Supplementary Material: Accelerating Adaptive Online Learning by Matrix Approximation
|
|
- Charleen Atkinson
- 5 years ago
- Views:
Transcription
1 Supplemenary Maerial: Acceleraing Adapive Online Learning by Marix Approximaion Yuanyu Wan and Lijun Zhang Naional Key Laboraory for Novel Sofware Technology Nanjing Universiy, Nanjing 1003, China A Theoreical Analysis In his supplemenary maerial, we provide proof of Theorems 1 and. A.1 Supporing Resuls The following resuls are used hroughou our analysis. Lemma 1. (Proposiion 3 of [1]). Le sequence {β } be generaed by ADA-RP. We have R(T ) 1 η [ BΨ+1(β, β + B Ψ (β, β + ] + 1 η B Ψ 1 (β, β + η f (β ) Ψ. Lemma. Le X = i=1 x ix i and A denoe he pseudo-inverse of A, hen x, (X 1/ ) x x, (X 1/ T ) x = r(x 1/ T ). Lemma can be proved in he same way as Lemma 10 of [1]. Theorem 3. (Theorem.3 of [11]). Le 0 <, δ < 1 and S = 1 k R R k n where he enries R i,j of R are independen sandard normal random variables. Then if k = Θ( d+log(1/δ) ), hen for any fixed n d marix A, wih probabiliy 1 δ, simulaneously for all x R d, (1 ) Ax SAx (1 + ) Ax. Based on he above heorem, we derive he following corollary. Corollary 1. Le 0 <, δ < 1 and each enry of r R τ is a Gaussian random variable drawn from N (0, 1/ τ) independenly. Then, if τ = Ω( r+log(t/δ) ), wih probabiliy 1 δ, simulaneously for all = 1,..., T, (1 )C C S S (1 + )C C.
2 Theorem. (Theorem 10 of [0]). Le R be a Gaussian random marix of size p n. Le C = diag(c 1,..., c p ) and S = diag(s 1,..., s p ) be p p diagonal marices, where c i 0 and c i + s i = 1 for all i. Le M = C + 1 n SRR S and r = i s i. P r(λ 1 (M) 1 + ) q exp ( cn ), max i (s i )r ) P r(λ p (M) 1 ) q exp ( cn max i (s i )r, where he consan c is a leas 1/3, and q is he rank of S. Based on he above heorem, we derive he following corollary. σ i, r α+σi = max 1 T σ 1. Le K = αi d + C C, K = αi d + S S, and Corollary. Le c 1/3, α > 0, σ i = λ i(c C ), r = i max r and σ 1 = k T Ĩ = K / K K / r. If τ σ 1 c (α+σ 1 1 δ, simulaneously for all = 1,, T, dt log ) δ (1 )I d Ĩ (1 + )I d., hen wih probabiliy a leas A. Proof of Theorem 1 Le X denoe S S. Firs, we consider bounding he firs erm in he upper bound of Lemma 1. Wih probabiliy 1 δ, we have B Ψ+1 (β, β + B Ψ (β, β + = 1 β β +1, ( X 1/ 1/ +1 X )(β β + 1 β β +1, 1 + X 1/ +1 (β β + 1 β β +1, 1 X 1/ (β β + 1 β β +1, (X 1/ +1 X1/ )(β β + + β β +1, (X 1/ +1 + X1/ )(β β + 1 β β +1 (X 1/ +1 X1/ ) + β β +1, (X 1/ +1 + X1/ )(β β + 1 β β +1 r(x 1/ +1 X1/ ) + β β +1, (X 1/ +1 + X1/ )(β β +
3 where he firs inequaliy is due o Corollary 1. Thus, we can ge 1 [ BΨ+1(β, β + B Ψ (β, β + ] β β +1 r(x 1/ +1 X1/ ) + β β +1, (X 1/ +1 + X1/ )(β β + 1 max T β β r(x 1/ T ) 1 β β 1 r(x 1/ + max T β β X 1/ β β 1 r(x 1/. Noe ha β 1 = 0, hen B Ψ1 (β, β = 1 β 1/, (σi d + X β 1 σ β + + () β r(x 1/ where he inequaliy is due o Corollary 1. Then, we consider he upper bound of T f (β ) Ψ. Wih probabiliy 1 δ, we have 1 f (β ) Ψ = 1/ g, (σi d + X ) g 1 g, (X ) 1/ g = l (β x ) x, (X ) 1/ x 1 1 (3) where he inequaliy is due o Corollary 1. According o Lemma, we have f (β ) Ψ T l (β x ) x, (X ) 1/ x 1 max T l (β x ) T x, (X ) 1/ x 1 1 max T l (β x ) r(x 1/ T ). We complee he proof by subsiuing (3), (), and (5) ino Lemma 1. (5) A.3 Proof of Theorem Inspired by he proof of Theorem 1, we can derive Theorem by respecively bounding each erm in he upper bound of Lemma 1. Before ha, we need o derive he lower and upper bounds of (S S ) 1/ based on Corollary.
4 Le he SVD of C be C = UΣV where U R d d, Σ R d d, V R d. According o Corollary, wih probabiliy a leas 1 δ, simulaneously for all = 1,..., T, S S = K αi d = K 1/ Ĩ K 1/ αi d and (1 + )K αi d = (1 + )C C + αi d = U ( (1 + )ΣΣ + αi d ) U S S + αi d = K αi d + αi d = K 1/ Ĩ K 1/ αi d + αi d (1 )K αi d + αi d = (1 )C C. Then simulaneously for all = 1,..., T, we have and (S S ) 1/ 1 + U(ΣΣ) 1/ U + αui d U = 1 + X 1/ + αi d (6) (S S ) 1/ = (S S ) 1/ + αi d αi d ( (S S ) + αi d ) 1/ αid 1 X 1/ αi d. Then we consider bounding he firs erm in he upper bound of Lemma 1. Le X denoe S S. Simulaneously for all = 1,..., T, we have B Ψ+1 (β, β + B Ψ (β, β + = 1 β β +1, ( X 1/ 1/ +1 X )(β β + 1 β β +1, 1 + X 1/ +1 (β β + 1 β β +1, 1 X 1/ )(β β β β +1, αi d (β β + = 1 β β +1, 1 + X 1/ +1 (β β + 1 β β +1, 1 X 1/ )(β β + + α (β β + 1 β β +1 r(x 1/ +1 X1/ ) + β β +1, (X 1/ +1 + X1/ )(β β + + α (β β + (7)
5 where he firs inequaliy is due o (6), (7) and he las inequaliy has been proved in he proof of Theorem 1. Thus, we can ge [ BΨ+1 (β, β + B Ψ (β, β + ] Noe ha β 1 = 0, hen 1 max T β β r(x 1/ T ) 1 β β 1 r(x 1/ + max T β β β β 1 r(x 1/ X 1/ + α(t 1) max T β β. B Ψ1 (β, β = 1 β 1/, (σi d + X β 1 σ β + + β r(x 1/ + 1 α β. (8) (9) Before considering he upper bound of T f (β ) Ψ, we need o derive he upper bound of H. Le he SVD of S be S = UΣV where U R d d, Σ R d d, V R d. We also have, for all = 1,..., T, H = σi d + (S S ) 1/ = U ( σi d + (ΣΣ) 1/) U U ( αi d + (ΣΣ) ) 1/ U = (αi d + S S ) 1/ due o σ α λ i (S S ) + α λ i (S S ) for all i = 1,, d. Then according o Corollary, wih probabiliy a leas 1 δ, simulaneously for all = 1,..., T, H ( (αi d + S S ) 1/) ( 1/ = (K Ĩ K 1/ 1 (K ) 1/ 1 ( = (αid + X ) ) 1/. 1 1 ) ) 1/ Thus, we can ge f (β ) Ψ = g, H g g, ( (αi d + X ) ) 1/ g 1 = l (β x ) 1 x, (X ) 1/ x.
6 According o Lemma, we have f (β ) Ψ 1 max T l (β x ) x, (X ) 1/ x (10) max 1 T l (β x ) r(x 1/ T ). We complee he proof by subsiuing (8), (9), and (10) ino Lemma 1. A. Proof of Corollary 1 Le C = UΣV be he singular value decomposiion of C. Noice ha U R r, ΣV R r d. According o Theorem 3, we have if τ = Θ( r+log(1/δ) ), hen simulaneously x R r, wih probabiliy 1 δ, (1 ) Ux R Ux (1 + ) Ux Le y R d be arbirary vecor, hen C y = UΣV y = Ux where x = ΣV y R r. Then we have y S S y = y C R R C y = R Ux (1 + ) Ux = (1 + )y C C y and y S S y = y C R R C y = R Ux (1 ) Ux = (1 )y C C y. Then, we have (1 )C C S S (1+)C C wih probabiliy 1 δ, provided τ = Ω( r+log(1/δ) ). Using he union bound, we have if τ = Ω( r+log(t/δ) ), wih probabiliy 1 δ, simulaneously for all = 1,..., T, (1 )C C S S (1 + )C C. A.5 Proof of Corollary Le he SVD of C be C = UΣV where U R d d, Σ R d d, V R d. Then we have K = U(αI d + ΣΣ )U and Ĩ = K / K K / = K / (αi d + C R R C )K / ( = U αi d (αi d + ΣΣ) + (αi p + ΣΣ) / ΣV R R VΣ(αI d + ΣΣ ) /) U ( = U αi d (αi d + ΣΣ) + (αi p + ΣΣ) / ΣRR Σ(αI d + ΣΣ ) /) U where R = V R R d τ is a Gaussian random marix due o ha V is an orhogonal marix and R is a Gaussian random marix.
7 α α+σ i Le c i = a leas 1 δ, and s i = r σ 1 σ i α+σi. Then according o Theorem, wih probabiliy (1 )I d Ĩ (1 + )I d provided τ c (α+σ1 δ where he consan c is a leas 1/3. Using he union bound, we complee he proof. ) log d
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 informationExercises: Similarity Transformation
Exercises: Similariy Transformaion Problem. Diagonalize he following marix: A [ 2 4 Soluion. Marix A has wo eigenvalues λ 3 and λ 2 2. Since (i) A is a 2 2 marix and (ii) i has 2 disinc eigenvalues, we
More informationCourse Notes for EE227C (Spring 2018): Convex Optimization and Approximation
Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3
More informationMath 315: Linear Algebra Solutions to Assignment 6
Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen
More informationTracking Adversarial Targets
A. Proofs Proof of Lemma 3. Consider he Bellman equaion λ + V π,l x, a lx, a + V π,l Ax + Ba, πax + Ba. We prove he lemma by showing ha he given quadraic form is he unique soluion of he Bellman equaion.
More informationThe General Linear Test in the Ridge Regression
ommunicaions for Saisical Applicaions Mehods 2014, Vol. 21, No. 4, 297 307 DOI: hp://dx.doi.org/10.5351/sam.2014.21.4.297 Prin ISSN 2287-7843 / Online ISSN 2383-4757 The General Linear Tes in he Ridge
More informationApproximation Algorithms for Unique Games via Orthogonal Separators
Approximaion Algorihms for Unique Games via Orhogonal Separaors Lecure noes by Konsanin Makarychev. Lecure noes are based on he papers [CMM06a, CMM06b, LM4]. Unique Games In hese lecure noes, we define
More informationTHE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX
J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he
More informationState-Space Models. Initialization, Estimation and Smoothing of the Kalman Filter
Sae-Space Models Iniializaion, Esimaion and Smoohing of he Kalman Filer Iniializaion of he Kalman Filer The Kalman filer shows how o updae pas predicors and he corresponding predicion error variances when
More informationMODULE 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 informationMachine Learning 4771
ony Jebara, Columbia Universiy achine Learning 4771 Insrucor: ony Jebara ony Jebara, Columbia Universiy opic 20 Hs wih Evidence H Collec H Evaluae H Disribue H Decode H Parameer Learning via JA & E ony
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 informationODEs 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 informationU( θ, θ), U(θ 1/2, θ + 1/2) and Cauchy (θ) are not exponential families. (The proofs are not easy and require measure theory. See the references.
Lecure 5 Exponenial Families Exponenial families, also called Koopman-Darmois families, include a quie number of well known disribuions. Many nice properies enjoyed by exponenial families allow us o provide
More informationChapter 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 informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
More information2 Some Property of Exponential Map of Matrix
Soluion Se for Exercise Session No8 Course: Mahemaical Aspecs of Symmeries in Physics, ICFP Maser Program for M 22nd, January 205, a Room 235A Lecure by Amir-Kian Kashani-Poor email: kashani@lpensfr Exercise
More informationEmpirical Process Theory
Empirical Process heory 4.384 ime Series Analysis, Fall 27 Reciaion by Paul Schrimpf Supplemenary o lecures given by Anna Mikusheva Ocober 7, 28 Reciaion 7 Empirical Process heory Le x be a real-valued
More informationAppendix to Online l 1 -Dictionary Learning with Application to Novel Document Detection
Appendix o Online l -Dicionary Learning wih Applicaion o Novel Documen Deecion Shiva Prasad Kasiviswanahan Huahua Wang Arindam Banerjee Prem Melville A Background abou ADMM In his secion, we give a brief
More informationOptimal Paired Choice Block Designs. Supplementary Material
Saisica Sinica: Supplemen Opimal Paired Choice Block Designs Rakhi Singh 1, Ashish Das 2 and Feng-Shun Chai 3 1 IITB-Monash Research Academy, Mumbai, India 2 Indian Insiue of Technology Bombay, Mumbai,
More informationDISCRETE 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 informationSPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990),
SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F Trench SIAM J Marix Anal Appl 11 (1990), 601-611 Absrac Le T n = ( i j ) n i,j=1 (n 3) be a real symmeric
More informationChapter 2. Models, Censoring, and Likelihood for Failure-Time Data
Chaper 2 Models, Censoring, and Likelihood for Failure-Time Daa William Q. Meeker and Luis A. Escobar Iowa Sae Universiy and Louisiana Sae Universiy Copyrigh 1998-2008 W. Q. Meeker and L. A. Escobar. Based
More informationGRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256
Tile Auhor(s) GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION Zhao, Liang Ciaion Osaka Journal of Mahemaics. 51(1) P.45-P.56 Issue Dae 014-01 Tex Version publisher URL hps://doi.org/10.18910/9195
More informationT L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB
Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal
More informationOscillation 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 informationV L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode.
ECE 445 Analysis and Design of Power Elecronic Circuis Problem Se 7 Soluions Problem PS7.1 Erickson, Problem 5.1 Soluion (a) Firs, recall he operaion of he buck-boos converer in he coninuous conducion
More informationψ(t) = V x (0)V x (t)
.93 Home Work Se No. (Professor Sow-Hsin Chen Spring Term 5. Due March 7, 5. This problem concerns calculaions of analyical expressions for he self-inermediae scaering funcion (ISF of he es paricle in
More informationLECTURE 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 informationDouble system parts optimization: static and dynamic model
Double sysem pars opmizaon: sac and dynamic model 1 Inroducon Jan Pelikán 1, Jiří Henzler 2 Absrac. A proposed opmizaon model deals wih he problem of reserves for he funconal componens-pars of mechanism
More informationWhat 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 informationMath 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 informationEMS 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 informationResearch Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations
Hindawi Publishing Corporaion Boundary Value Problems Volume 11, Aricle ID 19156, 11 pages doi:1.1155/11/19156 Research Aricle Exisence and Uniqueness of Periodic Soluion for Nonlinear Second-Order Ordinary
More informationSupplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence
Supplemen for Sochasic Convex Opimizaion: Faser Local Growh Implies Faser Global Convergence Yi Xu Qihang Lin ianbao Yang Proof of heorem heorem Suppose Assumpion holds and F (w) obeys he LGC (6) Given
More informationMath-Net.Ru All Russian mathematical portal
Mah-NeRu All Russian mahemaical poral Roman Popovych, On elemens of high order in general finie fields, Algebra Discree Mah, 204, Volume 8, Issue 2, 295 300 Use of he all-russian mahemaical poral Mah-NeRu
More informationt 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 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 informationNotes 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 informationOnline Convex Optimization Example And Follow-The-Leader
CSE599s, Spring 2014, Online Learning Lecure 2-04/03/2014 Online Convex Opimizaion Example And Follow-The-Leader Lecurer: Brendan McMahan Scribe: Sephen Joe Jonany 1 Review of Online Convex Opimizaion
More informationRobert Kollmann. 6 September 2017
Appendix: Supplemenary maerial for Tracable Likelihood-Based Esimaion of Non- Linear DSGE Models Economics Leers (available online 6 Sepember 207) hp://dx.doi.org/0.06/j.econle.207.08.027 Rober Kollmann
More informationHomework 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 informationLet us start with a two dimensional case. We consider a vector ( x,
Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our
More informationChapter Three Systems of Linear Differential Equations
Chaper Three Sysems of Linear Differenial Equaions In his chaper we are going o consier sysems of firs orer orinary ifferenial equaions. These are sysems of he form x a x a x a n x n x a x a x a n x n
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 informationLie Derivatives operator vector field flow push back Lie derivative of
Lie Derivaives The Lie derivaive is a mehod of compuing he direcional derivaive of a vecor field wih respec o anoher vecor field We already know how o make sense of a direcional derivaive of real valued
More informationFinish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!
MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his
More informationModel Reduction for Dynamical Systems Lecture 6
Oo-von-Guericke Universiä Magdeburg Faculy of Mahemaics Summer erm 07 Model Reducion for Dynamical Sysems ecure 6 v eer enner and ihong Feng Max lanck Insiue for Dynamics of Complex echnical Sysems Compuaional
More informationMean-square Stability Control for Networked Systems with Stochastic Time Delay
JOURNAL OF SIMULAION VOL. 5 NO. May 7 Mean-square Sabiliy Conrol for Newored Sysems wih Sochasic ime Delay YAO Hejun YUAN Fushun School of Mahemaics and Saisics Anyang Normal Universiy Anyang Henan. 455
More informationAsymptotic Equipartition Property - Seminar 3, part 1
Asympoic Equipariion Propery - Seminar 3, par 1 Ocober 22, 2013 Problem 1 (Calculaion of ypical se) To clarify he noion of a ypical se A (n) ε and he smalles se of high probabiliy B (n), we will calculae
More informationin Engineering Prof. Dr. Michael Havbro Faber ETH Zurich, Switzerland Swiss Federal Institute of Technology
Risk and Saey in Engineering Pro. Dr. Michael Havbro Faber ETH Zurich, Swizerland Conens o Today's Lecure Inroducion o ime varian reliabiliy analysis The Poisson process The ormal process Assessmen o he
More informationSupplementary Document
Saisica Sinica (2013): Preprin 1 Supplemenary Documen for Funcional Linear Model wih Zero-value Coefficien Funcion a Sub-regions Jianhui Zhou, Nae-Yuh Wang, and Naisyin Wang Universiy of Virginia, Johns
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 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 informationψ ( t) = c n ( t ) n
p. 31 PERTURBATION THEORY Given a Hamilonian H ( ) = H + V( ) where we know he eigenkes for H H n = En n we ofen wan o calculae changes in he ampliudes of n induced by V( ) : where ψ ( ) = c n ( ) n n
More information1 Review of Zero-Sum Games
COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any
More informationbe a Householder matrix. Then prove the followings H = I 2 uut Hu = (I 2 uu u T u )u = u 2 uut u
MATH 434/534 Theoretical Assignment 7 Solution Chapter 7 (71) Let H = I 2uuT Hu = u (ii) Hv = v if = 0 be a Householder matrix Then prove the followings H = I 2 uut Hu = (I 2 uu )u = u 2 uut u = u 2u =
More informationPENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD
PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD HAN XIAO 1. Penalized Leas Squares Lasso solves he following opimizaion problem, ˆβ lasso = arg max β R p+1 1 N y i β 0 N x ij β j β j (1.1) for some 0.
More informationSingular Value Decomposition
Singular Value Decomposition Motivatation The diagonalization theorem play a part in many interesting applications. Unfortunately not all matrices can be factored as A = PDP However a factorization A =
More informationFréchet derivatives and Gâteaux derivatives
Fréche derivaives and Gâeaux derivaives Jordan Bell jordan.bell@gmail.com Deparmen of Mahemaics, Universiy of Torono April 3, 2014 1 Inroducion In his noe all vecor spaces are real. If X and Y are normed
More informationSystem of Linear Differential Equations
Sysem of Linear Differenial Equaions In "Ordinary Differenial Equaions" we've learned how o solve a differenial equaion for a variable, such as: y'k5$e K2$x =0 solve DE yx = K 5 2 ek2 x C_C1 2$y''C7$y
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 informationLecture 12: Multiple Hypothesis Testing
ECE 830 Fall 00 Saisical Signal Processing insrucor: R. Nowak, scribe: Xinjue Yu Lecure : Muliple Hypohesis Tesing Inroducion In many applicaions we consider muliple hypohesis es a he same ime. Example
More informationMath Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.
Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need
More informationL p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity
ANNALES POLONICI MATHEMATICI LIV.2 99) L p -L q -Time decay esimae for soluion of he Cauchy problem for hyperbolic parial differenial equaions of linear hermoelasiciy by Jerzy Gawinecki Warszawa) Absrac.
More informationOperators related to the Jacobi setting, for all admissible parameter values
Operaors relaed o he Jacobi seing, for all admissible parameer values Peer Sjögren Universiy of Gohenburg Join work wih A. Nowak and T. Szarek Alba, June 2013 () 1 / 18 Le Pn α,β be he classical Jacobi
More informationOutline. lse-logo. Outline. Outline. 1 Wald Test. 2 The Likelihood Ratio Test. 3 Lagrange Multiplier Tests
Ouline Ouline Hypohesis Tes wihin he Maximum Likelihood Framework There are hree main frequenis approaches o inference wihin he Maximum Likelihood framework: he Wald es, he Likelihood Raio es and he Lagrange
More informationBOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS
BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS XUAN THINH DUONG, JI LI, AND ADAM SIKORA Absrac Le M be a manifold wih ends consruced in [2] and be he Laplace-Belrami operaor on M
More informationThen. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)
Ger sgorin Circle Chaper 9 Approimaing Eigenvalues Per-Olof Persson persson@berkeley.edu Deparmen of Mahemaics Universiy of California, Berkeley Mah 128B Numerical Analysis (Ger sgorin Circle) Le A be
More informationMA 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 informationChapter 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 information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationMulti-component Levi Hierarchy and Its Multi-component Integrable Coupling System
Commun. Theor. Phys. (Beijing, China) 44 (2005) pp. 990 996 c Inernaional Academic Publishers Vol. 44, No. 6, December 5, 2005 uli-componen Levi Hierarchy and Is uli-componen Inegrable Coupling Sysem XIA
More informationLecture 2 October ε-approximation of 2-player zero-sum games
Opimizaion II Winer 009/10 Lecurer: Khaled Elbassioni Lecure Ocober 19 1 ε-approximaion of -player zero-sum games In his lecure we give a randomized ficiious play algorihm for obaining an approximae soluion
More informationSupplementary Material
Dynamic Global Games of Regime Change: Learning, Mulipliciy and iming of Aacks Supplemenary Maerial George-Marios Angeleos MI and NBER Chrisian Hellwig UCLA Alessandro Pavan Norhwesern Universiy Ocober
More informationConcourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations
Concourse Mah 80 Spring 0 Worked Examples: Marix Mehods for Solving Sysems of s Order Linear Differenial Equaions The Main Idea: Given a sysem of s order linear differenial equaions d x d Ax wih iniial
More informationStochastic 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 informationMatrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality
Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]
More informationMonotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type
In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria
More informationBias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé
Bias in Condiional and Uncondiional Fixed Effecs Logi Esimaion: a Correcion * Tom Coupé Economics Educaion and Research Consorium, Naional Universiy of Kyiv Mohyla Academy Address: Vul Voloska 10, 04070
More informationdy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page
Assignmen 1 MATH 2270 SOLUTION Please wrie ou complee soluions for each of he following 6 problems (one more will sill be added). You may, of course, consul wih your classmaes, he exbook or oher resources,
More informationMATH 2050 Assignment 9 Winter Do not need to hand in. 1. Find the determinant by reducing to triangular form for the following matrices.
MATH 2050 Assignmen 9 Winer 206 Do no need o hand in Noe ha he final exam also covers maerial afer HW8, including, for insance, calculaing deerminan by row operaions, eigenvalues and eigenvecors, similariy
More informationLecture 10: The Poincaré Inequality in Euclidean space
Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?
More informationLecture Notes 2. The Hilbert Space Approach to Time Series
Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship
More informationTransform Techniques. Moment Generating Function
Transform Techniques A convenien way of finding he momens of a random variable is he momen generaing funcion (MGF). Oher ransform echniques are characerisic funcion, z-ransform, and Laplace ransform. Momen
More informationnon -negative cone Population dynamics motivates the study of linear models whose coefficient matrices are non-negative or positive.
LECTURE 3 Linear/Nonnegaive Marix Models x ( = Px ( A= m m marix, x= m vecor Linear sysems of difference equaions arise in several difference conexs: Linear approximaions (linearizaion Perurbaion analysis
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 informationSINGULAR VALUE DECOMPOSITION
DEPARMEN OF MAHEMAICS ECHNICAL REPOR SINGULAR VALUE DECOMPOSIION Andrew Lounsbury September 8 No 8- ENNESSEE ECHNOLOGICAL UNIVERSIY Cookeville, N 38 Singular Value Decomposition Andrew Lounsbury Department
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 informationψ ( t) = c n ( t) t n ( )ψ( ) t ku t,t 0 ψ I V kn
MIT Deparmen of Chemisry 5.74, Spring 4: Inroducory Quanum Mechanics II p. 33 Insrucor: Prof. Andrei Tokmakoff PERTURBATION THEORY Given a Hamilonian H ( ) = H + V ( ) where we know he eigenkes for H H
More informationMath 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 informationNavneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi
Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec
More informationRepresentation 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 informationBasic Entropies for Positive-Definite Matrices
Journal of Mahemaics and Sysem Science 5 (05 3-3 doi: 0.65/59-59/05.04.00 D DAVID PUBLISHING Basic nropies for Posiive-Definie Marices Jun Ichi Fuii Deparmen of Ars and Sciences (Informaion Science, Osaa
More informationVariational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial
More informationOnline Learning with Partial Feedback. 1 Online Mirror Descent with Estimated Gradient
Avance Course in Machine Learning Spring 2010 Online Learning wih Parial Feeback Hanous are joinly prepare by Shie Mannor an Shai Shalev-Shwarz In previous lecures we alke abou he general framework of
More informationOn Boundedness of Q-Learning Iterates for Stochastic Shortest Path Problems
MATHEMATICS OF OPERATIONS RESEARCH Vol. 38, No. 2, May 2013, pp. 209 227 ISSN 0364-765X (prin) ISSN 1526-5471 (online) hp://dx.doi.org/10.1287/moor.1120.0562 2013 INFORMS On Boundedness of Q-Learning Ieraes
More informationOrthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind
Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence
More informationThe Singular Value Decomposition and Least Squares Problems
The Singular Value Decomposition and Least Squares Problems Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo September 27, 2009 Applications of SVD solving
More informationKEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow
KEY Mah 334 Miderm III Winer 008 secion 00 Insrucor: Sco Glasgow Please do NOT wrie on his exam. No credi will be given for such work. Raher wrie in a blue book, or on your own paper, preferably engineering
More information