A Rigorous Introduction to Brownian Motion

Size: px
Start display at page:

Download "A Rigorous Introduction to Brownian Motion"

Transcription

1 A Rigorous Inroducion o Brownian Moion Andy Dahl Augus 19, 1 Absrac In his paper we develop he basic properies of Brownian moion hen go on o answer a few quesions regarding is zero se and is local maxima. Conens 1 The Basics 1 The Relevan Measure Theory 5 3 Markov Properies of Brownian moion 6 4 Furher Properies of Brownian moion 9 1 The Basics The concep of a Brownian moion was discovered when Einsein observed paricles oscillaing in liquid. Since fluid dynamics are so chaoic and rapid a he molecular level, his process can be modeled bes by assuming he paricles move randomly and independenly of heir pas moion. We can also hink of Brownian moion as he limi of a random walk as is ime and space incremens shrink o. In addiion o is physical imporance, Brownian moion is a cenral concep in sochasic calculus which can be used in finance and economics o model sock prices and ineres raes. 1.1 Brownian Moion Defined Since we are rying o capure physical inuiion, we define a Brownian moion by he properies we wan i o have and worry abou proving he exisence of and explicily consrucing such a process laer. 1

2 Definiion 1. An R d -valued sochasic process {B() : } is called a d-dimensional Brownian moion saring a x R d if i has he following four properies: Sar a x: B() x Independen incremens: for all 1... n, he incremens B( n ) B( n 1 ),..., B( ) B( 1 ) are independen random variables Normaliy: for all and h > he incremen B( + h) B() is disribued N(, h) Coninuiy: almos surely, B() is coninuous The firs propery anchors he sochasic process in space. The second capures he coninually random naure of a paricle ha is being consanly buffeed by fluid molecules. The hird is required because he expeced displacemen of a paricle should be proporional o he ime i has been raveling and should be symmerically disribued abou he saring poin. Physical moion is coninuous which explains he fourh requiremen. While a Brownian moion is frequenly denoed {B() } o sress he fac ha i is acually an uncounable family of random variables, we will use B as shorhand, undersanding ha varies over he non-negaive reals. The bulk of he firs and hird secions apply o general Brownian moions and in he fourh we specialize o he linear case. The consrucion of Brownian moion is edious and beyond he scope of his paper. Bu we should remember ha i is he characerisics of Brownian moion, raher han is consrucion, which define i. Indeed, here are even differen consrucions. The deails of he consrucion will no be used in his paper. 1. Nondiffereniabiliy of Brownian moion The mos sriking qualiy of Brownian moion is probably is nowhere differeniabiliy. Theorem 1. Almos surely, Brownian moion is nowhere differeniable The proof consiss primarily of a long compuaion which we do no presen. We will prove laer ha in any small inerval o he righ of some ime s, B aains values greaer han and less han B s. So for all ɛ > and s, we can choose some h (s, s + ɛ) such ha B s+h B s is eiher posiive h or negaive. This suppors he idea ha he upper and lower derivaives

3 of B a every poin are + and, respecively, alhough a good deal of compuaional work goes ino proving ha he upper and lower limis diverge as ɛ. Noneheless, knowing ha hey do diverge does give us insigh ino how rapidly and erraically Brownian moion jumps around. The heorem can also be undersood direcly from he definiion of Brownian moion. If B were differeniable a some poin s, we would know where i was going in some small ime inerval in he fuure, bu he independen incremen propery of B should make us skepical of such a predicion. The nex proposiion is a manifesaion of he combinaion of Brownian moion s nondifferniabiliy and is coninuiy. Proposiion 1. Almos surely, B is no monoonic on any inerval. Proof. Fix a < b. Le P (a, b) be he probabiliy ha B is monoonic on (a, b). Then, by independence of incremens, P (a, b) 1 P (a, a + b ) P (a + b, b) 1 P (a, a + b ) since, even if B is monoonic on (a, a+b a+b ) and (, b), he probabiliy ha i is monoonic in he same direcion on boh inervals is 1. Ieraing he divisions of he inerval ino halves n imes we ge P (a, b) ( 1 )n P (a, a + b a n ) Taking he limi as n, we see P (a, b) ( 1 )n P (a, a + b a ) 1 n, n showing P (a, b), so any fixed inerval is almos surely no monoonic. By aking he counable union over all inervals wih raional endpoins we can see ha B is almos surely no monoonic on any inerval wih raional endpoins. By he densiy of Q R, here is an inerval wih raional endpoins conained wihin every inerval. So every inerval conains a subinerval which is almos surely no monoonic, hus every inerval is almos surely no monoonic. We will use his resul laer when discussing he maxima of B. 1.3 Scaling Properies of Brownian Moion We ofen sudy ransformaions of funcions which leave cerain properies invarian, and i is naural o ask wha ransformaions of B have he same disribuion. 3

4 Example 1. B is a Brownian moion. Coninuiy and independence are clearly mainained by negaive muliplicaion and, since he normal disribuion is symmeric abou zero, all he incremens have he proper means and variances. We now move on o more ineresing and useful ransformaions. Proposiion. Rescaling: If B is a sandard Brownian moion, hen so is he process X ab, for all a >. a Proof. Coninuiy and independence of incremens sill hold. For all > s, he normal random variable X() X(s) a(b( ) B( s )) is disribued a a an(, s ) d N(, s), so X() X(s) N(, s) as desired. a This proposiion ells us ha B is a Brownian moions on all ime scales as long as we compensae for he change in variance of he incremens by aking a scalar muliple of he process. More surprisingly, we can inver he domain of B and sill have a Brownian moion. Proposiion 3. Time-inversion: Le B be a sandard Brownian moion. Then he process { : X : is also a sandard Brownian moion Proof. For Brownian moions, B 1 Cov(B, B +s ) Cov(B, B +s B ) + Cov(B, B ) for all, s. For our process X, Cov(X, X +s ) Cov(B 1, ( + s)b 1 ) +s ( + s)cov(b 1, B 1 ) ( + s) +s 1 + s So Cov(X, X +s X ) Cov(X, X +s ) Var(X ). Because he random variables X +s and X are normal, Cov(X, X +s X ) implies ha X +s X and X are independen. And Var(X +s X ) Var(X +s ) + Var(X ) Cov(X +s, X ) ( + s) + s, so our incremens are independen and have he righ variances. Coninuiy is clear for >. We know ha X has he disribuion of a Brownian moion on Q, so lim n X( 1 n ) lim X() 4

5 and we conclude ha X is coninuous a, so X saisfies he properies of a sandard Brownian moion. We end wih secion wih an example which demonsraes he compuaional usefulness of hese alernaive expressions for Brownian moion. Example. Le B be a sandard Brownian moion and X B 1. X is a sandard Brownian moion, so X lim lim B 1 B The Relevan Measure Theory We assume he reader is familiar wih he elemens of basic probabiliy heory such as expecaion, covariance, normal random variables, ec. Bu we do add rigor o hese noions by developing he underlying measure heory, which will be necessary for our discussion of he Markov properies. Definiion. A σ-algebra Σ on a se S is a subse of S, where S is he power se of S, saisfying: {Ø} Σ for all A Σ, A c Σ for all sequences A, A 1,... Σ, i A i Σ By de Morgan s laws we can see ha σ-algebras are closed under counable inersecions as well. The σ-algebra will be our objec of measuremen, so now we need o develop our mehod of measuremen. Definiion 3. A measure is a counably addiive map µ : Σ [, ], where Σ S is our σ-algebra on some se S. A counably addiive map is one such ha for any sequence A 1, A,... Σ of disjoin evens, µ( i1 A i) i1 µ(a i). A probabiliy measure is a measure µ such ha µ(s) 1. Our definiion implies ha µ({ø}) because µ({ø}) µ({ø} {Ø}) µ({ø}) + µ({ø}). Our nex definiion collecs hese noions. Definiion 4. The probabiliy riple is he riple (Ω, F, P ) where F is a σ-algebra on he se Ω and P : Σ [, 1] is a probabiliy measure. We call Ω he sample space and F he collecion of (P -measurable) evens. This riple provides he background for he sudy probabiliy. foreground are random variables. In he 5

6 Definiion 5. A random variable is an F-measurable map X : Ω R, meaning ha he preimage X 1 (B) F for all B B(R). The law of X is P (X 1 ) : B(R) [, 1]. The random variable X is a correspondence beween evens and ses in R, which formalizes he noion ha X akes on cerain values when cerain evens occur. Of course, his correspondence is no ha ineresing in iself; wha ineress us is he probabiliy of X lying in ses in R, which is given by he law of X. For he law of X o be well defined we need X 1 (B(R) F, since F is he domain of P, which is why we require X o be F-measurable. A sochasic process is a family of random variables ha evolves over ime, and up o his poin we have viewed hese random variables from ime. Bu we can also look a he process a some ime s a which he se {X s} is known, and he probabiliy of evens occuring pas s will depend on his informaion. Definiion 6. A filraion on a probabiliy space (Ω, F, P ) is a family {F } of σ-algebras such ha F s F F for all s <. A sochasic process {X } is adaped o he filraion if X is F measurable for all. An adaped filraion capures he inuiion of our informaion which evolves along wih our process: our informaion grows as ime goes on. 3 Markov Properies of Brownian moion The Markov properies ell us a wha imes s a Brownian moion {B +s } referred o as B +s in he fuure has he same disribuion as a Brownian moion sared a B s or, alernaively, when he process B +s B s is a sandard Brownian moion. We will refer o his phenomenon as Brownian moion saring anew a ime s. Our independence of incremens requiremen migh seem o make his propery rivial, and, for deerminisic imes, i does. Theorem. (Markov Propery) Le B be a Brownian moion and fix s. B +s B s is a sandard Brownian moion independen of {B s}. Proof. I is clear ha B +s is a Brownian moion. Subracing a consan only changes he saring poin, and, in paricular, subracing B s makes he process a sandard Brownian moion. Independence of B before ime s follows from he independence of incremens of Brownian moion. 6

7 A far more ineresing and imporan class of imes is random imes, meaning imes defined by some randomly occurring even. Brownian moion does no necessarily sar afresh a such imes. We provide an example, bu firs sae a definiion. Definiion 7. A coninuous funcion f is said o aain a maximum on an inerval I a s I if f(s) f() for all I We say f aains a local maximum a s if here exiss a non-degenerae inerval I conaining s on which f(s) is a maximum. We say he (local) maximum is sric if he above inequaliy can be replaced by a sric inequaliy. Example 3. Le s be a ime ha B aains a sric local maximum and define X B +s B s. Then here exiss some δ such ha for all r (s δ, s + δ), B r < B s. So P (X δ X < ) P (B s+ δ B s > ). So he incremen X δ X < is cerainly no normal, hus X is no a Brownian moion and B does no sar anew a s. This example shows we need o be careful when considering random imes. Noneheless, Brownian moion does sar anew a some random imes. Definiion 8. A random ime T [, ] defined on a probabiliy space wih filraion F is a sopping ime if {T s} F s for every s >. Given our heurisic undersanding of F as he informaion up o ime, a random ime is a sopping ime if we can deermine wheher i has occurred before s based only on knowing he informaion up o s. This explains why B does no sar anew a he ime s where B aains a local maximum because we do no know ha B s is a local maximum unil ime s + δ. Sopping imes ge heir name because if we sop exacly a ime s we can deermine wheher s is our sopping ime; we do no need o go forward in ime o see ha s is in fac he ime we wan. We provide an example of a sopping ime. Definiion 9. For a Brownian moion in R d and a R d, define T a inf{ B() a} as he firs ime B his a. T a is a sopping ime because we can deermine if s T a by observing wheher B s a and wheher B r a for any r < s, boh of which are known a ime s. For he same reason, he second, hird, or nh ime B his a are also sopping imes, bu he las ime B his a is no a sopping ime because we would need o see infiniely far ino he fuure o know he process never reurns o a again. 7

8 T a is really only useful for linear Brownian moions, as i urns ou ha Brownian moions almos surely never hi any specific a R \ {} for d, while in he 1-dimensional case T a is almos surely finie for all a. We now sae he srong Markov propery of Brownian moion and jusify our emphasis on sopping imes. Theorem 3. (Srong Markov Propery) For every almos surely finie sopping ime T, he process B T + B T is a sandard Brownian moion independen of F T. Equivalenly, condiional on F T, B T + is a Brownian moion sared a B T, so, for Brownian moions, we can say ha he only useful informaion conained in F T is he value of B a T : Brownian moion sars anew a T. The srong Markov propery allows us o prove he reflecion principle. Theorem 4. (Reflecion Principle)Le T be a sopping ime. The process given by reflecing a Brownian moion abou ime T is a Brownian moion. More precisely, he process defined by { B(T ) B() : T B B() : T is a Brownian moion. Proof. By he srong Markov propery, B( + T ) B(T ) is a sandard Brownian moion independen of {B() T }. So B(T ) B( + T ) mus be as well. If we aach he process {B() T } in fron of {B( + T ) B(T ) } we will ge a new Brownian moion: he properies of Brownian moion all hold independenly wihin he concaenaed processes, independence of incremens holds beween hem because he processes we concaenae are independen by he srong Markov propery and coninuiy holds because he process are equal a T, he poin where we glue hem ogeher. In he same way, we aach {B() T } o he fron of B(T ) B(+T ), which will give us a process idenical o he former concaenaion, which is jus B. Since his laer concaenaion is B, we conclude B is a sandard Brownian moion. The reflecion principle is exremely useful. We will firs use i o compue he densiy of he maximal process. Proposiion 4. Le B be a linear Brownian moion and M be is maximal process, defined as M max s B s. Then P (M > a) P (B > a) for all a >. 8

9 Proof. P (M > a) P (B > a or M > a while B a) P (B > a) + P (M > a and B a) since he wo evens are disjoin. M > a implies T a <, so by reflecing abou T a, we see ha M > a and B a if and only if B > a. So P (M > a) P (B > a) + P (B > a) P (B > a) 4 Furher Properies of Brownian moion Throughou his secion we specialize o linear Brownian moions. 4.1 The Zeroes of Brownian moion We define he Zero se, Z, as he imes B his, or Z { B }. We firs show ha Z is small in he sense of area. Theorem 5. Wih probabiliy one, he Lebesgue measure of Z is. Proof. Le Z be he Lebesgue measure of Z. We compue he expecaion: E Z E χ {} (W ) d P (W ) d (1 P (W ) + P (W )) d We know Z is non-negaive since i is a measure. We now show ha non-negaive random variables wih expecaion are almos surely. Suppose X is a random variable wih EX and fix a >. Then EX X dp X dp a P (X a) Ω {X a} So P (X a) for all a >. Leing a +, we see P (X > ), and X is almos surely. We conclude ha E Z Z almos surely. We should have expeced his resul because we know ha B is almos surely nonzero for all nonzero since he incremen B B B is a normal random variable. Noneheless, B his infiniely many imes in any inerval o he righ of he origin. Proposiion 5. Almos surely, B has infiniely many zeros in every ime inerval (, ɛ), where ɛ >. 9

10 Proof. We induc on he number of zeros in (, ɛ). Firs, we show ha here mus be a zero in his inerval. Le M + and M be he maximal and minimal processes, respecively, and fix ɛ >. We know ha P (M ɛ + > a) P (B ɛ > a). By aking he limi as a +, we see P (M ɛ + > ) P (B ɛ > ) 1 since B is symmeric. By symmery, P (M (ɛ) < ) 1. Since B is almos surely coninuous, we employ he inermediae value heorem and conclude ha B for some (, ɛ). Now ake some finie se S of zeros of B on he inerval (, ɛ). Le T min( S) be he earlies member of S. Since ɛ was arbirary when we esablished ha B had a zero in (, ɛ), by he same argumen we can see ha B almos surely has a zero in (, T ). By he minimaliy of T his zero mus no be in S, hus here is no finie se conaining all he imes B his zero, so Z is almos surely infinie. This allows us o fully characerize Z. Theorem 6. Almos surely, Z is a perfec se, ha is, Z is closed and has no isolaed poins. Proof. Since B is coninuous, Z B 1 ({}) mus be closed because i is he inverse image of he closed se {}. Consider he ime τ q inf{ q B }, where q is a raional number. This is clearly a sopping ime, and i is almos surely finie because B almos surely crosses for arbirarily large. Moreover, he infimum is a minimum because Z is almos surely closed. We apply he srong Markov propery a τ q and ge ha B +τq B τq B +τq is a sandard Brownian moion. Because we already know ha a Brownian moion crosses in every small inerval o he righ of he origin, τ q is no isolaed from he righ in Z. Now suppose we have some z Z ha is no in {τ q q Q}. Take some sequence, q n, of raional numbers ha converges o z. For each q n, here mus exis some n Z such ha q n n < z since z τ qn. Because q n z, n z, so z is no isolaed from he lef in Z. I is a fac from analysis ha perfec ses are uncounable. This shows ha even hough Z has measure, i sill is very big in a sense. 4. Maxima of Brownian moion Because Brownian moions change direcions so frequenly and dramaically i is no surprising ha hey frequenly aains local maxima. Theorem 7. Almos surely, he se of imes where B() aains a local maximum is dense in [, ) 1

11 Proof. We begin by showing ha B almos surely has a local maximum on every fixed inerval. A ime B aains local maximum is a poin preceded by an increasing inerval and followed by a decreasing inerval. So B has no local max on (a, b) if and only if i is monoonic on (a, b) or monoonically decreasing unil some poin c (a, b) hen monoonically increasing. The former even has probabiliy. And for all c (a, b), (a, a+b ) (a, c) or ( a+b, b) (c, b), so B being monoonic on (a, c) and (c, b) implies ha B is monoonic on eiher (a, a+b a+b ) or (, b), and boh hese evens occur wih probabiliy. By aking a counable union, we see ha all inervals wih raional endpoins almos surely have a ime B aains a local maximum. By he densiy of Q R, here exiss such a raional inerval wihin every inerval. So every real inerval conains a raional inerval which conains a ime B aains a local max, hus conains a ime B aains a local max. Coninuing a heme, having shown ha he se of imes Brownian moion aains a maximum is big in he sense of densiy in [, ), we now show ha i is small in he sense of cardinaliy. Firs we mus prove wo lemmas. Lemma 1. On any wo fixed inervals, B almos surely does no aain he same maximum. Proof. Fix wo disjoin closed inervals, le M be he maximal process and le m be he maximum value aained by B on he firs of he wo disjoin inervals. Name he second inerval [a, b]. Consider he ime τ inf{ a B m}. Since m is known sricly before he ime a, τ is a sopping ime. If τ [a, b], hen B never aains m on [a, b] and cerainly does no have m as a maximum on his inerval, so suppose τ [a, b]. Since B b m almos surely, we can suppose τ [a, b). By he srong Markov propery, X B +τ B τ B +τ m is a Brownian moion. Fix < ɛ < b τ so ha (τ, ɛ + τ) [a, b). We know here exiss some s (, ɛ) such ha X s > since X is a sandard Brownian moion. Thus here exiss some s s + τ (τ, ɛ + τ) (a, b] such ha B s m + X s τ m + X s > m, showing ha he maximum of B on [a, b] is sricly greaer han m. I is imporan o noe ha we have no proved ha almos surely no wo disjoin inervals have he same maximum. In fac, his is no rue; almos surely, here exis disjoin inervals wih he same maximum. Le T a,n be he nh ime he process hi a. Since B is sricly above or below a on he inervals (T a,n 1, T a,n ) for all n, and i has equal probabiliy of being above or below, here almos surely exiss some n such ha he maximum of B on [T a,n 1, T a,n ] is a, which is also he maximum of B on [, T a,1 ]. 11

12 Lemma. Almos surely, every local maximum of Brownian moion is a sric local maximum. Proof. Suppose B aains a local maximum a ime s. Then here exiss some δ such ha B s is a maximum on he inerval (s δ, s+δ). If B s is no a sric maximum, hen here exiss some r (s δ, s + δ) such ha B r B s. We can find disjoin closed inervals wih raional endpoins around r and s conained in (s δ, s + δ). Bu, wih probabiliy 1, B does no aain he same maximum on any wo raional inervals, so such an r almos surely does no exis. Thus, almos surely, every ime B aains a local maximum, i aains a sric local maximum. Wih hese wo lemma we can move on o a major resul. Theorem 8. Almos surely, he se of imes B aains a local maximum is counable. Proof. Le S be he se of imes B aains a local maximum. Define f : Q Q S by f(p, q) inf{ p B max p s q (B s )}. This will conain S, and hus show ha S is almos surely counable, if B almos surely aains a sric maximum on some raional inerval a every ime i aains a local maximum. By he above lemma, we can almos surely find neighborhoods N s around each s S on which B s is a sric maximum. And, by he densiy of Q R, we can find raional inervals wihin each N s conaining each s on which B s is a sric maximum. This classificaion of local maxima is very imporan: now, if we prove ha some propery almos surely holds for an arbirary local maximum, we can ake a counable union and show ha he propery almos surely holds for all local maxima. We demonsrae his echnique. Corollary 1. The local maxima of B are almos surely disinc. Proof. Since here is a counable number of imes B aains a local maximum, here is a counable number of disjoin inervals on which hese local maxima are maxima, and hus here is counable number of pairs of hese inervals. We know ha, almos surely, B does no aain he same maximum on any pair of inervals. Thus we ake a counable union over all pairs of disjoin inervals on which a local maximum of B is a max and prove he corollary. We move on o providing a few compuaions. The reflecion principle will be our key ingredien. 1

13 Proposiion 6. T a has he disribuion given by Proof. P (T a d) a π 3 exp( a )d P (T a ) P (M a) P (B a) s a πs 3 exp( a s )ds a 1 π exp( x )dx subsiuing x a. Differeniaing wih respec o gives he resul. We will use he reflecion principle again in he nex proposiion. Proposiion 7. The processes M and M B have he join disribuion Proof. P (M da, M B db) (a + b) π 3 + b) exp( (a )dadb P (M a, B b) P (T a, B b) P (T a, a B b) P (a B b) P (B a b) a (y b) exp( )dy π a b 1 π exp( x )dx where B is he Brownian moion B refleced abou T a and we subsiued x y b. Taking he derivaive wih respec o b we ge P (M a, B db) Now differeniaing wih respec o a we ge So P (M a, B db) a (y b) (y b) exp( )dydb π 3 (a b) π 3 exp( P (M a, M B db) P (M da, B a db) (a b) )dadb (a + b) π 3 + b) exp( (a )dadb 13

14 Corollary. We can now show ha M B has he same disribuion as B. Inegraing P (M a, M B db) over a gives P (M B da) (a + b) exp( )da exp( a π π )da This proposiion leads us o anoher calculaion. Proposiion 8. Le θ max{s B(s) M(s)}. The join disribuion of θ and M is given by P (M da, θ ds) a π ( s)s 3 exp( a s )dads and hus he cumulaive disribuion funcion of θ is P {θ s} π arcsin s Proof. Le X be he sandard Brownian moion given by X B +s B s and le N be he maximal process of X. Then N s max{x u u s} max{b u+s B s u s} max{b u s u } B s We know θ s if and only if M s M which happens if and only if M s max{b u s u } N s + B s, and we can almos surely replace he inequaliy by a sric inequaliy. So P (M da, θ s) P (M s da, M s B s > N s ) P (M s da, M s B s > c N s dc) P (N s dc) c [, ) P (M s da, M s B s > c) P (N s dc) c [, ) P (M s da, M s W s db) P (N s dc) c [, ) b>c c da π s( s) da π s( s) (a + b) πs 3 da π exp( a ) exp( (a + b) s exp( (a + c) s s (c + a) exp( a s s c ) exp( π( s) ( s) )dbdcda c ) exp( ( s) )dc s( s) ) exp( a )dc exp( u )du 14

15 where we subsiued u respec o s, we ge s c+ a s( s) P (M da, θ ds) da π exp( a )(exp( (a c + a s. Differeniaing wih s( s) s s s ) da π exp( a )( ( s) a exp( a )ds) s ( s)s 3 a π ( s)s 3 exp( a s )dads To ge o he cumulaive disribuion of θ, we inegrae: P (θ s) P (M da, θ dr) s s r [,s] a [, ) a π ( r)r 3 exp( a r )dadr du π 1 u π arcsin where we subsiued u r. s Acknowledgmens s )ds) d s ds (a ) s dr π ( r)r The help and guidance my menor Yuan Shao provided was invaluable. He suggesed a opic which urned ou o be ineresing and useful, provided ineresing problems and insighful advice along he way, and was even willing o help me chug hrough some ugly inegrals. I would also like o he Universiy of Chicago REU for providing me wih a producive and fun summer doing mah. References [1] Peer Mörers and Yuval Peres, Brownian Moion, hp:// 15

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

5. Stochastic processes (1)

5. Stochastic processes (1) Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly

More information

Two Coupled Oscillators / Normal Modes

Two 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 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

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

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

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

Lecture Notes 2. The Hilbert Space Approach to Time Series

Lecture 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 information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 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 information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

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

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities: Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

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

T 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

T 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 information

Some Basic Information about M-S-D Systems

Some Basic Information about M-S-D Systems Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,

More information

Optimality Conditions for Unconstrained Problems

Optimality Conditions for Unconstrained Problems 62 CHAPTER 6 Opimaliy Condiions for Unconsrained Problems 1 Unconsrained Opimizaion 11 Exisence Consider he problem of minimizing he funcion f : R n R where f is coninuous on all of R n : P min f(x) x

More information

Martingales Stopping Time Processes

Martingales Stopping Time Processes IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765. Volume 11, Issue 1 Ver. II (Jan - Feb. 2015), PP 59-64 www.iosrjournals.org Maringales Sopping Time Processes I. Fulaan Deparmen

More information

4.6 One Dimensional Kinematics and Integration

4.6 One Dimensional Kinematics and Integration 4.6 One Dimensional Kinemaics and Inegraion When he acceleraion a( of an objec is a non-consan funcion of ime, we would like o deermine he ime dependence of he posiion funcion x( and he x -componen of

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

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15. SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

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

Effects of Coordinate Curvature on Integration

Effects of Coordinate Curvature on Integration Effecs of Coordinae Curvaure on Inegraion Chrisopher A. Lafore clafore@gmail.com Absrac In his paper, he inegraion of a funcion over a curved manifold is examined in he case where he curvaure of he manifold

More information

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions Muli-Period Sochasic Models: Opimali of (s, S) Polic for -Convex Objecive Funcions Consider a seing similar o he N-sage newsvendor problem excep ha now here is a fixed re-ordering cos (> 0) for each (re-)order.

More information

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

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance

More information

Integration Over Manifolds with Variable Coordinate Density

Integration Over Manifolds with Variable Coordinate Density Inegraion Over Manifolds wih Variable Coordinae Densiy Absrac Chrisopher A. Lafore clafore@gmail.com In his paper, he inegraion of a funcion over a curved manifold is examined in he case where he curvaure

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

Introduction to Probability and Statistics Slides 4 Chapter 4

Introduction to Probability and Statistics Slides 4 Chapter 4 Inroducion o Probabiliy and Saisics Slides 4 Chaper 4 Ammar M. Sarhan, asarhan@mahsa.dal.ca Deparmen of Mahemaics and Saisics, Dalhousie Universiy Fall Semeser 8 Dr. Ammar Sarhan Chaper 4 Coninuous Random

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

Markov Processes and Stochastic Calculus

Markov 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 information

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish 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 information

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates Biol. 356 Lab 8. Moraliy, Recruimen, and Migraion Raes (modified from Cox, 00, General Ecology Lab Manual, McGraw Hill) Las week we esimaed populaion size hrough several mehods. One assumpion of all hese

More information

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A

More information

Expert Advice for Amateurs

Expert Advice for Amateurs Exper Advice for Amaeurs Ernes K. Lai Online Appendix - Exisence of Equilibria The analysis in his secion is performed under more general payoff funcions. Wihou aking an explici form, he payoffs of he

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

More information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix 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 information

ES.1803 Topic 22 Notes Jeremy Orloff

ES.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 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

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

Lecture 33: November 29

Lecture 33: November 29 36-705: Inermediae Saisics Fall 2017 Lecurer: Siva Balakrishnan Lecure 33: November 29 Today we will coninue discussing he boosrap, and hen ry o undersand why i works in a simple case. In he las lecure

More information

arxiv: v1 [math.fa] 9 Dec 2018

arxiv: v1 [math.fa] 9 Dec 2018 AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse

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

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

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

GMM - Generalized Method of Moments

GMM - Generalized Method of Moments GMM - Generalized Mehod of Momens Conens GMM esimaion, shor inroducion 2 GMM inuiion: Maching momens 2 3 General overview of GMM esimaion. 3 3. Weighing marix...........................................

More information

Christos Papadimitriou & Luca Trevisan November 22, 2016

Christos Papadimitriou & Luca Trevisan November 22, 2016 U.C. Bereley CS170: Algorihms Handou LN-11-22 Chrisos Papadimiriou & Luca Trevisan November 22, 2016 Sreaming algorihms In his lecure and he nex one we sudy memory-efficien algorihms ha process a sream

More information

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature On Measuring Pro-Poor Growh 1. On Various Ways of Measuring Pro-Poor Growh: A Shor eview of he Lieraure During he pas en years or so here have been various suggesions concerning he way one should check

More information

Monochromatic Infinite Sumsets

Monochromatic Infinite Sumsets Monochromaic Infinie Sumses Imre Leader Paul A. Russell July 25, 2017 Absrac WeshowhahereisaraionalvecorspaceV suchha,whenever V is finiely coloured, here is an infinie se X whose sumse X+X is monochromaic.

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math 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 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

Families with no matchings of size s

Families with no matchings of size s Families wih no machings of size s Peer Franl Andrey Kupavsii Absrac Le 2, s 2 be posiive inegers. Le be an n-elemen se, n s. Subses of 2 are called families. If F ( ), hen i is called - uniform. Wha is

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

SPECTRAL 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. 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 information

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively: XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

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

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

= ( ) ) or a system of differential equations with continuous parametrization (T = R

= ( ) ) or a system of differential equations with continuous parametrization (T = R XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

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

Chapter 2. Models, Censoring, and Likelihood for Failure-Time Data

Chapter 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 information

An Excursion into Set Theory using a Constructivist Approach

An Excursion into Set Theory using a Constructivist Approach An Excursion ino Se Theory using a Consrucivis Approach Miderm Repor Nihil Pail under supervision of Ksenija Simic Fall 2005 Absrac Consrucive logic is an alernaive o he heory of classical logic ha draws

More information

The Arcsine Distribution

The Arcsine Distribution The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we

More information

An random variable is a quantity that assumes different values with certain probabilities.

An random variable is a quantity that assumes different values with certain probabilities. Probabiliy The probabiliy PrA) of an even A is a number in [, ] ha represens how likely A is o occur. The larger he value of PrA), he more likely he even is o occur. PrA) means he even mus occur. PrA)

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

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law Vanishing Viscosiy Mehod. There are anoher insrucive and perhaps more naural disconinuous soluions of he conservaion law (1 u +(q(u x 0, he so called vanishing viscosiy mehod. This mehod consiss in viewing

More information

BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS

BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS Elecronic Journal of Differenial Equaions, Vol. 18 (18, No. 8, pp. 1 13. ISSN: 17-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS JACEK

More information

ACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H.

ACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H. ACE 56 Fall 005 Lecure 5: he Simple Linear Regression Model: Sampling Properies of he Leas Squares Esimaors by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Inference in he Simple

More information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. 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 information

Echocardiography Project and Finite Fourier Series

Echocardiography Project and Finite Fourier Series Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let 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 information

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016 UNIVERSITÁ DEGLI STUDI DI PADOVA, DIPARTIMENTO DI MATEMATICA TULLIO LEVI-CIVITA Bernoulli numbers Francesco Chiai, Maeo Pinonello December 5, 206 During las lessons we have proved he Las Ferma Theorem

More information

Weyl sequences: Asymptotic distributions of the partition lengths

Weyl sequences: Asymptotic distributions of the partition lengths ACTA ARITHMETICA LXXXVIII.4 (999 Weyl sequences: Asympoic disribuions of he pariion lenghs by Anaoly Zhigljavsky (Cardiff and Iskander Aliev (Warszawa. Inroducion: Saemen of he problem and formulaion of

More information

We just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n

We just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n Lecure 3 - Kövari-Sós-Turán Theorem Jacques Versraëe jacques@ucsd.edu We jus finished he Erdős-Sone Theorem, and ex(n, F ) ( /(χ(f ) )) ( n 2). So we have asympoics when χ(f ) 3 bu no when χ(f ) = 2 i.e.

More information

ON THE DEGREES OF RATIONAL KNOTS

ON THE DEGREES OF RATIONAL KNOTS ON THE DEGREES OF RATIONAL KNOTS DONOVAN MCFERON, ALEXANDRA ZUSER Absrac. In his paper, we explore he issue of minimizing he degrees on raional knos. We se a bound on hese degrees using Bézou s heorem,

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

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013 IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher

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

Lecture 10: The Poincaré Inequality in Euclidean space

Lecture 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 information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

Sections 2.2 & 2.3 Limit of a Function and Limit Laws Mah 80 www.imeodare.com Secions. &. Limi of a Funcion and Limi Laws In secion. we saw how is arise when we wan o find he angen o a curve or he velociy of an objec. Now we urn our aenion o is in general

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

Some Ramsey results for the n-cube

Some Ramsey results for the n-cube Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

Mixing times and hitting times: lecture notes

Mixing times and hitting times: lecture notes Miing imes and hiing imes: lecure noes Yuval Peres Perla Sousi 1 Inroducion Miing imes and hiing imes are among he mos fundamenal noions associaed wih a finie Markov chain. A variey of ools have been developed

More information

Instructor: Barry McQuarrie Page 1 of 5

Instructor: Barry McQuarrie Page 1 of 5 Procedure for Solving radical equaions 1. Algebraically isolae one radical by iself on one side of equal sign. 2. Raise each side of he equaion o an appropriae power o remove he radical. 3. Simplify. 4.

More information

18 Biological models with discrete time

18 Biological models with discrete time 8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so

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

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN Inernaional Journal of Scienific & Engineering Research, Volume 4, Issue 10, Ocober-2013 900 FUZZY MEAN RESIDUAL LIFE ORDERING OF FUZZY RANDOM VARIABLES J. EARNEST LAZARUS PIRIYAKUMAR 1, A. YAMUNA 2 1.

More information

Chapter 7: Solving Trig Equations

Chapter 7: Solving Trig Equations Haberman MTH Secion I: The Trigonomeric Funcions Chaper 7: Solving Trig Equaions Le s sar by solving a couple of equaions ha involve he sine funcion EXAMPLE a: Solve he equaion sin( ) The inverse funcions

More information

E β t log (C t ) + M t M t 1. = Y t + B t 1 P t. B t 0 (3) v t = P tc t M t Question 1. Find the FOC s for an optimum in the agent s problem.

E β t log (C t ) + M t M t 1. = Y t + B t 1 P t. B t 0 (3) v t = P tc t M t Question 1. Find the FOC s for an optimum in the agent s problem. Noes, M. Krause.. Problem Se 9: Exercise on FTPL Same model as in paper and lecure, only ha one-period govenmen bonds are replaced by consols, which are bonds ha pay one dollar forever. I has curren marke

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

ACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H.

ACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H. ACE 56 Fall 5 Lecure 8: The Simple Linear Regression Model: R, Reporing he Resuls and Predicion by Professor Sco H. Irwin Required Readings: Griffihs, Hill and Judge. "Explaining Variaion in he Dependen

More information

10. State Space Methods

10. 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 information

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information

Two Popular Bayesian Estimators: Particle and Kalman Filters. McGill COMP 765 Sept 14 th, 2017

Two Popular Bayesian Estimators: Particle and Kalman Filters. McGill COMP 765 Sept 14 th, 2017 Two Popular Bayesian Esimaors: Paricle and Kalman Filers McGill COMP 765 Sep 14 h, 2017 1 1 1, dx x Bel x u x P x z P Recall: Bayes Filers,,,,,,, 1 1 1 1 u z u x P u z u x z P Bayes z = observaion u =

More information

arxiv: v2 [math.ap] 16 Oct 2017

arxiv: v2 [math.ap] 16 Oct 2017 Unspecified Journal Volume 00, Number 0, Pages 000 000 S????-????XX0000-0 MINIMIZATION SOLUTIONS TO CONSERVATION LAWS WITH NON-SMOOTH AND NON-STRICTLY CONVEX FLUX CAREY CAGINALP arxiv:1708.02339v2 [mah.ap]

More information

Class Meeting # 10: Introduction to the Wave Equation

Class 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 information

Lecture 4 Notes (Little s Theorem)

Lecture 4 Notes (Little s Theorem) Lecure 4 Noes (Lile s Theorem) This lecure concerns one of he mos imporan (and simples) heorems in Queuing Theory, Lile s Theorem. More informaion can be found in he course book, Bersekas & Gallagher,

More information