informationMathematische Annalen
Mah. Ann. 39, 33 339 (997) Mahemaiche Annalen c Springer-Verlag 997 Inegraion by par in loop pace Elon P. Hu Deparmen of Mahemaic, Norhweern Univeriy, Evanon, IL 628, USA (e-mail: elon@@mah.nwu.edu) Received:
More informationLecture 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 informationCash 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 informationarxiv: v1 [math.pr] 11 Jun 2013
On Iô differenial equaion in rough pah heory Terry J Lyons Danyu Yang arxiv:1362589v1 [mahpr] 11 Jun 213 June 12, 213 Absrac The Iô soluion can be recovered pahwisely by concaenaing a mean of Sraonovich
More informationAMartingaleApproachforFractionalBrownian Motions and Related Path Dependent PDEs
AMaringaleApproachforFracionalBrownian Moions and Relaed Pah Dependen PDEs Jianfeng ZHANG Universiy of Souhern California Join work wih Frederi VIENS Mahemaical Finance, Probabiliy, and PDE Conference
More informationHamilton- 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 informationu(t) Figure 1. Open loop control system
Open loop conrol v cloed loop feedbac conrol The nex wo figure preen he rucure of open loop and feedbac conrol yem Figure how an open loop conrol yem whoe funcion i o caue he oupu y o follow he reference
More informationSome estimates for the parabolic Anderson model
Some esimaes for he parabolic Anderson model Samy Tindel Purdue Universiy Probabiliy Seminar - Urbana Champaign 2015 Collaboraors: Xia Chen, Yaozhong Hu, Jingyu Huang, Khoa Lê, David Nualar Samy T. (Purdue)
More informationSimulation 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 informationDifferential 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 informationChapter 7: Inverse-Response Systems
Chaper 7: Invere-Repone Syem Normal Syem Invere-Repone Syem Baic Sar ou in he wrong direcion End up in he original eady-ae gain value Two or more yem wih differen magniude and cale in parallel Main yem
More information4.2 The Fourier Transform
4.2. THE FOURIER TRANSFORM 57 4.2 The Fourier Transform 4.2.1 Inroducion One way o look a Fourier series is ha i is a ransformaion from he ime domain o he frequency domain. Given a signal f (), finding
More informationElements of Stochastic Processes Lecture II Hamid R. Rabiee
Sochasic Processes Elemens of Sochasic Processes Lecure II Hamid R. Rabiee Overview Reading Assignmen Chaper 9 of exbook Furher Resources MIT Open Course Ware S. Karlin and H. M. Taylor, A Firs Course
More informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
More informationLet. x y. denote a bivariate time series with zero mean.
Linear Filer Le x y : T denoe a bivariae ime erie wih zero mean. Suppoe ha he ime erie {y : T} i conruced a follow: y a x The ime erie {y : T} i aid o be conruced from {x : T} by mean of a Linear Filer.
More informationAn introduction to the (local) martingale problem
An inroducion o he (local) maringale problem Chri Janjigian Ocober 14, 214 Abrac Thee are my preenaion noe for a alk in he Univeriy of Wiconin - Madion graduae probabiliy eminar. Thee noe are primarily
More informationInstrumentation & Process Control
Chemical Engineering (GTE & PSU) Poal Correpondence GTE & Public Secor Inrumenaion & Proce Conrol To Buy Poal Correpondence Package call a -999657855 Poal Coure ( GTE & PSU) 5 ENGINEERS INSTITUTE OF INDI.
More informationCouplage 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 informationLaplace Transform. Inverse Laplace Transform. e st f(t)dt. (2)
Laplace Tranform Maoud Malek The Laplace ranform i an inegral ranform named in honor of mahemaician and aronomer Pierre-Simon Laplace, who ued he ranform in hi work on probabiliy heory. I i a powerful
More informationf(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 informationLoss of martingality in asset price models with lognormal stochastic volatility
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
More information1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.
. Use Simpson s rule wih n 4 o esimae an () +. Soluion: Since we are using 4 seps, 4 Thus we have [ ( ) f() + 4f + f() + 4f 3 [ + 4 4 6 5 + + 4 4 3 + ] 5 [ + 6 6 5 + + 6 3 + ]. 5. Our funcion is f() +.
More informationAdditional Methods for Solving DSGE Models
Addiional Mehod for Solving DSGE Model Karel Meren, Cornell Univeriy Reference King, R. G., Ploer, C. I. & Rebelo, S. T. (1988), Producion, growh and buine cycle: I. he baic neoclaical model, Journal of
More informationUndetermined 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 informationMath 2214 Solution Test 1 B Spring 2016
Mah 14 Soluion Te 1 B Spring 016 Problem 1: Ue eparaion of ariable o ole he Iniial alue DE Soluion (14p) e =, (0) = 0 d = e e d e d = o = ln e d uing u-du b leing u = e 1 e = + where C = for he iniial
More informationU T,0. t = X t t T X T. (1)
Gauian bridge Dario Gabarra 1, ommi Soinen 2, and Eko Valkeila 3 1 Deparmen of Mahemaic and Saiic, PO Box 68, 14 Univeriy of Helinki,Finland dariogabarra@rnihelinkifi 2 Deparmen of Mahemaic and Saiic,
More informationOn Delayed Logistic Equation Driven by Fractional Brownian Motion
On Delayed Logiic Equaion Driven by Fracional Brownian Moion Nguyen Tien Dung Deparmen of Mahemaic, FPT Univeriy No 8 Ton Tha Thuye, Cau Giay, Hanoi, 84 Vienam Email: dungn@fp.edu.vn ABSTRACT In hi paper
More informationMon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5
Mah 225-4 Week 2 April 2-6 coninue.-.3; alo cover par of.4-.5, EP 7.6 Mon Apr 2:.-.3 Laplace ranform and iniial value problem like we udied in Chaper 5 Announcemen: Warm-up Exercie: Recall, The Laplace
More informationChapter 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 informationParameter Estimation for Fractional Ornstein-Uhlenbeck Processes: Non-Ergodic Case
Parameer Eimaion for Fracional Ornein-Uhlenbeck Procee: Non-Ergodic Cae R. Belfadli 1, K. E-Sebaiy and Y. Ouknine 3 1 Polydiciplinary Faculy of Taroudan, Univeriy Ibn Zohr, Taroudan, Morocco. Iniu de Mahémaique
More informationInstitute for Mathematical Methods in Economics. University of Technology Vienna. Singapore, May Manfred Deistler
MULTIVARIATE TIME SERIES ANALYSIS AND FORECASTING Manfred Deisler E O S Economerics and Sysems Theory Insiue for Mahemaical Mehods in Economics Universiy of Technology Vienna Singapore, May 2004 Inroducion
More informationON FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES
Communicaion on Sochaic Analyi Vol. 5, No. 1 211 121-133 Serial Publicaion www.erialpublicaion.com ON FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES TERHI KAARAKKA AND PAAVO SALMINEN Abrac. In hi paper we udy
More informationSimulation 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/ Sochasic Analysis Seminar Oxford, June 1, 213 Inroducion
More informationClass Meeting # 10: Introduction to the Wave Equation
MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion
More informationMATH 128A, SUMMER 2009, FINAL EXAM SOLUTION
MATH 28A, SUMME 2009, FINAL EXAM SOLUTION BENJAMIN JOHNSON () (8 poins) [Lagrange Inerpolaion] (a) (4 poins) Le f be a funcion defined a some real numbers x 0,..., x n. Give a defining equaion for he Lagrange
More informationAn introduction to the theory of SDDP algorithm
An inroducion o he heory of SDDP algorihm V. Leclère (ENPC) Augus 1, 2014 V. Leclère Inroducion o SDDP Augus 1, 2014 1 / 21 Inroducion Large scale sochasic problem are hard o solve. Two ways of aacking
More informationCHAPTER. Forced Equations and Systems { } ( ) ( ) 8.1 The Laplace Transform and Its Inverse. Transforms from the Definition.
CHAPTER 8 Forced Equaion and Syem 8 The aplace Tranform and I Invere Tranform from he Definiion 5 5 = b b {} 5 = 5e d = lim5 e = ( ) b {} = e d = lim e + e d b = (inegraion by par) = = = = b b ( ) ( )
More informationInterpolation and Pulse Shaping
EE345S Real-Time Digial Signal Proceing Lab Spring 2006 Inerpolaion and Pule Shaping Prof. Brian L. Evan Dep. of Elecrical and Compuer Engineering The Univeriy of Texa a Auin Lecure 7 Dicree-o-Coninuou
More informationOptimal Investment Strategy Insurance Company
Opimal Invesmen Sraegy for a Non-Life Insurance Company Łukasz Delong Warsaw School of Economics Insiue of Economerics Division of Probabilisic Mehods Probabiliy space Ω I P F I I I he filraion saisfies
More informationThe 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 informationSemilinear Kolmogorov equations and applications to stochastic optimal control
Semilinear Kolmogorov equaions and applicaions o sochasic opimal conrol Federica Masiero 1 Advisor: Prof. Marco Fuhrman 2 1 Diparimeno di Maemaica, Universià degli sudi di Milano, Via Saldini 5, 2133 Milano,
More informationUtility 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 informationdt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.
Mah Rahman Exam Review Soluions () Consider he IVP: ( 4)y 3y + 4y = ; y(3) = 0, y (3) =. (a) Please deermine he longes inerval for which he IVP is guaraneed o have a unique soluion. Soluion: The disconinuiies
More informationAlgorithmic 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 informationChapter 1 Fundamental Concepts
Chaper 1 Fundamenal Conceps 1 Signals A signal is a paern of variaion of a physical quaniy, ofen as a funcion of ime (bu also space, disance, posiion, ec). These quaniies are usually he independen variables
More informationarxiv: v1 [math.pr] 28 Nov 2016
Backward Sochasic Differenial Equaions wih Nonmarkovian Singular Terminal Values Ali Devin Sezer, Thomas Kruse, Alexandre Popier Ocober 15, 2018 arxiv:1611.09022v1 mah.pr 28 Nov 2016 Absrac We solve a
More informationA Risk-Averse Insider and Asset Pricing in Continuous Time
Managemen Science and Financial Engineering Vol 9, No, May 3, pp-6 ISSN 87-43 EISSN 87-36 hp://dxdoiorg/7737/msfe39 3 KORMS A Rik-Avere Inider and Ae Pricing in oninuou Time Byung Hwa Lim Graduae School
More informationES.1803 Topic 22 Notes Jeremy Orloff
ES.83 Topic Noes Jeremy Orloff Fourier series inroducion: coninued. Goals. Be able o compue he Fourier coefficiens of even or odd periodic funcion using he simplified formulas.. Be able o wrie and graph
More informationOptimal 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 informationStability in Distribution for Backward Uncertain Differential Equation
Sabiliy in Diribuion for Backward Uncerain Differenial Equaion Yuhong Sheng 1, Dan A. Ralecu 2 1. College of Mahemaical and Syem Science, Xinjiang Univeriy, Urumqi 8346, China heng-yh12@mail.inghua.edu.cn
More informationOn Solving the Perturbed Multi- Revolution Lambert Problem: Applications in Enhanced SSA
On Solving he Perurbed Muli- Revoluion Lamber Problem: Applicaions in Enhanced SSA John L. Junkins and Robyn M. Woollands Texas A&M Universiy Presened o Sacie Williams (AFOSR/RT) AFOSR REMOTE SENSING PORTFOLIO
More informationFractional Brownian Bridge Measures and Their Integration by Parts Formula
Journal of Mahemaical Reearch wih Applicaion Jul., 218, Vol. 38, No. 4, pp. 418 426 DOI:1.377/j.in:295-2651.218.4.9 Hp://jmre.lu.eu.cn Fracional Brownian Brige Meaure an Their Inegraion by Par Formula
More informationarxiv: 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 informationMarkov Processes and Stochastic Calculus
Markov Processes and Sochasic Calculus René Caldeney In his noes we revise he basic noions of Brownian moions, coninuous ime Markov processes and sochasic differenial equaions in he Iô sense. 1 Inroducion
More informationReminder: Flow Networks
0/0/204 Ma/CS 6a Cla 4: Variou (Flow) Execie Reminder: Flow Nework A flow nework i a digraph G = V, E, ogeher wih a ource verex V, a ink verex V, and a capaciy funcion c: E N. Capaciy Source 7 a b c d
More information23.5. 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 information4 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 informationA Theoretical Model of a Voltage Controlled Oscillator
A Theoreical Model of a Volage Conrolled Ocillaor Yenming Chen Advior: Dr. Rober Scholz Communicaion Science Iniue Univeriy of Souhern California UWB Workhop, April 11-1, 6 Inroducion Moivaion The volage
More informationENGI 9420 Engineering Analysis Assignment 2 Solutions
ENGI 940 Engineering Analysis Assignmen Soluions 0 Fall [Second order ODEs, Laplace ransforms; Secions.0-.09]. Use Laplace ransforms o solve he iniial value problem [0] dy y, y( 0) 4 d + [This was Quesion
More informationRepresenting a Signal. Continuous-Time Fourier Methods. Linearity and Superposition. Real and Complex Sinusoids. Jean Baptiste Joseph Fourier
Represening a Signal Coninuous-ime ourier Mehods he convoluion mehod for finding he response of a sysem o an exciaion aes advanage of he lineariy and imeinvariance of he sysem and represens he exciaion
More informationMATH 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 informationResearch Article Existence and Uniqueness of Solutions for a Class of Nonlinear Stochastic Differential Equations
Hindawi Publihing Corporaion Abrac and Applied Analyi Volume 03, Aricle ID 56809, 7 page hp://dx.doi.org/0.55/03/56809 Reearch Aricle Exience and Uniquene of Soluion for a Cla of Nonlinear Sochaic Differenial
More informationMATH 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 informationCONTROL SYSTEMS. Chapter 3 Mathematical Modelling of Physical Systems-Laplace Transforms. Prof.Dr. Fatih Mehmet Botsalı
CONTROL SYSTEMS Chaper Mahemaical Modelling of Phyical Syem-Laplace Tranform Prof.Dr. Faih Mehme Boalı Definiion Tranform -- a mahemaical converion from one way of hinking o anoher o make a problem eaier
More informationEE650R: Reliability Physics of Nanoelectronic Devices Lecture 9:
EE65R: Reliabiliy Physics of anoelecronic Devices Lecure 9: Feaures of Time-Dependen BTI Degradaion Dae: Sep. 9, 6 Classnoe Lufe Siddique Review Animesh Daa 9. Background/Review: BTI is observed when he
More informationf t te e = possesses a Laplace transform. Exercises for Module-III (Transform Calculus)
Exercises for Module-III (Transform Calculus) ) Discuss he piecewise coninuiy of he following funcions: =,, +, > c) e,, = d) sin,, = ) Show ha he funcion ( ) sin ( ) f e e = possesses a Laplace ransform.
More informationA variational radial basis function approximation for diffusion processes.
A variaional radial basis funcion approximaion for diffusion processes. Michail D. Vreas, Dan Cornford and Yuan Shen {vreasm, d.cornford, y.shen}@ason.ac.uk Ason Universiy, Birmingham, UK hp://www.ncrg.ason.ac.uk
More informationCHAPTER 7: SECOND-ORDER CIRCUITS
EEE5: CI RCUI T THEORY CHAPTER 7: SECOND-ORDER CIRCUITS 7. Inroducion Thi chaper conider circui wih wo orage elemen. Known a econd-order circui becaue heir repone are decribed by differenial equaion ha
More informationPROPERTIES OF MAXIMUM LIKELIHOOD ESTIMATES IN DIFFUSION AND FRACTIONAL-BROWNIAN MODELS
eor Imov r. a Maem. Sais. heor. Probabiliy and Mah. Sais. Vip. 68, 3 S 94-9(4)6-3 Aricle elecronically published on May 4, 4 PROPERIES OF MAXIMUM LIKELIHOOD ESIMAES IN DIFFUSION AND FRACIONAL-BROWNIAN
More informationSUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL
HE PUBLISHING HOUSE PROCEEDINGS OF HE ROMANIAN ACADEMY, Series A, OF HE ROMANIAN ACADEMY Volume, Number 4/200, pp 287 293 SUFFICIEN CONDIIONS FOR EXISENCE SOLUION OF LINEAR WO-POIN BOUNDARY PROBLEM IN
More informationExam 1 Solutions. 1 Question 1. February 10, Part (A) 1.2 Part (B) To find equilibrium solutions, set P (t) = C = dp
Exam Soluions Februar 0, 05 Quesion. Par (A) To find equilibrium soluions, se P () = C = = 0. This implies: = P ( P ) P = P P P = P P = P ( + P ) = 0 The equilibrium soluion are hus P () = 0 and P () =..
More informationarxiv: 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 informationLecture #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 informationApproximate Controllability of Fractional Stochastic Perturbed Control Systems Driven by Mixed Fractional Brownian Motion
American Journal of Applied Mahemaic and Saiic, 15, Vol. 3, o. 4, 168-176 Available online a hp://pub.ciepub.com/ajam/3/4/7 Science and Educaion Publihing DOI:1.1691/ajam-3-4-7 Approximae Conrollabiliy
More informationTo become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship
Laplace Tranform (Lin & DeCarlo: Ch 3) ENSC30 Elecric Circui II The Laplace ranform i an inegral ranformaion. I ranform: f ( ) F( ) ime variable complex variable From Euler > Lagrange > Laplace. Hence,
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationKEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow
1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering
More informationMALLIAVIN CALCULUS FOR BACKWARD STOCHASTIC DIFFERENTIAL EQUATIONS AND APPLICATION TO NUMERICAL SOLUTIONS
The Annal of Applied Probabiliy 211, Vol. 21, No. 6, 2379 2423 DOI: 1.1214/11-AAP762 Iniue of Mahemaical Saiic, 211 MALLIAVIN CALCULUS FOR BACKWARD STOCHASTIC DIFFERENTIAL EQUATIONS AND APPLICATION TO
More informationEXISTENCE 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 informationMethod For Solving Fuzzy Integro-Differential Equation By Using Fuzzy Laplace Transformation
INERNAIONAL JOURNAL OF SCIENIFIC & ECHNOLOGY RESEARCH VOLUME 3 ISSUE 5 May 4 ISSN 77-866 Meod For Solving Fuzzy Inegro-Differenial Equaion By Using Fuzzy Laplace ransformaion Manmoan Das Danji alukdar
More informationProperties Of Solutions To A Generalized Liénard Equation With Forcing Term
Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick
More information(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)
Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion
More informationCurvature. Institute of Lifelong Learning, University of Delhi pg. 1
Dicipline Coure-I Semeer-I Paper: Calculu-I Leon: Leon Developer: Chaianya Kumar College/Deparmen: Deparmen of Mahemaic, Delhi College of r and Commerce, Univeriy of Delhi Iniue of Lifelong Learning, Univeriy
More information