Copyright by Tianran Geng 2017

Size: px
Start display at page:

Download "Copyright by Tianran Geng 2017"

Transcription

1 Copyrigh by Tinrn Geng 207

2 The Disserion Commiee for Tinrn Geng cerifies h his is he pproved version of he following disserion: Essys on forwrd porfolio heory nd finncil ime series modeling Commiee: Thlei Zriphopoulou, Supervisor Rfel Mendoz-Arrig Mihi Sîrbu Sephen Wlker Gordn Žiković

3 Essys on forwrd porfolio heory nd finncil ime series modeling by Tinrn Geng, B.S., M.A. DISSERTATION Presened o he Fculy of he Grdue School of The Universiy of Texs Ausin in Pril Fulfillmen of he Requiremens for he Degree of DOCTOR OF PHILOSOPHY THE UNIVERSITY OF TEXAS AT AUSTIN My 207

4 Dediced o my moher.

5 Acknowledgmens Firs, I wish o express my sincere griude o my supervisor, Professor Thlei Zriphopoulou, for her guidnce nd suppor during my grdue sudies. Her words of wisdom nd srong work ehic hve been consn source of inspirion nd moivion for me. I would lso like o cknowledge he members of my disserion commiee: Professors Rfel Mendoz-Arrig, Mihi Sîrbu, Sephen Wlker, nd Gordn Žiković, for heir ime nd dvice. I m greful for he suppor nd ssisnce I hve received over he yers from he fculy nd sff he Deprmen of Mhemics, in priculr, Elis Bss, Sndr Cle, Ev Hernndez, nd Professor Dn Knopf. Finlly, I hnk ll my friends nd collegues for heir friendship. I m forever indebed o my moher, Huiln Wng, for her uncondiionl love nd suppor hrough he yers. This disserion is dediced o her. v

6 Essys on forwrd porfolio heory nd finncil ime series modeling Publicion No. Tinrn Geng, Ph.D. The Universiy of Texs Ausin, 207 Supervisor: Thlei Zriphopoulou This disserion conins four self-conined essys h explore he pplicion of sochsic nd sisicl modeling echniques o he problem of opiml porfolio choice nd finncil ime series nlysis. The firs essy presens urnpike-ype resuls for he risk olernce funcion in n incomplee Iô-diffusion mrke seing under ime-monoone forwrd performnce crieri. We show h, conrry o he clssicl cse, he emporl nd spil limis do no coincide. Rher, we esblish h hey depend direcly on he lef- nd righ-end of he suppor of n underlying mesure, used o consruc he forwrd performnce crierion. We provide exmples wih discree nd coninuous mesures, nd discuss he sympoic behvior of he risk olernce for ech cse. The second essy exmines he long erm behvior of he opiml welh nd opiml porfolio weighs processes in n Iô-diffusion mrke under he vi

7 ime-monoone forwrd performnce crieri. We show h he underlying mesure µ ssocied wih he forwrd performnce crierion defines he risk profile of he invesor, nd in urn deermines he opiml porfolio sregy nd opiml welh in he long run. The hird essy considers wo fund mngers who rde under relive performnce concerns, depending on ech oher s sregies, in n Iô-diffusion mrke, We nlyze boh he pssive nd he compeiive cses, nd under boh sse specilizion nd diversificion. To llow for dynmic model revision nd flexible invesmen horizons, we inroduce he concep of relive forwrd performnce for he pssive cse, nd he noion of forwrd Nsh equilibrium for he compeiive one. For homoheic forwrd crieri, we provide explici soluions for ll cses. In he fourh essy, we ssess he dynmics of relized bes, relive o he dynmics in he underlying mrke vrince nd covrinces wih he mrke, using 5-minue high-frequency sse prices of he DJIA componen socks from Jnury, 200 o December 3, 204. We find h, unlike he relized vrinces nd covrinces which flucue widely nd re highly persisence, he relized be series, on he oher hnd, disply much less persisence. We hen consruc simple uoregressive plus noise DLM ime series model for he relized be, where he mesuremen error follows norml disribuion cenered zero wih sympoiclly vlid vrince given in [7]. This pproch helps us obin smples from filered nd smoohed rue underlying be series nd forecs fuure bes. vii

8 Tble of Conens Acknowledgmens Absrc Lis of Tbles Lis of Figures v vi xi xii Chper. Temporl nd spil urnpike-ype resuls under forwrd ime-monoone performnce crieri. Inroducion The model nd he invesmen performnce crierion A moiving exmple Spil sympoic resuls Temporl (urnpike) sympoic resuls Spil nd emporl limis for he relive prudence funcion Exmples Finie sum of Dirc funcions Temporl sympoic expnsion of h ( ) (x 0, ) for lrge Spil sympoic expnsion of h ( ) (x, 0 ) for lrge x Spil nd emporl sympoics of r(x, ) Lebesgue mesure Temporl sympoic expnsion of h ( ) (x 0, ) for lrge Spil sympoic expnsion of h ( ) (x, 0 ) for lrge x Spil sympoics of r(x, 0 ) for lrge x Exensions viii

9 Chper 2. On he opiml welh nd porfolio weighs processes under ime-monoone forwrd performnce crieri in n Iô-diffusion mrke Inroducion The model nd he invesmen performnce crierion Long erm behvior of opiml welh process Long erm behvior of opiml porfolio weighs process Chper 3. Pssive nd compeiive invesmen sregies under relive forwrd performnce crieri Inroducion Asse specilizion nd forwrd relive performnce crieri Forwrd relive performnce crieri The CRRA cse Forwrd Nsh equilibrium The CRRA cse Diversificion (no sse specilizion) nd relive forwrd performnce crieri Pssive forwrd performnce crieri The CRRA cse Forwrd Nsh equilibrium The CRRA cse Exensions Chper 4. Modeling relized be ime series using high-frequency inr-dy sse prices Inroducion Theoreicl frmework Empiricl nlysis DLM frmework Sep : prior specificions nd sufficien sisics Sep 2: FFBS Empiricl nlysis Conclusion Tbles nd figures ix

10 Appendix 33 Bibliogrphy 42 x

11 Lis of Tbles 4. The Dow Jones Thiry The Dynmics of Monhly Relized Mrke Vrince, Covrinces, nd Bes xi

12 Lis of Figures 4. Time Series Plo of Monhly Relized Mrke Vrince Voliliy Index (VIX) of S&P Time Series Plos of Monhly Relized Covrinces Time Series Plos of Monhly Relized Bes Smple Auocorrelions of Monhly Relized Mrke Vrince, Medin Smple Auocorrelions of Monhly Relized Covrinces, nd Medin Smple Auocorrelions of Monhly Relized Bes Smple Auocorrelions of Monhly Relized Covrinces Smple Auocorrelions of Monhly Relized Bes % Confidence Inervls for Monhly Be, Five-minue Smpling % Confidence Inervls for Monhly Be of BA/IBM/DD, Five-minue Smpling % Confidence Inervls for Qurerly Be of BA/IBM/DD, Dily Smpling Smples from Poserior Disribuion of, b, nd σ 2 for Monhly Relized Be of IBM Time Series Plo of Medin Smoohed Smples nd Acul Relizion for Monhly Relized Be for IBM Time Series Plo of Medin Smoohed Smples nd 95% Confidence Bnds for Monhly Relized Be for IBM Forecsing Phs for he Nex 2 Monhs of Monhly Relized Be for IBM nd heir 95% Confidence Inervl xii

13 Chper Temporl nd spil urnpike-ype resuls under forwrd ime-monoone performnce crieri. Inroducion Turnpike resuls in mximl expeced uiliy models yield he behvior of opiml porfolio funcions when he invesmen horizon is long, under sympoic ssumpions on he invesor s risk preferences. The essence of he urnpike resul (sed, for simpliciy, for single log-norml sock wih coefficiens µ nd σ) is he following: ssume h he invesmen horizon is [0, T ] nd h he invesor s uiliy U T behves like power funcion for lrge welh levels, i.e., U T (x) γ xγ, x lrge. (.) Then, if his horizon is very long, he ssocied opiml porfolio funcion π (x, ; T ) is close o he one corresponding o his power uiliy, i.e., for ech x > 0, [0, T ], π (x, ; T ) x µ, T lrge. (.2) σ 2 γ

14 In oher words, he sympoic spil behvior of he erminl dum dices he long-erm emporl behvior of he porfolio funcion for every welh level. We recll h he funcion π (x, ; T ) is he one he deermines he opiml welh process in feedbck form, in h he opiml welh process X, [0, T ], is genered by he invesmen sregy π = π (X, ; T ). Turnpike resuls cn be found in [20] where coninuous-ime model ws firs considered, nd he urnpike properies were esblished using coningen clim mehods. Their resuls were ler exended in [35] using n uonomous equion h he funcion π (x, ; T ) sisfies nd rgumens from viscosiy soluions. Duliy mehods were used in [22] for complee mrkes nd he incomplee mrke cse ws sudied in [33]. More recenly, he uhors of [] esblished he re of convergence in log-norml model, showing h here exis posiive consn c nd funcion D (x), such h, for ll x > 0, π (x, ; T ) µ σ 2 γ x D (x) e c(t ). A closer look hese urnpike resuls yields h we re essenilly working in single invesmen horizon seing, [0, T ], which is ken o be very long. As resul, however, one needs o commi o mrke model for his long horizon, bu his choice cnno be modified ler on, if ime-consisency is desired. Furhermore, one pre-commis iniil ime o uiliy funcion for very fr in he fuure, T. We lso remrk h no mer how big T is, 2

15 he opiml invesmen problem is no defined beyond his poin, becuse he uiliy funcion is given for T only. Herein, we ke n lernive poin of view. Insed of commiing o single long horizon [0, T ], we define n invesmen problem for ll imes [0, ). Moreover, insed of choosing n iniil ime he uiliy U T for he remoe horizon T, we choose he uiliy his iniil ime. We lso depr from he log-norml seing nd work wih generl Io-diffusion mulisecuriy incomplee mrke model. We mesure he performnce of invesmen sregies vi he so-clled forwrd invesmen performnce crierion. This crierion ws inroduced by Musiel nd one of he uhors in [55] nd offers flexibiliy for performnce mesuremen nd risk mngemen under model dpion nd mbiguiy, lernive mrke views, rolling horizons, nd ohers. We recll is definiion nd refer he reder o, mong ohers, [57], [59], for n overview of he forwrd pproch. Herein, we focus on he clss of ime-monoone forwrd performnce crieri, sudied in [58] nd briefly reviewed in he nex secion. They re given by ime-decresing nd dped o he mrke informion process, U (x, ), (x, ) R + [0, ), of he form U (x, ) = u (x, A ), where u (x, ) is deerminisic funcion (see (.4)) nd A wih he process λ being he mrke price of risk. = 0 λ s 2 ds, Noe h U (x, ) is 3

16 compilion of deerminisic invesor-specific inpu, u (x, ), nd sochsic mrke-specific inpu, A. The opiml invesmen process π urns ou o be, for 0, π = σ + λ r (X, A ) wih r (x, ) := u x (x, ) u xx (x, ), (.3) where σ + is he pseudo-inverse of he voliliy mrix, nd X, 0, he opiml welh genered by his invesmen sregy π (cf. (.2)). The funcion r (x, ) is he (locl) risk olernce nd will be he min objec of sudy herein. Conrry o he clssicl cse, in which erminl dum is pre-ssigned for T nd he soluion is hen consruced for [0, T ), in he forwrd seing, he crierion is defined for ll imes, sring wih n iniil (nd no erminl) dum u 0 (x) = U (x, 0). In nlogy o he clssicl urnpike seing, we re hus moived o sudy he following quesion: if he iniil condiion u 0 (x) is such h u 0 (x) γ xγ, x lrge, (.4) does his imply h, for ech x > 0, r(x, ) x γ, lrge? There re fundmenl differences beween he clssicl nd he forwrd seings, for one is no mere vriion of he oher by ime reversl. Rher, he clssicl problem is well-posed while he forwrd is n inverse problem. 4

17 Nurlly, vrious properies used for he clssicl urnpike resuls fil, wih he mos imporn being he lck of comprison principle for vrious PDEs (cf. (.4) nd (.22)) hnd. The firs sriking difference beween he wo seings is he disinc nure of he emporl nd spil limis. Indeed, in he rdiionl urnpike resuls in [35] nd [], he emporl limi in (.2) coincides wih he spil one, in h for fixed ime T 0 nd welh level x 0, π (x, ; T 0 ) lim x x = lim T π (x 0, ; T ) x 0. However, his is no he cse in he forwrd seing. Indeed, he emporl nd spil limis of he funcion r(x,) x do no coincide. This cn be seen, for insnce, in he moivionl exmple in secion 2.. limis The im herein hen becomes he sudy of he spil nd emporl r(x, 0 ) lim x x nd r(x 0, ) lim, (.5) x for fixed 0 > 0, x 0 > 0, respecively, under pproprie condiions for he sympoic behvior of he iniil dum u 0 (x), for lrge x. Pivol role for deermining hese limis is plyed by n underlying posiive finie Borel mesure, µ, which is he defining elemen for he consrucion of he forwrd performnce process. Indeed, i ws shown in [58] h he bove funcion u is uniquely (up o n ddiive consn) reled o hrmonic funcion h : R [0, ) R +, nd, furhermore, he ler is 5

18 uniquely chrcerized by n inegrl rnsform, specificlly, u x (h (z, ), ) = e x+ 2 wih h (z, ) = for 0 b. b e zy 2 y2 µ (dy), (.6) An immedie consequence of his generl soluion is h he iniil dum is direcly reled o his mesure µ, in h (u 0) ( ) needs o be of he inegrl form (u 0) ( ) (x) = b x y µ (dy). As resul, i is nurl o expec h he sympoic properies of u 0 (x), which ener in he urnpike ssumpions, re lso direcly linked o he form nd properies of µ. Furhermore, his mesure lso ppers in he specificion of he risk olernce funcion. Indeed, we deduce from (.3) nd (.6) h r (x, ) cn be represened s wih boh h x nd h ( ) depending on µ. r (x, ) = h x ( h ( ) (x, ), ), (.7) The min resuls herein re h, if he suppor of he mesure is finie, b <, hen he spil limi coincides wih he righ-end poin of he suppor while he emporl limi wih he lef-end one, nmely, r(x, 0 ) lim x x = b nd lim r(x 0, ) x =. (.8) The firs sep in obining he bove limis is o undersnd he connecion beween he sympoic behvior of he iniil (mrginl) dum nd he 6

19 finieness of he mesure s suppor. We sudy he following wo cses, which correspond o he spil nd emporl limis, respecively. he mrginl, We firs show h he sympoic ssumpion (.4), sed in erms of u 0 (x) x γ, (.9) if nd only if he righ end of he mesure s suppor sisfies boh b = γ nd µ ({b}) =. In oher words, condiion (.9) implies h he mesure mus hve finie suppor wih is righ boundry equl o γ nd, furhermore, wih mss his poin. Conversely, for he mesure o hve hese properies, condiion (.9) mus hold. We hen esblish he firs limi in (.8) using represenion (.6), he equion (.4) sisfied by u (x, ), nd vrious convexiy properies of h nd is derivives. We sress h he requiremen h µ ({b}) 0 cnno be relxed. Indeed, we show in Exmple 6.2, where he mesure is he Lebesgue one, h he spil urnpike propery fils. For he second cse, we rele he finieness of he mesure s suppor wih relxed version of (.9). We show h if here exiss γ <, γ 0, such h for ll γ (γ, ) nd γ < γ, u 0 (x) lim x x γ u 0 (x) = 0 nd lim x x γ =, (.0) hen he righ boundry of he mesure s suppor mus sisfy b = γ, nd vice-vers. This regulr vriion ssumpion is weker hn (.9), needed for he spil limi nd, nurlly, yields weker resul. Indeed, while he 7

20 suppor hs o be finie wih righ boundry equl o, i does no need o γ hve mss γ. We in urn esblish he second limi in (.8), which is he genuine nlogue of he clssicl urnpike resul. Obining his limi is considerbly more chllenging hn in he clssicl cse due o he ill-posed nure of he problem. Indeed, he mehodology used in [35] is inpplicble becuse of lck of comprison resuls for he ergodic version of he equion sisfied by r (x, ). The pproch of [] does no pply eiher becuse of he lck of connecion beween he soluions of he ill-posed he equion nd Feynmn-Kc ype sochsic represenion of is soluion. Therefore, one needs o work direcly wih he funcion r (x, ), which, from (.7) nd (.6), is given in he implici form r (x, ) = b ye yh( ) (x,) 2 y2 µ (dy), where however he spil inverse h ( ) is involved. The key sep in obining he emporl limi is o show h h ( ) (x, ) lim = 2, where is he lef end poin of he mesure s suppor. Then he emporl convergence in (.8) nd he re of convergence is shown using he implici represenion r (x, ) x = b ( ) (y ) e y h ( ) (x,) 2 y µ (dy). In ddiion o he generl spil nd emporl convergence resuls, we presen wo represenive exmples. In he firs, he mesure is finie sum 8

21 of Dirc funcions while, in he second, i is ken o be he Lebesgue mesure. We clcule he limis of (.8), nd lso provide sympoic expnsions for he risk olernce funcion. The pper is srucured s follows. In secion 2, we presen he mrke model, he invesmen performnce crierion nd moiving exmple demonsring h he emporl nd spil limis do no in generl coincide. In secions 3 nd 4, we nlyze respecively he spil nd emporl sympoic behvior of he relive risk olernce, while in secion 5 we nlyze he sympoic properies of he relive prudence funcion. In secion 6 we presen he wo represenive exmples, nd conclude in secion 7 wih fuure reserch direcions..2 The model nd he invesmen performnce crierion The mrke environmen consiss of one riskless nd k risky securiies. The prices of he risky securiies re modelled s Iô processes, nmely, he price S i of he i h risky sse follows ds i = S i ( ) µ i d + Σ d j=σ ji dw j, wih S0 i > 0, for i =,..., k. The process W = ( ) W,..., W d, 0, is sndrd Brownin moion, defined on filered probbiliy spce (Ω, F, P). The coefficiens µ i nd σ i = ( ) σ i,..., σ di, i =,..., k, 0, re F dped processes nd vlues in R nd R d, respecively. We denoe by σ he voliliy 9

22 mrix, i.e. he d k rndom mrix ( ) σ ji, whose i h column represens he voliliy σ i of he i h sse. We my, hen, lernively, wrie he bove equion s ds i = S i ( µ i d + σ i dw ). The riskless sse, he svings ccoun, hs price process B sisfying db = r B d wih B 0 =, nd for nonnegive F dped ineres re process r. Also, we denoe by µ he k-dimensionl vecor wih coordines µ i nd by he k-dim vecor wih every componen equl o one. The processes µ, σ nd r sisfy he pproprie inegrbiliy condiions. We ssume h µ r Lin ( σ T ), where Lin ( σ T ) denoes he liner spce genered by he columns of σ T. Therefore, he equion σ T z = µ r hs soluion, known s he mrke price of risk, λ = ( σ T ) + (µ r ). (.) I is ssumed h here exiss deerminisic consn c > 0, such h λ c nd h lim 0 λ s 2 ds =. Sring = 0 wih n iniil endowmen x 0, he invesor invess ny ime > 0 in he risky nd riskless sses. The presen vlue of he mouns invesed re denoed by he processes π 0 nd π, i i =,..., k, respecively, which re ken o be self-finncing. The presen vlue of her invesmen is hen given by he discouned welh process X π = π, i > 0, which solves dx π = σ π (λ d + dw ) (.2) 0

23 wih he (column) vecor π = (π i ; i =,..., k). I is ken o sisfy he nonnegiviy consrin X π 0, > 0. The se of dmissible policies is given by A = {π : self-finncing, π F, E P 0 } σ s π s 2 ds <, X π 0, > 0. The performnce of dmissible invesmen sregies is evlued vi he soclled forwrd invesmen performnce crieri, inroduced in [55] (see, lso [56], [57] nd [59]). We review heir definiion nex. [0, ). We inroduce he domin noion D + = R + [0, ) nd D = R Definiion.2.. An F -dped process U(x, ) is forwrd invesmen performnce if for (x, ) D, i) he mpping x U(x, ) is sricly incresing nd sricly concve; ii) for ech π A, E P (U(X π, )) + <, nd for s, U (X π, ) E P (U(X π s, s) F ), iii) here exiss π A such h for s, U ( X π, ) ( = E P U(X π s, s) ) F. Herein we focus on he clss of ime-monoone forwrd performnce processes. For he reder s convenience, we rewrie some of he resuls we

24 sed in he inroducion. Time-monoone forwrd processes were exensively sudied in [58], nd re given by U(x, ) = u(x, A ), (.3) where u : D + R + is sricly incresing nd sricly concve in x, sisfying u 2 x u =. (.4) 2 u xx The mrke inpu processes A nd M, 0, re defined s M = 0 λ s dw s nd A = 0 λ s 2 ds = M. (.5) The opiml porfolio process π is given by π = σ + λ r(x, A ), where he (locl) risk olernce funcion r (x, ) : D + R + is defined s r (x, ) := u x (x, ) u xx (x, ). (.6) Cenrl role in he consrucion of he performnce crierion, he opiml policies nd heir welh plys hrmonic funcion h : D R +, defined vi he rnsformion u x (h(z, ), ) = e z+ 2. (.7) I solves, s i follows from (.4) nd (.7), he ill-posed he equion h + 2 h zz = 0. (.8) Moreover, i is posiive nd sricly incresing in z. I ws shown in [58], h such soluions re uniquely represened by h(z, ) = b e yz 2 y2 ν(dy) + C, y 2

25 where = 0 + or > 0, b nd C generic consn. The mesure ν is defined on B + (R), he se of posiive Borel mesures, wih he ddiionl properies h, for z R, b eyz ν(dy) < nd b ν(dy) < y. To simplify he presenion nd wihou loss of generliy, we choose C := b ν(dy) nd, lso, inroduce he normlized mesure µ (dy) = ν(dy). y y Then, he funcion h hs, for (z, ) D, he represenion h(z, ) = b wih b yeyz µ(dy) <, = 0 +, > 0, b. e yz 2 y2 µ(dy), (.9) We esily deduce h for ech 0 0, he funcion h (., 0 ) is bsoluely monoonic, since i h (z, 0 ) / z i > 0, i =, 2... Such funcions sisfy, for ech 0 0, i =, 2,..., he inequliy i+ h (z, 0 ) i h (z, 0 ) z i+ z i ( ) i 2 h (z, 0 ) > 0. (.20) From (.7), (.6) nd (.9), we obin h he risk olernce funcion is represened s r(x, ) = h z ( h ( ) (x, ), ) = b z i ye yh( ) (x,) 2 y2 µ(dy). (.2) Furhermore, he firs equliy ogeher wih (.8) yields h i sisfies he (ill-posed) non-liner equion wih r(x, 0) = b yeyh( ) (x,0) µ(dy). r + 2 r2 r xx = 0, (.22) 3

26 We lso hve h r x (x, ) = h ( zz h ( ) (x, ), ) r (x, ) = r (x, ) b y 2 e yh( ) (x,) 2 y2 µ(dy) > 0. (.23) Furhermore, r xx (x, ) = where we used (.20). ( hzzz (z, ) h r 3 z (z, ) h zz (z, ) 2) (x, ) z=h > 0, (.24) ( ) (x,) We noe h we will frequenly differenie under he inegrl sign in (.9), which is permied s explined in [58]. I cn be lso seen direcly since, fer differeniion, one cn show h he relevn inegrnds re joinly coninuous in heir respecive rgumens nd hus uniformly loclly inegrble. This llows us o differenie under he inegrl sign (see, for exmple, Theorem 24.5 in [3] nd he remrks following i). As sed in he inroducion, he im herein is o invesige he spil nd emporl limis in (.5), wih r (x, ) s in (2.3) when he mesure hs finie suppor. We firs provide n exmple which shows h, conrry o he clssicl cse, hese wo limis do no in generl coincide..2. A moiving exmple Le he underlying mesure µ be Dirc funcion, γ <. From γ (.9) nd (.7) we hve h, for 0, h(x, ) = e γ x 2( γ ) 2 nd u x (x, ) = x γ e γ 2( γ). 4

27 Therefore, he locl risk olernce funcion is given by r(x, ) = γ x nd hus he spil nd emporl limis coincide, r(x, 0 ) lim x x for fixed 0, x 0 respecively. = γ nd r(x 0, ) lim = x 0 γ, Nex, le he mesure µ be he sum of wo Dirc funcions poins = θ nd b = γ µ = δ θ such h b = 2, wih 0 < θ < nd γ <, i.e., + δ γ wih Then, (.9) nd (.7) yield h h(x, 0) = e θ x + e γ x, γ = 2 θ. (.25) u x (x, 0) = 2 θ ( + 4x ) θ nd u ( ) x (x, 0) = x θ + x γ. In urn, u x (x, 0) lim x x γ Moreover, expression (.9) gives, for > 0, h(x, ) = e (.26) ( ) 2 2( γ) 2(γ ) + 4x = lim =. (.27) x x γ θ x 2 ( θ) 2 + e 2 θ x 2 2 ( θ) 2, nd, hus, h ( ) (x, ) = e ( θ) 2 + 4x e ( + ( θ) ln θ 2 θ) 2 In urn, rnsformion (.7) yields ( γ u x (x, ) = 2 θ e ( 2 θ ) e ( θ) 2 + 4x e ( θ) ) 2.. (.28) 5

28 Differeniing he bove o obin u xx (x, ) (or using (.9), (.28) nd (2.3)), we deduce h he risk olernce funcion is given by r(x, ) = x 4x + e ( θ) 2 γ e. (.29) ( θ )2 + 4x + e ( θ )2 Therefore, for ech 0 0, while, for ech x 0 > 0, r(x, 0 ) lim x x = 2 θ = γ. (.30) r(x 0, ) lim = x 0 θ. (.3) Therefore, he spil nd emporl limis do no coincide. Nex, we mke he following wo imporn observions. Firsly, noe h (.25) yields h he suppor of he mesure is supp (µ) = { } θ,. γ Therefore, he spil limi coincides wih he righ-end of he suppor while he emporl limi wih he lef-end one. Secondly, for ech x 0 > 0 he emporl limi of he rio h( ) (x 0,) equl o hlf of he lef-end poin, since (.28) yields is h ( ) (x 0, ) lim ( = lim θ + θ ( ( ln e ( θ )2 + 4x 2 e ( θ )2 ))) = 2 ( θ). 6

29 In secion 4 we will show h hese wo properies re lwys vlid. In priculr, we will see h i is he limi of he bove rio h plys he key role in esblishing he emporl urnpike limi for generl mesures. To juxpose he bove resuls wih he ones in he rdiionl expeced erminl uiliy seing, we compue he nlogous quniies nd ssocied limis for he cses nlyzed in [35] nd [] for log-norml mrkes. Wihou loss of generliy, we consider mrke wih riskless bond of zero ineres re nd single log-norml sock wih men re of reurn µ nd voliliy σ. To his end, we fix n rbirry horizon T > 0 nd, in nlogy o (.26), we ke he erminl inverse mrginl uiliy, I (x) = (U ) ( ) (x), o be I (x) = x θ + x γ, for x > 0 nd θ, γ s in (.25). This corresponds o erminl mrginl uiliy ( +4x ) θ U (x) = nd, hus, in nlogy o (.27), 2 U (x) lim =. x x γ We now consider he vlue funcion, sy u (x, ; T ) of he ssocied Meron problem, for [0, T ]. Leing τ = T be he ime o he end of he invesmen horizon, we deduce, using well known resuls, h he funcion ũ (x, τ) u (x, T ; T ), sisfies, for (x, τ) R + [0, T ), he Hmilon- Jcobi-Bellmn equion ũ τ + 2 λ2 ũ2 x ũ xx = 0. 7

30 The inverse spil mrginl vlue funcion ṽ : R + [0, T ) R + hen solves ṽ τ = 2 λ2 x 2 ṽ xx + λ 2 xṽ x, wih ṽ(x, 0) = I (x). We esily deduce h ṽ(x, τ) = e ατ x α + e βτ x 2α, wih α = 2 λ2 θ nd β = λ 2 +θ. Noe h β > 2α. ( θ) 2 ( θ) 2 Tking he spil inverse of ṽ(x, τ) yields ũ x (x, τ) = ( e ατ + e 2ατ + 4xe βτ 2x ) θ. Therefore, he ssocied risk olernce funcion is given by r(x, τ) = θ 2x + + 4xe + 8x 2 ( (β 2α)τ e (2α β)τ + 2. e (2α β)τ + 4x) In urn, for ech τ 0 > 0 nd x 0 > 0, we obin, respecively, he spil nd he emporl limis, r(x, τ 0 ) lim x x = θ nd r(x 0, τ) lim = τ x 0 θ..3 Spil sympoic resuls We exmine he spil sympoic behvior of he risk olernce funcion s x, for ech 0 0, under sympoic ssumpions for lrge welh levels of he invesor s iniil risk preferences. In ccordnce wih similr 8

31 ssumpions in [35] nd [], we impose his sympoic ssumpion on he mrginl u 0 (x) insed of he funcion iself. Assumpion : The iniil dum u 0 sisfies, for some γ <, lim x u 0(x) =. (.32) xγ The nex resul yields necessry nd sufficien condiions on b, he righ end of he suppor of he mesure, for he bove ssumpion o hold. Lemm.3.. Assumpion (.32) holds if nd only if he ssocied mesure µ sisfies b = γ ({ }) nd µ =. (.33) γ Proof. From (.32), (.7) nd he fc h h(x, 0) is sricly incresing nd of full rnge, we hve = lim x u x (x, 0) x γ = lim z u x (h(z, 0), 0) (h(z, 0)) γ Therefore, represenion (.9) gives lim z b = lim z ( ) γ h(z, 0). (.34) e γ z e z(y γ ) µ(dy) =. (.35) If = b, hen (.33) follows direcly. If < b, hen, i mus be h γ, oherwise, we ge conrdicion. In urn, for ε > 0, b b ( e z(y γ ) µ(dy) e z(y γ ) µ(dy) e εz µ [ γ +ε γ ) + ε, b]. (.36) 9

32 Sending ε 0 nd using (.35) yield h µ((, b]) = 0, nd hus, supp(µ) γ (, ]. Moreover, we hve from (.35) h γ ( γ ) = lim e z(y γ ) µ(dy) + µ({ }) = µ({ z γ γ }), nd we conclude. The res of he proof follows esily. We nex se he min spil sympoic resul. Proposiion.3.. Suppose h he iniil dum u 0 sisfies he sympoic propery (.32). Then, for ech 0 0, he relive risk olernce converges o he righ-end of he suppor of he mesure µ, r(x, 0 ) lim x x = γ. (.37) Proof. Le 0 0. From represenion (.36) we hve h h (z, 0 ) = ( γ ) e zy 2 0y 2 µ(dy) + e γ z 2( γ ) 2 0, nd, in urn, he domined convergence heorem implies lim z h(z, 0 ) e γ z 2( γ ) 2 0 =. (.38) Therefore, from (.7), ogeher wih he sric monooniciy nd full rnge of h(z, 0 ), we deduce h since lim x lim x u x (x, 0 ) x γ e γ 2( γ) 0 u x (x, 0 ) x γ e = lim z γ 2( γ) 0 =, (.39) e z+ 02 h γ (z, 0 )e γ 2( γ) 0 20

33 Nex, we clim h = lim z lim x ( h(z, 0 ) e γ z 2( γ ) 2 0 u xx (x, 0 ) x γ 2 e γ 2( γ) 0 ) γ =. = γ. (.40) To prove his, i suffices o show h for ny 0 0, u x (x, 0 ) is convex since he bove would hen follow from he rgumens in Lemm 3. (ii) in [35]. To his end, differeniing (.7) yields u xxx (h(z, 0 ), 0 ) (h z (z, 0 )) 2 + u xx (h(z, 0 ), 0 )h zz (z, 0 ) = e z (.4) The sric convexiy of h nd he sric concviy of u hen give u xxx (h(z, 0 ), 0 ) > 0, (.42) nd using he sric monooniciy nd full rnge of h we conclude. Combining (.39) nd (.40) yields = lim x ( r(x, 0 ) lim x x u x(x, 0 ) x γ e γ 2( γ) 0 ( = lim u ) x(x, 0 ) x xu xx (x, 0 ) ( ) ) uxx (x, 0 ) x γ 2 e γ 2( γ) 0 = γ. We sress h ssumpion (.32), or equivlenly (.33), cnno be wekened. Indeed, s we will see in exmple 6.2, where we ke he mesure o be he Lebesgue on [, b], nd hus here is no mss b, he spil urnpike propery does no hold. 2

34 Corollry.3.. Suppose h he iniil dum u 0 sisfies he sympoic propery (.32). Then, for ech 0 0, lim r x (x, 0 ) = x γ. (.43) Proof. From (.24) we hve h, for ech 0 0, lim x r x (x, 0 ) exiss, nd we esily conclude..4 Temporl (urnpike) sympoic resuls We invesige he emporl sympoic behvior of he relive risk olernce s, for ech x 0 > 0, under sympoic ssumpion of he iniil mrginl uiliy for lrge welh levels. This is he genuine urnpike nlogue of similr resuls in clssicl expeced uiliy models nd he min finding herein. I shows h he relive risk olernce will converge o he lef-end of he suppor of he underlying mesure µ. As in he spil cse, we firs rele he properies of he mesure o he sympoic behvior of he iniil (mrginl) dum. Assumpion 2: There exiss γ < such h for ll γ (γ, ), u 0 (x) lim x x γ = 0, (.44) while, for ll γ < γ, u 0 (x) lim x x γ =. (.45) 22

35 As we show nex, he bove ssumpion is direcly reled o condiion inroduced in [36] nd [22], for discree nd coninuous-ime cse, respecively. Lemm.4.. Assumpion 2 is equivlen o he funcion u 0 (x) vrying regulrly infiniy wih exponen γ, i.e. for ll k > 0, u lim 0(kx) x u 0(x) = kγ. (.46) Proof. We firs show h condiion (.46) implies (.44) nd (.45). We rgue by conrdicion. Suppose h (.44) does no hold. Then, here exiss γ (γ, ) nd ε > 0 such h for x lrge enough, u 0 (x) x γ > ε. On he oher hnd, u condiion (.46) implies h, for ll k > 0 nd x lrge enough, 0 (kx) u < 0 (x)kγ ε. Thus, for lrge enough x, 0 < u 0(kx) (kx) γ = Since γ γ < 0, lim k esblish (.45). u 0(kx) u 0(x)k γ u 0(x) x γ kγ γ < ( + ε) u 0(x) x γ kγ γ. u 0 (kx) (kx) γ = 0, nd we conclude. Working similrly, we Nex, we show he reverse direcion. Assume h (.45) nd (.44) hold. Then, for ll δ, k > 0 nd x lrge enough, u 0(kx) (kx) γ+δ < nd x γ δ u 0(x) <. Muliplying hese wo equions nd rerrnging gives, for ll δ > 0, u 0(kx) u 0(x) < (kx)γ+δ x γ δ = k γ+δ x 2δ. 23

36 Similrly, i follows from inerchnging kx nd x in he bove wo inequliies h u 0(kx) u 0(x) > (kx)γ δ x γ+δ = k γ δ x 2δ, nd condiion (.46) follows by sending firs δ 0 nd hen x. Assumpion 2 is weker hn Assumpion, nd implies, s we show nex, h he mesure µ hs suppor wih righ-end poin, bu wihou γ necessrily hving mss herein. Lemm.4.2. Assumpion 2 holds if nd only if he mesure µ hs finie suppor wih is righ boundry γ, nmely, inf {y > 0 : µ ((y, )) = 0} = γ. (.47) Proof. We show h Assumpion 2 implies propery (.47). For ech γ (γ, ), we deduce from (.44) h nd, hus, 0 = lim x u x (x, 0) x γ = lim z u x (h(z, 0), 0) (h(z, 0)) γ lim z b = lim z ( h (z, 0) e z γ ) γ e z ( y γ )µ (dy) = 0. (.48) Nex, observe h if b, hen i will conrdic he bove limi, nd hus we need o hve b <. Assume now h here exiss γ (γ, ) wih b = γ. Then, for ech γ (γ, γ ) we hve γ < γ enough, nd he bove gives, for ε smll, 24

37 lim z ( ( γ +ε) Therefore, i mus be h µ e z(y γ ) µ (dy) + b γ +ε e z(y γ ) µ (dy) ) = 0. ( [ γ + ε, b] ) = 0. Sending ε 0, gives µ (( ]), b = γ 0, which is conrdicion. Thus, we mus hve b. Similrly, using (.45) γ we obin h b, nd, hus, b =. γ γ To show he reverse direcion, we firs observe h propery (.47) nd he domined convergence heorem yield h, for ny ε > 0, lim z h(z, 0)e ( γ +ε)z = lim γ z e z(y ( γ +ε)) µ(dy) = 0. Then, seing γ such h γ = γ + ε, we deduce (.44) for ll γ (γ, ). The res of he proof follows esily nd i is hus omied. We hve so fr esblished h under Assumpion 2 he ssocied mesure µ hs finie righ boundry (bu no necessrily mss) γ, nd vice-vers. by, where We now urn our enion o he lef boundry of he suppor, denoed := inf{y 0 : µ ((0, y]) > 0}. (.49) In he upcoming proofs we will frequenly use he ideniy x 0 = γ e yh( ) (x 0,) 2 y2 µ(dy), (.50) 25

38 for x 0 > 0, which follows direcly from (.9) for b = γ. Lemm.4.3. Le h ( ) : D + R be he spil inverse of h, nd s in (.49). Then, for ech x 0 > 0, lim h ( ) (x 0, ) exiss nd, moreover, for 0, 2 h( ) (x 0, ) Proof. Le x 0 > 0 nd observe h (.8) yields (x 0, ) = ( h xx h ( ) (x 0, ) ) 2 h x (h ( ) (x 0, ), ) = 2 h ( ) nd hus inequliy (.5) holds, for ll 0. 2 ( γ). (.5) γ γ y 2 e yh( ) (x 0,) 2 y2 µ(dy) ye yh( ) (x 0,) 2 y2 µ(dy) To show h lim h ( ) (x 0, ) exiss, i suffices o show h h ( ) (x 0, ) is decresing in ime. Indeed, direc clculions yield h ( ) (x 0, ) = γ ( yh ( ) (x 0, ) ) 2 2 y2 e yh( ) (x 0,) 2 y2 µ(dy) γ ye yh( ) (x 0,) 2 y2 µ(dy) < 0. (.52) Alernively, differeniing h ( h ( ) (x 0, ), ) = x 0 wice yields, seing z = h ( ) (x 0, ), ( ) 2 h ( ) (x 0, )h x (z, )+ h ( ) (x 0, ) hxx (z, )+2h ( ) (x 0, ) h x (z, )+h (z, ) = 0. We hve h boh h x, h xx > 0, s i follows direcly from (.9) nd differeniion. Furhermore, he bove qudric in h ( ) (x, ) remins posiive, 26

39 which would hen yield h h ( ) (x 0, ) < 0. Indeed, h 2 x (z, ) h xx (z, ) h (z, ) = h 2 xxx (z, ) h xx (z, ) h xxxx (z, ) < 0, s i follows from (.20). We re now redy o presen one of he min findings herein, which yields he limi s of he rio h( ) (x 0, ). We show h i converges o hlf of he lower-end of he mesure s suppor. Some reled weker resuls cn be found in [63]. Proposiion.4.. Le h ( ) : D + R be he spil inverse of he funcion h (cf. (.9)) nd le, b be he lef nd righ end of he suppor, respecively, wih = 0 + or > 0, nd b <. Then, for ech x 0 > 0, he following sserions hold. i) I holds h ii) Le h ( ) (x 0, ) lim (x 0, ) := h( ) (x 0, ) = 2. (.53) 2. (.54) If > 0, hen ( ) (x 0, ) ln µ [, ] γ, if (x 0, ) < 0, (.55) x 0 nd x 0 µ ([, + (x 0, )]) e 2 (x0,), if (x 0, ) > 0. (.56) 27

40 If = 0 +, hen (x 0, ) > 0, nd, moreover, for ech θ (0, ), x 0 µ ([ (x 0, ), ( + θ) (x 0, )]) e 2 ( θ2 ) 2 (x 0,). (.57) Proof. i). Le x 0 > 0 fixed. Recll h h ( ) (x 0, ) > 0 (cf. (.5)) nd, hus, lim h ( ) (x 0, ) exiss. Moreover, rewriing (.50) s x 0 = γ ( ) e y h ( ) (x 0,) 2 y µ(dy), (.58) we see h lim h ( ) (x 0, ) =, oherwise, sending we ge conrdicion. In urn, from Lemm 7 nd L Hospil s rule, we deduce h nd hus A(x 0 ) := lim h ( ) (x 0, ) 2 A(x 0) = lim h ( ) (x 0, ), (.59) 2( γ). (.60) Nex, we clim h A (x 0 ) < 2( γ). Le > 0. If = γ, hen = b nd h( ) (x 0, ) = ln x γ nd he resul follows direcly. 0 +, 2 γ Le 0 < < γ. Assume h here exiss x 0 such h A (x 0 ) = 2( γ). Then, for ε > 0, here exiss 0 (x 0, ε) such h, for 0, ε h( ) (x 0, ) 2( γ) ε. In urn, for δ > 0 smll enough, he bove nd (.50) yield x 0 ( γ 2ε δ) e y( 2( γ) ε y) γ 2 µ(dy) + e y( γ 2ε δ 28 2( γ) ε 2 y) µ(dy),

41 which yields conrdicion s, becuse he firs inegrl would converge o. Nex, ssume h here exiss x 0 > 0 such h 2 < A(x 0) < Then, for ε, δ > 0 smll enough we hve 2( γ). (.6) < 2(A(x 0 ) ε) δ < 2(A(x 0 ) ε) < γ. (.62) From (.50), we hen deduce h, for 0 (x 0, ε), x 0 γ e (y(a(x 0) ε) 2 y2) µ(dy). If µ ({}) 0, hen x 0 e 2 (2(A(x 0) ε) ) µ ({}), nd sending yields conrdicion. If µ ({}) = 0, hen x 0 γ e (y(a(x 0) ε) 2 y2) µ(dy) 2(A(x0 ) ε) δ Consider he qudric B (y) = y(a(x 0 ) ε) 2 y2. We hve e (y(a(x 0) ε) 2 y2) µ(dy). B (y ) = B (y 2 ) = 0, for y = 0 nd y 2 = 2 (A(x 0 ) ε), (.63) B (y) > 0, for 0 < y < 2 (A(x 0 ) ε), nd B (y) chieves mximum y = A(x 0 ) ε. h Nex, we look is minimum, y = min y 2(A(x) ε) δ (y), nd clim y = 2(A(x 0 ) ε) δ. (.64) Indeed, if 0 < y, hen choosing δ <, direc clculions yield () > (y ). If y <, hen (.62) yields < y < y 2, nd, hus, he minimum lso occurs y. 29

42 Clerly, becuse y < y < y 2, we hve B (y ) = 2 δ (2(A(x 0) ε) δ) > 0. Therefore, for 0 (x 0, ε), x 0 2(A(x0 ) ε) δ e B(y ) µ(dy). (.65) As, he righ hnd side of (.65) converges o, unless i holds h µ ([, 2(A(x 0 ) ε) δ]) = 0. Sending δ 0 nd ε 0, we hen hve µ([, 2A(x 0 )]) = 0, which, however, conrdics (.6). Therefore, i mus be h h, for ll x > 0, A(x 0 ), nd we esily conclude. 2 If = 0 +, similr rgumens yield h for every θ (0, A (x 0 )], we hve h µ([θ, 2A(x 0 )]) = 0. Sending θ 0 yields µ (0, 2A (x 0 )] = 0, which conrdics (.6). ii). Le > 0. If (x 0, ) < 0, from (.50) we hve x 0 = e (x γ 0,) nd (.55) follows. γ e y( (x 0,)+ 2 ( y)) µ(dy) e 2 y( y) µ (dy) e (x 0,) µ ([ ]),, γ If (x 0, ) > 0, hen (.53) yields h, for ε smll enough nd 0 (x 0, ε), 0 < h( ) (x 0,) 2 < ε. Choosing ε such h ε < 2( γ) 2 yields 0 < h( ) (x 0,) <, nd using h <, gives 2 2( γ) 2 γ h( ) 2 + (x 0, ) 30 γ.

43 From (.28) we hen deduce h x h( )(x 0,) ( ) e y h ( ) (x 0,) y 2 µ (dy). ( ) The qudric H (y) := y h ( ) (x 0,) y 2 in he bove inegrnd becomes zero y = 0 nd y 3 = 2 h( ) (x 0,) > nd, herefore, is minimum occurs one of he end poins or + h( ) (x 0,). Noe h < + h( ) (x0,) < y If i occurs, hen H () = (x 0, ), while if i occurs ( ) ( ) + 2 h ( ) (x 0,), hen H + h( ) (x0,) = + h( ) (x0,) (x , ) > (x 2 0, ). Combining he bove gives x h ( ) (x0,) e 2 (x 0,) µ (dy) = µ ([, + (x 0, )]) e 2 (x 0,). Finlly, le = 0 +. Then, (x 0, ) = h( ) (x 0,). Recll h lim h ( ) (x 0, ) =, nd hus h( ) (x 0,) > 0, for lrge. ( h For ε ( ) (x 0,), 2 h( ) (x0 ),) we hen hve x 0 ε h ( ) (x 0,) ( ) e y h ( ) (x 0 ( ),) y ε 2 µ (dy) e ε h ( ) (x 0,) ε 2 µ (dy). h ( ) (x 0,) Seing ε = ( + θ) h( ) (x 0,), (.57) follows. We re now redy o prove one of he min resuls herein. Theorem.4.. Le be he lef end of he suppor of he mesure µ. Then, for ech x 0 > 0, r (x 0, ) lim =. (.66) x 0 3

44 Furhermore, here exiss funcion G (x 0, ) given by γ G (x 0, ) := y y( (y )e 2 ) µ(dy), (x 0, ) < 0 2 (x 0, ) x (x γ 0,)+ y +2 (x 0,)(y )ey( 2 ) µ(dy), (x 0, ) > 0, sisfying wih lim G (x 0, ) = 0 nd, for lrge enough, 0 r(x 0, ) x 0 G (x 0, ). (.67) Proof. We presen wo lernive convergence proofs. The firs yields (.66) while he second gives he re of convergence G (x 0, ). To his end, differeniing (.7) gives ( ) u x (x 0, ) = 2 h( ) (x 0, ) u x (x 0, ). (.68) Moreover, (.4) nd (.6) imply h u (x 0, ) = 2 u x(x 0, )r(x 0, ) nd, in urn, u x (x 0, ) = 2 u xx (x 0, ) r (x 0, ) 2 u x (x 0, ) r x (x 0, ). (.69) Combining he bove we deduce nd from Proposiion 8 nd (.59) On he oher hnd, lim c r x(x 0, ) = h ( ) (x 0, ), (.70) lim r x (x 0, ) = lim 2h ( ) (x 0, ) =. (.7) x0 c r x (ρ, )dρ = r(x 0, ) lim r(c, ). c

45 Using he fc h, for ll 0, lim x 0 + r(x, ) = 0 (see [58]), we ge h, for x 0 > 0, r(x 0, ) = x0 r x (ρ, )dρ. (.72) Finlly, we deduce from (.70) nd (.52) h r x (x 0, ) < 0, nd hus, for x 0 > 0, we hve for y (0, x 0 ], r x (y, ) r x (x 0, 0). However, for ll x 0 > 0, r x (x 0, 0) <. This follows direcly from (2.3),(.9) nd he full rnge of h (x, 0), since γ r x (h (z, 0), 0) = h zz (z, 0) h z (z, 0) = y 2 e yz 2 2y µ (dy) γ ye yz 2 2y µ (dy) γ. Using he domined convergence heorem nd pssing o he limi s in (.70), we deduce (.66). Nex, we give he second convergence proof, which lso yields he re of convergence. Firs noe h 0 r(x 0, ) x 0. (.73) This follows direcly from (2.3), (.9) nd (.50), for r (x 0, ) = γ ye (y h( ) (x 0,) 2 y2) µ(dy) γ Furhermore, from (2.3), (.9), (.50) nd (.54), we hve r(x 0, ) x 0 = γ e (y h( ) (x 0,) 2 y2) µ(dy). (y )e y( 2 (x 0,)+ y 2 ) µ(dy). (.74) If (x 0, ) < 0 (which occurs only if > 0, s shown in he previous proof), hen he bove yields r(x 0, ) x 0 γ 33 y y( (y )e 2 ) µ(dy),

46 nd (.67) follows direcly wih G () := γ y y( (y )e 2 ) µ(dy). Le (x 0, ) > 0 nd > 0 or = 0 +. If =, hen he resul γ follows rivilly. For < γ, observe h for lrge enough, 0 < + 2 (x 0, ) < γ, nd hus represenion (.74) gives r (x 0, ) x 0 = (+2 (x0,)) (y )e y( 2 (x 0,)+ y 2 ) µ(dy) + γ +2 (x 0,) (y )e y( 2 (x 0,)+ y 2 ) µ(dy). Le C (x 0, ) := (+2 (x 0,)) 2 (x y( 0,)+ y (y )e 2 ) µ(dy), nd observe h (+2 (x0,)) C (x 0, ) 2 (x 0, ) e y( 2 (x 0,)+ y 2 ) µ(dy) 2 (x 0, ) x 0, where we used (.50). Thus Le lso C 2 (x 0, ) := γ (y ) e y( 2 (x 0,)+ y 2 ), y +2 (x 0,) lim C (x 0, ) = 0. (.75) 2 (x 0,)+ y (y )ey( 2 ) µ(dy) nd F (y,, x 0 ) := ]. Then, F ( + 2 (x 0, ),, x 0 ) = [ + 2 (x 0, ), γ 2 (x 0, ), nd hus lim F ( + 2 (x 0, ),, x 0 ) = 0. Furhermore, for ech ( ] y + 2 (x 0, ),, we lso hve lim γ F (y,, x 0 ) = 0. In urn, he domined convergence heorem gives lim C 2 (x 0, ) = 0. (.76) Seing G (x 0, ) := C (x 0, )+C 2 (x 0, ), nd using (3.4) nd (.76), we obin (.67). 34

47 .5 Spil nd emporl limis for he relive prudence funcion We now rever our enion o he relive prudence funcion p (x, ) defined, for (x, ) D +, s wih u solving (.4). p (x, ) = xu xxx (x, ) u xx (x, ), (.77) Proposiion.5.. For (x, ) D +, we hve h p (x, ) > 0. Moreover, he following spil nd emporl limis hold. i) If Assumpion holds, hen, for ech 0 0, lim p(x, 0) = 2 γ. (.78) x ii) If Assumpion 2 holds, hen, for ech x 0 > 0, +, if > 0 lim p(x 0, ) =, if = 0 +. (.79) Proof. Using (.77) nd (.6), we deduce h, for ech 0 0, p (x, 0 ) = x r (x, 0 ) ( + r x (x, 0 )), nd he fc h p (x, 0 ) > 0 nd (.78) follow direcly from (.23) nd (.37), respecively. From (.77) nd equion (.4) we lso obin h, for ech x 0 > 0, u x (x 0, ) u x (x 0, ) = 2 Using h lim h ( ) (x 0, ) = 2 r (x 0, ) p (x 0, ) = x 0 2 h( ) (x 0, ). (.80) we esily conclude. 35

48 .6 Exmples We presen wo represenive exmples in which he mesure is, respecively, sum of Dirc funcions nd he Lebesgue mesure. The firs exmple generlizes he resuls of he exmple in subsecion 2., while he second demonsres h he spil urnpike propery fils if here is no mss he righ end of he mesure s suppor..6. Finie sum of Dirc funcions We ssume h µ = N n= δ yn, wih 0 < y < < y N = γ. Then, h(z, 0) = N n= eynz nd, hus, lim z h (z, 0) e zy N =. In urn, (.34) yields u x (x, 0) lim =, x x γ which verifies he resuls of Lemm 2. We lso hve, for (z, ) D, h(z, ) = N n= (cf. (.9)), nd, herefore, for x > 0, Furhermore, x = N n= ( exp y n z ) 2 y2 n. ( ( h ( ) (x, ) exp y n )) 2 y n. (.8) h ( ) (x, ) 2 y y ln x. (.82) 36

49 .6.. Temporl sympoic expnsion of h ( ) (x 0, ) for lrge We clim h, for ech x 0 > 0, s, h ( ) (x 0, ) = 2 y + y ln x 0 + o(). (.83) Indeed, using he limi (.53), we hve ( h ( ) (x 0, ) lim ) { 2 y < 0, < n N n = 0, n =. Therefore, s, ll he erms in (.8) vnish excep for he firs one, nd hus, ( x 0 = lim exp y h ( ) (x 0, ) ) 2 y2. (.84) Tking logrihm nd rerrnging erms yields (.83) Spil sympoic expnsion of h ( ) (x, 0 ) for lrge x We clim h, for ech 0 0, h ( ) (x, 0 ) = ( γ) ln x + To obin his, we firs esblish h h ( ) (x, 0 ) lim x ln x Indeed, fix 0 0, le δ (0, ) nd ssume h γ 2 ( γ) 0 + o(). (.85) = ( γ). (.86) lim inf x h ( ) (x, 0 ) ln x < + δ. γ 37

50 Then, using (.8) nd h h ( ) (x, 0 ) > 0, for lrge x, we hve x = x n= nd using h γ N ( ( ) h ( ) (x, 0 ) exp y n ln x 2 ) ln x y2n 0 n= N ( ( )) h ( ) (x, 0 ) exp y n ln x ln x δ( γ) = +δ +δ( γ) γ Since δ is rbirry, we deduce h Nx h ( ) (x, 0 ) γ ln x, < 0, we ge conrdicion s x. h ( ) (x, 0 ) lim inf x ln x ( ) Similrly, ssume h for δ 0,, γ lim sup x h ( ) (x, 0 ) ln x ( γ). (.87) > δ. γ Then, (.82) gives ( > x exp xh( ) γ ln (x, 0 ) ln x 2 ( ) ) 2 0 γ nd using h γ = x h ( ) (x, 0 ) γ ln x e 2( γ ) 2 0 = γ δ δ( γ) δ( γ) Since δ is rbirry, we deduce h > 0, we ge conrdicion s x. lim sup x h ( ) (x, 0 ) ln x ( γ), (.88) nd we esily conclude. 38

51 Nex, we rewrie (.8) s = = N n= N n= ( exp y n h ( ) (x, 0 ) ) 2 y2 n 0 ln x ( ( h ( ) (x, 0 ) exp y n ln x ) ) ln x y n 2 y2 n 0. Noe h from he limi in (.86) we hve h ( h ( ) (x, 0 ) lim ) = x ln x y n { < 0, n < N = 0, n = N. (.89) Therefore, s x, he firs N erms in (.89) vnish, nd we deduce h lim exp x ( γ h( ) (x, 0 ) ln x 2 ( ) ) 2 0 =. γ We hen obin (.85) by king he logrihm nd rerrnging he erms Spil nd emporl sympoics of r(x, ) From represenion (2.3), we hve for he risk olernce funcion r(x, ) = N n= Le x 0 > 0. Then, (.82) gives r(x 0, ) N n= = y x 0 + ( y n exp y n h ( ) (x, ) ) 2 y2 n. (.90) ( y n exp y n ( 2 y + ln x 0 ) ) y 2 y2 n N n=2 ( ) yn y n exp 2 y n(y y n ) x y 0. 39

52 Therefore, he emporl sympoic expnsion of r(x 0, ) s is given by ( ) r(x 0, ) = y x 0 + O e 2 y 2(y y 2 ). (.9) Nex, le 0 0. Then, lim r(x, 0) = lim x x nd, hus, s x, r(x, 0 ) = n= N n= ( y n exp y n (( γ) ln x + 2 ( γ) 0) ) 2 y2 n 0, N ( ) y n exp 2 y n 0 ( γ y n) x ( γ)yn + o(). (.92) Therefore, for ech x 0 > 0 nd 0 0, we hve he emporl sympoic expnsion (.9) yields r(x 0, ) r (x, 0 ) lim = y nd lim x 0 x x = y N = γ, nd hese limis re consisen wih he findings in Proposiion 3 nd Theorem 9, respecively..6.2 Lebesgue mesure We consider cse of mesure wih coninuous suppor bu wihou mss is righ boundry. We derive he ssocied limis nd lso show h he spil urnpike propery fils. Lebesgue mesure on [ ],, > 0 γ 40

53 Consider he funcions ϕ(z) := e z2 2 nd Φ(z) := z ϕ(y)dy, for z R. Then, represenions (.9) nd (.50) yield, respecively, nd x = h(z, ) = γ γ e yz 2 y2 dy = ez2 /2 γ z/ z/ ϕ(y)dy, (.93) ( ) e y h ( ) (x,) 2 y dy = e h( ) (x,) 2 h ( ) (x,) γ 2 ϕ(y)dy. (.94) h( ) (x,).6.2. Temporl sympoic expnsion of h ( ) (x 0, ) for lrge We clim h for x 0 > 0, s, h ( ) (x 0, ) = 2 + ( ln + ln x 0 + ln ) + o(). (.95) 2 To show his, we firs esblish h x 0 = lim Using (.94) nd h, for z < 0, we hve, for lrge enough, e (h( )(x0,) 2 ) 2. (.96) Φ(z) ϕ(z) z, (.97) x 0 ( ) ( h ( ) (x 0, ) 2 exp Φ ) + h( ) (x 0, ) 2 exp h( ) (x 0,) ( h ( ) (x 0, ) 2 2 ) ( ϕ ) + h( ) (x 0, ) 4

54 In urn, Nex, we show h = e(h( ) (x 0,) 2 ) h ( ) (x 0, ). x 0 lim inf e (h( ) (x 0,) 2 ) h ( ) (x 0, ). (.98) x 0 lim sup e (h( ) (x 0,) 2 ) h ( ) (x 0, ), which wih (.98) will yield (.96). To his end, we use h for ny b > > 0, he inequliy Φ(b) Φ() (ϕ() ϕ(b)) b holds. Le < k <. From (.94) nd he bove, we hve, for lrge ( γ) enough, h x 0 e h( ) (x 0,) 2 2 ( ( Φ k ) ( h( ) (x 0, ) Φ )) h( ) (x 0, ) = k h( ) (x 0,) ( ( ϕ ) h( ) (x 0, ) ϕ e h ( ) (x0,) 2 2 ( k )) h( ) (x 0, ) ) (e (h( ) (x 0,) k h ( ) 2 ) e k(h( ) (x 0,) 2 k). (x 0, ) From Proposiion 8 nd since k >, we hve e k(h( )(x0,) 2 k) lim k h ( ) (x 0, ) = lim ( e k2 ( h( ) (x 0,) k 2 ) k h( ) (x 0,) ) = 0. 42

55 Therefore, x 0 lim sup lim sup ) (e (h( ) (x 0,) k h ( ) 2 ) e k(h( ) (x 0,) 2 k) (x 0, ) e k(h( ) (x 0,) 2 k) k h ( ) (x 0, ) lim e k(h( ) (x 0,) 2 k) k h ( ) (x 0, ) nd sending k we conclude. = lim sup e (h( ) (x 0,) 2 ) k h ( ) (x 0, ), Nex, we uilize he Lmber-W funcion W (x), defined s he inverse funcion of F (x) = xe x, o derive he explici sympoic expnsion of h ( ) (x 0, ) s. Reclling he noion (x 0, ) = h ( ) (x 0, ) 2, we deduce from (.96) h here exiss ε() wih lim ε() = 0, such h Rewriing i yields e (x 0,) (x 2 0, ) = x 0( + ε()). ( ) 2 (x 0, ) e ( 2 (x0,)) = x 0 ( + ε()) e 2 2, Using h he lef hnd side is of he form F (( 2 (x 0, ))), we obin ( ( ) 2 (x 0, )) = W x 0 ( + ε()) e 2 2, nd, in urn, (x 0, ) = 2 ( ) W x 0 ( + ε()) e 2 2. I is esblished in [8] h he sympoic expnsion of W (x), for lrge x, is given by W (x) = ln x ln(ln x) + o(). 43

56 Therefore, (x 0, ) = 2 ( ) ln x 0 ( + ε()) e ( ) ln ln x 0 ( + ε()) e o() = ( ln x 0 + ln( + ε()) + ln ( ln Using h s, ln( + ε()) = o() nd h sserion (.95) follows. x 0 ( + ε()) ( ) ( ) ln ln = ln x 0 ( + ε()) o(), )) + o() Spil sympoic expnsion of h ( ) (x, 0 ) for lrge x Le 0 0. We show h, s x, h ( ) (x, 0 ) = We firs esblish h ( ) 2( γ) 0 + ( γ) ln x + ln ln x ln + o(). (.99) γ h ( ) (x, 0 ) lim x ln x Indeed, le f(z, ) := z e γ z 2( γ ) 2. Then, = lim z = lim z ( γ ( = ( γ). (.00) h(z, 0 ) lim z f(z, 0 ) = lim γ ze z(y γ ) 2 (y2 ( γ ) 2 ) 0 dy z (z y 0 )e z(y γ ) 2 (y2 ( γ ) 2 γ ) 0 dy + y 0 e z(y γ ) 2 (y2 ( γ ) 2 ) 0 dy ) e ( γ )z 2 (2 ( γ ) 2 ) 0 + γ y 0 e z(y γ ) 2 (y2 ( γ ) 2 ) 0 dy =, ) 44

57 where we used h < γ heorem. Therefore, for ech 0 0, nd, for he hird erm, he monoone convergence h(x, 0 ) lim x f (x, 0 ) =. (.0) We now use resul on he inverses of sympoic funcions (see [23]) o prove he limi in (.00) by verifying he necessry ssumpions for his resul o hold. To his end, consider he funcion g(z) := ( γ) ln z, nd noice h g(f(z, 0 )) = ( γ) ln z + z 2 ( γ) 0 z, s z. Thus, lim z z g(f(z, 0 )) =. Since, on he oher hnd, lim z f(z, 0 ) =, we deduce h f ( ) (x, 0 ) g(x), s x. Moreover, g(x) is sricly incresing nd he rio gx(x, 0) g(x, 0 = O( ), for sufficienly lrge x. I hen ) x ln x x follows from he foremenioned resul h g(x) h ( ) (x, 0 ), s x, nd (.00) follows. Nex, we clim h, for ech 0 0, e lim x γ (h( ) (x, 0 ) 2 γ 0) x ln x = γ. (.02) Indeed, for 0 = 0, we hve from (.94) h x = γ e yh( ) (x,0) dy = ) (e h ( ) γ h( ) (x,0) e h( ) (x,0), (.03) (x, 0) nd (.00) yields h lim x e γ h( ) (x,0) x ln x 45

58 = lim x e γ h( ) (x,0) e γ h( ) (x,0) e h( ) (x,0) For 0 > 0, we deduce from (.94) h h ( ) (x, 0) ln x = γ. x = ( ) ( e h ( ) (x,0 ) (Φ 0 h( ) (x, 0 ) Φ )) 0 h( ) (x, 0 ). 0 γ 0 0 (.04) Then, using (.97), we hve, for lrge x, x 0 exp ( h ( ) (x, 0 ) 2 ) ( ) Φ 0 h( ) (x, 0 ) γ ( ) x e h ( ) (x,0 ) h ( ) (x, 0 0 ) ϕ 0 h( ) (x, 0 ) 0 0 γ 0 γ nd, in urn, lim inf x = lim inf x (e = e γ (h( ) (x, 0 ) 2 γ 0) x(h ( ) (x, 0 ) γ 0), γ (h( ) (x, 0 ) 2 γ 0) xh ( ) (x, 0 ) e γ (h( ) (x, 0 ) 2 γ 0) xh ( ) (x, 0 ) = lim inf x Similrly, we use h, for < b < 0, lim x e γ (h( ) (x, 0 ) 2 γ 0) xh ( ) (x, 0 ) ) h ( ) (x, 0 ) h ( ) (x, 0 ) γ 0 h ( ) (x, 0 ) h ( ) (x, 0 ) γ 0. (.05) Φ(b) Φ() ϕ() ϕ(b), (.06) 46

59 nd deduce from (.04) h, for lrge x, x e h ( ) (x,0 ) h( ) (x, 0 ) 0 ( ϕ( 0 h( ) (x, 0 ) ) ϕ( 0 = e γ (h( ) (x, 0 ) 2 γ 0) For he second erm, we hve Therefore, lim x x(h ( ) (x, 0 ) 0 ) e h( ) (x, 0 ) x(h ( ) (x, 0 ) 0 ) e = lim x exp lim sup x = lim sup x γ 2 0 = lim x ( ( h ( ) (x, 0 ) ln x ln x (e e = lim sup x γ (h( ) (x, 0 ) 2 γ 0) x(h ( ) (x, 0 ) 0 ) e γ (h( ) (x, 0 ) 2 γ 0) x(h ( ) (x, 0 ) 0 ) lim x = lim sup x γ (h( ) (x, 0 ) 2 γ 0) xh ( ) (x, 0 ) = lim sup x ) 0 h( ) (x, 0 ) ) 0 e(h( )(x,0) 2 0) x(h ( ) (x, 0 ) 0 ). e h( )(x,0) ln x 2 0 e h ( ) (x, 0 ) 0 )) = 0. h ( ) (x, 0 ) 0 e γ (h( ) (x, 0 ) 2 γ 0) x(h ( ) (x, 0 ) 0 ) lim x e γ (h( ) (x, 0 ) 2 γ 0) xh ( ) (x, 0 ) From (.05) nd (.07), we hen obin ) e(h( )(x,0) 2 0) x(h ( ) (x, 0 ) 0 ) e (h( ) (x, 0 ) 2 0) x(h ( ) (x, 0 ) 0 ) xh ( ) (x, 0 ) x(h ( ) (x, 0 ) 0 ). (.07) lim sup x e γ (h( ) (x, 0 ) 2 γ 0) xh ( ) (x, 0 ) =, 47

e t dt e t dt = lim e t dt T (1 e T ) = 1

e t dt e t dt = lim e t dt T (1 e T ) = 1 Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie

More information

3. Renewal Limit Theorems

3. Renewal Limit Theorems Virul Lborories > 14. Renewl Processes > 1 2 3 3. Renewl Limi Theorems In he inroducion o renewl processes, we noed h he rrivl ime process nd he couning process re inverses, in sens The rrivl ime process

More information

A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR IAN KNOWLES

A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR IAN KNOWLES A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR j IAN KNOWLES 1. Inroducion Consider he forml differenil operor T defined by el, (1) where he funcion q{) is rel-vlued nd loclly

More information

Contraction Mapping Principle Approach to Differential Equations

Contraction Mapping Principle Approach to Differential Equations epl Journl of Science echnology 0 (009) 49-53 Conrcion pping Principle pproch o Differenil Equions Bishnu P. Dhungn Deprmen of hemics, hendr Rn Cmpus ribhuvn Universiy, Khmu epl bsrc Using n eension of

More information

REAL ANALYSIS I HOMEWORK 3. Chapter 1

REAL ANALYSIS I HOMEWORK 3. Chapter 1 REAL ANALYSIS I HOMEWORK 3 CİHAN BAHRAN The quesions re from Sein nd Shkrchi s e. Chper 1 18. Prove he following sserion: Every mesurble funcion is he limi.e. of sequence of coninuous funcions. We firs

More information

Convergence of Singular Integral Operators in Weighted Lebesgue Spaces

Convergence of Singular Integral Operators in Weighted Lebesgue Spaces EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 10, No. 2, 2017, 335-347 ISSN 1307-5543 www.ejpm.com Published by New York Business Globl Convergence of Singulr Inegrl Operors in Weighed Lebesgue

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM Elecronic Journl of Differenil Equions, Vol. 208 (208), No. 50, pp. 6. ISSN: 072-669. URL: hp://ejde.mh.xse.edu or hp://ejde.mh.un.edu EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE

More information

5.1-The Initial-Value Problems For Ordinary Differential Equations

5.1-The Initial-Value Problems For Ordinary Differential Equations 5.-The Iniil-Vlue Problems For Ordinry Differenil Equions Consider solving iniil-vlue problems for ordinry differenil equions: (*) y f, y, b, y. If we know he generl soluion y of he ordinry differenil

More information

4.8 Improper Integrals

4.8 Improper Integrals 4.8 Improper Inegrls Well you ve mde i hrough ll he inegrion echniques. Congrs! Unforunely for us, we sill need o cover one more inegrl. They re clled Improper Inegrls. A his poin, we ve only del wih inegrls

More information

Probability, Estimators, and Stationarity

Probability, Estimators, and Stationarity Chper Probbiliy, Esimors, nd Sionriy Consider signl genered by dynmicl process, R, R. Considering s funcion of ime, we re opering in he ime domin. A fundmenl wy o chrcerize he dynmics using he ime domin

More information

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q).

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q). INTEGRALS JOHN QUIGG Eercise. Le f : [, b] R be bounded, nd le P nd Q be priions of [, b]. Prove h if P Q hen U(P ) U(Q) nd L(P ) L(Q). Soluion: Le P = {,..., n }. Since Q is obined from P by dding finiely

More information

September 20 Homework Solutions

September 20 Homework Solutions College of Engineering nd Compuer Science Mechnicl Engineering Deprmen Mechnicl Engineering A Seminr in Engineering Anlysis Fll 7 Number 66 Insrucor: Lrry Creo Sepember Homework Soluions Find he specrum

More information

0 for t < 0 1 for t > 0

0 for t < 0 1 for t > 0 8.0 Sep nd del funcions Auhor: Jeremy Orloff The uni Sep Funcion We define he uni sep funcion by u() = 0 for < 0 for > 0 I is clled he uni sep funcion becuse i kes uni sep = 0. I is someimes clled he Heviside

More information

An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples.

An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples. Improper Inegrls To his poin we hve only considered inegrls f(x) wih he is of inegrion nd b finie nd he inegrnd f(x) bounded (nd in fc coninuous excep possibly for finiely mny jump disconinuiies) An inegrl

More information

Green s Functions and Comparison Theorems for Differential Equations on Measure Chains

Green s Functions and Comparison Theorems for Differential Equations on Measure Chains Green s Funcions nd Comprison Theorems for Differenil Equions on Mesure Chins Lynn Erbe nd Alln Peerson Deprmen of Mhemics nd Sisics, Universiy of Nebrsk-Lincoln Lincoln,NE 68588-0323 lerbe@@mh.unl.edu

More information

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX Journl of Applied Mhemics, Sisics nd Informics JAMSI), 9 ), No. ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX MEHMET ZEKI SARIKAYA, ERHAN. SET

More information

A new model for limit order book dynamics

A new model for limit order book dynamics Anewmodelforlimiorderbookdynmics JeffreyR.Russell UniversiyofChicgo,GrdueSchoolofBusiness TejinKim UniversiyofChicgo,DeprmenofSisics Absrc:Thispperproposesnewmodelforlimiorderbookdynmics.Thelimiorderbookconsiss

More information

Minimum Squared Error

Minimum Squared Error Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > 0 for ll smples y i solve sysem of liner inequliies MSE procedure y i i for ll smples

More information

HUI-HSIUNG KUO, ANUWAT SAE-TANG, AND BENEDYKT SZOZDA

HUI-HSIUNG KUO, ANUWAT SAE-TANG, AND BENEDYKT SZOZDA Communicions on Sochsic Anlysis Vol 6, No 4 2012 603-614 Serils Publicions wwwserilspublicionscom THE ITÔ FORMULA FOR A NEW STOCHASTIC INTEGRAL HUI-HSIUNG KUO, ANUWAT SAE-TANG, AND BENEDYKT SZOZDA Absrc

More information

Minimum Squared Error

Minimum Squared Error Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > for ll smples y i solve sysem of liner inequliies MSE procedure y i = i for ll smples

More information

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function ENGR 1990 Engineering Mhemics The Inegrl of Funcion s Funcion Previously, we lerned how o esime he inegrl of funcion f( ) over some inervl y dding he res of finie se of rpezoids h represen he re under

More information

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration. Moion Accelerion Pr : Consn Accelerion Accelerion Accelerion Accelerion is he re of chnge of velociy. = v - vo = Δv Δ ccelerion = = v - vo chnge of velociy elpsed ime Accelerion is vecor, lhough in one-dimensionl

More information

Mathematics 805 Final Examination Answers

Mathematics 805 Final Examination Answers . 5 poins Se he Weiersrss M-es. Mhemics 85 Finl Eminion Answers Answer: Suppose h A R, nd f n : A R. Suppose furher h f n M n for ll A, nd h Mn converges. Then f n converges uniformly on A.. 5 poins Se

More information

Solutions to Problems from Chapter 2

Solutions to Problems from Chapter 2 Soluions o Problems rom Chper Problem. The signls u() :5sgn(), u () :5sgn(), nd u h () :5sgn() re ploed respecively in Figures.,b,c. Noe h u h () :5sgn() :5; 8 including, bu u () :5sgn() is undeined..5

More information

A Kalman filtering simulation

A Kalman filtering simulation A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer

More information

Hermite-Hadamard-Fejér type inequalities for convex functions via fractional integrals

Hermite-Hadamard-Fejér type inequalities for convex functions via fractional integrals Sud. Univ. Beş-Bolyi Mh. 6(5, No. 3, 355 366 Hermie-Hdmrd-Fejér ype inequliies for convex funcions vi frcionl inegrls İmd İşcn Asrc. In his pper, firsly we hve eslished Hermie Hdmrd-Fejér inequliy for

More information

1.0 Electrical Systems

1.0 Electrical Systems . Elecricl Sysems The ypes of dynmicl sysems we will e sudying cn e modeled in erms of lgeric equions, differenil equions, or inegrl equions. We will egin y looking fmilir mhemicl models of idel resisors,

More information

GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS

GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS - TAMKANG JOURNAL OF MATHEMATICS Volume 5, Number, 7-5, June doi:5556/jkjm555 Avilble online hp://journlsmhkueduw/ - - - GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS MARCELA

More information

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6.

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6. [~ o o :- o o ill] i 1. Mrices, Vecors, nd Guss-Jordn Eliminion 1 x y = = - z= The soluion is ofen represened s vecor: n his exmple, he process of eliminion works very smoohly. We cn elimine ll enries

More information

Chapter 2: Evaluative Feedback

Chapter 2: Evaluative Feedback Chper 2: Evluive Feedbck Evluing cions vs. insrucing by giving correc cions Pure evluive feedbck depends olly on he cion ken. Pure insrucive feedbck depends no ll on he cion ken. Supervised lerning is

More information

Some Inequalities variations on a common theme Lecture I, UL 2007

Some Inequalities variations on a common theme Lecture I, UL 2007 Some Inequliies vriions on common heme Lecure I, UL 2007 Finbrr Hollnd, Deprmen of Mhemics, Universiy College Cork, fhollnd@uccie; July 2, 2007 Three Problems Problem Assume i, b i, c i, i =, 2, 3 re rel

More information

f t f a f x dx By Lin McMullin f x dx= f b f a. 2

f t f a f x dx By Lin McMullin f x dx= f b f a. 2 Accumulion: Thoughs On () By Lin McMullin f f f d = + The gols of he AP* Clculus progrm include he semen, Sudens should undersnd he definie inegrl s he ne ccumulion of chnge. 1 The Topicl Ouline includes

More information

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX.

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX. ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX. MEHMET ZEKI SARIKAYA?, ERHAN. SET, AND M. EMIN OZDEMIR Asrc. In his noe, we oin new some ineuliies

More information

1 jordan.mcd Eigenvalue-eigenvector approach to solving first order ODEs. -- Jordan normal (canonical) form. Instructor: Nam Sun Wang

1 jordan.mcd Eigenvalue-eigenvector approach to solving first order ODEs. -- Jordan normal (canonical) form. Instructor: Nam Sun Wang jordnmcd Eigenvlue-eigenvecor pproch o solving firs order ODEs -- ordn norml (cnonicl) form Insrucor: Nm Sun Wng Consider he following se of coupled firs order ODEs d d x x 5 x x d d x d d x x x 5 x x

More information

white strictly far ) fnf regular [ with f fcs)8( hs ) as function Preliminary question jointly speaking does not exist! Brownian : APA Lecture 1.

white strictly far ) fnf regular [ with f fcs)8( hs ) as function Preliminary question jointly speaking does not exist! Brownian : APA Lecture 1. Am : APA Lecure 13 Brownin moion Preliminry quesion : Wh is he equivlen in coninuous ime of sequence of? iid Ncqe rndom vribles ( n nzn noise ( 4 e Re whie ( ie se every fm ( xh o + nd covrince E ( xrxs

More information

1. Introduction. 1 b b

1. Introduction. 1 b b Journl of Mhemicl Inequliies Volume, Number 3 (007), 45 436 SOME IMPROVEMENTS OF GRÜSS TYPE INEQUALITY N. ELEZOVIĆ, LJ. MARANGUNIĆ AND J. PEČARIĆ (communiced b A. Čižmešij) Absrc. In his pper some inequliies

More information

Physics 2A HW #3 Solutions

Physics 2A HW #3 Solutions Chper 3 Focus on Conceps: 3, 4, 6, 9 Problems: 9, 9, 3, 41, 66, 7, 75, 77 Phsics A HW #3 Soluions Focus On Conceps 3-3 (c) The ccelerion due o grvi is he sme for boh blls, despie he fc h he hve differen

More information

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions ISSNOnline : 39-8753 ISSN Prin : 347-67 An ISO 397: 7 Cerified Orgnizion Vol. 5, Issue 5, My 6 A Time Trunced Improved Group Smpling Plns for Ryleigh nd og - ogisic Disribuions P.Kvipriy, A.R. Sudmni Rmswmy

More information

THREE IMPORTANT CONCEPTS IN TIME SERIES ANALYSIS: STATIONARITY, CROSSING RATES, AND THE WOLD REPRESENTATION THEOREM

THREE IMPORTANT CONCEPTS IN TIME SERIES ANALYSIS: STATIONARITY, CROSSING RATES, AND THE WOLD REPRESENTATION THEOREM THR IMPORTANT CONCPTS IN TIM SRIS ANALYSIS: STATIONARITY, CROSSING RATS, AND TH WOLD RPRSNTATION THORM Prof. Thoms B. Fomb Deprmen of conomics Souhern Mehodis Universi June 8 I. Definiion of Covrince Sionri

More information

arxiv: v1 [math.pr] 24 Sep 2015

arxiv: v1 [math.pr] 24 Sep 2015 RENEWAL STRUCTURE OF THE BROWNIAN TAUT STRING EMMANUEL SCHERTZER rxiv:59.7343v [mh.pr] 24 Sep 25 Absrc. In recen pper [LS5], M. Lifshis nd E. Seerqvis inroduced he u sring of Brownin moion w, defined s

More information

Chapter Direct Method of Interpolation

Chapter Direct Method of Interpolation Chper 5. Direc Mehod of Inerpolion Afer reding his chper, you should be ble o:. pply he direc mehod of inerpolion,. sole problems using he direc mehod of inerpolion, nd. use he direc mehod inerpolns o

More information

Journal of Mathematical Analysis and Applications. Two normality criteria and the converse of the Bloch principle

Journal of Mathematical Analysis and Applications. Two normality criteria and the converse of the Bloch principle J. Mh. Anl. Appl. 353 009) 43 48 Conens liss vilble ScienceDirec Journl of Mhemicl Anlysis nd Applicions www.elsevier.com/loce/jm Two normliy crieri nd he converse of he Bloch principle K.S. Chrk, J. Rieppo

More information

Procedia Computer Science

Procedia Computer Science Procedi Compuer Science 00 (0) 000 000 Procedi Compuer Science www.elsevier.com/loce/procedi The Third Informion Sysems Inernionl Conference The Exisence of Polynomil Soluion of he Nonliner Dynmicl Sysems

More information

On the Pseudo-Spectral Method of Solving Linear Ordinary Differential Equations

On the Pseudo-Spectral Method of Solving Linear Ordinary Differential Equations Journl of Mhemics nd Sisics 5 ():136-14, 9 ISS 1549-3644 9 Science Publicions On he Pseudo-Specrl Mehod of Solving Liner Ordinry Differenil Equions B.S. Ogundre Deprmen of Pure nd Applied Mhemics, Universiy

More information

MTH 146 Class 11 Notes

MTH 146 Class 11 Notes 8.- Are of Surfce of Revoluion MTH 6 Clss Noes Suppose we wish o revolve curve C round n is nd find he surfce re of he resuling solid. Suppose f( ) is nonnegive funcion wih coninuous firs derivive on he

More information

Tax Audit and Vertical Externalities

Tax Audit and Vertical Externalities T Audi nd Vericl Eernliies Hidey Ko Misuyoshi Yngihr Ngoy Keizi Universiy Ngoy Universiy 1. Inroducion The vericl fiscl eernliies rise when he differen levels of governmens, such s he federl nd se governmens,

More information

S Radio transmission and network access Exercise 1-2

S Radio transmission and network access Exercise 1-2 S-7.330 Rdio rnsmission nd nework ccess Exercise 1 - P1 In four-symbol digil sysem wih eqully probble symbols he pulses in he figure re used in rnsmission over AWGN-chnnel. s () s () s () s () 1 3 4 )

More information

3D Transformations. Computer Graphics COMP 770 (236) Spring Instructor: Brandon Lloyd 1/26/07 1

3D Transformations. Computer Graphics COMP 770 (236) Spring Instructor: Brandon Lloyd 1/26/07 1 D Trnsformions Compuer Grphics COMP 770 (6) Spring 007 Insrucor: Brndon Lloyd /6/07 Geomery Geomeric eniies, such s poins in spce, exis wihou numers. Coordines re nming scheme. The sme poin cn e descried

More information

Asymptotic relationship between trajectories of nominal and uncertain nonlinear systems on time scales

Asymptotic relationship between trajectories of nominal and uncertain nonlinear systems on time scales Asympoic relionship beween rjecories of nominl nd uncerin nonliner sysems on ime scles Fim Zohr Tousser 1,2, Michel Defoor 1, Boudekhil Chfi 2 nd Mohmed Djemï 1 Absrc This pper sudies he relionship beween

More information

Honours Introductory Maths Course 2011 Integration, Differential and Difference Equations

Honours Introductory Maths Course 2011 Integration, Differential and Difference Equations Honours Inroducory Mhs Course 0 Inegrion, Differenil nd Difference Equions Reding: Ching Chper 4 Noe: These noes do no fully cover he meril in Ching, u re men o supplemen your reding in Ching. Thus fr

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

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

Average & instantaneous velocity and acceleration Motion with constant acceleration

Average & instantaneous velocity and acceleration Motion with constant acceleration Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission

More information

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 2

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 2 ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER Seion Eerise -: Coninuiy of he uiliy funion Le λ ( ) be he monooni uiliy funion defined in he proof of eisene of uiliy funion If his funion is oninuous y hen

More information

FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES

FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES FRACTIONAL ORNSTEIN-ULENBECK PROCESSES Prick Cheridio Deprmen of Mhemics, ET Zürich C-89 Zürich, Swizerlnd dio@mh.ehz.ch ideyuki Kwguchi Deprmen of Mhemics, Keio Universiy iyoshi, Yokohm 3-85, Jpn hide@999.jukuin.keio.c.jp

More information

ASYMPTOTIC BEHAVIOR OF INTERMEDIATE SOLUTIONS OF FOURTH-ORDER NONLINEAR DIFFERENTIAL EQUATIONS WITH REGULARLY VARYING COEFFICIENTS

ASYMPTOTIC BEHAVIOR OF INTERMEDIATE SOLUTIONS OF FOURTH-ORDER NONLINEAR DIFFERENTIAL EQUATIONS WITH REGULARLY VARYING COEFFICIENTS Elecronic Journl of Differenil Equions, Vol. 06 06), No. 9, pp. 3. ISSN: 07-669. URL: hp://ejde.mh.xse.edu or hp://ejde.mh.un.edu ASYMPTOTIC BEHAVIOR OF INTERMEDIATE SOLUTIONS OF FOURTH-ORDER NONLINEAR

More information

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh.

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh. How o Prove he Riemnn Hohesis Auhor: Fez Fok Al Adeh. Presiden of he Srin Cosmologicl Socie P.O.Bo,387,Dmscus,Sri Tels:963--77679,735 Emil:hf@scs-ne.org Commens: 3 ges Subj-Clss: Funcionl nlsis, comle

More information

A 1.3 m 2.5 m 2.8 m. x = m m = 8400 m. y = 4900 m 3200 m = 1700 m

A 1.3 m 2.5 m 2.8 m. x = m m = 8400 m. y = 4900 m 3200 m = 1700 m PHYS : Soluions o Chper 3 Home Work. SSM REASONING The displcemen is ecor drwn from he iniil posiion o he finl posiion. The mgniude of he displcemen is he shores disnce beween he posiions. Noe h i is onl

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

Properties of Logarithms. Solving Exponential and Logarithmic Equations. Properties of Logarithms. Properties of Logarithms. ( x)

Properties of Logarithms. Solving Exponential and Logarithmic Equations. Properties of Logarithms. Properties of Logarithms. ( x) Properies of Logrihms Solving Eponenil nd Logrihmic Equions Properies of Logrihms Produc Rule ( ) log mn = log m + log n ( ) log = log + log Properies of Logrihms Quoien Rule log m = logm logn n log7 =

More information

( ) ( ) ( ) ( ) ( ) ( y )

( ) ( ) ( ) ( ) ( ) ( y ) 8. Lengh of Plne Curve The mos fmous heorem in ll of mhemics is he Pyhgoren Theorem. I s formulion s he disnce formul is used o find he lenghs of line segmens in he coordine plne. In his secion you ll

More information

Fractional Calculus. Connor Wiegand. 6 th June 2017

Fractional Calculus. Connor Wiegand. 6 th June 2017 Frcionl Clculus Connor Wiegnd 6 h June 217 Absrc This pper ims o give he reder comforble inroducion o Frcionl Clculus. Frcionl Derivives nd Inegrls re defined in muliple wys nd hen conneced o ech oher

More information

IX.2 THE FOURIER TRANSFORM

IX.2 THE FOURIER TRANSFORM Chper IX The Inegrl Trnsform Mehods IX. The Fourier Trnsform November, 7 7 IX. THE FOURIER TRANSFORM IX.. The Fourier Trnsform Definiion 7 IX.. Properies 73 IX..3 Emples 74 IX..4 Soluion of ODE 76 IX..5

More information

Endogenous Formation of Limit Order Books: Dynamics Between Trades.

Endogenous Formation of Limit Order Books: Dynamics Between Trades. Endogenous Formion of Limi Order Books: Dynmics Beween Trdes. Romn Gyduk nd Sergey Ndochiy Curren version: June 9, 7 Originl version: My 6, 6 Absrc In his work, we presen coninuous-ime lrge-populion gme

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

Application on Inner Product Space with. Fixed Point Theorem in Probabilistic

Application on Inner Product Space with. Fixed Point Theorem in Probabilistic Journl of Applied Mhemics & Bioinformics, vol.2, no.2, 2012, 1-10 ISSN: 1792-6602 prin, 1792-6939 online Scienpress Ld, 2012 Applicion on Inner Produc Spce wih Fixed Poin Theorem in Probbilisic Rjesh Shrivsv

More information

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

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

More information

MAT 266 Calculus for Engineers II Notes on Chapter 6 Professor: John Quigg Semester: spring 2017

MAT 266 Calculus for Engineers II Notes on Chapter 6 Professor: John Quigg Semester: spring 2017 MAT 66 Clculus for Engineers II Noes on Chper 6 Professor: John Quigg Semeser: spring 7 Secion 6.: Inegrion by prs The Produc Rule is d d f()g() = f()g () + f ()g() Tking indefinie inegrls gives [f()g

More information

Some basic notation and terminology. Deterministic Finite Automata. COMP218: Decision, Computation and Language Note 1

Some basic notation and terminology. Deterministic Finite Automata. COMP218: Decision, Computation and Language Note 1 COMP28: Decision, Compuion nd Lnguge Noe These noes re inended minly s supplemen o he lecures nd exooks; hey will e useful for reminders ou noion nd erminology. Some sic noion nd erminology An lphe is

More information

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION Avilble online hp://scik.org Eng. Mh. Le. 15, 15:4 ISSN: 49-9337 CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION PANDEY, C. P. 1, RAKESH MOHAN AND BHAIRAW NATH TRIPATHI 3 1 Deprmen o Mhemics, Ajy

More information

Solutions of half-linear differential equations in the classes Gamma and Pi

Solutions of half-linear differential equations in the classes Gamma and Pi Soluions of hlf-liner differenil equions in he clsses Gmm nd Pi Pvel Řehák Insiue of Mhemics, Acdemy of Sciences CR CZ-6662 Brno, Czech Reublic; Fculy of Educion, Msryk Universiy CZ-60300 Brno, Czech Reublic

More information

Hamilton Jacobi equations

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

More information

Non-oscillation of perturbed half-linear differential equations with sums of periodic coefficients

Non-oscillation of perturbed half-linear differential equations with sums of periodic coefficients Hsil nd Veselý Advnces in Difference Equions 2015 2015:190 DOI 10.1186/s13662-015-0533-4 R E S E A R C H Open Access Non-oscillion of perurbed hlf-liner differenil equions wih sums of periodic coefficiens

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 9: The High Beta Tokamak

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 9: The High Beta Tokamak .65, MHD Theory of Fusion Sysems Prof. Freidberg Lecure 9: The High e Tokmk Summry of he Properies of n Ohmic Tokmk. Advnges:. good euilibrium (smll shif) b. good sbiliy ( ) c. good confinemen ( τ nr )

More information

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π RESPONSE UNDER A GENERAL PERIODIC FORCE When he exernl force F() is periodic wih periodτ / ω,i cn be expnded in Fourier series F( ) o α ω α b ω () where τ F( ) ω d, τ,,,... () nd b τ F( ) ω d, τ,,... (3)

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

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

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment Mgneosics Br Mgne As fr bck s 4500 yers go, he Chinese discovered h cerin ypes of iron ore could rc ech oher nd cerin mels. Iron filings "mp" of br mgne s field Crefully suspended slivers of his mel were

More information

How to prove the Riemann Hypothesis

How to prove the Riemann Hypothesis Scholrs Journl of Phsics, Mhemics nd Sisics Sch. J. Phs. Mh. S. 5; (B:5-6 Scholrs Acdemic nd Scienific Publishers (SAS Publishers (An Inernionl Publisher for Acdemic nd Scienific Resources *Corresonding

More information

USING ITERATIVE LINEAR REGRESSION MODEL TO TIME SERIES MODELS

USING ITERATIVE LINEAR REGRESSION MODEL TO TIME SERIES MODELS Elecronic Journl of Applied Sisicl Anlysis EJASA (202), Elecron. J. App. S. Anl., Vol. 5, Issue 2, 37 50 e-issn 2070-5948, DOI 0.285/i20705948v5n2p37 202 Universià del Sleno hp://sib-ese.unile.i/index.php/ejs/index

More information

Integral Transform. Definitions. Function Space. Linear Mapping. Integral Transform

Integral Transform. Definitions. Function Space. Linear Mapping. Integral Transform Inegrl Trnsform Definiions Funcion Spce funcion spce A funcion spce is liner spce of funcions defined on he sme domins & rnges. Liner Mpping liner mpping Le VF, WF e liner spces over he field F. A mpping

More information

Utility maximization in incomplete markets

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

More information

Solutions to Assignment 1

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

More information

Systems Variables and Structural Controllability: An Inverted Pendulum Case

Systems Variables and Structural Controllability: An Inverted Pendulum Case Reserch Journl of Applied Sciences, Engineering nd echnology 6(: 46-4, 3 ISSN: 4-7459; e-issn: 4-7467 Mxwell Scienific Orgniion, 3 Submied: Jnury 5, 3 Acceped: Mrch 7, 3 Published: November, 3 Sysems Vribles

More information

SOME USEFUL MATHEMATICS

SOME USEFUL MATHEMATICS SOME USEFU MAHEMAICS SOME USEFU MAHEMAICS I is esy o mesure n preic he behvior of n elecricl circui h conins only c volges n currens. However, mos useful elecricl signls h crry informion vry wih ime. Since

More information

Analytic solution of linear fractional differential equation with Jumarie derivative in term of Mittag-Leffler function

Analytic solution of linear fractional differential equation with Jumarie derivative in term of Mittag-Leffler function Anlyic soluion of liner frcionl differenil equion wih Jumrie derivive in erm of Mig-Leffler funcion Um Ghosh (), Srijn Sengup (2), Susmi Srkr (2b), Shnnu Ds (3) (): Deprmen of Mhemics, Nbdwip Vidysgr College,

More information

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218 Chper Moion long srigh line 9/9/05 Physics 8 Gols for Chper How o describe srigh line moion in erms of displcemen nd erge elociy. The mening of insnneous elociy nd speed. Aerge elociy/insnneous elociy

More information

FURTHER GENERALIZATIONS. QI Feng. The value of the integral of f(x) over [a; b] can be estimated in a variety ofways. b a. 2(M m)

FURTHER GENERALIZATIONS. QI Feng. The value of the integral of f(x) over [a; b] can be estimated in a variety ofways. b a. 2(M m) Univ. Beogrd. Pul. Elekroehn. Fk. Ser. M. 8 (997), 79{83 FUTHE GENEALIZATIONS OF INEQUALITIES FO AN INTEGAL QI Feng Using he Tylor's formul we prove wo inegrl inequliies, h generlize K. S. K. Iyengr's

More information

MATH 124 AND 125 FINAL EXAM REVIEW PACKET (Revised spring 2008)

MATH 124 AND 125 FINAL EXAM REVIEW PACKET (Revised spring 2008) MATH 14 AND 15 FINAL EXAM REVIEW PACKET (Revised spring 8) The following quesions cn be used s review for Mh 14/ 15 These quesions re no cul smples of quesions h will pper on he finl em, bu hey will provide

More information

TIMELINESS, ACCURACY, AND RELEVANCE IN DYNAMIC INCENTIVE CONTRACTS

TIMELINESS, ACCURACY, AND RELEVANCE IN DYNAMIC INCENTIVE CONTRACTS TIMELINESS, ACCURACY, AND RELEVANCE IN DYNAMIC INCENTIVE CONTRACTS by Peer O. Chrisensen Universiy of Souhern Denmrk Odense, Denmrk Gerld A. Felhm Universiy of Briish Columbi Vncouver, Cnd Chrisin Hofmnn

More information

Solutions for Nonlinear Partial Differential Equations By Tan-Cot Method

Solutions for Nonlinear Partial Differential Equations By Tan-Cot Method IOSR Journl of Mhemics (IOSR-JM) e-issn: 78-578. Volume 5, Issue 3 (Jn. - Feb. 13), PP 6-11 Soluions for Nonliner Pril Differenil Equions By Tn-Co Mehod Mhmood Jwd Abdul Rsool Abu Al-Sheer Al -Rfidin Universiy

More information

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

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

More information

ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS

ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS Hceepe Journl of Mhemics nd Sisics Volume 45) 0), 65 655 ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS M Emin Özdemir, Ahme Ock Akdemir nd Erhn Se Received 6:06:0 : Acceped

More information

ON THE STABILITY OF DELAY POPULATION DYNAMICS RELATED WITH ALLEE EFFECTS. O. A. Gumus and H. Kose

ON THE STABILITY OF DELAY POPULATION DYNAMICS RELATED WITH ALLEE EFFECTS. O. A. Gumus and H. Kose Mhemicl nd Compuionl Applicions Vol. 7 o. pp. 56-67 O THE STABILITY O DELAY POPULATIO DYAMICS RELATED WITH ALLEE EECTS O. A. Gumus nd H. Kose Deprmen o Mhemics Selcu Universiy 47 Kony Turey ozlem@selcu.edu.r

More information

14. The fundamental theorem of the calculus

14. The fundamental theorem of the calculus 4. The funmenl heorem of he clculus V 20 00 80 60 40 20 0 0 0.2 0.4 0.6 0.8 v 400 200 0 0 0.2 0.5 0.8 200 400 Figure : () Venriculr volume for subjecs wih cpciies C = 24 ml, C = 20 ml, C = 2 ml n (b) he

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

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

The Taiwan stock market does follow a random walk. Abstract

The Taiwan stock market does follow a random walk. Abstract The Tiwn soc mre does follow rndom wl D Bue Loc Feng Chi Universiy Absrc Applying he Lo nd McKinly vrince rio es on he weely reurns from he Tiwn soc mre from 990 o mid 006, I obined resuls srongly indicive

More information

On Hadamard and Fejér-Hadamard inequalities for Caputo k-fractional derivatives

On Hadamard and Fejér-Hadamard inequalities for Caputo k-fractional derivatives In J Nonliner Anl Appl 9 8 No, 69-8 ISSN: 8-68 elecronic hp://dxdoiorg/75/ijn8745 On Hdmrd nd Fejér-Hdmrd inequliies for Cpuo -frcionl derivives Ghulm Frid, Anum Jved Deprmen of Mhemics, COMSATS Universiy

More information

Yan Sun * 1 Introduction

Yan Sun * 1 Introduction Sun Boundry Vlue Problems 22, 22:86 hp://www.boundryvlueproblems.com/conen/22//86 R E S E A R C H Open Access Posiive soluions of Surm-Liouville boundry vlue problems for singulr nonliner second-order

More information