Matching and Saving in Continuous Time: Proofs

Size: px
Start display at page:

Download "Matching and Saving in Continuous Time: Proofs"

Transcription

1 Mainz School of Management and Economics Discussion Pape Seies Matching and Saving in Continuous Time: Poofs Chistian Baye and Klaus Wälde Apil 200 Discussion pape numbe 005 Johannes Gutenbeg Univesity Mainz Mainz School of Management and Economics Jakob-Welde-Weg Mainz Gemany wiwi.uni-mainz.de

2 Contact details Chistian Baye TU Belin Institute of Mathematics Staße des 7. Juni Belin Gemany bayemath.tu-belin.de Klaus Wälde Chai in Macoeconomics Johannes Gutenbeg-Univesität Mainz Jakob Welde-Weg Mainz Gemany klaus.waeldeuni-mainz.de All discussion papes can be downloaded fom

3 Matching and Saving in Continuous Time: Poofs Chistian Baye (a) and Klaus Wälde (b) (a) TU Belin and (b) Univesity of Mainz, CESifo and Univesité catholique de Louvain Apil 200 This pape povides the poofs to the analysis of a continuous time matching model with saving in Baye and Wälde (200a). The pape poves the esults on consumption gowth, povides an existence poof fo optimal consumption and a detailed deivation of the Fokke-Planck equations. JEL Codes: Keywods: C62, C65 continuous time uncetainty, Fokke-Planck equations, existence poof Intoduction The pape by Baye and Wälde (200a) BW0 in what follows studies optimal saving in a matching model in continuous time. It states many esults without poving them. All poofs ae pesented hee. This pape stats by ecapitulating the essential equations of BW0 in the next section. The Keynes-Ramsey ule (Eule equation) in BW0 descibes the impact of the inteest ate, the time-pefeence ate and the pecautionay savings tem on consumption gowth. Section 3 povides the poofs behind this desciption. This section also poves concavity of the value function, a esult which is useful fo numeical analysis. The only assumption we base ou poofs on is continuous di eentiability of the consumption function and a nite numbe of sign changes in a nite inteval. These ae vey weak assumptions which ae easily acceptable fo ou applications. Once the Keynes-Ramsey ule is undestood, BW0 continues by using a phase diagam to illustate consumption-wealth dynamics. The existence poof of optimal consumption paths that coesponds to the phase-diagam (in some appoximative sense) is povided in section 4. Such an existence poof is of impotance as it establishes that intuitive easoning is in fact tue. What is moe, as numeical identi cation Lage pats of this pape wee witten while the authos wee woking at the Royal Institute of Technology (KTH) in Stockholm and the Univesity of Glasgow, espectively. We ae gateful to these institutions fo thei stimulating eseach envionment. Chistian Baye: TU Belin, Institute of Mathematics, Staße des 7. Juni 36, 0623 Belin, bayemath.tu-belin.de, Klaus Wälde: Univesity of Mainz, Mainz School of Management and Economics, Jakob-Welde-Weg 4, 5528 Mainz. klauswaelde.com, We ae vey gateful to Walte Schachemaye fo comments and guidance, Michael Gabe, Giuseppe Moscaini, Sevi Rodíguez Moa, Josef Teichmann and Calos Caillo Tudela fo comments and Jeemy Lise fo discussions. The second autho is indebted to Ken Sennewald and Chistian Baue fo ealie collaboation on this topic. 2

4 of an optimal path is not always staightfowad, knowing that the objective one looks fo actually exists is vey eassuing. The analysis of BW0 becomes a geneal equilibium analysis by using Fokke- Planck equations to descibe the evolution of the density of the state vaiables ove time. This density is equied to close the model and obtain an endogenous inteest and wage ate which is linked to the aggegate capital stock. The deivation of these equations is in section 5. This deivation is elatively detailed in ode to show that applications in othe contexts ae possible as well. Having obtained Fokke-Planck equations as a tool to descibe the evolution of distibutions aises the question about existence, uniqueness and stability of the limiting distibution fo the state vaiables. A companion pape (Baye and Wälde, 200b) poves that the low inteest ate case exhibits a unique invaiant distibution and the system is egodic: the distibution always conveges to the invaiant distibution as time appoaches in nity. Ou poofs ae elated to vaious methods and stands in the liteatue. Tools fo the Keynes-Ramsey poofs ae elementay. The existence poof fo optimal consumption builds on the classical theoem of continuous dependence of the solution to an odinay di eential equation on its initial value. The poof continues by showing that hitting times ae continuous in initial values - which is fa fom obvious. We conclude by applying a vesion of the intemediate value theoem, speci cally designed fo ou pupose. We note that the classical theoy of odinay di eential equation, see, fo instance, Mattheij and Molenaa (2002) is only applicable in ou case afte some modi cations, because the ight hand side satis es the standad Lipschitz conditions only afte a vaiable tansfomation. The pinciples behind and the deivation of the Fokke-Planck equation fo Bownian motion ae teated e.g. in Fiedman (975, ch. 6.5) o Øksendal (998, ch. 8.). Fo ou case of a stochastic di eential equation diven by a Makov chain, we use the in nitesimal geneato as pesented e.g. in Potte (995, ex. V.7). Fom geneal mathematical theoy, we know that the density satis es the coesponding Fokke- Planck equation t p(t; x) = A p(t; x), whee p denotes the density of the pocess at time t and A is the adjoint opeato of the in nitesimal geneato A of the pocess (x is the state vaiable). We follow this appoach in ou famewok and obtain the Fokke-Planck equation fo the law of the employment-wealth pocess. Ou appoach constitutes a consideable genealization to the closed-fom solution esults used fo stuctual estimation e.g. by Posch (2009) o Aït-Sahalia (2004). In these models, estimation is possible only if a closed-fom solution fo the density can be found. In many othe stuctual estimation appoaches, at least some stuctue fo the density is known, e.g. the genealized exponential distibution in many duation models (Eckstein and Wolpin, 995, Cahuc et al., 2006 o Launov and Wälde, 200). In ou setup, the density is only implicitly given, i.e. one can deive densities fo estimating models with any dynamic popety which is based on Bownian motions o Poisson pocesses (o Lévy pocesses) and not only with popeties which allow fo a (closed to) closed-fom solution. As we pesent a vey detailed deivation of the di eential equations fo the density, it should be easy to use this tool fo stuctual estimation in othe contexts as well. Lo (988) deives a Fokke-Planck equation as 3

5 well fo a one-dimensional stochastic pocess. We povide a setup with two pocesses which also makes clea how the Fokke-Planck appoach can be genealized to thee o moe pocesses. 2 Backgound In ode to make this pape self-contained, we pesent all equations equied fo subsequent poofs in this section. The economic backgound of these equations is in Baye and Wälde (200a). 2. The model Conside an individual that behaves optimally, accoding to some objective function and given cetain constaints (see () and (2) below), by following a consumption function c (a () ; z ()). Aguments of this function ae the state vaiables wealth a () and the labou maket status z () 2 fw; bg : Wealth of such an individual follows the budget constaint da () = fa () + z () c (a () ; z ())g d () whee is the constant but endogenous inteest ate and z () simultaneously denotes labou maket income. Labou maket status and labou maket income follow a pocess z () diven by two Poisson pocesses with state-dependent aival ates, dz () = dq dq s ; w b: (2) Aival ates ae (b) = > 0 and (w) = 0 fo q and s (w) = s > 0 and s (b) = 0 fo q s : Since q s is only active when z is in the state w, while q is only active when z is in the state b, this equation implies that z () jumps between the states w and b: Labou income w (net wage) and b (unemployment bene ts) ae constant but endogenous as well. This implies that z() is a time-homogeneous Makov chain (in continuous time) with state space fw; bg. The instantaneous utility function is of the CRRA type, whee all poofs will wok with a positive 6= : 2.2 The educed fom u (c ()) = c (), (3) The educed fom in BW0 (sect. 4.2) descibing optimal behaviou is expessed with wealth a as the exogenous vaiable (instead of time t). De ning x(a) c(a; w); y(a) c(a; b); (4) 4

6 the educed fom can be witten as h i x(a) y(a) + s _x(a) = a + w x (a) h _y(a) = a + b y (a) y(a) x(a) i x (a) ; (5a) y (a) : (5b) Hee, _x and _y denote the espective deivatives of x and y with espect to a. Additional paametes appeaing hee ae the time pefeence ate ; the sepaation ate s and the matching ate plus the degee of isk-avesion : We will assume fo all poofs that < : This is a non-autonomous system due to the appeaance of a in the denominatos in both equations. BW0 has shown that thee is a natual boowing limit which implies that any solution to (5) must satisfy y ( b=) = 0: (6) 2.3 Bounday conditions When gaphically illustating the full stochastic system in a phase diagam, BW0 intoduced a point (a w; c (a w; w)) = (a w; x (a w)) in R 2 called tempoay steady state (TSS). At this point, the stochastic system (a(); c(a(); w)) (the stochastic Keynes- Ramsey ules and the budget constaints, see (8) () in BW0) is tempoaily (until the next jump of q s ) at est. We know about the TSS fom BW0 that x (a w) = a w + w; (7) and that the value of consumption afte a jump, i.e. c (a w; b) = y (a w) ; is given by y (a w) = x (a w) whee = < : (8) s In all cases whee is used, is su ciently low such that is a eal numbe. As the TSS must be pat of any optimal consumption path c (a; z) ; we ae inteested in solutions to the educed fom (5) which contain the point (a w; x (a w) ; y (a w)) : Note that this point is fom R 3 in contast to the TSS which is fom R 2 : Note also that this point is not a steady state of this ODE system: _y (a w) is negative and what is wose in a sense _x (a w) is not de ned as _x (a w) = 0=0. Fo the latte eason, BW0 intoduced an auxiliay tempoay steady state (atss) de ned by (a w; x v (a w)) fom R 2 whee x v (a w) = a w + w v (9) and whee v > 0 is an abitaily small positive numbe. This value fo x (a w) eplaces the value in (7). Obviously, (a w; x 0 (a w)) = (a w; x (a w)). The value fo y adjusts as well as it is given by y v (a w) = x v (a w) (0) 5

7 whee is the value in (8). This atss coesponds to a point (a w; x v (a w) ; y v (a w)) fo the ODE (5) fom R 3. This point, witten as v (^a) = (^a; x v (^a) ; y v (^a)) () will late seve as teminal values when solving ou ODE systems. depends on v. Note that 2.4 The famewok fo the poofs The only assumption we make fo ou poofs is an assumption on continuity. Assumption Relative consumption (a) c (a; w) =c (a; b) is continuously di eentiable in wealth a: The numbe of sign changes of 0 (a) in any inteval of nite length is nite. 2 This is obviously a vey weak assumption which does not impose any economically elevant estiction on ou solutions. In addition to this assumption, we have no ambition in undestanding the system (5) in all geneality. We athe estict ouselves to the domain whee equilibium dynamics take place. This egion was identi ed in the g. in BW0 as the one delimited by b= and a w fo wealth and by the zeo-motion lines fo consumption levels, whee we intepet the zeo-motion lines as planes in the (a; x; y)-space. Moeove, we estict ou attention to cases whee x y, i.e. the consumption of the unemployed cannot be lage than the consumption of the employed. 3 Altogethe, we conside the domain Q v = f(a; x; y) 2 R 3 j a b=; x a + w v; y a + b; y 0; x yg: (2) whee v is the small positive constant used in (9) as well. In the poofs, it will be convenient to estict attention to a bounded set. Thus, we conside R v; = Q v \ (a; x; y) 2 R 3 j x < ; a ( w + v)= (3) whee only seves to make R v; R 3 a compact set, which we need to obtain global, unifom Lipschitz constants. We shall see below that has to be chosen lage than. In this case, howeve, does not intefee with the constuction. 0 = w b ( ) 2 The second sentence of this assumption is equied to ule out pathological cases. One can constuct continuously di eentiable functions that change sign in nitely often in a nite neighbohood (think of x sin (=x) in a neighbohood of zeo). None of these functions would be economically plausible in any way. This second sentence is used in the poof of pop We will pove late in lem. 3.0 that x > y: In this sense, the estiction fo ou domain Q v is not binding in any economic sense. 6

8 3 Poof of the pedictions of the Keynes-Ramsey ule We will now pove pop. 3 of BW0. We epeat it hee fo efeence, as ou pop. 3.. Poposition 3. Conside a low inteest ate, i.e. 0 <. De ne a theshold level a w by u 0 (c (a w; b)) u 0 (c (a w; w)) : (4) s Fo ou instantaneous utility function (3), this de nition eads c (a w; b) = c (a w; w) (5) whee is fom (8). (i) Consumption of employed wokes inceases if the woke owns a su ciently low wealth level, a < a w. Employed wokes with a > a w choose falling consumption paths. (ii) Consumption of unemployed wokes always deceases. (iii) Consumption of employed wokes exceeds consumption of unemployed wokes at the theshold a w; i.e. in (5) fo : Let us ecall the ndings in BW0 on consumption gowth. Hee, and fo the emainde of this section, we use the notation as in BW0, i.e. a w and a b satisfy the ODE _a z () = a z () + z c(a z (); z) fo xed z 2 fw; bg. Lemma 3.2 (BW0) Individual consumption ises if and only if cuent consumption elative to consumption in the othe state is su ciently high. Fo the employed woke, consumption ises if and only if c (a w ; w) elative to c (a w ; b) is su ciently high, dc (a w (); w) d 0, u0 (c (a w (); b)) u 0 (c (a w (); w)) s, c (a w(); w) c (a w (); b) = ; (6) whee is fom (8). Fo the unemployed woke, consumption ises if and only if c (a b ; b) elative to c (a b ; w) is su ciently high, dc (a b (); b) d 0, u0 (c (a b (); w)) u 0 (c (a b (); b)) : (7) 3. Poof of pat (i) 3.. A local esult We st show that consumption c (a w ; w) ises in time fo wealth smalle than but close to a w. 7

9 Given that, by ass., the numbe of sign changes of 0 (a) in any inteval fo a of nite length is nite, fo any a 0 we can nd an " > 0 such that (a) c (a; w) =c (a; b) is monotonic in [a 0 "; a 0 ]. Exploiting this fo a w; whateve the popeties of elative consumption, we can always nd an " such that one of the following thee cases must holds fo " [a w "; a w[ 9 8 = < (i) (ii) (iii) ; 0 (a)j a2" : < > = 9 = ; 0: Note that we do not make any statement about the deivative in a w: In fact, in case (i) 0 (a)j a2a w can be negative o zeo, in case (ii), it can be positive o zeo. Lemma 3.3 (a) Consumption of employed wokes ises ove time fo a wealth level a 2 " if and only if case (i) holds, dc (a w (); w) d > 0 fo a w () 2 ", case (i) holds. (b) Consumption c (a w (); w) falls ove time fo a w () 2 " if and only if (ii) holds. dc(a Poof. (a) By (6), w();w) > 0, c (a d w (); w) =c (a w (); b) > =. As c (a w; w) =c (a w; b) = = at a w, as w and b ae paametes and using ass., this is a condition on the deivative of elative consumption with espect to wealth a in " : dc (a w (); w) =d is positive fo a w () 2 " if and only if case (i) holds. (b) By (6), consumption falls ove time if elative consumption lies below = : This can be the case in " only if case (ii) holds. Lemma 3.4 Relative consumption falls in wealth fo a 2 ", 0 (a)j a2" case (i) holds. < 0; i.e. Poof. a) Assume that case (ii) holds, i.e. 0 (a)j a2" > 0. Then, by lem. 3.3, dc(a w();w) < 0 fo a d w () < a w: Consumption of unemployed wokes would still decease in time fo all wealth levels. In ou set Q v, daw() > 0 and theefoe dc(a;w) < 0: d da As dc(a b();b) < 0 and da b() < 0 in Q d d v ; we know that dc(a;b) > 0: As a consequence, da 0 (a) < 0: This contadicts the assumption that case (ii) holds and case (ii) can be excluded. b) Now assume that case (iii) holds, i.e. elative consumption is at, 0 (a)j = a2"[a w 0. As c (a w; w) =c (a w; b) = =, dc (a w (); w) =d = 0 fo a w () 2 " : As dc (a b (); b) =d < 0; elative consumption is not constant which contadicts the assumption that elative consumption is at in wealth. As case (iii) is theeby excluded as well, the poof is complete. 8

10 3..2 A global esult We now complete the poof by a global esult on consumption gowth. Lemma 3.5 Consumption c (a w ; w) (a) ises in time fo all a < a w and (b) deceases in time fo all a > a w. Poof. (a) Imagine to the contay of c (a w ; w) ises in time fo all a < a w that thee is an inteval ] ; 2[ with 2 < a w such that this is is the last inteval befoe a w whee c (a w ; w) falls in time, dc (a w (); w) =d < 0; 8 < a w () < 2 < a w: (8) We now poceed as in the poof of lem As daw() > 0 in Q d v ; this would imply that dc(a;w) < 0 fo da < a < 2 : We know that dc(a;b) > 0 in Q da v : Hence, we would conclude that 0 (a) < 0; 8 < a < 2 : (9) By (6), the assumption in (8) would hold if and only if elative consumption c(a w;w) dc(a c(a w;b) is below = fo < a < 2 : w();w) < 0, c(aw();w) c(a;w) d c(a w();b) < = : As is c(a;b) continuous in wealth by ass. and as case (i) holds by lem. 3.4, c(a;w) can be smalle c(a;b) than = only if thee is some ange ] 3; 2[ in which 0 (a) > 0: (An example of such a path is shown in g..) This is a contadiction to the conclusion in (9). Hence, consumption must ise in time fo all a < a w: (b) This poof is in analogy to the poof of (a). Figue An example fo elative consumption (a) c(a;w) c(a;b) 9

11 3.2 Intemediay steps Befoe we pove the est of pop. 3., we need some futhe intemediay esults which, howeve, ae of some inteest in thei own ight. Given that maginal utility fom (3) is positive and deceasing, u 0 (c) > 0 and u 00 (c) < 0; we can establish that x (a) > y (a) ; i.e. consumption in the state of employment is lage than in the state of unemployment, keeping wealth constant. We pove in passing that the value functions V (a; z) ae stictly concave in wealth a: Lemma 3.6 Consumption ises in wealth, c a (a; z) > 0: Poof. Pop. 3. (i) shows that dc (a w (); w) =d > 0 in Q v : As da w ()=d > 0 as well, the deivative _x (a) in (5) is positive in Q v : Lemma 3.7 As maginal utility fom consumption is positive, the value function V (a; z) ises in wealth, V a (a; z) > 0: Poof. The st-ode condition fo optimal consumption is given by (47) in the appendix and eads u 0 (c (a; z)) = V a (a; z) : (20) As maginal utility is positive by (3), the value function ises in wealth. Lemma 3.8 As u 00 (c) < 0 and as consumption ises in a by lemma 3.6, the value function is stictly concave in a. Poof. The patial deivative of the st-ode condition with espect to wealth implies u 00 (c (a; z)) c a (a; z) = V aa (a; z) : (2) As u 00 (c (a; z)) < 0 fom the concavity of (3) and c a (a; z) is positive by lem. 3.6, V aa (a; z) must be negative. With lem. 3.7, the value function is stictly concave. Lemma 3.9 The shadow pice fo wealth is highe in the state of unemployment, V a (a; b) > V a (a; w) : Poof. The deivation of the Keynes-Ramsey ule gives us (see app. A.) ( ) V a (a; z) s (z) [V a (a; b) V a (a; w)] (z) [V a (a; w) V a (a; b)] = [a + z c (a; z)] V aa (a; z) : In state z = w; this means ( ) V a (a; w) s (z) [V a (a; b) V a (a; w)] = [a + w x (a)] V aa (a; w) : (22) Given the egion we ae inteested in (whee a + w x (a) > 0) and given lemma 3.8, the ight-hand side is negative. Hence, the left-hand side must be negative as well. As ( ) V a (a; w) is positive due to <, the second tem must be negative. This is the case only fo V a (a; b) > V a (a; w) : 0

12 Lemma 3.0 Consumption of the employed woke is highe than consumption of the unemployed woke, x (a) > y (a) : Poof. As V a (a; b) > V a (a; w) ; the st-ode condition implies u 0 (c (a; b)) > u 0 (c (a; w)) : As the maginal utility is deceasing, c (a; w) > c (a; b), x (a) > y(a): 3.3 Poof of pats (ii) and (iii) We now complete the nal bits of the poof. Poof of pop. 3. continuation. (ii) By (7), dc (a b (); b) =d < 0, u 0 (c (a b (); w)) < {u 0 (c (a b (); b)) whee { as : As u0 (c (a b (); w)) < u 0 (c (a b (); b)) with c (a b (); w) > c (a b (); b) fom lem. 3.0, this condition always holds. (iii) This follows fom solving (4) fo elative consumption. 4 The existence of an optimal consumption path De nition 4. (Optimal consumption path) (i) A consumption path is a solution 4 (a; x(a); y(a)) of the ODE-system (5) fo the ange b= a ^a in R v; with teminal condition fom (). 5 The teminal condition satis es (9), (0) fo an abitay ^a > b=: (ii) An optimal consumption path is a consumption path which additionally satis- es y ( b=) = 0: If such a path exists, we denote the wealth level ^a of the teminal condition by a w. We emak that the notion of an optimal consumption path depends on v (via ). The objective of this section consists in poving the following Theoem 4.2 Thee is an optimal consumption path. 4. Peliminaies In what follows, we will use classical theoems fo initial value poblems fo ODEs. Cuently, we have fomulated ou system (5) as a teminal value poblem, since we have set a value, which the system should attain at ^a = a w, i.e. at the end of the inteval [ b=; a w] unde consideation. Fo ease of notation and to help intuition, we shall now ecast the poblem into a classical initial value poblem, i.e. we will equie the value to be attained at the xed beginning = 0 of an inteval [0; ], on which we study the poblem. 4 By a solution to (5), we hee undestand continuous maps x : [ b=; ^a]! R, y : [ b=; ^a]! R, which ae continuously di eentiable in ] b=; ^a[ and solve (5a) and (5b), espectively, in the open inteval. In paticula, we do not equie the deivatives of x and y to convege fo a! b=. 5 In the sense that an optimal consumption path satis es x(^a) = x v (^a), y(^a) = y v (^a).

13 To this end, it is moe useful to wok with an autonomous system. Hence, we ewite (5) by including m (a) = a as thid vaiable which eplaces wealth a, which now puely seves as a paamete, i.e. as the independent vaiable. This gives the system _m(a) = ; h i + s x(a) y(a) _x (a) = m (a) + w h _y (a) = m (a) + b x (a) i y(a) x(a) y (a) x (a) ; y (a) : Now de ne ^a a, x () m (^a ), x 2 () x (^a ), x 3 () y (^a ) : d Then, x d () _x () = d d m (^a ) = m (a) = d m (a) = _m (a) : Doing d d[^a a] da the same fo x and y; the inveted autonomous system theefoe eads _x () = ; (23a) h i + s x2 x 3 () x 2 () _x 2 () = x () + w x 2 () ; (23b) h i x2 () x 3 () x 3 (a) _x 3 () = x 2 () + b x 3 () ; (23c) whee now _x i denotes the deivative of x i () with espect to, i = ; 2; 3. De nition 4.3 Given (23) and fo 0; let X(; ) = (x (); x 2 (); x 3 ()) denote the solution of (23) stated at X(0; ) = 2 R v; fom () whee b= ^a +v w. Fo late use, we also intoduce the notation x i () = x i (; ), i = ; 2; 3. By passing fom (5) to (23) we have eveted the time-diection moe pecisely, in ou setting, the wealth-diection and tuned a non-autonomous system into an autonomous one by including the independent vaiable as an additional component of the solution. Thus, the cuve a 7! (a; x(a); y(a)) with teminal value x(^a) = x v (^a), y(^a) = y v (^a) is equal to the cuve 7! X(; ) with = (^a), which is the solution of an initial value poblem in the classical sense. Howeve, the paametization is eveted in the sense that in the fome case we stat at the left endpoint ( left in the sense of the smallest value of the a-component) and end in the ight endpoint, wheeas in the latte case we stat at the ight endpoint and end in the left one. In paticula, the absolute value of the speed long the cuve is equal, but the diection is evesed. 4.2 Continuity of the solution in initial values In ode to be able to apply classical theoems, we need nite deivatives on the ighthand side of an ODE system. The ight-hand side of the ODE (5), howeve, exhibits 2

14 singulaities at the bounday y = a+b of Q v : This is of paticula impotance as the de nition of the optimal consumption path in De nition 4. uses y ( b=) = 0 which lies on this bounday. We obtain nite deivatives by (i) a coodinate tansfomation and by (ii) (tempoaily) educing the set on which we ae inteested in a solution by demanding that y ". We will late show how this eduction can then be emoved again by passing "! 0. Lemma 4.4 (Coodinate tansfomation) Let x(a) and y(a) be solutions of (5). The mapping a 7! y(a) is bijective. Change vaiables a = a(y) and conside x and a as functions of y. Then i x 0 (y) dx(y) dy a 0 (y) da(y) dy = = + s h x(y) y h y x(y) a(y) + b y h y x(y) i x(y) y i y : a(y) + b y a(y) + w x(y) ; (24a) (24b) Poof. Since _y(a) > 0, y is a bijective function of a: As a 0 (y) =, we obtain _y(a) the second equation by inseting (5b). The st equation follows fom dividing (5a) by (5b). We ae going to avoid the singulaity at y ( b=) = 0 by tempoaily equiing these popeties only to hold up to an abitaily small numbe ". We do this by consideing the domain R ";v; as given in the following De nition 4.5 Fix a numbes " > 0 and de ne R ";v; = R v; \ (a; x; y) 2 R 3 j y " : (25) This de nition implies that we tempoaily eplace the equiement that y ( b=) = 0 by y (a) = " fo some b= a b= + "=. Lemma 4.6 The ight-hand side given in (24) is unifomly Lipschitz on R ";v;. Poof. Conside the ight-hand side of (24a). The only possible points, whee the Lipschitz constant can explode, ae when the denominatos in the ight-hand side become 0 o when a tem unde a factional powe (i.e. with exponent ) becomes 0. In R = R ";v;, y is unifomly bounded away fom 0 and x is unifomly bounded away fom a+w. Moeove, note that y x = 0 if and only if y x =. Now > by the assumption that <. On the othe hand, y < x, implying y that x <. Consequently, all the denominatos ae unifomly bounded away fom 0. Fo the factional powes, note that x=y > is tivially unifomly bounded away fom 0. As x, y x > 3

15 is unifomly bounded away fom 0 on R ";v;. This shows that (24a) is unifomly Lipschitz. The same aguments show that the ight-hand side of (24b) is unifomly Lipschitz, too. Remak 4.7 Since the ight hand side of (24) is unifomly Lipschitz, we can now apply the classical theoy of ODEs. Fo instance, we have existence and uniqueness of the solution by the Picad-Lindelöf theoem, see Mattheij and Molenaa (2002, th. II.2.3, th. II.3.). Moeove, the solution will be continuous as a function of the initial value, see, again, Mattheij and Molenaa (2002, th. II.4.7). In the lemma below, we will see how this even implies the coesponding popeties fo the nontansfomed system (23). Lemma 4.8 (Continuity in initial values) Conside the set R = R ";v; fom (25) and the solution X(; ) fom De nition 4.3 with initial condition given in (). The solution X(; ) depends continuously on its initial values. Moe pecisely, thee is a constant L > 0 and an inceasing map : [0; [! [0; [ (a modulus of continuity) with lim t&0 (t) = (0) = 0 such that kx( ; ) X( 2 ; 2 )k Lk 2 k + (j 2 j); povided that ; 2 2 R and X(; i ) 2 R fo all 0 max( ; 2 ), i = ; 2. Hee, kk denotes the Euclidean nom on R 3. Poof. By classical esults fom the theoy of odinay di eential equations, see fo instance Mattheij and Molenaa (2002, th. II.4.7), the solution of an ODE-system depends continuously on the initial data as long as the ight-hand side is unifomly Lipschitz. Moe pecisely, let Y (; ) denote the solution of an ODE with unifomly Lipschitz ight-hand side (with Lipschitz constant C), stated at Y ( 0 ; ) =, then ky (; ) Y (; 2 )k exp (C( 0 )) k 2 k: Now conside the tansfomed system (a(y); x(y)) fom (24). By Lemma 4.6, the ight-hand side is unifomly Lipschitz. The solution of (24) theefoe depends continuously on its initial data (a 0 ; x 0 ). It is then obvious that the tajectoy (a(y); x(y); y) depends continuously on (a 0 ; x 0 ; y 0 ): As system (24) is a epaameteized vesion of (5), the solution (a; x (a) ; y (a)) to (5) fom def. 4. is also continuous in its bounday conditions even though the ight hand side of (5) is not unifomly Lipschitz. Similaly, as (23) is just a epaameteization of (5), the solution X (; ) to (23) fom def. 4.3 is also continuous in its initial condition. In ode to get the estimate, we now conside the ODE (23) and note that we only conside it on the compact set R ";v;. In the paametization by y given in (24), y is the independent vaiable, i.e. plays the ole of in the above estimate. By compactness of R ";v;, y only uns though a bounded set, theefoe we can ewite the constant in the above inequality as exp(c(y y 0 )) L fo some suitable L > 0. 4

16 Given 2 R ";v;. Then a w w+v, which implies that the solution X(; w) can only stay inside R ";v; until time = w+v+b, at most. Conside D = f(; ) 2 [0; [R ";v; j X(; ) 2 R ";v; g: Then D is a closed subset of 0; w+v+b R";v;, implying that D is compact. Consequently, X : D! R ";v; is unifomly continuous, which implies the existence of a modulus of continuity with kx( ; ) X( 2 ; 2 )k (j 2 j + k 2 k): The inequality in the lemma then follows by the tiangle inequality. 4.3 Continuity of the st hitting-wealth in initial values While we have shown in the pevious section that the solutions to all systems (5), (23) and (24) ae continuous in initial values, this does not automatically imply that the solutions will be continuous on the bounday of the domain we ae inteested in, in the sense that the place whee the solution leaves the domain R might not depend continuously on the initial data. This will now be poved in this section. In the poofs and also in a late step, we will use the following De nition 4.9 (Fist hitting-wealth) Conside the set R ";v; fom (25) and the solution X (; ) to the system (23). Conside the path y (a) that coesponds to x 2 () of this solution. Then we de ne ^a st = f (^a) as the st hitting-wealth (in analogy to st hitting-time), i.e. the wealth level whee the path y (a) hits any bounday of R ";v; fo the st time. Similaly denote () inff 0 j X(; ) 2 R ";v; g and F () X((); ). We know that ^a st exists because in the set R ";v; the deivatives in (23) ae wellde ned and a solution theefoe exists. Notice that ^a st equals the st component of F ((^a)). We also need De nition 4.0 Let N R ";v; with N = (^a) b ^a 2 ; [w v] b [ ] be the set of all potential initial conditions fom () fo a solution in the sense of def. 4.. Hee we implicitly assume that is lage enough that indeed N R ";v;. 6 De ne M as M = M [ M 2 [ M 3 R ";v; (26) 6 This is the only necessay condition on fo the constuction to wok. In the sequel, we shall assume this condition without futhe notice. 5

17 with M = f(a; x; y) 2 R ";v; j y = a + bg; M 2 = f(a; x; y) 2 R ";v; j a = b=g; M 3 = f(a; x; y) 2 R ";v; j y = "g: This set will tun out to be the set of all potential st hitting-wealths. Since we know that x > y, the tajectoy will not hit the bounday of R at the pat fx = yg. Theefoe, we have the Coollay 4. F : N! M is a well-de ned map fom R 3 to R 3, i.e. fo evey 2 N, the coesponding solution path X(; ) exists and stays in R ";v; until it nally hits M (and no othe bounday of R ";v; ). Befoe fomulating the main lemma of this section, let us st deive a simple bound on the deivative _y(a) of the consumption of the unemployed. Lemma 4.2 Fo (a; x; y) in the inteio of Q v fom (2), we have Poof. By (5b) we have h _y (a) = y(a) x(a) _y(a) i a + b y (a) 0 = a + b y (a) y (a) a + b h a + b y(a) y(a) x(a) y(a) : i y (a) A y (a) > a + b y (a) y (a) : The last inequality follows fom the fact that [ ( x(a)) y(a) ] is negative (and theefoe a+b y(a) [ ( x(a)) y(a) ] is positive) as a + b y (a) is negative in the inteio of Q a+b y(a) v. The key esult in this section is pesented in Lemma 4.3 The map F : N! M is continuous. Poof. We need to pove that fo evey 2 N and evey > 0 thee is an > 0 such that k 0 k < =) kf ( 0 ) F ()k < : (27) We stat the poof by xing 0 ; 2 N such that k 0 k < fo some > 0. Let us st assume that ( 0 ) (). By the tiangle inequality and Lemma 4.8, we have kx(( 0 ); 0 ) X((); )k kx(( 0 ); 0 ) X(( 0 ); )k + + kx(( 0 ); ) X((); )k L k 0 k + (j( 0 ) ()j); (28) 6

18 fo a constant L > 0 and the modulus of continuity. In ode to get an estimate fo j( 0 ) ()j, we have to distinguish between thee di eent cases. Case (i): F ( 0 ) 2 M. By Lemma 4.2, thee ae constants L 2 ; `2 > 0 such that _y L 2 fo jy (a+b)j `2. Moe pecisely, we can choose `2 > 0 feely and obtain the bound fo L 2 = `2 ( )". If L `2, we can bound the absolute value of the deivative of x 3 (; ) fom below by L 2 (fo t ( 0 )). This implies that the path X(; ) hits M befoe time ( 0 ) + fo (L 2 ) = `2 () = `2 L 2 ; unless it hits anothe bounday of R ";v; befoe that. Inseting into (28), this gives the estimate `2 kf ( 0 ) F ()k L + : Choosing `2 = L, the bound is smalle than povided that! L C L L 2 + L < ; (29) whee C ( )". Note that the left hand side in (29) conveges to zeo fo! 0, theefoe we can nd an 0 () > 0 (only depending on the constants C, L and and the modulus of continuity, but not on 0 o ) such that the desied inequality (27) holds fo < 0. We have tacitly assumed that L 2 = C=`2 = C L >, which can be ealized by choosing small enough. Case (ii): F ( 0 ) 2 M 2. Let ^a denote the st component of, and ^a 0 the st component of 0. Note that x (; ) = ^a, fo evey 0. Since X(( 0 ); 0 ) 2 M 2, we have b= = x (( 0 ); 0 ) = ^a 0 ( 0 ), implying that ( 0 ) = ^a 0 + b=. On the othe hand, x ((); ) b=, implying that () ^a + b=. Combining these two esults, we obtain j( 0 ) ()j = () ( 0 ) ^a ^a 0 k 0 k : Consequently, the inequality (28) implies kf ( 0 ) F ()k L k 0 k + (k 0 k) L + (); and (27) holds fo small enough such that L + () < : (30) Case (iii): F ( 0 ) 2 M 3. Since x 3 (( 0 ); 0 ) = ", we have 0 x 3 (( 0 ); ) " L. By Lemma 4.2, we can nd a constant L 3 > 0 such that _y L 3 on R ";v; note that L 3 depends on ". Thus, X(s; ) will hit the bounday M 3 befoe time ( 0 ) + with = L =L 3, unless it hits anothe bounday of R ";v; befoe. In any case, j( 0 ) ()j L =L 3, and we obtain L kf ( 0 ) F ()k L + ; L 3 7

19 and (27) is satis ed fo L L + < : (3) L 3 Choosing small enough that both (29) and (30) and (3) ae satis ed, settles the poof fo ( 0 ) (). Notice that none of the conditions (29), (30) and (3) depends on 0. Theefoe, in the othe case ( 0 ) (), we can just evet the ôles of and 0 and obtain the same esults in cases (i), (ii) and (iii). 4.4 Existence of a solution This section poves ou main esult fomulated in Theoem 4.2. Poof of Theoem 4.2. Fix some " > 0 and conside R ";v;. By an intemediate value theoem applied to F : N! M, we will obtain a point o points 2 N such that F () 2 M 3 as used in (26), i.e. x 3 ((); ) = " povided that we can show the existence of points (that could be called uppe and lowe bounds) min v ; max v 2 N with F ( min v ) 2 M 2 and F ( max v ) 2 M. (Note that F = F " and all the M i = M i ("), i = ; 2; 3, depend on " and v, but not on, povided that is lage enough.) Choose min v = ( b=) = ( b=; w b v; [w b v]); max v = (w v) b ( ) By constuction, both min v and max v ae contained in N. Moeove, we tivially have F " ( min v ) 2 M 2 ("), F " ( max v ) 2 M (") fo evey " > 0 small enough. Note, in paticula, that Lemma 4.3 also implies continuity of F in the bounday points min v and max v of N. Theefoe, the image set F " (N) is a connected set, with non-empty intesection with both M and M 2. Since the distance dist(m ; M 2 ) = inf fk 2 k j 2 M ; 2 2 M 2 g = " > 0; we may conclude that F " (N) \ M 3 (") 6= ;. This establishes that thee must be a such that F " () 2 M 3 : In wods, thee is an initial condition (^a) such that the path (a; x(a); y (a)) hits the bounday at y = ": Now de ne N 3 (") F " (M 3 (")) = f 2 N j F " () 2 M 3 (")g : By continuity of F " : N! M("), the set N 3 (") is compact. Moeove, the family (N 3 (")) ">0 is diected in the sense that 0 < " 2 < " =) N 3 (" 2 ) N 3 (" ): By standad esults fom topology, the intesection of a diected family of non-empty, compact sets is non-empty, i.e. N 3 (0) \ ">0 N 3 (") 6= ;: : 8

20 Indeed, take a deceasing sequence (" n ) n of positive numbes conveging to zeo. Fo evey n choose some n 2 N 3 (" n ). By compactness of the lagest set N 3 (" ), we can nd a subsequence n k such that ( nk ) k conveges to some. Note that 2 N 3 (" nk ) fo evey k, since = lim l!; lk nl and each such nl lies in the closed set N 3 (" nk ). Now choose any " > 0 and pick a k such that " nk < ". Then 2 N 3 (" nk ) N 3 ("), implying that 2 T ">0 N 3("). We claim that evey element 2 N 3 (0) coesponds to an atss. Indeed, the path (a; x(a); y(a)) with teminal value (^a; ^x; ^y) = (coesponding to the path X(; )) satis es the ODE (5) on ] b=; ^a]. Moeove, it stats at N by constuction, and fo evey " > 0, it takes on the value " somewhee on the inteval ] b=; b= + "[. Thus, using monotonicity of y, we may conclude that lim y(a) = 0: a& b= This establishes that thee is an initial condition (^a) such that the path y (a) hits the bounday at y = 0 in the sense that y( b=) = 0. Remak 4.4 It is essential fo the poof of Theoem 4.2 that the tajectoy X(; ) o, equivalently, (a; x(a); y(a)) does not depend on ", which only detemines how long we obseve the tajectoy. This means that we obseve the tajectoy X(; ) fo 0 (), with the hitting time () obviously depending on ". Theefoe, we can, fo xed 2 N 3 (0), easily take the limit "! 0, which means that we take the limit in (), but do not change the tajectoy itself. As a consequence, the ODE is automatically satis ed fo the limit, at least fo 0 < lim "!0 (). Let us illustate why we had to use the speci c popeties of the dynamic system (23) in the poof of lem Continuity in initial conditions does not imply continuity of st hitting values in geneal. Indeed, the st hitting times ae inheently non-continuous functionals, even if both the paths and the set, which detemines the hitting times, ae smooth. This is sketched in ex Figue 2 Non-continuity of the st hitting time in ex

21 Example 4.5 Conside the di eential equation _z (t) = ( z (t)) z (t) whose solution is z (t) = + z0 e t : This solution is continuous in the initial level z 0 (fo z 0 > 0 which we assume) and the solution is plotted fo z 0 2 f0:; 0:2g in g. 2. Now conside the st-hitting time on the staight line 0:05 + t=5 as dawn. Obviously, this time is not continuous in the initial values z 0. 5 Deiving the Fokke-Planck equations This section deives the Fokke-Planck equations of the wealth-employment pocess (a(t); z(t)) as descibed in Section 2, i.e. the patial di eential equations which descibe the dynamics in time of the density of these andom vaiables. The deivation is in geat detail as this facilitates applications fo othe puposes. Befoe we go though individual steps, hee is the geneal idea. Step : We stat with some function f having as aguments the vaiables whose density we would like to undestand. We compute the di eential of this function in the usual way. Step 2: The stating point hee is Dynkin s fomula. This fomula, intuitively speaking, gives the expected value of some function f; whose aguments ae the andom vaiables we ae inteested in, as the sum of the cuent value of f plus the integal ove expected futue changes of f. The expected change of f is expessed by using the density of ou andom vaiables. The Dynkin fomula is di eentiated with espect to time. Step 3: By using integation by pats o the adjoint opeato, we get an expession fo the change of the expected value of f: Step 4: A di eent expession fo this change of the expected value can be obtained by stating fom the expected value and di eentiating it. Step 5: Equating the two gives the di eential equations fo the density. 5. The expected change of some function f Assume thee is a function f having as aguments the state vaiables a and z. This function has a bounded suppot S, i.e. f(a; z) = 0 outside this suppot. 7 Heuistically, the di eential of this function, using a change of vaiable fomula, 8 gives df (a () ; z ()) = f a (:) fa () + z () c (a () ; z ())g d + ff (a () ; z () + ) f (a () ; z ())g dq + ff (a () ; z () ) f (a () ; z ())g dq s : Due to the state-dependent aival ates (see table ), only one Poisson pocess is active at a time. When we ae inteested in the expected change, we need to fom expectations. We view a () and z () with t as two stochastic pocesses which stat in t and whee initial conditions a (t) and z (t) can be andom vaiables. We theefoe fom expectations about df by using the unconditional expectations opeato 7 We can make this assumption without any estiction. As we will see below, this function will not play any ole in the detemination of the actual density. 8 Thee ae fomal deivations of this equation in mathematical textbooks like Potte (995). Fo a moe elementay pesentation, see Wälde (2009, pat IV). 20

22 E as the andomness of initial values ae then also taken into account. This is useful fo its geneality and also when it comes to applications (see the discussion in BW0 on initial conditions and especially distibutions). Applying the conditional expectations opeato E and dividing by d yields the heuistic equation E df (:) d = f a (:) fa () + z () c (a () ; z ())g + [f (a () ; z () + ) f (a () ; z ())] fbg (z()) + s [f (a () ; z () ) f (a () ; z ())] fwg (z()) (32) In what follows, we denote this expession by Af (a () ; z ()) E df (a () ; z ()) d which is, moe pecisely, the in nitesimal geneato A de ned by (33) E (f(z( + ); a( + ))jz() = z; a() = a) f(a; z) Af(a; z) = lim : &0 Notice that Af(a; z) does not depend on, because the Makov-pocess (a(); z()) is time-homogeneous. We undestand A as an opeato mapping functions (in a and z) to othe such functions. Moeove, note that all test-functions, i.e. C functions of bounded suppot, ae in the domain of the opeato A, i.e. the domain of all functions f such that the above limit exists (fo all a and z). 5.2 Dynkin s fomula and its manipulation To abbeviate notation, we now de ne x () (a () ; z ()) : The expected value of ou function f (x ()) is by Dynkin s fomula (e.g. Yuan and Mao, 2003) given by Ef (x ()) = Ef (x (t)) + Z t E (Af (x (s))) ds: (34) To undestand this equation, use the de nition in (33) and fomally wite it as Ef (x ()) = Ef (x (t)) + Z t Edf (x (s)) ds = Ef (x (t)) + ds Z t Edf (x (s)) : Intuitively speaking, Dynkin s fomula says that the expected value of f (x ()) is the expectation fo the cuent value, Ef (x (t)) (given that we allow fo a andom initial condition x (t)), plus the sum of expected futue changes, R Edf (x (s)) : t Let us now di eentiate (34) with espect to time and nd Ef (x ()) = Z t E (Af(x (s))) ds = E (Af (x ())) ; (35) 2

23 whee the st equality used that Ef(x (t)) is a constant and pulled the expectations opeato into the integal. This equation says the following: We fom expectations in t about f (x ()) : We now ask how this expectation changes when moves futhe into the futue, i.e. we look at E [f (x ())]. We see that this change is given by the expected change of f(x ()); whee the change is Af (x ()) : Now de ne p (a; z; ) as the joint density of z () and a (). Notice that z; a and ae independent vaiables now: as soon as we integate with espect to the density p(a; z; ), the whole time-dependence has been absobed into. The expectation opeato E integates ove all possible states of x () : When we expess this joint density as p (a; z; ) p (a; jz) p z (), we can wite equation (35) as Ef (x ()) = E (Af (x ())) = p w () Z Af (a; w) p (a; jw) da + p b () Z Af (a; b) p (a; jb) da: Now pull p w () and p b () back into the integal and use p (a; z; ) p (a; jz) p z () again fo z = w and z = b. Then Ef (x ()) = Z Af (a; w) p (a; w; ) da + Z Af (a; b) p (a; b; ) da w + b : (36) Remak 5. The law of x() will not have a density, unless we aleady stat with a density at the initial time t. In geneal, p will theefoe be a measue o a distibution (in the sense of a genealized function, see (Yosida 995), not a tue function. Even in that case, the following deivation emains valid, though, using the usual calculus fo genealized functions. 5.3 The adjoint opeato and integation by pats This is now the cucial step in obtaining a di eential equation fo the density. It consists in applying an integation by pats fomula which allows to move the deivatives in Af(x ()) into the density p (x; ) : Let us bie y eview this method, without getting into technical details. Given two functions f; g : R! R and two xed eal numbes c < d, the facto ule of di eentiation d(f(x) g(x)) = df(x) g(x) + f(x) dg(x) (37) implies that f(d)g(d) f(c)g(c) = R d f 0 (x)g(x)dx+ R d c c f(x)g0 (x)dx; a fomula efeed to as patial integation ule. In paticula, it also holds fo c = and d = +, if the function evaluations ae undestood as limits fo c! and d! +, espectively. If f has bounded suppot, i.e. is equal to zeo outside a xed bounded set, then the function evaluations at vanish and we get Z + f 0 (x)g(x)dx = Z + f(x)g 0 (x)dx: (38) 22

24 We now apply (38) to equation (36). We can do this as the expessions in (36) lost all stochastic featues. To this end, inset the de nition of A given in (33) togethe with (32) into (36). To avoid getting lost in long expessions, we look at the both integals in (36) in tun. Fo the second, obseve that Af (a; b) = f a (:) fa + b c (a; b)g + [f (a; w) f (a; b)] ; i.e. the tem with s in (32) is missing given that we ae in state b. Hence, b = = + Z Z Z [f a (a; b) fa + b c (a; b)g + [f (a; w) f (a; b)]] p (a; b; ) da f a (a; b) fa + b [f (a; w) c (a; b)g p (a; b; ) da f (a; b)] p (a; b; ) da: Now integate by pats. As this integal shows, we only need to integate by pats fo the f a tem. The est emains untouched. This gives with (38), whee g (x) stands fo fa + b c (a; b)g p (a; b; ) and x fo a; b = + Z Z f (a; b) c (a; b) p (a; b; ) + fa + b c (a; b)g a a p (a; b; ) da [f (a; w) f (a; b)] p (a; b; ) da: (39) Now look at the st integal of (36). Afte simila steps (as the pinciple is the same, we eplace b by w and the aival ate by s in the last equation), this eads Z w = f (a; w) c (a; w) p (a; w; ) + fa + w c (a; w)g a a p (a; w; ) da + Z s [f (a; b) f (a; w)] p (a; w; ) da: (40) Summaizing, we nd = Z Z Z Z f (a; w) s [f (a; b) f (a; b) Ef (x ()) = w + b c (a; w) p (a; w; ) fa + w c (a; w)g a a p (a; w; ) da f (a; w)] p (a; w; ) da c (a; b) p (a; b; ) fa + b c (a; b)g a a p (a; b; ) da [f (a; w) f (a; b)] p (a; b; ) da: (4) 23

25 5.4 The expected value again and nish The expected value again Let us now deive the second expession fo the change in the expected value. By de nition, and as an altenative to the Dynkin fomula (34), we have Ef (x ()) = Z f (a; b) p (a; b; ) da + Z When we di eentiate this expession with espect to time, we get Note that we can use Z Ef (x ()) = + Z Z f (a; z) p (a; z; ) da = f (a; b) p (a; b; ) da f (a; w) p (a; w; ) da: (42) f (a; w) p (a; w; ) da: (43) Z f (a; z) p (a; z; ) da as z and a inside this integal ae no longe functions of time. Step 5 - Equating the two expessions We now equate (4) with (43). Collecting tems belonging to f (a; w) and f (a; b) gives Z Z f (a; w) ' w da + f (a; b) ' b da = 0; (44) whee ' w c (a; w) + s p (a; w; ) a fa + w c (a; w)g p (a; w; ) a + p (a; b; ) p (a; w; ) and ' b + sp (a; w; ) c (a; b) + p (a; b; ) a fa + b c (a; b)g p (a; b; ) a p (a; b; ) : Obviously, the above equation is satis ed if These ae the Fokke-Planck equations used in BW0. ' b = ' w = 0: (45) 24

26 It is easy to see that the integal equation can only be satis ed fo all functions f, if these Fokke-Planck equations ae satis ed. Indeed, assume that ' b > 0 on an inteval I = [d ; d + ]. One can nd a non-negative function f smooth in a such that f(a; w) = 0 fo all a and ( ; a 2 [d =2; d + =2]; f(a; b) = 0; a 2] ; d ] [ [d + ; [: Inseting this test function into the integal equation gives Z f (a; w) ' w da + Z f (a; b) ' b da = 0 + Z d+ d f (a; b) ' b da > 0 by constuction. Theefoe, ' b = 0 has to hold fo all a 2 R, and similaly fo ' w. 6 Conclusion This pape poves the esults stated in Baye and Wälde (200a). In section 3, we pove concavity of the value function and the link between the inteest ate and consumption gowth. This poof is of inteest as it is based only on vey weak assumptions about popeties of optimal consumption. In section 4, we give an existence poof fo an optimal consumption path given an auxiliay tempoay steady state (atss). The atss is chaacteized by the fact that we only end v-close to the zeo-motion line of the employed, fo any v > 0, howeve small. It has poven to be vey simple to wok with this atss numeically. Due to the non-continuity of hitting times of dynamic systems, see g. 2, the poof is designed fo ou puposes. We use the speci c fom of the dynamic system (5) at hand in ode to establish continuity in this special case. If this poof is to be used fo othe systems, one always would have to make sue that lem. 4.3 o a coesponding vaiant of it will hold. In section 5, we give an easily accessible exposition into the mathematical methods used to establish Fokke-Planck patial di eential equations fo the dynamics of densities of stochastic pocesses given by stochastic di eential equations. While the deivation is based on the paticula model intoduced in section 2, we have tied to keep it athe geneal. Fo systems diven by di eent stochastic di eential equations, the in nitesimal geneato A will have a di eent fom, thus equiing di eent integations by pats. In some abstact sense, these integations by pats seve to compute the adjoint opeato to A, which in tun detemines the Fokke- Planck equation. Theefoe, the deivation used in section 5 can be applied fo a wide class of stochastic models. Concening futue wok, it would be desiable fom a theoetical pespective to extend the poof of the auxiliay tempoay steady state to an existence poof fo a tempoay steady state of the wealth dynamics. In the notation used in section 4, this means that we would like to take the limit v! 0, like we took the limit "! 0. Thee ae, howeve, cetain complications as compaed with the latte situation. Fo 25

27 once, note that the tajectoy X(; ), = v, does not depend on ". Only the time (), when X(; ) hits the bounday R ";v;k does. Theefoe, we only had to establish the existence of an initial value v, such that the coesponding tajectoy satis es x 3 ( b=) = 0. In contast, X(; v ) obviously does depend on v. Thus, taking a limit v! 0 involves taking a limit of solutions to the ODE, and we would have to additionally show that the limiting tajectoy again solves the ODE. We could avoid this poblem, if we knew how to choose v = v (^a), such that two tajectoies X(; v (^a)) and X(; 0 (^a 0 )) coincide (on R ";v;k ). This aleady indicates the dilemma, because we do not know how to solve the ODE fo v = 0 because of the singulaity in (5a) at the zeo-motion line of the employed. If we could ovecome this poblem, we would still face a simila kind of shooting poblem as in theo This time, howeve, we would have to hit a line f(a; a + w; (a + w))j b= a a max g in (a; x; y)-space instead of the line f( b=; x; 0)jx 0g. 7 Appendix Thee is a shot appendix which is available upon equest. Refeences Aït-Sahalia, Y. (2004): Disentangling di usion fom jumps, Jounal of Financial Economics, 74, Baye, C., and K. Wälde (200a): Matching and Saving in Continuous Time : Theoy, CESifo Woking Pape (200b): Matching and Saving in Continuous Time: Stability, mimeo - available at Cahuc, P., F. Postel-Vinay, and J.-M. Robin (2006): Wage Bagaining with On-thejob Seach: Theoy and Evidence, Econometica, 74, Eckstein, Z., and K. I. Wolpin (995): Duation to Fist Job and the Retun to Schooling: Estimates fom a Seach-Matching Model, Review of Economic Studies, 62, Fiedman, A. (975): Stochastic di eential equations and applications. Vol.. Academic Pess [Hacout Bace Jovanovich Publishes], New Yok, Pobability and Mathematical Statistics, Vol. 28. Launov, A., and K. Wälde (200): Estimating Incentive and Welfae E ects of Non- Stationay Unemployment Bene ts, mimeo - available at Lo, A. W. (988): Maximum Likelihood Estimation of Genealised Ito pocesses with discetely sampled data, Econometic Theoy, 4,

Internet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks

Internet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks Intenet Appendix fo A Bayesian Appoach to Real Options: The Case of Distinguishing Between Tempoay and Pemanent Shocks Steven R. Genadie Gaduate School of Business, Stanfod Univesity Andey Malenko Gaduate

More information

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0}, ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability

More information

Macro Theory B. The Permanent Income Hypothesis

Macro Theory B. The Permanent Income Hypothesis Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with

More information

EM Boundary Value Problems

EM Boundary Value Problems EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do

More information

THE CONE THEOREM JOEL A. TROPP. Abstract. We prove a fixed point theorem for functions which are positive with respect to a cone in a Banach space.

THE CONE THEOREM JOEL A. TROPP. Abstract. We prove a fixed point theorem for functions which are positive with respect to a cone in a Banach space. THE ONE THEOEM JOEL A. TOPP Abstact. We pove a fixed point theoem fo functions which ae positive with espect to a cone in a Banach space. 1. Definitions Definition 1. Let X be a eal Banach space. A subset

More information

Compactly Supported Radial Basis Functions

Compactly Supported Radial Basis Functions Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically

More information

4/18/2005. Statistical Learning Theory

4/18/2005. Statistical Learning Theory Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse

More information

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India

More information

Math 124B February 02, 2012

Math 124B February 02, 2012 Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial

More information

Lecture 28: Convergence of Random Variables and Related Theorems

Lecture 28: Convergence of Random Variables and Related Theorems EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An

More information

JENSEN S INEQUALITY FOR DISTRIBUTIONS POSSESSING HIGHER MOMENTS, WITH APPLICATION TO SHARP BOUNDS FOR LAPLACE-STIELTJES TRANSFORMS

JENSEN S INEQUALITY FOR DISTRIBUTIONS POSSESSING HIGHER MOMENTS, WITH APPLICATION TO SHARP BOUNDS FOR LAPLACE-STIELTJES TRANSFORMS J. Austal. Math. Soc. Se. B 40(1998), 80 85 JENSEN S INEQUALITY FO DISTIBUTIONS POSSESSING HIGHE MOMENTS, WITH APPLICATION TO SHAP BOUNDS FO LAPLACE-STIELTJES TANSFOMS B. GULJAŠ 1,C.E.M.PEACE 2 and J.

More information

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

More information

A Comment on Increasing Returns and Spatial. Unemployment Disparities

A Comment on Increasing Returns and Spatial. Unemployment Disparities The Society fo conomic Studies The nivesity of Kitakyushu Woking Pape Seies No.06-5 (accepted in Mach, 07) A Comment on Inceasing Retuns and Spatial nemployment Dispaities Jumpei Tanaka ** The nivesity

More information

Unobserved Correlation in Ascending Auctions: Example And Extensions

Unobserved Correlation in Ascending Auctions: Example And Extensions Unobseved Coelation in Ascending Auctions: Example And Extensions Daniel Quint Univesity of Wisconsin Novembe 2009 Intoduction In pivate-value ascending auctions, the winning bidde s willingness to pay

More information

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.

More information

Solution to HW 3, Ma 1a Fall 2016

Solution to HW 3, Ma 1a Fall 2016 Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.

More information

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

A Bijective Approach to the Permutational Power of a Priority Queue

A Bijective Approach to the Permutational Power of a Priority Queue A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation

More information

Surveillance Points in High Dimensional Spaces

Surveillance Points in High Dimensional Spaces Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage

More information

Notes on McCall s Model of Job Search. Timothy J. Kehoe March if job offer has been accepted. b if searching

Notes on McCall s Model of Job Search. Timothy J. Kehoe March if job offer has been accepted. b if searching Notes on McCall s Model of Job Seach Timothy J Kehoe Mach Fv ( ) pob( v), [, ] Choice: accept age offe o eceive b and seach again next peiod An unemployed oke solves hee max E t t y t y t if job offe has

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

Multiple Criteria Secretary Problem: A New Approach

Multiple Criteria Secretary Problem: A New Approach J. Stat. Appl. Po. 3, o., 9-38 (04 9 Jounal of Statistics Applications & Pobability An Intenational Jounal http://dx.doi.og/0.785/jsap/0303 Multiple Citeia Secetay Poblem: A ew Appoach Alaka Padhye, and

More information

Do Managers Do Good With Other People s Money? Online Appendix

Do Managers Do Good With Other People s Money? Online Appendix Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth

More information

Syntactical content of nite approximations of partial algebras 1 Wiktor Bartol Inst. Matematyki, Uniw. Warszawski, Warszawa (Poland)

Syntactical content of nite approximations of partial algebras 1 Wiktor Bartol Inst. Matematyki, Uniw. Warszawski, Warszawa (Poland) Syntactical content of nite appoximations of patial algebas 1 Wikto Batol Inst. Matematyki, Uniw. Waszawski, 02-097 Waszawa (Poland) batol@mimuw.edu.pl Xavie Caicedo Dep. Matematicas, Univ. de los Andes,

More information

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany Relating Banching Pogam Size and omula Size ove the ull Binay Basis Matin Saueho y Ingo Wegene y Ralph Wechne z y B Infomatik, LS II, Univ. Dotmund, 44 Dotmund, Gemany z ankfut, Gemany sauehof/wegene@ls.cs.uni-dotmund.de

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

Exploration of the three-person duel

Exploration of the three-person duel Exploation of the thee-peson duel Andy Paish 15 August 2006 1 The duel Pictue a duel: two shootes facing one anothe, taking tuns fiing at one anothe, each with a fixed pobability of hitting his opponent.

More information

Handout: IS/LM Model

Handout: IS/LM Model Econ 32 - IS/L odel Notes Handout: IS/L odel IS Cuve Deivation Figue 4-4 in the textbook explains one deivation of the IS cuve. This deivation uses the Induced Savings Function fom Chapte 3. Hee, I descibe

More information

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012 Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,

More information

A proof of the binomial theorem

A proof of the binomial theorem A poof of the binomial theoem If n is a natual numbe, let n! denote the poduct of the numbes,2,3,,n. So! =, 2! = 2 = 2, 3! = 2 3 = 6, 4! = 2 3 4 = 24 and so on. We also let 0! =. If n is a non-negative

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

More information

Math 301: The Erdős-Stone-Simonovitz Theorem and Extremal Numbers for Bipartite Graphs

Math 301: The Erdős-Stone-Simonovitz Theorem and Extremal Numbers for Bipartite Graphs Math 30: The Edős-Stone-Simonovitz Theoem and Extemal Numbes fo Bipatite Gaphs May Radcliffe The Edős-Stone-Simonovitz Theoem Recall, in class we poved Tuán s Gaph Theoem, namely Theoem Tuán s Theoem Let

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

An Application of Fuzzy Linear System of Equations in Economic Sciences

An Application of Fuzzy Linear System of Equations in Economic Sciences Austalian Jounal of Basic and Applied Sciences, 5(7): 7-14, 2011 ISSN 1991-8178 An Application of Fuzzy Linea System of Equations in Economic Sciences 1 S.H. Nassei, 2 M. Abdi and 3 B. Khabii 1 Depatment

More information

Fractional Zero Forcing via Three-color Forcing Games

Fractional Zero Forcing via Three-color Forcing Games Factional Zeo Focing via Thee-colo Focing Games Leslie Hogben Kevin F. Palmowski David E. Robeson Michael Young May 13, 2015 Abstact An -fold analogue of the positive semidefinite zeo focing pocess that

More information

On a quantity that is analogous to potential and a theorem that relates to it

On a quantity that is analogous to potential and a theorem that relates to it Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics

More information

A generalization of the Bernstein polynomials

A generalization of the Bernstein polynomials A genealization of the Benstein polynomials Halil Ouç and Geoge M Phillips Mathematical Institute, Univesity of St Andews, Noth Haugh, St Andews, Fife KY16 9SS, Scotland Dedicated to Philip J Davis This

More information

ac p Answers to questions for The New Introduction to Geographical Economics, 2 nd edition Chapter 3 The core model of geographical economics

ac p Answers to questions for The New Introduction to Geographical Economics, 2 nd edition Chapter 3 The core model of geographical economics Answes to questions fo The New ntoduction to Geogaphical Economics, nd edition Chapte 3 The coe model of geogaphical economics Question 3. Fom intoductoy mico-economics we know that the condition fo pofit

More information

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr. POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and

More information

MEASURING CHINESE RISK AVERSION

MEASURING CHINESE RISK AVERSION MEASURING CHINESE RISK AVERSION --Based on Insuance Data Li Diao (Cental Univesity of Finance and Economics) Hua Chen (Cental Univesity of Finance and Economics) Jingzhen Liu (Cental Univesity of Finance

More information

Moment-free numerical approximation of highly oscillatory integrals with stationary points

Moment-free numerical approximation of highly oscillatory integrals with stationary points Moment-fee numeical appoximation of highly oscillatoy integals with stationay points Sheehan Olve Abstact We pesent a method fo the numeical quadatue of highly oscillatoy integals with stationay points.

More information

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension Intenational Mathematical Foum, 3, 2008, no. 16, 763-776 Functions Defined on Fuzzy Real Numbes Accoding to Zadeh s Extension Oma A. AbuAaqob, Nabil T. Shawagfeh and Oma A. AbuGhneim 1 Mathematics Depatment,

More information

Scattering in Three Dimensions

Scattering in Three Dimensions Scatteing in Thee Dimensions Scatteing expeiments ae an impotant souce of infomation about quantum systems, anging in enegy fom vey low enegy chemical eactions to the highest possible enegies at the LHC.

More information

Goodness-of-fit for composite hypotheses.

Goodness-of-fit for composite hypotheses. Section 11 Goodness-of-fit fo composite hypotheses. Example. Let us conside a Matlab example. Let us geneate 50 obsevations fom N(1, 2): X=nomnd(1,2,50,1); Then, unning a chi-squaed goodness-of-fit test

More information

Brief summary of functional analysis APPM 5440 Fall 2014 Applied Analysis

Brief summary of functional analysis APPM 5440 Fall 2014 Applied Analysis Bief summay of functional analysis APPM 5440 Fall 014 Applied Analysis Stephen Becke, stephen.becke@coloado.edu Standad theoems. When necessay, I used Royden s and Keyzsig s books as a efeence. Vesion

More information

Math 2263 Solutions for Spring 2003 Final Exam

Math 2263 Solutions for Spring 2003 Final Exam Math 6 Solutions fo Sping Final Exam ) A staightfowad appoach to finding the tangent plane to a suface at a point ( x, y, z ) would be to expess the cuve as an explicit function z = f ( x, y ), calculate

More information

A Multivariate Normal Law for Turing s Formulae

A Multivariate Normal Law for Turing s Formulae A Multivaiate Nomal Law fo Tuing s Fomulae Zhiyi Zhang Depatment of Mathematics and Statistics Univesity of Noth Caolina at Chalotte Chalotte, NC 28223 Abstact This pape establishes a sufficient condition

More information

arxiv: v1 [physics.pop-ph] 3 Jun 2013

arxiv: v1 [physics.pop-ph] 3 Jun 2013 A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,

More information

On the Poisson Approximation to the Negative Hypergeometric Distribution

On the Poisson Approximation to the Negative Hypergeometric Distribution BULLETIN of the Malaysian Mathematical Sciences Society http://mathusmmy/bulletin Bull Malays Math Sci Soc (2) 34(2) (2011), 331 336 On the Poisson Appoximation to the Negative Hypegeometic Distibution

More information

I. CONSTRUCTION OF THE GREEN S FUNCTION

I. CONSTRUCTION OF THE GREEN S FUNCTION I. CONSTRUCTION OF THE GREEN S FUNCTION The Helmohltz equation in 4 dimensions is 4 + k G 4 x, x = δ 4 x x. In this equation, G is the Geen s function and 4 efes to the dimensionality. In the vey end,

More information

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx.

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx. 9. LAGRANGIAN OF THE ELECTROMAGNETIC FIELD In the pevious section the Lagangian and Hamiltonian of an ensemble of point paticles was developed. This appoach is based on a qt. This discete fomulation can

More information

Markscheme May 2017 Calculus Higher level Paper 3

Markscheme May 2017 Calculus Higher level Paper 3 M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted

More information

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,

More information

q i i=1 p i ln p i Another measure, which proves a useful benchmark in our analysis, is the chi squared divergence of p, q, which is defined by

q i i=1 p i ln p i Another measure, which proves a useful benchmark in our analysis, is the chi squared divergence of p, q, which is defined by CSISZÁR f DIVERGENCE, OSTROWSKI S INEQUALITY AND MUTUAL INFORMATION S. S. DRAGOMIR, V. GLUŠČEVIĆ, AND C. E. M. PEARCE Abstact. The Ostowski integal inequality fo an absolutely continuous function is used

More information

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496

More information

-Δ u = λ u. u(x,y) = u 1. (x) u 2. (y) u(r,θ) = R(r) Θ(θ) Δu = 2 u + 2 u. r = x 2 + y 2. tan(θ) = y/x. r cos(θ) = cos(θ) r.

-Δ u = λ u. u(x,y) = u 1. (x) u 2. (y) u(r,θ) = R(r) Θ(θ) Δu = 2 u + 2 u. r = x 2 + y 2. tan(θ) = y/x. r cos(θ) = cos(θ) r. The Laplace opeato in pola coodinates We now conside the Laplace opeato with Diichlet bounday conditions on a cicula egion Ω {(x,y) x + y A }. Ou goal is to compute eigenvalues and eigenfunctions of the

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

More information

SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS

SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS Fixed Point Theoy, Volume 5, No. 1, 2004, 71-80 http://www.math.ubbcluj.o/ nodeacj/sfptcj.htm SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS G. ISAC 1 AND C. AVRAMESCU 2 1 Depatment of Mathematics Royal

More information

An Exact Solution of Navier Stokes Equation

An Exact Solution of Navier Stokes Equation An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in

More information

On the ratio of maximum and minimum degree in maximal intersecting families

On the ratio of maximum and minimum degree in maximal intersecting families On the atio of maximum and minimum degee in maximal intesecting families Zoltán Lóánt Nagy Lale Özkahya Balázs Patkós Máté Vize Mach 6, 013 Abstact To study how balanced o unbalanced a maximal intesecting

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

More information

arxiv: v1 [math.co] 1 Apr 2011

arxiv: v1 [math.co] 1 Apr 2011 Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and

More information

A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM

A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM DIEGO AVERNA AND GABRIELE BONANNO Abstact. The aim of this pape is twofold. On one hand we establish a thee citical

More information

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function Abstact and Applied Analysis Volume 011, Aticle ID 697547, 7 pages doi:10.1155/011/697547 Reseach Aticle On Alze and Qiu s Conjectue fo Complete Elliptic Integal and Invese Hypebolic Tangent Function Yu-Ming

More information

Exceptional regular singular points of second-order ODEs. 1. Solving second-order ODEs

Exceptional regular singular points of second-order ODEs. 1. Solving second-order ODEs (May 14, 2011 Exceptional egula singula points of second-ode ODEs Paul Gaett gaett@math.umn.edu http://www.math.umn.edu/ gaett/ 1. Solving second-ode ODEs 2. Examples 3. Convegence Fobenius method fo solving

More information

On Computing Optimal (Q, r) Replenishment Policies under Quantity Discounts

On Computing Optimal (Q, r) Replenishment Policies under Quantity Discounts Annals of Opeations Reseach manuscipt No. will be inseted by the edito) On Computing Optimal, ) Replenishment Policies unde uantity Discounts The all - units and incemental discount cases Michael N. Katehakis

More information

ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS

ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS L. MICU Hoia Hulubei National Institute fo Physics and Nuclea Engineeing, P.O. Box MG-6, RO-0775 Buchaest-Maguele, Romania, E-mail: lmicu@theoy.nipne.o (Received

More information

9.1 The multiplicative group of a finite field. Theorem 9.1. The multiplicative group F of a finite field is cyclic.

9.1 The multiplicative group of a finite field. Theorem 9.1. The multiplicative group F of a finite field is cyclic. Chapte 9 Pimitive Roots 9.1 The multiplicative goup of a finite fld Theoem 9.1. The multiplicative goup F of a finite fld is cyclic. Remak: In paticula, if p is a pime then (Z/p) is cyclic. In fact, this

More information

Chapter 3: Theory of Modular Arithmetic 38

Chapter 3: Theory of Modular Arithmetic 38 Chapte 3: Theoy of Modula Aithmetic 38 Section D Chinese Remainde Theoem By the end of this section you will be able to pove the Chinese Remainde Theoem apply this theoem to solve simultaneous linea conguences

More information

DonnishJournals

DonnishJournals DonnishJounals 041-1189 Donnish Jounal of Educational Reseach and Reviews. Vol 1(1) pp. 01-017 Novembe, 014. http:///dje Copyight 014 Donnish Jounals Oiginal Reseach Pape Vecto Analysis Using MAXIMA Savaş

More information

SPECTRAL SEQUENCES. im(er

SPECTRAL SEQUENCES. im(er SPECTRAL SEQUENCES MATTHEW GREENBERG. Intoduction Definition. Let a. An a-th stage spectal (cohomological) sequence consists of the following data: bigaded objects E = p,q Z Ep,q, a diffeentials d : E

More information

Regularity for Fully Nonlinear Elliptic Equations with Neumann Boundary Data

Regularity for Fully Nonlinear Elliptic Equations with Neumann Boundary Data Communications in Patial Diffeential Equations, 31: 1227 1252, 2006 Copyight Taylo & Fancis Goup, LLC ISSN 0360-5302 pint/1532-4133 online DOI: 10.1080/03605300600634999 Regulaity fo Fully Nonlinea Elliptic

More information

A New Approach to General Relativity

A New Approach to General Relativity Apeion, Vol. 14, No. 3, July 7 7 A New Appoach to Geneal Relativity Ali Rıza Şahin Gaziosmanpaşa, Istanbul Tukey E-mail: aizasahin@gmail.com Hee we pesent a new point of view fo geneal elativity and/o

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

Brad De Long è Maury Obstfeld, Petra Geraats è Galina Hale-Borisova. Econ 202B, Fall 1998

Brad De Long è Maury Obstfeld, Petra Geraats è Galina Hale-Borisova. Econ 202B, Fall 1998 uggested olutions to oblem et 4 Bad De Long Mauy Obstfeld, eta Geaats Galina Hale-Boisova Econ 22B, Fall 1998 1. Moal hazad and asset-pice bubbles. a The epesentative entepeneu boows B on date 1 and invests

More information

Bifurcation Analysis for the Delay Logistic Equation with Two Delays

Bifurcation Analysis for the Delay Logistic Equation with Two Delays IOSR Jounal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 5 Ve. IV (Sep. - Oct. 05), PP 53-58 www.iosjounals.og Bifucation Analysis fo the Delay Logistic Equation with Two Delays

More information

COLLAPSING WALLS THEOREM

COLLAPSING WALLS THEOREM COLLAPSING WALLS THEOREM IGOR PAK AND ROM PINCHASI Abstact. Let P R 3 be a pyamid with the base a convex polygon Q. We show that when othe faces ae collapsed (otated aound the edges onto the plane spanned

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

More information

ANA BERRIZBEITIA, LUIS A. MEDINA, ALEXANDER C. MOLL, VICTOR H. MOLL, AND LAINE NOBLE

ANA BERRIZBEITIA, LUIS A. MEDINA, ALEXANDER C. MOLL, VICTOR H. MOLL, AND LAINE NOBLE THE p-adic VALUATION OF STIRLING NUMBERS ANA BERRIZBEITIA, LUIS A. MEDINA, ALEXANDER C. MOLL, VICTOR H. MOLL, AND LAINE NOBLE Abstact. Let p > 2 be a pime. The p-adic valuation of Stiling numbes of the

More information

Galois points on quartic surfaces

Galois points on quartic surfaces J. Math. Soc. Japan Vol. 53, No. 3, 2001 Galois points on quatic sufaces By Hisao Yoshihaa (Received Nov. 29, 1999) (Revised Ma. 30, 2000) Abstact. Let S be a smooth hypesuface in the pojective thee space

More information

Measure Estimates of Nodal Sets of Polyharmonic Functions

Measure Estimates of Nodal Sets of Polyharmonic Functions Chin. Ann. Math. Se. B 39(5), 08, 97 93 DOI: 0.007/s40-08-004-6 Chinese Annals of Mathematics, Seies B c The Editoial Office of CAM and Spinge-Velag Belin Heidelbeg 08 Measue Estimates of Nodal Sets of

More information

Efficiency Loss in a Network Resource Allocation Game: The Case of Elastic Supply

Efficiency Loss in a Network Resource Allocation Game: The Case of Elastic Supply Efficiency Loss in a Netwok Resouce Allocation Game: The Case of Elastic Supply axiv:cs/0506054v1 [cs.gt] 14 Jun 2005 Ramesh Johai (johai@stanfod.edu) Shie Manno (shie@mit.edu) John N. Tsitsiklis (jnt@mit.edu)

More information

TANTON S TAKE ON CONTINUOUS COMPOUND INTEREST

TANTON S TAKE ON CONTINUOUS COMPOUND INTEREST CURRICULUM ISPIRATIOS: www.maa.og/ci www.theglobalmathpoject.og IOVATIVE CURRICULUM OLIE EXPERIECES: www.gdaymath.com TATO TIDBITS: www.jamestanton.com TATO S TAKE O COTIUOUS COMPOUD ITEREST DECEMBER 208

More information

and the initial value R 0 = 0, 0 = fall equivalence classes ae singletons fig; i = 1; : : : ; ng: (3) Since the tansition pobability p := P (R = j R?1

and the initial value R 0 = 0, 0 = fall equivalence classes ae singletons fig; i = 1; : : : ; ng: (3) Since the tansition pobability p := P (R = j R?1 A CLASSIFICATION OF COALESCENT PROCESSES FOR HAPLOID ECHANGE- ABLE POPULATION MODELS Matin Mohle, Johannes Gutenbeg-Univesitat, Mainz and Seik Sagitov 1, Chalmes and Gotebogs Univesities, Gotebog Abstact

More information

Probablistically Checkable Proofs

Probablistically Checkable Proofs Lectue 12 Pobablistically Checkable Poofs May 13, 2004 Lectue: Paul Beame Notes: Chis Re 12.1 Pobablisitically Checkable Poofs Oveview We know that IP = PSPACE. This means thee is an inteactive potocol

More information

Numerical approximation to ζ(2n+1)

Numerical approximation to ζ(2n+1) Illinois Wesleyan Univesity Fom the SelectedWoks of Tian-Xiao He 6 Numeical appoximation to ζ(n+1) Tian-Xiao He, Illinois Wesleyan Univesity Michael J. Dancs Available at: https://woks.bepess.com/tian_xiao_he/6/

More information

f h = u, h g = v, we have u + v = f g. So, we wish

f h = u, h g = v, we have u + v = f g. So, we wish Answes to Homewok 4, Math 4111 (1) Pove that the following examples fom class ae indeed metic spaces. You only need to veify the tiangle inequality. (a) Let C be the set of continuous functions fom [0,

More information

d 2 x 0a d d =0. Relative to an arbitrary (accelerating frame) specified by x a = x a (x 0b ), the latter becomes: d 2 x a d 2 + a dx b dx c

d 2 x 0a d d =0. Relative to an arbitrary (accelerating frame) specified by x a = x a (x 0b ), the latter becomes: d 2 x a d 2 + a dx b dx c Chapte 6 Geneal Relativity 6.1 Towads the Einstein equations Thee ae seveal ways of motivating the Einstein equations. The most natual is pehaps though consideations involving the Equivalence Pinciple.

More information

arxiv: v1 [math.co] 4 May 2017

arxiv: v1 [math.co] 4 May 2017 On The Numbe Of Unlabeled Bipatite Gaphs Abdullah Atmaca and A Yavuz Ouç axiv:7050800v [mathco] 4 May 207 Abstact This pape solves a poblem that was stated by M A Haison in 973 [] This poblem, that has

More information

6 Matrix Concentration Bounds

6 Matrix Concentration Bounds 6 Matix Concentation Bounds Concentation bounds ae inequalities that bound pobabilities of deviations by a andom vaiable fom some value, often its mean. Infomally, they show the pobability that a andom

More information

Vanishing lines in generalized Adams spectral sequences are generic

Vanishing lines in generalized Adams spectral sequences are generic ISSN 364-0380 (on line) 465-3060 (pinted) 55 Geomety & Topology Volume 3 (999) 55 65 Published: 2 July 999 G G G G T T T G T T T G T G T GG TT G G G G GG T T T TT Vanishing lines in genealized Adams spectal

More information

10/04/18. P [P(x)] 1 negl(n).

10/04/18. P [P(x)] 1 negl(n). Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the

More information

On a generalization of Eulerian numbers

On a generalization of Eulerian numbers Notes on Numbe Theoy and Discete Mathematics Pint ISSN 1310 513, Online ISSN 367 875 Vol, 018, No 1, 16 DOI: 10756/nntdm018116- On a genealization of Euleian numbes Claudio Pita-Ruiz Facultad de Ingenieía,

More information

Solution to Problem First, the firm minimizes the cost of the inputs: min wl + rk + sf

Solution to Problem First, the firm minimizes the cost of the inputs: min wl + rk + sf Econ 0A Poblem Set 4 Solutions ue in class on Tu 4 Novembe. No late Poblem Sets accepted, so! This Poblem set tests the knoledge that ou accumulated mainl in lectues 5 to 9. Some of the mateial ill onl

More information

C/CS/Phys C191 Shor s order (period) finding algorithm and factoring 11/12/14 Fall 2014 Lecture 22

C/CS/Phys C191 Shor s order (period) finding algorithm and factoring 11/12/14 Fall 2014 Lecture 22 C/CS/Phys C9 Sho s ode (peiod) finding algoithm and factoing /2/4 Fall 204 Lectue 22 With a fast algoithm fo the uantum Fouie Tansfom in hand, it is clea that many useful applications should be possible.

More information

F-IF Logistic Growth Model, Abstract Version

F-IF Logistic Growth Model, Abstract Version F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth

More information

THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX. Jaejin Lee

THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX. Jaejin Lee Koean J. Math. 23 (2015), No. 3, pp. 427 438 http://dx.doi.og/10.11568/kjm.2015.23.3.427 THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX Jaejin Lee Abstact. The Schensted algoithm fist descibed by Robinson

More information

Suggested Solutions to Homework #4 Econ 511b (Part I), Spring 2004

Suggested Solutions to Homework #4 Econ 511b (Part I), Spring 2004 Suggested Solutions to Homewok #4 Econ 5b (Pat I), Sping 2004. Conside a neoclassical gowth model with valued leisue. The (epesentative) consume values steams of consumption and leisue accoding to P t=0

More information