Long-term returns in stochastic interest rate models
|
|
- Chrystal Doyle
- 5 years ago
- Views:
Transcription
1 Long-term return in tochatic interet rate model G. Deeltra F. Delbaen Vrije Univeriteit Bruel Departement Wikunde Abtract In thi paper, we oberve the convergence of the long-term return, uing an extenion of the Cox-Ingeroll-Ro (985) tochatic model of the hort interet rate r. Uing the theory of Beel procee, we are able to prove the convergence almot everywhere of t Xd with X a t generalized Beelquare proce with drift with tochatic reverion level. Key word Long-term return, tochatic procee, generalized Beelquare procee, convergence almot everywhere. Abbreviated title: Long-term return G. Deeltra, Departement Wikunde, Vrije Univeriteit Bruel, Pleinlaan, B-5 Bruel, Belgium tel: fax: gdeeltr@vnet3.vub.ac.be
2 Introduction. In thi paper, we are intereted in the long-term return t t r udu where (r u ) u denote the intantaneou interet rate. Inurance companie promie a certain fixed percentage of interet on their inurance product uch a bond, lifeinurance, etcetera. We wonder how thi percentage hould be determined. It ha to be lower than the etimated random return in order to cover expene and to hold ome reerve o that the company can get through difficult period of economic crii without bankruptcy. On the other hand, the competitive truggle, trengthened by the open market of the European Community, force rival companie to take the wihe of the clientele into conideration. Naturally, the cotumer want a return a high a poible. In thi light, we think it i intereting to tudy and to model the long-term return in a mathematical way. We analye the convergence of the long-term return, uing an extenion of the Cox, Ingeroll and Ro (985) tochatic model of the hort interet rate r. Cox, Ingeroll and Ro expre the hort interet rate dynamic a dr t = κ(γ r t )dt + σ r t db t. with (B t ) t a Brownian motion and κ, γ and σ poitive contant. It i a wellknown fact that thi model ha ome empirically relevant propertie. In thi model, r never become negative and for κγ σ, r doe not reach zero. For κ > and γ, the randomly moving interet rate i elatically pulled toward the long-term contant value γ. However, it i reaonable to conjecture that the market will contantly change thi level γ and the volatility σ. In the foottep of Schaefer and Schwartz (984), Hull and White (99) and Longtaff and Schwartz (99), we extend the CIR model in order to reflect the time-dependence caued by the cyclical nature of the economy or by expectation concerning the future impact of monetary policie. We aume the reverion level to be tochatic and we alo generalize the volatility. In thi ituation, we examine the convergence of the long-term return t t r udu and we propoe ome application. We conider a family of tochatic procee X, which contain the Beelquare procee with drift. The many reult known about thee procee, e.g. Pitman-Yor (98), Revuz-Yor (99), convinced u that thee procee are very tractable. Uing the theory of Beel procee, we found the following theorem, which i very ueful for deducing the convergence almot everywhere of the long-term return in quite general ituation: Theorem Suppoe that a probability pace (Ω, (F t ) t, IP ) i given and that a Brownian
3 motion (B t ) t i defined on it. A tochatic proce X : Ω IR + IR + i aumed to atify the tochatic differential equation dx = (βx + δ )d + g(x )db IR + with β < and g : IR IR + a function, vanihing at zero and uch that there i a contant b with g(x) g(y) b x y. The meaurable and adapted proce δ : Ω IR + IR + i aumed to atify: δ u du a.e. δ with δ : Ω IR +. Under thee condition, the following convergence almot everywhere hold X u du a.e. δ β. We will give a proof of thi theorem in ection. In ection 3, we how an immediate application of theorem. We conider the long-term return in the two-factormodel: dr t = κ(γ t r t )dt + σ r t db t dγ t = κ(γ γ t )dt + σ γ t d B t with (B t ) t and ( B t ) t two Brownian Motion and with κ, κ, σ, σ and γ poitive contant. The hort interet rate proce ha a reverion level which i a tochatic proce itelf. We do not need any aumption about the correlation between the Brownian motion of the intantaneou interet rate and of the tochatic reverion level proce. We tre thi fact becaue it i not trivial. Mot author of two-factormodel require, for technical reaon, that the Wiener procee are uncorrelated or have a determinitic and fixed correlation. Without further notice we aume that the filtration (F t ) t atifie the uual aumption with repect to IP, a fixed probability on the igma-algebra F = t F t. Alo B i a continuou proce that i a Brownian motion with repect to (F t ) t. 3
4 Convergence a.e. of the long-term return. Uing the theory of Beel procee, ee Pitman-Yor (98), we found a theorem which i very ueful for deducing the convergence almot everywhere of the long-term return in quite general ituation. In thi ection, we give a proof of the convergence reult, which relie on the theory of tochatic differential equation and on Kronecker lemma. Firt, we recall Kronecker lemma which i a tandard lemma, even for tochatic integral [ee Revuz-Yor (99, p.75 exercie.6)]. For completene, we give a proof. Kronecker lemma Let u aume a continuou emimartingale Y and a trictly poitive increaing function f which tend to infinity. If dy u f(u) exit a.e., then Yt f(t) a.e. Proof If we denote dz t = dyt f(t), then Y t = Y + f(u)dz u. By partial integration, recall that the emimartingale Z i continuou, we find that: Conequently, Y t = Y + f(t)z t f()z = Y + f()z t + Z u df(u) (Z t Z u )df(u) f()z. Y t f(t) = Y + f()z t f()z + f(t) f(t) (Z t Z u )df(u). Since Z = dy u f(u) exit a.e., (Z t) t converge to Z a.e. and therefore up Z t < a.e.. Hence, the firt term converge to zero a.e.. Let u look at the econd term: f(t) (Z t Z u )df(u) = f(t) (Z t Z u )df(u) + f(t) (Z t Z u )df(u). Since (Z t ) t converge to Z a.e., we can chooe for a given ε >, a number large enough uch that Z t Z u < ε for all t, u. For thi fixed, we can chooe t uch that max u Z u f() f(t) < ε. q.e.d. 4
5 To tudy the convergence a.e. of the long-term return, we conider a family of tochatic procee X, which contain the Beelquare procee with drift. We define the (continuou) adapted proce X by the tochatic differential equation dx = (βx + δ )d + g(x )db IR + with β trictly negative and g a function, vanihing at zero and atifying a Hölder condition of order one half. In order to have a unique olution of thi tochatic differential equation, we uppoe that δ d < for all t. The unique olution X i non-negative and atifie ) X = e (X β + δ u e βu du + e βu g(x u ) db u. () In view of the application, we think that the problem of exitence and uniquene goe beyond the cope of thi paper. The intereted reader i referred to Deeltra-Delbaen (994). For thi family of tochatic procee, we firt prove a technical lemma needed in the proof of the main theorem. Lemma Suppoe that a probability pace (Ω, (F t ) t, IP ) i given and that a tochatic proce X : Ω IR + IR + i defined by the tochatic differential equation with β, dx = (βx + δ )d + g(x )db IR + g : IR IR + i a function, vanihing at zero and uch that there i a contant b with g(x) g(y) b x y, δ : Ω IR + IR + i an adapted and meaurable proce, δ udu < a.. for all t. Then for all t we have up ut X u i finite and if IE[δ u]du < we have for all t: IE[X ] = e β X + e β( u) IE[δ u ]du. 5
6 Proof Let u firt conider the cae E[δ u]du <. We define the equence (T n ) n of topping time by From (), we have that for all t e β( Tn) X Tn = X + T n = inf{u X u n}. Tn δ u e βu du + Tn g(x u )e βu db u. () Since X i bounded on the interval [, T n ] and ince g(x) i bounded by b ( x, Tn we obtain that g(x u )e βu db u i a martingale, bounded in L )t. Indeed, let u calculate the quare of the L norm: [ ] t Tn IE g (X u )e 4βu du [ ] t Tn e 4βt IE b X u du [ ] t Tn b e 4βt IE X u du b e 4βt nt <. Therefore, the expected value of T n e βu g(x u ) db u i zero and equation () reduce to [ ] ] Tn IE [e β( Tn) X Tn = X + IE δ u e βu du. Taking the limit for n going to infinity and applying Fatou lemma, we obtain for all t: [ ] IE[X ] e β X + e β IE δ u e βu du [ ] e β X + IE δ u du <. We now how that up t X i integrable. From the olution of the tochatic differential equation, it i known that ( )) up X up (e β X + δ u e βu du + g(x u )e βu db u t t X + δ u du + up g(x u )e βu db u. t 6
7 Conequently, [ ] IE up X X + t IE[δ u ] du + up t g(x u )e βu db u. Uing Doob inequality, we remark that the lat term i bounded. up g(x u )e βu db u t 4 g(x u )e βu db u [ ] 4e 4βt IE g(x u ) du <. [ 4e 4βt IE ] b X u du 4e 4βt b IE[X u ] du Thi how that (X Tn ) t,n i a uniformly integrable family and that we are allowed to interchange limit and expectation in the expreion ( [ [ ] ]) Tn lim IE e β( Tn) X Tn = lim X + IE e βu δ u. n n We conclude that in the cae of IE[δ u]du <, the reult i obtained: IE[X ] = e β X + e β( u) IE[δ u ]du. Let u now look at the general cae with the local aumption δ udu < a.e. for all t. We define the equence (σ n ) n by σ n = inf{t δ u n} and we denote δ u [,σn ] by δ u (n). The tochatic differential equation dx (n) = ( βx (n) + δ (n) ) d + g(x (n) )db ha a unique olution and by the definition of σ n, we have IE[δ(n) u ]du n. Applying the firt part of the proof, we obtain up t X (n) < a.e.. On [, σ n ], all X (k), k n are equal by the uniquene of the olution of the tochatic differential equation. Since [, σ n ] [, t], the reult hold under the local aumption δ udu < a.e. for all t. q.e.d. 7
8 Now, we are ready for the convergence theorem itelf. Theorem Suppoe that a probability pace (Ω, (F t ) t, IP ) i given and that a Brownian motion (B t ) t i defined on it. A tochatic proce X : Ω IR + IR + i aumed to atify the tochatic differential equation dx = (βx + δ )d + g(x )db IR + with β < and g : IR IR + a function, vanihing at zero and uch that there i a contant b with g(x) g(y) b x y. The meaurable and adapted proce δ : Ω IR + IR + i aumed to atify: δ u du a.e. δ with δ : Ω IR +. Under thee condition, the following convergence almot everywhere hold X u du a.e. δ β. Proof Integrating the tochatic differential equation dx = (βx + δ )d + g(x )db IR + over the time-interval [,t] and dividing thi integral by β(t + ), give u the equality: t + (X + δ β )d = g(x ) β(t + ) db + X t X β(t + ). (3) It remain to prove that both term on the right hand ide converge to zero almot everywhere. In order to how that g(x ) β(t+) db converge to zero a.e., we ue Kronecker lemma and check the exitence a.e. of g(x u) u+ db u. Let u introduce the equence (T n ) n of topping time: { } δ u T n = inf t (u + ) du n. Since by hypothei + δ udu a.e. δ, we obtain that u δ d K(u + ) a.e. for ome contant K, depending on ω. Straightforward calculation how that 8
9 δ u (u+) du < a.e.: δ u (u + ) du = lim u <. u δ d (u + ) u δ d (u + ) + + ( u K(u + ) (u + ) 3 du ) du δ d (u + ) 3 Hence, {T n = } Ω and conequently, we only need to prove the exitence a.e. of g(x Tn u ) u+ db u on {T n = }. Moreover, ince g(x Tn u ) u+ db u i a local martingale, it uffice to remark that g(x Tn u ) u+ db u i a L -bounded martingale: = g(xu Tn ) u + db u IE [ g (X Tn u ) ] (u + ) du IE [ ] b Xu Tn (u + ) du. In order to evaluate thi lat integral, we remark that IE [ ] [ Xu Tn = IE Xu (utn)] e βu IE [ e βu ] X u (utn) ] e βu IE [e β(u Tn) X u Tn. In lemma, we obtained the equality [ ] Tn IE[e β( Tn) X Tn ] = X + IE e βu δ u du. Conequently: IE [ ] Xu Tn [ ]) u Tn e (X βu + IE e β δ d Uing thi reult, we obtain u e βu X + e βu e β IE [ δ (Tn)] d. IE [ ] Xu Tn (u + ) du 9
10 X + e βu (u + ) du e βu (u + ) du u e β IE [ δ (Tn)] d. Obviouly, the firt term i uniformly bounded in t. It remain to look at the econd term. We apply Fubini theorem to find a bound which i not depending on t: = e βu (u + ) du u e β IE [ δ (Tn)] d e β IE [ ] t e βu δ (Tn) d (u + ) du IE [ ( ) ] δ (Tn) ( + ) d β [ ] Tn β IE n β. δ ( + ) d In order to how that the econd term of (3), namely Xt X β(t+), converge to zero a.e., we divide the olution of the tochatic differential equation () by t + : X t t + = eβt X t + + e β(t u) t + δ udu + e β(t u) t + g(x u)db u. (4) Under the hypothei + δ udu a.e. δ, the econd term in (4) can be made arbitrarily mall, ince for all ω Ω and for all ε > : t + t + e β(t u) δ(ω, u)du t Given ε >, the firt term can be rewritten t + t e β t δ(ω, u)du + t + t δ(ω, u)du. t t + t e β t δ(ω, u)du t δ( + ε)e β t. e β t δ(ω, u)du
11 Conequently, the firt term converge to zero for t going to infinity. The econd term alo tend to zero ince lim t t + = lim t t δ(ω, u)du t ( t ) t t δ(ω, u)du t + t + δ(ω, u)du t ) t + + t t t + δ(ω, u)du t t t t t + t + δ(ω, u)du t ( + lim t = δ δ + lim t =. In order to check the convergence a.e. of eβt t+ e βu g(x u )db u to zero, we again ue Kronecker lemma and we look at the exitence of e βt g(x t) db (t+)e βt t. However, ince thi integral i equal to g(x t) t+ db t, the reult follow from the calculation above. q.e.d. Thi theorem can be generalized to tochatic procee X with a time-dependent trictly negative drift rate β. Let u define the proce X by the tochatic differential equation dx = (β X + δ )d + g(x )db for all IR + where the function g and the proce δ atify the hypothei of theorem ; and where up β < and dvie[δ v ]e v βd v following convergence almot everywhere hold: e u βd (u+) ( X u + δ ) u du a.e.. β u du <. Then, the
12 3 A two-factor CIR model. In thi ection, we give an example of theorem. We tudy the two-factormodel dr t = κ(γ t r t )dt + σ r t db t dγ t = κ(γ γ t )dt + σ γ t d B t with κ, κ > ; γ, σ and σ poitive contant and (B t ) t and ( B t ) t two Brownian motion. The hort interet rate r follow an extended Cox, Ingeroll and Ro quare root proce with reverion level (γ t ) t, which follow a quare root proce itelf. We know that the time-dependent reverion level (γ t ) t i itelf elatically pulled toward the long-term contant value γ. We are intereted in the convergence of the long term return t t r udu. Remark that we do not make any aumption about the way the two Wiener procee are correlated. In contrat with mot author, we do not demand the Brownian motion to be independent, they may have an arbitrary random correlation. Before looking at the convergence almot everywhere of the long-term return r udu itelf, we firt ue theorem to check that indeed γ u du a.e. γ. If we define Y u = 4 σ γ u, then Y u atifie the tochatic differential equation : ( ( ) ) 4 κγ κ dy u = σ + Y u du + Y u d B u. Thu, (Y u ) u i a Beelquare proce with drift, namely in the notation of Pitman-Yor : Y κ/ 4 κγ σ IQ 4γ. σ In general, dy u = (δ u + βy ) u du + g (Y u ) d B u with β = κ < δ u = 4 κγ σ u IR + g (Y u ) = Y u. Trivially, the condition of theorem are atified and it follow that Y u du a.e. 4γ σ
13 and conequently: γ u du a.e. γ. Analogouly, we conider the intantaneou interet rate r u itelf. The tranformation X u = 4 σ r u atifie the tochatic differential equation dx u = In term of theorem : with β = κ < δ u = 4κγu σ u IR + g (X u ) = X u. ( 4κγu σ + ( κ ) X u ) du + X u db u. dx u = (δ u + βx u ) du + g (X u ) db u Since δ i a tranformation of the continuou, adapted proce γ, δ itelf i meaurable and adapted. Becaue γ udu a.e. γ, we know that δ u du = ( ) 4κ γ u du σ a.e. γ 4κ σ. Therefore, the condition of theorem are fulfilled and we find that and finally that X u du a.e. 4γ σ r u du a.e. γ. We conclude that the long-term return converge a.e. to γ, the long-term contant value toward which the drift rate i pulled in thi two-factormodel. 3
14 REFERENCES. Cox, J.C., J.E.Ingeroll and S.A. Ro (985). A theory of the term tructure of interet rate. Econometrica 53, Deeltra G. and F. Delbaen (994). Exitence of Solution of Stochatic Differential Equation related to the Beel proce. Submitted Hull J. and A. White (99). Pricing Interet-Rate-Derivative Securitie. The Review of Financial Studie, Vol. 3, nr 4, Longtaff, F.A. and E.S. Schwarz (99). Interet rate volatility and the term tructure: a two-factor general equilibrium model. The Journal of Finance 47, nr 4, Pitman J. and M. Yor (98). A decompoition of Beel Bridge. Zeitchrift für Wahrcheinlichkeittheorie und Verwandte Gebiete, 59, Revuz D. and M. Yor (99). Continuou Martingale and Brownian motion. Springer-Verlag, Berlin-Heidelberg, New-York. Schaefer, S.M. and E.S. Schwarz (984). A two-factor model of the term tructure: An approximate analytical olution. Journal of Financial and Quantitive Analyi, 9,
Problem 1. Construct a filtered probability space on which a Brownian motion W and an adapted process X are defined and such that
Stochatic Calculu Example heet 4 - Lent 5 Michael Tehranchi Problem. Contruct a filtered probability pace on which a Brownian motion W and an adapted proce X are defined and uch that dx t = X t t dt +
More informationChapter 4. The Laplace Transform Method
Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination
More informationHyperbolic Partial Differential Equations
Hyperbolic Partial Differential Equation Evolution equation aociated with irreverible phyical procee like diffuion heat conduction lead to parabolic partial differential equation. When the equation i a
More informationSOME RESULTS ON INFINITE POWER TOWERS
NNTDM 16 2010) 3, 18-24 SOME RESULTS ON INFINITE POWER TOWERS Mladen Vailev - Miana 5, V. Hugo Str., Sofia 1124, Bulgaria E-mail:miana@abv.bg Abtract To my friend Kratyu Gumnerov In the paper the infinite
More informationBogoliubov Transformation in Classical Mechanics
Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How
More informationON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang
Proceeding of the 2008 Winter Simulation Conference S. J. Maon, R. R. Hill, L. Mönch, O. Roe, T. Jefferon, J. W. Fowler ed. ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION Xiaoqun Wang
More informationLecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004
18.997 Topic in Combinatorial Optimization April 29th, 2004 Lecture 21 Lecturer: Michel X. Goeman Scribe: Mohammad Mahdian 1 The Lovaz plitting-off lemma Lovaz plitting-off lemma tate the following. Theorem
More information6. KALMAN-BUCY FILTER
6. KALMAN-BUCY FILTER 6.1. Motivation and preliminary. A wa hown in Lecture 2, the optimal control i a function of all coordinate of controlled proce. Very often, it i not impoible to oberve a controlled
More informationSTOCHASTIC EVOLUTION EQUATIONS WITH RANDOM GENERATORS. By Jorge A. León 1 and David Nualart 2 CINVESTAV-IPN and Universitat de Barcelona
The Annal of Probability 1998, Vol. 6, No. 1, 149 186 STOCASTIC EVOLUTION EQUATIONS WIT RANDOM GENERATORS By Jorge A. León 1 and David Nualart CINVESTAV-IPN and Univeritat de Barcelona We prove the exitence
More informationMulti-dimensional Fuzzy Euler Approximation
Mathematica Aeterna, Vol 7, 2017, no 2, 163-176 Multi-dimenional Fuzzy Euler Approximation Yangyang Hao College of Mathematic and Information Science Hebei Univerity, Baoding 071002, China hdhyywa@163com
More information7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281
72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition
More informationTRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL
GLASNIK MATEMATIČKI Vol. 38583, 73 84 TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL p-laplacian Haihen Lü, Donal O Regan and Ravi P. Agarwal Academy of Mathematic and Sytem Science, Beijing, China, National
More informationc n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k
1. Exitence Let x (0, 1). Define c k inductively. Suppoe c 1,..., c k 1 are already defined. We let c k be the leat integer uch that x k An eay proof by induction give that and for all k. Therefore c n
More informationLecture 3. January 9, 2018
Lecture 3 January 9, 208 Some complex analyi Although you might have never taken a complex analyi coure, you perhap till know what a complex number i. It i a number of the form z = x + iy, where x and
More information1. The F-test for Equality of Two Variances
. The F-tet for Equality of Two Variance Previouly we've learned how to tet whether two population mean are equal, uing data from two independent ample. We can alo tet whether two population variance are
More informationEVOLUTION EQUATION OF A STOCHASTIC SEMIGROUP WITH WHITE-NOISE DRIFT
The Annal of Probability, Vol. 8, No. 1, 36 73 EVOLUTION EQUATION OF A STOCHASTIC SEMIGROUP WITH WHITE-NOISE DRIFT By David Nualart 1 and Frederi Vien Univeritat de Barcelona and Univerity of North Texa
More informationarxiv: v2 [math.nt] 30 Apr 2015
A THEOREM FOR DISTINCT ZEROS OF L-FUNCTIONS École Normale Supérieure arxiv:54.6556v [math.nt] 3 Apr 5 943 Cachan November 9, 7 Abtract In thi paper, we etablih a imple criterion for two L-function L and
More informationIEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation
IEOR 316: Fall 213, Profeor Whitt Topic for Dicuion: Tueday, November 19 Alternating Renewal Procee and The Renewal Equation 1 Alternating Renewal Procee An alternating renewal proce alternate between
More informationSOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document.
SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU CİHAN BAHRAN I will collect my olution to ome of the exercie in thi book in thi document. Section 2.1 1. Let A = k[[t ]] be the ring of
More informationMATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.:
MATEMATIK Datum: 20-08-25 Tid: eftermiddag GU, Chalmer Hjälpmedel: inga A.Heintz Telefonvakt: Ander Martinon Tel.: 073-07926. Löningar till tenta i ODE och matematik modellering, MMG5, MVE6. Define what
More informationAppendix. Proof of relation (3) for α 0.05.
Appendi. Proof of relation 3 for α.5. For the argument, we will need the following reult that follow from Lemma 1 Bakirov 1989 and it proof. Lemma 1 Let g,, 1 be a continuouly differentiable function uch
More informationONLINE SUPPLEMENT FOR EVALUATING FACTOR PRICING MODELS USING HIGH FREQUENCY PANELS
ONLINE SUPPLEMEN FOR EVALUAING FACOR PRICING MODELS USING HIGH FREQUENCY PANELS YOOSOON CHANG, YONGOK CHOI, HWAGYUN KIM AND JOON Y. PARK hi online upplement contain ome ueful lemma and their proof and
More informationOnline Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat
Online Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat Thi Online Appendix contain the proof of our reult for the undicounted limit dicued in Section 2 of the paper,
More informationOne Class of Splitting Iterative Schemes
One Cla of Splitting Iterative Scheme v Ciegi and V. Pakalnytė Vilniu Gedimina Technical Univerity Saulėtekio al. 11, 2054, Vilniu, Lithuania rc@fm.vtu.lt Abtract. Thi paper deal with the tability analyi
More informationResearch Article Existence for Nonoscillatory Solutions of Higher-Order Nonlinear Differential Equations
International Scholarly Reearch Network ISRN Mathematical Analyi Volume 20, Article ID 85203, 9 page doi:0.502/20/85203 Reearch Article Exitence for Nonocillatory Solution of Higher-Order Nonlinear Differential
More informationLaplace Transformation
Univerity of Technology Electromechanical Department Energy Branch Advance Mathematic Laplace Tranformation nd Cla Lecture 6 Page of 7 Laplace Tranformation Definition Suppoe that f(t) i a piecewie continuou
More informationThe fractional stochastic heat equation on the circle: Time regularity and potential theory
Stochatic Procee and their Application 119 (9) 155 154 www.elevier.com/locate/pa The fractional tochatic heat equation on the circle: Time regularity and potential theory Eulalia Nualart a,, Frederi Vien
More informationFOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS
FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS Nguyen Thanh Lan Department of Mathematic Wetern Kentucky Univerity Email: lan.nguyen@wku.edu ABSTRACT: We ue Fourier erie to find a neceary
More informationComputers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order
Computer and Mathematic with Application 64 (2012) 2262 2274 Content lit available at SciVere ScienceDirect Computer and Mathematic with Application journal homepage: wwweleviercom/locate/camwa Sharp algebraic
More informationWEIGHTED NORM INEQUALITIES FOR FRACTIONAL MAXIMAL OPERATORS - A BELLMAN FUNCTION APPROACH
WEIGHTED NORM INEUALITIES FOR FRACTIONAL MAXIMAL OPERATORS - A BELLMAN FUNCTION APPROACH RODRIGO BAÑUELOS AND ADAM OSȨKOWSKI ABSTRACT. We tudy claical weighted L p L q inequalitie for the fractional maximal
More informationin a circular cylindrical cavity K. Kakazu Department of Physics, University of the Ryukyus, Okinawa , Japan Y. S. Kim
Quantization of electromagnetic eld in a circular cylindrical cavity K. Kakazu Department of Phyic, Univerity of the Ryukyu, Okinawa 903-0, Japan Y. S. Kim Department of Phyic, Univerity of Maryland, College
More informationTCER WORKING PAPER SERIES GOLDEN RULE OPTIMALITY IN STOCHASTIC OLG ECONOMIES. Eisei Ohtaki. June 2012
TCER WORKING PAPER SERIES GOLDEN RULE OPTIMALITY IN STOCHASTIC OLG ECONOMIES Eiei Ohtaki June 2012 Working Paper E-44 http://www.tcer.or.jp/wp/pdf/e44.pdf TOKYO CENTER FOR ECONOMIC RESEARCH 1-7-10 Iidabahi,
More informationNotes on the geometry of curves, Math 210 John Wood
Baic definition Note on the geometry of curve, Math 0 John Wood Let f(t be a vector-valued function of a calar We indicate thi by writing f : R R 3 and think of f(t a the poition in pace of a particle
More informationOPTIMAL STOPPING FOR SHEPP S URN WITH RISK AVERSION
OPTIMAL STOPPING FOR SHEPP S URN WITH RISK AVERSION ROBERT CHEN 1, ILIE GRIGORESCU 1 AND MIN KANG 2 Abtract. An (m, p) urn contain m ball of value 1 and p ball of value +1. A player tart with fortune k
More informationStochastic Neoclassical Growth Model
Stochatic Neoclaical Growth Model Michael Bar May 22, 28 Content Introduction 2 2 Stochatic NGM 2 3 Productivity Proce 4 3. Mean........................................ 5 3.2 Variance......................................
More informationOptimal financing and dividend control of the insurance company with proportional reinsurance policy
Inurance: Mathematic and Economic 42 28 976 983 www.elevier.com/locate/ime Optimal financing and dividend control of the inurance company with proportional reinurance policy Lin He a, Zongxia Liang b,
More informationTheoretical Computer Science. Optimal algorithms for online scheduling with bounded rearrangement at the end
Theoretical Computer Science 4 (0) 669 678 Content lit available at SciVere ScienceDirect Theoretical Computer Science journal homepage: www.elevier.com/locate/tc Optimal algorithm for online cheduling
More informationFILTERING OF NONLINEAR STOCHASTIC FEEDBACK SYSTEMS
FILTERING OF NONLINEAR STOCHASTIC FEEDBACK SYSTEMS F. CARRAVETTA 1, A. GERMANI 1,2, R. LIPTSER 3, AND C. MANES 1,2 Abtract. Thi paper concern the filtering problem for a cla of tochatic nonlinear ytem
More informationA SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho
A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES Sanghyun Cho Abtract. We prove a implified verion of the Nah-Moer implicit function theorem in weighted Banach pace. We relax the
More informationNULL HELIX AND k-type NULL SLANT HELICES IN E 4 1
REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Vol. 57, No. 1, 2016, Page 71 83 Publihed online: March 3, 2016 NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1 JINHUA QIAN AND YOUNG HO KIM Abtract. We tudy
More informationREVERSE HÖLDER INEQUALITIES AND INTERPOLATION
REVERSE HÖLDER INEQUALITIES AND INTERPOLATION J. BASTERO, M. MILMAN, AND F. J. RUIZ Abtract. We preent new method to derive end point verion of Gehring Lemma uing interpolation theory. We connect revere
More informationUNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE
UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE SEPPO GRANLUND AND NIKO MAROLA Abtract. We conider planar olution to certain quailinear elliptic equation ubject to the Dirichlet boundary
More informationPreemptive scheduling on a small number of hierarchical machines
Available online at www.ciencedirect.com Information and Computation 06 (008) 60 619 www.elevier.com/locate/ic Preemptive cheduling on a mall number of hierarchical machine György Dóa a, Leah Eptein b,
More informationGeometric Measure Theory
Geometric Meaure Theory Lin, Fall 010 Scribe: Evan Chou Reference: H. Federer, Geometric meaure theory L. Simon, Lecture on geometric meaure theory P. Mittila, Geometry of et and meaure in Euclidean pace
More informationConvex Hulls of Curves Sam Burton
Convex Hull of Curve Sam Burton 1 Introduction Thi paper will primarily be concerned with determining the face of convex hull of curve of the form C = {(t, t a, t b ) t [ 1, 1]}, a < b N in R 3. We hall
More informationDISCRETE ROUGH PATHS AND LIMIT THEOREMS
DISCRETE ROUGH PATHS AND LIMIT THEOREMS YANGHUI LIU AND SAMY TINDEL Abtract. In thi article, we conider it theorem for ome weighted type random um (or dicrete rough integral). We introduce a general tranfer
More informationSocial Studies 201 Notes for November 14, 2003
1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
More informationCOMPUTING DELTAS WITHOUT DERIVATIVES. This Version : May 23, 2015
COMPUING DELAS WIHOU DEIVAIVES D.. BAÑOS, S. DUEDAHL,. MEYE-BANDIS, AND F. POSKE hi Verion : May 23, 215 Abtract. A well-known application of Malliavin calculu in Mathematical Finance i the probabilitic
More informationQUENCHED LARGE DEVIATION FOR SUPER-BROWNIAN MOTION WITH RANDOM IMMIGRATION
Infinite Dimenional Analyi, Quantum Probability and Related Topic Vol., No. 4 28) 627 637 c World Scientific Publihing Company QUENCHED LARGE DEVIATION FOR SUPER-BROWNIAN MOTION WITH RANDOM IMMIGRATION
More informationarxiv: v2 [math.pr] 19 Aug 2016
Strong convergence of the ymmetrized Miltein cheme for ome CV-like SD Mireille Boy and Héctor Olivero arxiv:58458v mathpr 9 Aug 6 TOSCA Laboratory, INRIA Sophia Antipoli Méditerranée, France Departamento
More informationAdvanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis
Advanced Digital ignal Proceing Prof. Nizamettin AYDIN naydin@yildiz.edu.tr Time-Frequency Analyi http://www.yildiz.edu.tr/~naydin 2 tationary/nontationary ignal Time-Frequency Analyi Fourier Tranform
More informationManprit Kaur and Arun Kumar
CUBIC X-SPLINE INTERPOLATORY FUNCTIONS Manprit Kaur and Arun Kumar manpreet2410@gmail.com, arun04@rediffmail.com Department of Mathematic and Computer Science, R. D. Univerity, Jabalpur, INDIA. Abtract:
More informationμ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL =
Our online Tutor are available 4*7 to provide Help with Proce control ytem Homework/Aignment or a long term Graduate/Undergraduate Proce control ytem Project. Our Tutor being experienced and proficient
More informationSECTION x2 x > 0, t > 0, (8.19a)
SECTION 8.5 433 8.5 Application of aplace Tranform to Partial Differential Equation In Section 8.2 and 8.3 we illutrated the effective ue of aplace tranform in olving ordinary differential equation. The
More informationGeneral System of Nonconvex Variational Inequalities and Parallel Projection Method
Mathematica Moravica Vol. 16-2 (2012), 79 87 General Sytem of Nonconvex Variational Inequalitie and Parallel Projection Method Balwant Singh Thakur and Suja Varghee Abtract. Uing the prox-regularity notion,
More informationMULTIDIMENSIONAL SDES WITH SINGULAR DRIFT AND UNIVERSAL CONSTRUCTION OF THE POLYMER MEASURE WITH WHITE NOISE POTENTIAL
Submitted to the Annal of Probability arxiv: arxiv:151.4751 MULTIDIMENSIONAL SDES WITH SINGULAR DRIFT AND UNIVERSAL CONSTRUCTION OF THE POLYMER MEASURE WITH WHITE NOISE POTENTIAL BY GIUSEPPE CANNIZZARO,
More informationHilbert-Space Integration
Hilbert-Space Integration. Introduction. We often tink of a PDE, like te eat equation u t u xx =, a an evolution equation a itorically wa done for ODE. In te eat equation example two pace derivative are
More informationMath 273 Solutions to Review Problems for Exam 1
Math 7 Solution to Review Problem for Exam True or Fale? Circle ONE anwer for each Hint: For effective tudy, explain why if true and give a counterexample if fale (a) T or F : If a b and b c, then a c
More informationAssignment for Mathematics for Economists Fall 2016
Due date: Mon. Nov. 1. Reading: CSZ, Ch. 5, Ch. 8.1 Aignment for Mathematic for Economit Fall 016 We now turn to finihing our coverage of concavity/convexity. There are two part: Jenen inequality for concave/convex
More informationON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria
GLASNIK MATEMATIČKI Vol. 1(61)(006), 9 30 ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS Volker Ziegler Techniche Univerität Graz, Autria Abtract. We conider the parameterized Thue
More informationList coloring hypergraphs
Lit coloring hypergraph Penny Haxell Jacque Vertraete Department of Combinatoric and Optimization Univerity of Waterloo Waterloo, Ontario, Canada pehaxell@uwaterloo.ca Department of Mathematic Univerity
More informationThe continuous time random walk (CTRW) was introduced by Montroll and Weiss 1.
1 I. CONTINUOUS TIME RANDOM WALK The continuou time random walk (CTRW) wa introduced by Montroll and Wei 1. Unlike dicrete time random walk treated o far, in the CTRW the number of jump n made by the walker
More informationProblem Set 8 Solutions
Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem
More informationResearch Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation
Hindawi Function Space Volume 2017, Article ID 7916730, 8 page http://doi.org/10.1155/2017/7916730 Reearch Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation Huahui Zhan 1 and Bifen Xu
More information1 Routh Array: 15 points
EE C28 / ME34 Problem Set 3 Solution Fall 2 Routh Array: 5 point Conider the ytem below, with D() k(+), w(t), G() +2, and H y() 2 ++2 2(+). Find the cloed loop tranfer function Y () R(), and range of k
More informationIntroduction to Laplace Transform Techniques in Circuit Analysis
Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found
More informationSingular perturbation theory
Singular perturbation theory Marc R. Rouel June 21, 2004 1 Introduction When we apply the teady-tate approximation (SSA) in chemical kinetic, we typically argue that ome of the intermediate are highly
More informationStochastic differential equations with fractal noise
Math. Nachr. 78, No. 9, 197 116 (5) / DOI 1.1/mana.3195 Stochatic differential equation with fractal noie M. Zähle 1 1 Mathematical Intitute, Univerity of Jena, 7737 Jena, Germany Received 8 October, revied
More informationON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS
ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS VOLKER ZIEGLER Abtract We conider the parameterized Thue equation X X 3 Y (ab + (a + bx Y abxy 3 + a b Y = ±1, where a, b 1 Z uch that
More informationFactor Analysis with Poisson Output
Factor Analyi with Poion Output Gopal Santhanam Byron Yu Krihna V. Shenoy, Department of Electrical Engineering, Neurocience Program Stanford Univerity Stanford, CA 94305, USA {gopal,byronyu,henoy}@tanford.edu
More informationFIRST-ORDER EULER SCHEME FOR SDES DRIVEN BY FRACTIONAL BROWNIAN MOTIONS: THE ROUGH CASE
FIRST-ORDER EULER SCHEME FOR SDES DRIVEN BY FRACTIONAL BROWNIAN MOTIONS: THE ROUGH CASE YANGHUI LIU AND SAMY TINDEL Abtract. In thi article, we conider the o-called modified Euler cheme for tochatic differential
More informationON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS
Journal of Pure and Applied Mathematic: Advance and Application Volume, umber, 4, Page -35 O THE SMOOTHESS OF SOLUTIOS TO A SPECIAL EUMA PROBLEM O OSMOOTH DOMAIS ADREAS EUBAUER Indutrial Mathematic Intitute
More informationFebruary 5, :53 WSPC/INSTRUCTION FILE Mild solution for quasilinear pde
February 5, 14 1:53 WSPC/INSTRUCTION FILE Mild olution for quailinear pde Infinite Dimenional Analyi, Quantum Probability and Related Topic c World Scientific Publihing Company STOCHASTIC QUASI-LINEAR
More informationDemonstration of Riemann Hypothesis
Demontration of Riemann Hypothei Diego arin June 2, 204 Abtract We define an infinite ummation which i proportional to the revere of Riemann Zeta function ζ(). Then we demontrate that uch function can
More informationRobustness analysis for the boundary control of the string equation
Routne analyi for the oundary control of the tring equation Martin GUGAT Mario SIGALOTTI and Mariu TUCSNAK I INTRODUCTION AND MAIN RESULTS In thi paper we conider the infinite dimenional ytem determined
More informationUnbounded solutions of second order discrete BVPs on infinite intervals
Available online at www.tjna.com J. Nonlinear Sci. Appl. 9 206), 357 369 Reearch Article Unbounded olution of econd order dicrete BVP on infinite interval Hairong Lian a,, Jingwu Li a, Ravi P Agarwal b
More informationSome Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value
Journal of Mathematical Reearch with Application May, 205, Vol 35, No 3, pp 256 262 DOI:03770/jin:2095-26520503002 Http://jmredluteducn Some Set of GCF ϵ Expanion Whoe Parameter ϵ Fetch the Marginal Value
More informationAn example of a non-markovian stochastic two-point boundary value problem
Bernoulli 3(4), 1997, 371±386 An example of a non-markovian tochatic two-point boundary value problem MARCO FERRANTE 1 and DAVID NUALART 2 1 Dipartimento di Matematica, UniveritaÁ di Padova, via Belzoni
More informationFlag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle
Flag-tranitive non-ymmetric -deign with (r, λ = 1 and alternating ocle Shenglin Zhou, Yajie Wang School of Mathematic South China Univerity of Technology Guangzhou, Guangdong 510640, P. R. China lzhou@cut.edu.cn
More informationHylleraas wavefunction for He. dv 2. ,! r 2. )dv 1. in the trial function. A simple trial function that does include r 12. is ) f (r 12.
Hylleraa wavefunction for He The reaon why the Hartree method cannot reproduce the exact olution i due to the inability of the Hartree wave-function to account for electron correlation. We know that the
More informationTAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES
TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Abtract. We are concerned with the repreentation of polynomial for nabla dynamic equation on time cale. Once etablihed,
More informationLecture 10 Filtering: Applied Concepts
Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering
More informationWorking Papers / Documents de travail
Working Paper / Document de travail HJB Equation in Infinite Dimenion and Optimal Control of Stochatic Evolution Equation via Generalized Fukuhima Decompoition Giorgio Fabbri Franceco Ruo WP 2017 - Nr
More informationA Full-Newton Step Primal-Dual Interior Point Algorithm for Linear Complementarity Problems *
ISSN 76-7659, England, UK Journal of Information and Computing Science Vol 5, No,, pp 35-33 A Full-Newton Step Primal-Dual Interior Point Algorithm for Linear Complementarity Problem * Lipu Zhang and Yinghong
More informationChip-firing game and a partial Tutte polynomial for Eulerian digraphs
Chip-firing game and a partial Tutte polynomial for Eulerian digraph Kévin Perrot Aix Mareille Univerité, CNRS, LIF UMR 7279 3288 Mareille cedex 9, France. kevin.perrot@lif.univ-mr.fr Trung Van Pham Intitut
More informationA CATEGORICAL CONSTRUCTION OF MINIMAL MODEL
A ATEGORIAL ONSTRUTION OF MINIMAL MODEL A. Behera, S. B. houdhury M. Routaray Department of Mathematic National Intitute of Technology ROURKELA - 769008 (India) abehera@nitrkl.ac.in 512ma6009@nitrkl.ac.in
More informationOn Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces
On Uniform Exponential Trichotomy of Evolution Operator in Banach Space Mihail Megan, Codruta Stoica To cite thi verion: Mihail Megan, Codruta Stoica. On Uniform Exponential Trichotomy of Evolution Operator
More informationLinear System Fundamentals
Linear Sytem Fundamental MEM 355 Performance Enhancement of Dynamical Sytem Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Content Sytem Repreentation Stability Concept
More informationAsymptotic behavior of solutions of mixed problem for linear thermo-elastic systems with microtemperatures
Mathematica Aeterna, Vol. 8, 18, no. 4, 7-38 Aymptotic behavior of olution of mixed problem for linear thermo-elatic ytem with microtemperature Gulhan Kh. Shafiyeva Baku State Univerity Intitute of Mathematic
More informationTHE THERMOELASTIC SQUARE
HE HERMOELASIC SQUARE A mnemonic for remembering thermodynamic identitie he tate of a material i the collection of variable uch a tre, train, temperature, entropy. A variable i a tate variable if it integral
More informationA BATCH-ARRIVAL QUEUE WITH MULTIPLE SERVERS AND FUZZY PARAMETERS: PARAMETRIC PROGRAMMING APPROACH
Mathematical and Computational Application Vol. 11 No. pp. 181-191 006. Aociation for Scientific Reearch A BATCH-ARRIVA QEE WITH MTIPE SERVERS AND FZZY PARAMETERS: PARAMETRIC PROGRAMMING APPROACH Jau-Chuan
More informationRiemann s Functional Equation is Not a Valid Function and Its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.
Riemann Functional Equation i Not a Valid Function and It Implication on the Riemann Hypothei By Armando M. Evangelita Jr. armando78973@gmail.com On Augut 28, 28 ABSTRACT Riemann functional equation wa
More informationMAXIMUM LIKELIHOOD ESTIMATION OF HIDDEN MARKOV PROCESSES. BY HALINA FRYDMAN AND PETER LAKNER New York University
he Annal of Applied Probability 23, Vol. 13, No. 4, 1296 1312 Intitute of Mathematical Statitic, 23 MAXIMUM LIKELIHOOD ESIMAION OF HIDDEN MARKOV PROCESSES BY HALINA FRYDMAN AND PEER LAKNER New York Univerity
More informationPrimitive Digraphs with the Largest Scrambling Index
Primitive Digraph with the Larget Scrambling Index Mahmud Akelbek, Steve Kirkl 1 Department of Mathematic Statitic, Univerity of Regina, Regina, Sakatchewan, Canada S4S 0A Abtract The crambling index of
More informationNonlinear Single-Particle Dynamics in High Energy Accelerators
Nonlinear Single-Particle Dynamic in High Energy Accelerator Part 6: Canonical Perturbation Theory Nonlinear Single-Particle Dynamic in High Energy Accelerator Thi coure conit of eight lecture: 1. Introduction
More information1. Preliminaries. In [8] the following odd looking integral evaluation is obtained.
June, 5. Revied Augut 8th, 5. VA DER POL EXPASIOS OF L-SERIES David Borwein* and Jonathan Borwein Abtract. We provide concie erie repreentation for variou L-erie integral. Different technique are needed
More informationSocial Studies 201 Notes for March 18, 2005
1 Social Studie 201 Note for March 18, 2005 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
More informationStochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions
Stochatic Optimization with Inequality Contraint Uing Simultaneou Perturbation and Penalty Function I-Jeng Wang* and Jame C. Spall** The John Hopkin Univerity Applied Phyic Laboratory 11100 John Hopkin
More informationarxiv: v3 [math.pr] 21 Aug 2015
On dynamical ytem perturbed by a null-recurrent fat motion: The continuou coefficient cae with independent driving noie Zolt Pajor-Gyulai, Michael Salin arxiv:4.4625v3 [math.pr] 2 Aug 25 Department of
More informationChapter Landscape of an Optimization Problem. Local Search. Coping With NP-Hardness. Gradient Descent: Vertex Cover
Coping With NP-Hardne Chapter 12 Local Search Q Suppoe I need to olve an NP-hard problem What hould I do? A Theory ay you're unlikely to find poly-time algorithm Mut acrifice one of three deired feature
More information