Large time unimodality for classical and free Brownian motions with initial distributions

Size: px
Start display at page:

Download "Large time unimodality for classical and free Brownian motions with initial distributions"

Transcription

1 ALEA, La. Am. J. Probab. Mah. Sa. 5, (08) DOI: 0757/ALEA.v5-5 Large ime unimodaliy for classical and free Brownian moions wih iniial disribuions Takahiro Hasebe and Yuki Ueda Deparmen of Mahemaics, Hokkaido Universiy, Kia 0, Nishi 8, Kia-Ku, Sapporo, Hokkaido, , Japan address: UL: hps:// Deparmen of Mahemaics, Hokkaido Universiy, Kia 0, Nishi 8, Kia-Ku, Sapporo, Hokkaido, , Japan address: Absrac. We prove ha classical and free Brownian moions wih iniial disribuions are unimodal for sufficienly large ime, under some assumpion on he iniial disribuions. The assumpion is almos opimal in some sense. Similar resuls are shown for a symmeric sable process wih index and a posiive sable process wih index /. We also prove ha free Brownian moion wih iniial symmeric unimodal disribuion is unimodal, and discuss srong unimodaliy for free convoluion.. Inroducion A Borel measure µ on is unimodal if here exis a and a funcion f: [0, ) which is non-decreasing on (,a) and non-increasing on (a, ), such ha µ(dx) = µ({a})δ a +f(x)dx. (.) The mos ousanding resul on unimodaliy is Yamazao s heorem (Yamazao, 978) saying ha all classical selfdecomposable disribuions are unimodal. Afer his resul, in Hasebe and Thorbjørnsen (06), Hasebe and Thorbjørnsen proved he free analog of Yamazao s resul: all freely selfdecomposable disribuions are unimodal. The unimodaliy has several oher similariy poins beween he classical and free probabiliy heories Hasebe and Sakuma (07). However, i is no rue ha he unimodaliy shows complee similariy beween he classical and free probabiliy heories. For example, classical compound Poisson processes are likely o be eceived by he ediors Ocober 7h, 07; acceped March 3h, Mahemaics Subjec Classificaion. Primary 46L54; Secondary 60E07; 60G5, 60J65. Key words and phrases. unimodal, srongly unimodal, Brownian moion, Cauchy process, posiive sable process. esearch suppored by JSPS Gran-in-Aid for Young Scieniss (B) 5K7549 (for TH) and JSPS and MAEDI Japan France Inegraed Acion Program (SAKUA) (for boh auhors). 353

2 354 T. Hasebe and Y. Ueda non-unimodal in large ime (Wolfe, 978), while free Lévy processes wih compac suppor become unimodal in large ime (Hasebe and Sakuma, 07). In his paper, we mainly focus on he unimodaliy of classical and free Brownian moions wih iniial disribuions and consider wheher he classical and free versions share similariy poins or no. In free probabiliy heory, he semicircle disribuion is he free analog of he normal disribuion. In random marix heory, i appears as he limi of eigenvalue disribuions of Wigner marices as he size of he random marices goes o infiniy. Free Brownian moion is defined as a process wih free independen incremens, sared a 0 and disribued as he cenered semicircle disribuion S(0,) a ime > 0. Furhermore, we can provide free Brownian moion wih iniial disribuion µ which is a process wih free independen incremens disribued as µ a = 0 and as µ S(0,) a ime > 0. The definiion of, called addiive free convoluion, is provided in Secion.. The addiive free convoluion is he disribuion of he sum of wo random variables which are freely independen (for he definiion of free independence see Nica and Speicher, 006). In Biane (997), Biane gave he densiy funcion formula of free Brownian moion wih iniial disribuion (see Secion.). In our sudies, we firs consider he symmeric Bernoulli disribuion µ := δ + + δ as an iniial disribuion and compue he densiy funcion of µ S(0,). Then we see ha he probabiliy disribuion µ S(0,) is unimodal for 4 (and i is no unimodal for 0 < < 4). This compuaion leads o a naural problem: Problem.. Forwhich classofprobabiliymeasuresµon does he free Brownian moion wih iniial disribuion µ become unimodal for sufficienly large ime? We hen answer o his problem as follows (formulaed as Theorem 3. and Proposiion 3.4 in Secion 3.): Theorem.. () Le µ be a compacly suppored probabiliy measure on and D µ := sup{ x y : x,y supp(µ)}. Then µ S(0,) is unimodal for 4Dµ. () Le f: [0, ) be a Borel measurable funcion. Then here exiss a probabiliy measure µ on such ha µ S(0,) is no unimodal for any > 0 and f(x)dµ(x) <. (.) Noe ha such a measure µ is no compacly suppored by (). The funcion f can grow very fas such as e x, and so, a ail decay of he iniial disribuion does no imply large ime unimodaliy. The corresponding classical problem is naural, ha is, for which class of iniial disribuions on does Brownian moion become unimodal for sufficienly large ime > 0? We prove in his direcion he following resuls (formulaed as Theorem 4.3 and Proposiion 4. in Secion 4, respecively): Theorem.3. () Le µ be a probabiliy measure on such ha α := e εx dµ(x) < (.3) for some ε > 0. Then he disribuion µ N(0,) is unimodal for all 36 log(α) ε.

3 Unimodaliy for classical and free Brownian moions 355 () There exiss a probabiliy measure µ on saisfying ha e A x p dµ(x) < for all A > 0 and 0 < p < (.4) such ha µ N(0,) is no unimodal for any > 0. Thus, in he classical case, he ail decay (.3) is sufficien and almos necessary o guaranee he large ime unimodaliy. From hese resuls, we conclude ha he classical and free versions of he problems of unimodaliy for Brownian moions wih iniial disribuions share common feaures as boh become unimodal in large ime under each assumpion. Furher relaed resuls in his paper are as follows. In Secion 3. we prove ha µ S(0,) is always unimodal whenever µ is symmeric around 0 and unimodal (see Theorem 3.6). In Secion 3.3, we define freely srongly unimodal probabiliy measures as a naural free analogue of srongly unimodal probabiliy measures. We conclude ha he semicircle disribuions are no freely srongly unimodal (Lemma 3.9). More generally, we have he following resul (resaed as Theorem 3.0 laer): Theorem.4. Le λ be a probabiliy measure wih finie variance, no being a dela measure. Then λ is no freely srongly unimodal. On he oher hand, here are many srongly unimodal disribuions wih finie variance in classical probabiliy including he normal disribuions and exponenial disribuions. Thus he noion of srong unimodaliy breaks he similariy beween he classical and free probabiliy heories. In Secion 5, we focus on oher processes wih classical/free independen incremens wih iniial disribuions. We consider a symmeric sable process wih index and a posiive sable process wih index /. Then we prove large ime unimodaliy similar o he case of Brownian moion bu under differen ail decay assumpions.. Preliminaries.. Definiion of free convoluion. Le µ be a probabiliy measure on. The Cauchy ransform G µ (z) := dµ(x) (.) z x is analyic on he complex upper half plane C +. We define he runcaed cones Γ ± α,β := {z C± : e(z) < α Im(z), Im(z) > β}, α > 0,β. (.) In Bercovici and Voiculescu (993, Proposiion 5.4), i was proved ha for any γ < 0 here exis α,β > 0 and δ < 0 such ha G µ is univalen on Γ + α,β and Γ γ,δ G µ(γ + α,β ). Therefore he righ inverse funcion G µ exiss on Γ γ,δ. We define he -ransform of µ by µ (z) := G µ (z) z, z Γ γ,δ. (.3) Then for any probabiliy measures µ and ν on here exiss a unique probabiliy measure λ on such ha λ (z) = µ (z)+ ν (z), (.4)

4 356 T. Hasebe and Y. Ueda for all z in he inersecion of he domains of he hree ransforms. We denoe λ := µ ν and call i he (addiive) free convoluion of µ and ν... Free convoluion wih semicircle disribuions. Almos all he maerials and mehods in his secion are following (Biane, 997). The semicircle disribuion S(0,) of mean 0 and variance > 0 is he probabiliy measure wih densiy 4 x, (.5) π suppored on he inerval [, ]. We hen compue is Cauchy ransform and is -ransform (see, for example, Nica and Speicher, 006): G S(0,) (z) = z z 4, z C +, (.6) where he branch of he square roo on C\ + is such ha = i. Moreover S(0,) (z) = z, z C. (.7) Le µ be a probabiliy measure on and le µ = µ S(0,). Then we define he following se: { U := u (x u) dµ(x) > }, (.8) and he following funcion from o [0, ) by seing { v (u) := inf v 0 (x u) +v dµ(x) }. (.9) Then v is coninuous on and one has U = {x v (u) > 0}. Moreover, for every u U, v (u) is he unique soluion v > 0 of he equaion (x u) +v dµ(x) =. (.0) We define Ω,µ := {x+iy C y > v (x)}. (.) Then he map H (z) := z + S(0,) (G µ (z)), defined on C +, is a homeomorphism from Ω,µ o C + and i is conformal from Ω,µ ono C +. Hence here exiss an inverse funcion F : C + Ω,µ. By Biane (997, Lemma, Proposiion ), he domain Ω,µ is equal o he conneced componen of he se H (C + ) which conains iy for large y > 0 and for all z C + one has G µ (z) = G µ (H (F (z))) = G µ ( F (z)+ S(0,) ( Gµ (F (z)) )) = G µ (F (z)). (.) MoreoverG µ hasaconinuousexensiono C +. Then µ is Lebesgueabsoluely coninuous by Sieljes inversion and he densiy funcion p : [0, ) of µ is given by where p (ψ (x)) = π lim Im(G µ (ψ (x)+iy)) = v (x), x, (.3) y +0 π (x u) ψ (x) = H (x+iv (x)) = x+ (x u) dµ(u). (.4) +v (x)

5 Unimodaliy for classical and free Brownian moions 357 I can be shown ha ψ is a homeomorphism of. Furhermore he opological suppor of p is given by ψ (U ), and p exends o a coninuous funcion on and is real analyic in {x : p (x) > 0}. Example.. Le µ := δ + δ + be he symmeric Bernoulli disribuion. ecall ha he opological suppor of he densiy funcion p is equal o ψ (U ). If 0 <, we have U = u + +8 < u < ++ +8, (.5) and if >, we have U = u < u < +8. (.6) If 0 < hen he number of conneced componens of U is wo, and herefore µ is no unimodal. If > hen U is conneced. By he densiy formula (.3), he unimodaliy of µ is equivalen o he unimodaliy of he funcion v (u), he laer being expressed in he form (u v (u) = + )+ +6u. (.7) Calculaing is firs derivaive hen shows ha µ is unimodal if and only if 4; see Figures..6. According o Example., we have a quesion abou wha class of iniial disribuions implies he large ime unimodaliy of free Brownian moion. We will give a resul for his in Secion Figure.. p (x) Figure.. p (x) Figure.3. p (x) Figure.4. p 3 (x) Figure.5. p 4 (x) Figure.6. p 7 (x)

6 358 T. Hasebe and Y. Ueda.3. A basic lemma for unimodaliy. A unimodal disribuion is allowed o have a plaeau or a disconinuous poin in is densiy such as he uniform disribuion or he exponenial disribuion. If we exclude such cases, hen unimodaliy can be characerized in erms of levels of densiy. Lemma.. Le µ be a probabiliy measure on ha is Lebesgue absoluely coninuous. Suppose ha is densiy p(x) exends o a coninuous funcion on and is real analyic in {x : p(x) > 0}. Then µ is unimodal if and only if, for any a > 0, he equaion p(x) = a has a mos wo soluions x. The proof is jus o use he inermediae value heorem and he fac ha a real analyic funcion never has plaeaux. Noe ha he idea of he above lemma was firs inroduced by Haagerup and Thorbjørnsen(04) o prove ha a free gamma disribuion is unimodal. 3. Free Brownian moion wih iniial disribuion 3.. Large ime unimodaliy for free Brownian moion. The semicircular disribuion is he free analogue of he normal disribuion. Therefore, a process wih free independen incremens is called (sandard) free Brownian moion wih iniial disribuion µ if is disribuion a ime is given by µ S(0,). In his secion, we firsly prove ha free Brownian moion wih compacly suppored iniial disribuion is unimodal for sufficienly large ime, by using Biane s densiy formula (see Secion.). Lemma 3.. Suppose ha > 0. The following saemens are equivalen. () µ S(0,) is unimodal. () For any > 0 he equaion (x u) + dµ(x) = has a mos wo soluions u. (3.) Proof: We adop he noaions µ = µ S(0,),v,p and ψ in Secion.. This proofis similar o Hasebe and Thorbjørnsen (06, Proposiion 3.8). ecall ha µ is absoluely coninuous wih respec o Lebesgue measure and he densiy funcion p is coninuous on since is Cauchy ransform G µ has a coninuous exension o C +, and he densiy funcion is real analyic in ψ (U ) and coninuous on by Secion.. Suppose () firs. Since ψ is a homeomorphism of, by Lemma. i suffices o show ha for any a > 0 he equaion a = p (ψ (u)) = v (u), u (3.) π has a mos wo soluions u. Since v (u) is a unique soluion of he equaion (.0) if i is posiive, hen we have { u a = v } { (u) = u π (x u) +(πa) dµ(x) = }. (3.3) By he assumpion (), he equaion a = v(u) π has a mos wo soluions in.

7 Unimodaliy for classical and free Brownian moions 359 Conversely, suppose ha () does no hold. Then for some > 0 here are hree disinc soluions u,u,u 3 o (3.). By (3.3) his shows ha v (u i ) = and hence p (ψ (u i )) = π for i =,,3. Again by Lemma., µ is no unimodal. Now we are ready o prove Theorem. (). Theorem 3.. Le µ be a compacly suppored probabiliy measure, and le D µ be he diameer of he suppor: D µ = sup{ x y : x,y supp(µ)}. Then µ S(0,) is unimodal for 4D µ. Proof: Applying a shif we may assume ha µ is suppored on [ Dµ, Dµ ]. For fixed > 0, we define by ξ (u) := (x u) dµ(x), u. (3.4) + Then we have ξ (u) = Dµ Dµ Dµ ξ (u) = Dµ (x u) {(x u) + } dµ(x), 6(x u) {(x u) + } 3 dµ(x). (3.5) If u < Dµ, hen x u > Dµ ( Dµ ) = 0 for all x supp(µ), so ha ξ (u) > 0. If u > Dµ Dµ, hen x u < Dµ = 0 for all x supp(µ), so ha ξ (u) < 0. We ake 4Dµ and consider he form of ξ (u) on u ( Dµ, Dµ ). If 0 < < 3D µ, hen (x u) + < ( Dµ ξ (u) = + Dµ ) +( 3D µ ) = 4D µ, so ha (x u) + dµ(x) > (, u D µ, D ) µ. (3.6) Hence he equaion ξ (u) = has a mos wo soluions u if 4D µ. If 3D µ, hen he funcion ξ (u) saisfies he following hree condiions: ξ (u) > 0 for all u < Dµ and ξ Dµ (u) < 0 for all u >, ξ is coninuous on, ( ) ξ (u) < 0 for all u Dµ, Dµ. By he inermediae value heorem, ξ has a unique zero in [ Dµ, Dµ ] and hence ξ akes a unique local maximum in he inerval [ Dµ, Dµ ] (and herefore i is a unique global maximum on ). Therefore he equaion ξ (u) = has a mos wo soluions if 4Dµ. Hence we have ha he free convoluion µ S(0,) is unimodal if 4Dµ by Lemma 3.. Problem 3.3. Wha is he opimal universal consan C > 0 such ha µ S(0,) is unimodal for all CDµ and all probabiliy measures µ wih compac suppor? We have already shown ha C 4. ecall from Example. ha if µ is he symmeric Bernoulli disribuion on {,}, hen µ S(0,) is unimodal if and only if 4. Since he diameer D µ of he suppor of µ is, we conclude ha C 4. The nex quesion is wheher here exiss a probabiliy measure µ such ha µ S(0,) is no unimodal for any > 0 or a leas for sufficienly large > 0.

8 360 T. Hasebe and Y. Ueda Such a disribuion mus have an unbounded suppor if i exiss. Such an example can be consruced wih an idea similar o Huang (05, Proposiion 4.3) (see also Hasebe and Sakuma, 07, Example 5.3). Proposiion 3.4. Le f: [0, ) be a Borel measurable funcion. Then here exiss a probabiliy measure µ such ha µ S(0,) is no unimodal a any > 0 and f(x)dµ(x) <. (3.7) Proof: We follow he noaions in Secion.. Le {w n } n and {a n } n be sequences in saisfying w n > 0, n= w n =, a n+ > a n, n, lim (a n+ a n ) =. n Consider he probabiliy measure µ := n= w nδ an on and define he funcion X µ (u) := (u x) dµ(x) = w n (u a n ). (3.8) ecall ha U is he se of u such ha X µ (u) > /. Se b k := a k++a k for all k N. Then we have and so n= b k a n a k+ a k, k,n N (3.9) ( ) ( ) X µ (b k ) w n = 0 a k+ a k a k+ a k n= as k. This means ha for each > 0 here exiss an ineger K() > 0 such ha X µ (b k ) < for all k K(). This implies ha, for k K(), he closure of U does no conain b k. Noe ha he se U is an open se. Therefore, here exiss a sequence {ε k ()} k=k()+ of posiive numbers such ha U (b K(), ) = k=k()+ (a k ε k (),a k +ε k ()), (3.0) where he closures of he inervals are disjoin. Thus he se supp(µ ) = ψ (U ) consiss of infiniely many conneced componens for all > 0, and hence µ is no unimodal for any > 0. Inheaboveconsrucion,heweighsw n areonlyrequiredobeposiive. Therefore, we may ake c w n = n max{f(a n ),}, (3.) where c > 0 is a normalizing consan. Then he inegrabiliy condiion (3.7) is saisfied. Proposiion 3.4 shows ha ail decay esimaes of he iniial disribuion do no guaranee he large ime unimodaliy. In Secion 4 we shall see ha he siuaion is differen for classical Brownian moion.

9 Unimodaliy for classical and free Brownian moions Free Brownian moion wih symmeric iniial disribuion. This secion proves a unimodaliy resul of differen flavor. I is well known ha if µ and ν are symmeric unimodal disribuions, hen µ ν is also (symmeric) unimodal (see Sao, 03, Exercise 9.). The free analogue of his saemen is no known. Conjecure 3.5. Le µ and ν be symmeric unimodal disribuions. Then µ ν is unimodal. We can give a posiive answer in he special case when one disribuion is a semicircle disribuion. Theorem 3.6. Le µ be a symmeric unimodal disribuion on. Then µ S(0,) is unimodal for any > 0. emark 3.7. There is a unimodal probabiliy measure µ such ha µ S(0,) is no unimodal (see Lemma 3.9). Hence we canno remove he assumpion of symmery of µ. Proof of Theorem 3.6. By Lemma 3. i suffices o show ha for any > 0 he equaion (u x) + dµ(x) = (3.) has a mos wo soluions u. Up o a consan muliplicaion, he LHS is he densiy of µ C, which is unimodal since µ and C are symmeric unimodal. Since he densiy of µ C is real analyic, Lemma. implies ha he equaion (3.) has a mos wo soluions. This shows ha µ S(0,) is unimodal Freely srong unimodaliy. In classical probabiliy, a probabiliy measure is said o be srongly unimodal if µ ν is unimodal for all unimodal disribuions ν on. A disribuion is srongly unimodal if and only if he disribuion is Lebesgue absoluely coninuous, suppored on an inerval and a version of is densiy is log-concave (see Sao, 03, Theorem 5.3). From his characerizaion, he normal disribuions are srongly unimodal. We discuss he free version of srong unimodaliy. Definiion 3.8. Aprobabiliymeasureµon issaid obe freely srongly unimodal if µ ν is unimodal for all unimodal disribuions ν on. Lemma 3.9. The semicircle disribuions are no freely srongly unimodal. Proof: The Cauchy disribuion is no srongly unimodal since is densiy is no log-concave. Hence, here exiss a unimodal probabiliy measure µ such ha µ C is no unimodal. Since he densiy of µ C is real analyic on, by Lemma. here exiss > 0 such ha he equaion π d(µ C ) (x) = dx (x y) + dµ(y) = (3.3) has a leas hree disinc soluions x,x,x 3. Lemma 3. hen implies ha S(0,) µ is no unimodal. By changing he scaling, we conclude ha no semicircle disribuions are freely srongly unimodal. Theorem 3.0. Le λ be a probabiliy measure wih finie variance, no being a dela measure. Then λ is no freely srongly unimodal.

10 36 T. Hasebe and Y. Ueda Proof: We may assume ha λ has mean 0. Suppose ha λ is freely srongly unimodal. A simple inducion argumenshows ha λ n is freely sronglyunimodal for all n Z +. We derive a conradicion below. By Lemma 3.9 we can ake a unimodal probabiliy measure µ such ha µ S(0, ) is no unimodal. Our hypohesis shows ha he measure D nv(µ) λ n is unimodal, where v is he variance of λ and D c (ρ) is he push-forward of a measure ρ by he map x cx for c. By he free cenral limi heorem (Maassen, 99, Theorem 5.), he unimodal disribuions D / nv (D nv(µ) λ n ) = µ D / nv (λ n ) weakly converge o µ S(0,) as n. Since he se of unimodal disribuions is weakly closed (see Sao, 03, Exercise 9.0), we conclude ha µ S(0,) is unimodal, a conradicion. Problem 3.. Does here exis a freely srongly unimodal probabiliy measure ha is no a dela measure? 4. Classical Brownian moion wih iniial disribuion This secion discusses large ime unimodaliy for classical sandard Brownian moion wih an iniial disribuion µ, which is a process wih independen incremens disribued as µ N(0,) a ime 0. Before going o he general case, one example will be helpful in undersanding unimodaliy for µ N(0,). Example 4.. Elemenary calculus shows ha (δ +δ ) N(0,) (4.) is unimodal if and only if ; see Figures Figure 4.7. =.0 Figure 4.8. =.0 Figure 4.9. = Figure 4.0. = Figure 4.. = Figure 4.. = 4 This simple example suggess ha Brownian moion becomes unimodal for sufficienly large ime, possibly under some condiion on he iniial disribuion. In some sense, we give an almos opimal condiion on he iniial disribuion for he large ime unimodaliy o hold. We sar by providing an example of iniial disribuion wih which he Brownian moion never becomes unimodal.

11 Unimodaliy for classical and free Brownian moions 363 Proposiion 4.. There exiss a probabiliy measure µ on such ha µ N(0,) is no unimodal a any > 0, and e A x p dµ(x) < (4.) for all A > 0 and 0 < p <. Proof: We consider sequences {w n } n N (0, ) and {a n } n N such ha w n =, (4.3) n= b k := inf a k a n as k. (4.4) n Z +\{k} Moreover we assume ha for all > 0 here exiss k 0 = k 0 () N such ha k k 0 () w k e > bk e b k. (4.5) Define a probabiliy measure µ by seing µ := n= w nδ an and he following funcion: Then we have f (x) := π d(µ N(0,)) (x) = dx n= n= w n e (x an), x. (4.6) f (x) = ( w n x a n )e (x an), x. (4.7) If needed we may replace k 0 () by a larger ineger so ha b k > holds for all k k 0 (). For k k 0 () we have f (a k ) = w ( k e ak a n w n )e (a k an ) n N,n k w k e n N,n k w k e n N,n k w n a k a n w n b k e b ) (w k e bk e b k > 0, k e (a k an ) (4.8) where we used he fac ha x x e x akes he global maximum a x = ± on he hird inequaliy and he assumpion (4.5) on he las line. This implies ha µ N(0,) is no unimodal for any > 0. Nex we akespecific sequences {w n } n and {a n } n saisfying he condiions(4.3) (4.5). Se a k = a k, k N where a. Noe ha here exiss some consan c > 0 such ha b k ca k for all k N. Hence we have ha b k as k. Moreover we se w k := Me b kk, (4.9)

12 364 T. Hasebe and Y. Ueda where M > 0 is a normalized consan, ha is, M = ( k= e b kk ) (noe ha he series converges). Since b k as k, we have b k e b w k k = M b ke b k k b k 0, as k. (4.0) For all > 0 here exiss k 0 = k 0 () N such ha k k 0 implies ha e > b k e b k /w k. Therefore he sequences {w n } n and {a n } n saisfy he condiion (4.5). Finally we show ha µ = n= w nδ an has he propery (4.). For every A > 0 and 0 < p <, using he inequaliy b k ca k shows ha e A x p dµ(x) = w k e A a k p = M e k b k e Aa kp Thus he proof is complee. k= M k= e Aapk (c A k a ( p)k ) <. k= (4.) Noe ha for any sequences {w n } n and {a n } n saisfying he condiions (4.3) (4.5) he disribuion µ = n= w nδ an has he following propery: e εx dµ(x) = for all ε > 0. (4.) Then we have a naural quesion wheher he large ime unimodaliy of µ N(0,) holds or no if he iniial disribuion µ does no saisfy he condiion (4.). We solve his quesion as follows. Theorem 4.3. Le µ be a probabiliy measure on such ha α := e εx dµ(x) <. (4.3) for some ε > 0. Then µ N(0,) is unimodal for 36log(α) ε. emark 4.4. The proof becomes much easier if we assume ha µ has a compac suppor. Proof of Theorem 4.3: For x > 0 we have µ( y > x) = dµ(y) Le Then we have f (x) = = y >x y >x e εy dµ(y) αe εx. (4.4) e εx f (x) := π d(µ N(0,)) (x) = e (x y) dµ(y). (4.5) dx x For x > 0, we have x ( y x )e (y x) dµ(y) y x e (y x) dµ(y) y x e (y x) dµ(y) x x y e (x y) dµ(y). (4.6) e µ((x, )) α e εx. (4.7)

13 Unimodaliy for classical and free Brownian moions 365 For x, we have x x y x e (x y) 3 dµ(y) 3x Now he funcion g(x) := 4xe 8x x y e (x y) dµ(y) { min 3 e 8,4xe 8x } [ ] µ( ) 3x,x. 3 (4.8) has a local maximum a x = 4, and hence for all x, g(x) e < 3 e 8, (4.9) where e and 3 e Hence we have x x y e (x y) dµ(y) 4x [ ] e 8x µ( ) 3x,x 3 4x [ ] e 8x µ( ) 6, 6 e 8x ( αe ε 36 ), (4.0) where he las inequaliy holds hanks o (4.4) and x. Therefore if x hen f (x) α e εx e 8x ( αe ε 36 ) { = α e εx e 8x α eεx ( αe ε 36 ) }. (4.) If 6 ε hen 8x eεx e εx e ε 8. Hence if 6 ε hen f (x) α e εx { e α e ε 8 ( αe ε 36 ) }. (4.) If 36log(α) ε hen αe ε 36 and we have By aking max{ 6 Similarly, we have e α e ε 8 ( αe ε 36 ) e 9 α 7 < 0. (4.3) ε, 36log(α) ε } = 36log(α) ε, we have f (x) < 0 if x. (4.4) f (x) > 0 if x. (4.5)

14 366 T. Hasebe and Y. Ueda Nex, we will show ha f (x) < 0 for all x wih x <. We hen calculae he following f (x) = = (x y) e (x y) dµ(y) x y > x y (x y) e (x y) dµ(y) (x y) e (x y) dµ(y). (4.6) Since he funcion h(u) := u e u has a local maximum a u = ± 3, we have (x y) e (x y) dµ(y) e 3 µ([x,x+ ] c ). (4.7) x y > For all x wih x <, we have [x,x+ ] c [, ] c, and herefore ] c ) x y > (x y) e (x y) dµ(y) e 3 µ ([, Since he funcion h(u) is decreasing on [0, 3], we have x y (x y) e (x y) dµ(y) x y (x y) e 4 9 ([ µ x = 5 9 e 9 µ ([ x 5 9 e 9 µ ([ 6, e 3 αe ε 4. (4.8) e (x y) dµ(y) 3,x+ ]) 3 3,x+ ]) 3 ]) e 9 ( αe ε 36 ). (4.9) Therefore f (x) e 3 αe ε e 9 ( αe ε 36 ) = { e 3 αe ε e 9 ( αe ε 36 ) }. (4.30) If 36log(α) ε, hen e 3 αe ε e 9 ( αe ε 36 ) e 3 (α) e 9 < 0, (4.3) and herefore f (x) < 0 if x <.

15 Unimodaliy for classical and free Brownian moions 367 To summarize, if 36log(α) ε, hen we have he following properies: x f (x) > 0, x f (x) < 0, (4.3) x < f (x) < 0. ( Hence f (x) has a unique local maximum in, ) when 36log(α) ε, which is a unique global maximum on as well. Therefore µ N(0,) is unimodal for 36log(α) ε. emark 4.5. If µ is unimodal hen µ N(0,) is unimodal for all > 0. This is a consequence of he srong unimodaliy of he normal disribuion N(0, ) (see Secion 3.3), in conras wih he failure of freely srong unimodaliy of he semicircle disribuion (see Lemma 3.9). We close his secion by placing a problem for fuure research. Problem 4.6. Esimae he posiion of he mode of classical Brownian moion wih iniial disribuions saisfying he assumpion (4.3). Our proof shows ha for 36 ε log(α), he mode is locaed in he inerval [ /, /]. How abou free Brownian moion? 5. Large ime unimodaliy for sable processes wih index and index / wih iniial disribuions We invesigae large ime unimodaliy for sable processes wih index (following Cauchy disribuions) and index / (following Lévy disribuions) wih iniial disribuions. 5.. Cauchy process wih iniial disribuion. Le {C } 0 be he symmeric Cauchy disribuion C (dx) := π(x + ) (x)dx, x, C 0 = δ 0, (5.) which forms boh classical and free convoluion semigroups. A Cauchy process wih iniial disribuion µ is a process wih independen incremens ha follows he law µ C a ime 0. I is known ha he Cauchy disribuion saisfies he ideniy µ C = µ C (5.) foranyµand 0, and sohe disribuions µ C can alsobe realizedas he lawsa ime 0 of a process wih free independen incremens wih iniial disribuion µ. The auhors do no know a wrien proof of (5.) in he lieraure, so give a proof below. The Cauchy ransform of he Cauchy disribuion is given by G C (z) = /(z + i) on C + (e.g. by he residue heorem), and hence C (z) = iz. Then µ C (z) = µ (z) iz, and afersome compuaionwe can checkha G µ C (z) = G µ (z+i). The Sieljes inversionformulaimplies ha for > 0he freeconvoluion µ C has he densiy π Im(G µ(x+i)) = π((x y) + dµ(y), (5.3) )

16 368 T. Hasebe and Y. Ueda which is exacly he densiy of µ C. As in he cases of free and classical BMs, aking µ o be he symmeric Bernoulli (δ +δ ) is helpful. By calculus we can show ha µ C is unimodal if and only if 3; see Figures Thus i is again naural o expec ha a Cauchy process becomes unimodal for sufficienly large ime, under some condiion on he iniial disribuion. We sar from he following counerexample Figure 5.3. = 0.7 Figure 5.4. = 0.7 Figure 5.5. = Figure 5.6. = Figure 5.7. = 3 Figure 5.8. = 3 Proposiion 5.. There exiss a probabiliy measure µ on such ha µ C is no unimodal for any > 0, and x p dµ(x) <, 0 < p < 3. (5.4) Proof: Le {w n } n be a sequence of posiive numbers such ha n= w n = and {a n } n be a sequence of real numbers. Consider he probabiliy measure µ = w n δ an. (5.5) Suppose ha he sequence b k = n= inf a k a n, k Z + (5.6) n Z +\{k} saisfies he condiion lim w kb 3 k =. (5.7) k When {a n } is increasing, his condiion means ha he disance beween a n and a n+ grows sufficienly fas. Le f (x) := π d(µ C ) w n (x) = dx (x a n ) +. (5.8) Then we obain f (x) = n= n= w n (x a n ) [(x a n ) + ], (5.9)

17 Unimodaliy for classical and free Brownian moions 369 and so for sufficienly large k such ha b k > 0 and for each > 0 f (a k ) = w k (+ ) + n,n k w k (+ ) n,n k w k (+ ) w k (+ ) b 3 k w n b 3 k ( = w k n,n k w n (a k a n ) [(a k a n ) + ] w n a k a n 3 (+ ) w k b 3 k ). (5.0) The condiion (5.7) shows ha f (a k ) is posiive for sufficienly large k Z +. This shows ha µ C is no unimodal for any > 0. If we ake he paricular sequences a n = a n and w n = cn r a 3n, where a,r > 0 and c > 0 is a normalizing consan, hen he sequence b n saisfies b n Ca n for some consan C > 0 independen of n. Then he condiions (5.7) and (5.4) hold rue. In he above consrucion, for any posiive weighs {w n } n and any sequence {a n } n ha saisfies (5.7), he hird momen of µ is always infinie, x 3 dµ(x) =, (5.) due o he inequaliy a k b k a and he condiion (5.7). The nex quesion is hen wheher here exiss a probabiliy measure µ wih a finie hird momen such ha µ C is no unimodal for any > 0, or a leas for sufficienly large > 0. The complee answer is given below. Theorem 5.. Le µ be a probabiliy measure on which has a finie absolue hird momen β := x 3 dµ(x) <. Then µ C is unimodal for 0β 3. Proof: The Markov inequaliy implies he ail esimae I suffices o prove ha he funcion y>x f (x) := π µ([ x,x] c ) β x3, x > 0. (5.) d(µ C ) (x) = dx (x y) dµ(y) (5.3) + has a unique local maximum for large > 0. Suppose firs ha x > 0. The derivaive f splis ino he posiive and negaive pars f (x) (y x) = [(x y) + ] dµ(y) (x y) [(x y) + dµ(y). (5.4) ] y x

18 370 T. Hasebe and Y. Ueda By calculus he funcion u u (u + ) akes a global maximum a he unique poin u = / 3. Using he ail esimae (5.) yields he esimae of he posiive par y>x y x (y x) [(x y) + ] dµ(y) y>x 3 ( 3 + ) dµ(y) β 3 x 3. (5.5) On he oher hand he negaive par can be esimaed as (x y) [(x y) + ] dµ(y) (x y) [(x y) + dµ(y). ] (5.6) x<y<x/ Elemenary calculus shows ha for x < y < x/, { (x y) [(x y) + ] min and if we furher resric o he case x /4, hen { } 4x x min (4x + ), (x /4+ ) { min 4x x (4x + ), (x /4+ ) 4x x (4x +6x ), (x /4+6x ) } 0 3 x 3. }, (5.7) Thus we obain ( (x y) y x [(x y) + dµ(y) µ(( x/,x/)) ] x3 x 3 β ) (x/) 3 ( ) 0 3 x 3 83 β 3, x /4. (5.8) (5.9) Comparing (5.5) and (5.9), aking 0β /3 guaranees ha he posiive par is smaller han he negaive par, and hence Similarly, if 0β /3 hen f (x) < 0, x 4. (5.0) f (x) > 0, x 4. (5.) In order o show ha f has a unique zero, i suffices o show ha f (x) < 0 for x /4. Now we have y x >/ 3 f (x) = y x >/ 3 y x / 3 [3(y x) ] [(x y) + ] 3 dµ(y) [ 3(y x) ] [(x y) + ] 3 dµ(y). (5.) The funcion u (3u )/(u + ) 3 aains a global maximum a u = ± and a global minimum a u = 0. Therefore, he posiive par can be esimaed as follows: [3(y x) ] [(x y) + ] 3 dµ(y) (3 ) ( + ) 3 dµ(y) y x >/ 3 = 4µ ([ x 3,x+ 3 ] c ). (5.3)

19 Unimodaliy for classical and free Brownian moions 37 For all x such ha x /4, we have he inclusion [ x,x+ ] c [ ], c, (5.4) and hence we obain y x >/ 3 y x / 3 [3(y x) ] [(x y) + ] 3 dµ(y) 4µ ([ 5, ] c ) 53 β 5 7. (5.5) On he oher hand, he negaive par has he esimae [ 3(y x) ] [(x y) + ] 3 dµ(y) [ 3(y x) ] [(x y) + dµ(y). (5.6) ] 3 y x / By calculus, he funcion u ( 3u )/(u + ) 3 is decreasing on [0,], and so [ 3(y x) ] y x / [(x y) + ] 3 dµ(y) ( 3 4 ) ([ 3 dµ(y) = y x / ( 4 + ) 3 5 4µ x,x+ ]) (5.7) 3 ([ 5 4µ 4, ]) ( ) β 3 for all x /4. The posiive par (5.5) is smaller han he negaive par (5.7) if we ake in such a way ha 0β /3. Thus f (x) < 0 for all x /4 and 0β / Posiive sable process wih index / wih iniial disribuion. A posiive sable process wih index / has he disribuion L (dx) := e x π x (0, )(x)dx, x, (5.8) 3/ a ime 0 which is called he Lévy disribuion. We resric o he case where he iniial disribuion is compacly suppored. Theorem 5.3. If µ is a compacly suppored on wih diameer D µ hen µ L is unimodal for all (90/4) /4 D / µ. Proof: By performing a ranslaion we may assume ha µ is suppored on [0,γ], where γ = D µ. We se he following funcion: g,y (x) := e (x y) (x y) 3/ (0, )(x y), x,y. (5.9) Noe ha his funcion is C wih respec o x. Consider he following funcion π f (x) := d(µ L γ ) (x) = g,y (x)dµ(y), x, (5.30) dx which is suppored on (0, ) and has he derivaive d dx f (x) = γ 0 0 3(x y) e (x y) (0, ) (x y)dµ(y). (5.3) (x y) 7/ If 0 < x < /3 hen 3(x y) > 3 /3 = 0 for all 0 y γ, and herefore f (x) > 0. Moreover, if /3+γ < x hen we have ha 3(x y) <

20 37 T. Hasebe and Y. Ueda 3( /3 + γ) + 3γ = 0 for all 0 y γ, and herefore f (x) < 0. For /3 < x < /3+γ, he second derivaive of f is given by f (x) = γ 0 5(x y) 0 (x y)+ 4 4(x y) / Noe ha /3 γ < x y < /3+γ. Since for X if 3 0 e (x y) (0, ) (x y)dµ(y). (5.3) 5X 0 X + 4 < 0 iff < X < , (5.33) γ hen f (x) < 0. To summarize, we have obained ha if 3 0 γ hen f (x) > 0, x < /3, f (x) < 0, x > /3+γ, f (x) < 0, /3 < x < /3+γ. Hence f has a unique local maximum in [ /3, /3+γ], which is a unique global maximum on as well. Therefore µ L is unimodal for all 3 0 γ. We give a counerexample for large ime unimodaliy for posiive sable processes of index / when he iniial disribuion is no compacly suppored. Proposiion 5.4. There exiss a probabiliy measure µ on such ha µ L is no unimodal for any > 0, and x p dµ(x) <, 0 < p < 5. (5.34) Proof: Le {w n } n be a sequence of posiive numbers such ha n= w n = and {a n } n be a sequence of real numbers such ha he sequence b k = inf n N\{k} a k a n, k N (5.35) saisfies lim w kb 5/ k k =. (5.36) Consider he probabiliy measure µ = w n δ an. (5.37) Le Then we obain f (x) := where h(x) = 3x e x 7/ π n= d(µ L ) (x) = dx n,a n<x f (x) = f (a k + /6) = w k e 3 n,a n<x x, and for each k N and each > 0 n:n k a n<a k + /6 (x an) e w n (x a n ) 3/. (5.38) w n h(x a n ), (5.39) w n h(a k a n + /6). (5.40)

21 Unimodaliy for classical and free Brownian moions 373 Since b k as k, here exiss a posiive ineger k() such ha b k + /6 > for all k k(). For k k() and n k such ha a n < a k + /6, we can show ha a k a n b k ; oherwise, by he definiion of b k i mus hold ha a k a n b k < , which conradics a n < a k + /6. Since he map h is posiive and sricly decreasing on ( , ), for k k() we have f (a k + /6) w k e 3 n:n k a n<a k + /6 w n h(b k + /6) (5.4) w k e 3 h(b k + /6) (5.4) = w k e 3 3b k / (b k + /6) 7/e (b k + /6). (5.43) The condiion (5.36) shows ha f (a k+ /6) is posiive for sufficienly large k N. This shows ha µ L is no unimodal for any > 0. If we ake he paricular sequences a k = a k and w k = cka 5 k where a > and c > 0 is a normalizing consan, hen he sequence b k saisfies b k Ca k for some consan C > 0. Then he condiion (5.36) holds rue and x p dµ(x) = w k a k p = c k k ka (p 5/)k. (5.44) Hence he above inegral is finie if and only if 0 < p < 5/. In he above consrucion, for any posiive weighs {w n } n and any sequence {a n } n ha saisfies (5.36), he 5/-h momen of µ is always infinie, ha is, x 5/ dµ(x) =. (5.45) We conjecure ha if he inegral in (5.45) is finie hen µ L is unimodal in large ime. More generally, considering resuls on Cauchy processes in Secion 5., i is naural o expec he following. Conjecure 5.5. Suppose ha S (resp. T ) is he law a ime 0 of a classical (resp. free) sricly sable process of index α (0,). If µ is a probabiliy measure such ha x +α dµ(x) <, (5.46) hen µ S (resp. µ T ) is unimodal for sufficienly large > 0. Acknowledgemens The auhors express sincere hanks o he referee who gave useful commens o improve he manuscrip. eferences H. Bercovici and D. Voiculescu. Free convoluion of measures wih unbounded suppor. Indiana Univ. Mah. J. 4 (3), (993). M546.

22 374 T. Hasebe and Y. Ueda P. Biane. On he free convoluion wih a semi-circular disribuion. Indiana Univ. Mah. J. 46 (3), (997). M U. Haagerup and S. Thorbjørnsen. On he free gamma disribuions. Indiana Univ. Mah. J. 63 (4), (04). M T. Hasebe and N. Sakuma. Unimodaliy for free Lévy processes. Ann. Ins. Henri Poincaré Probab. Sa. 53 (), (07). M T. Hasebe and S. Thorbjørnsen. Unimodaliy of he freely selfdecomposable probabiliy laws. J. Theore. Probab. 9 (3), (06). M H.-W. Huang. Suppors of measures in a free addiive convoluion semigroup. In. Mah. es. No. IMN (), (05). M H. Maassen. Addiion of freely independen random variables. J. Func. Anal. 06 (), (99). M6586. A. Nica and. Speicher. Lecures on he combinaorics of free probabiliy, volume 335 of London Mahemaical Sociey Lecure Noe Series. Cambridge Universiy Press, Cambridge (006). ISBN ; M K. Sao. Lévy processes and infiniely divisible disribuions, volume 68 of Cambridge Sudies in Advanced Mahemaics. Cambridge Universiy Press, Cambridge (03). ISBN M S. J. Wolfe. On he unimodaliy of infiniely divisible disribuion funcions. Z. Wahrsch. Verw. Gebiee 45 (4), (978). M5778. M. Yamazao. Unimodaliy of infiniely divisible disribuion funcions of class L. Ann. Probab. 6 (4), (978). M04894.

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

4 Sequences of measurable functions

4 Sequences of measurable functions 4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences

More information

NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS

NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS QUANTUM PROBABILITY BANACH CENTER PUBLICATIONS, VOLUME 43 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 998 NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS MAREK

More information

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE Topics MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES 2-6 3. FUNCTION OF A RANDOM VARIABLE 3.2 PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE 3.3 EXPECTATION AND MOMENTS

More information

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation: M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno

More information

Representation of Stochastic Process by Means of Stochastic Integrals

Representation of Stochastic Process by Means of Stochastic Integrals Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of

More information

Convergence of the Neumann series in higher norms

Convergence of the Neumann series in higher norms Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann

More information

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

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]

More information

Heat kernel and Harnack inequality on Riemannian manifolds

Heat kernel and Harnack inequality on Riemannian manifolds Hea kernel and Harnack inequaliy on Riemannian manifolds Alexander Grigor yan UHK 11/02/2014 onens 1 Laplace operaor and hea kernel 1 2 Uniform Faber-Krahn inequaliy 3 3 Gaussian upper bounds 4 4 ean-value

More information

Optimality Conditions for Unconstrained Problems

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

More information

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

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

More information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick

More information

The Strong Law of Large Numbers

The Strong Law of Large Numbers Lecure 9 The Srong Law of Large Numbers Reading: Grimme-Sirzaker 7.2; David Williams Probabiliy wih Maringales 7.2 Furher reading: Grimme-Sirzaker 7.1, 7.3-7.5 Wih he Convergence Theorem (Theorem 54) and

More information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL: Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS

More information

arxiv: v1 [math.fa] 9 Dec 2018

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

More information

A problem related to Bárány Grünbaum conjecture

A problem related to Bárány Grünbaum conjecture Filoma 27:1 (2013), 109 113 DOI 10.2298/FIL1301109B Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma A problem relaed o Bárány Grünbaum

More information

arxiv: v1 [math.ca] 15 Nov 2016

arxiv: v1 [math.ca] 15 Nov 2016 arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

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

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details! MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his

More information

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

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

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

More information

On Two Integrability Methods of Improper Integrals

On Two Integrability Methods of Improper Integrals Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169

More information

arxiv: v1 [math.pr] 23 Jan 2019

arxiv: v1 [math.pr] 23 Jan 2019 Consrucion of Liouville Brownian moion via Dirichle form heory Jiyong Shin arxiv:90.07753v [mah.pr] 23 Jan 209 Absrac. The Liouville Brownian moion which was inroduced in [3] is a naural diffusion process

More information

arxiv: v1 [math.pr] 19 Feb 2011

arxiv: v1 [math.pr] 19 Feb 2011 A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of

More information

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his

More information

STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES

STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES Novi Sad J. Mah. Vol. 46, No. 1, 2016, 15-25 STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES N. Eghbali 1 Absrac. We deermine some sabiliy resuls concerning

More information

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

2. Nonlinear Conservation Law Equations

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

More information

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

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

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

Supplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence

Supplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence Supplemen for Sochasic Convex Opimizaion: Faser Local Growh Implies Faser Global Convergence Yi Xu Qihang Lin ianbao Yang Proof of heorem heorem Suppose Assumpion holds and F (w) obeys he LGC (6) Given

More information

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial

More information

THE WAVE EQUATION. part hand-in for week 9 b. Any dilation v(x, t) = u(λx, λt) of u(x, t) is also a solution (where λ is constant).

THE WAVE EQUATION. part hand-in for week 9 b. Any dilation v(x, t) = u(λx, λt) of u(x, t) is also a solution (where λ is constant). THE WAVE EQUATION 43. (S) Le u(x, ) be a soluion of he wave equaion u u xx = 0. Show ha Q43(a) (c) is a. Any ranslaion v(x, ) = u(x + x 0, + 0 ) of u(x, ) is also a soluion (where x 0, 0 are consans).

More information

Notes for Lecture 17-18

Notes for Lecture 17-18 U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up

More information

Average Number of Lattice Points in a Disk

Average Number of Lattice Points in a Disk Average Number of Laice Poins in a Disk Sujay Jayakar Rober S. Sricharz Absrac The difference beween he number of laice poins in a disk of radius /π and he area of he disk /4π is equal o he error in he

More information

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning

More information

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence

More information

f(s)dw Solution 1. Approximate f by piece-wise constant left-continuous non-random functions f n such that (f(s) f n (s)) 2 ds 0.

f(s)dw Solution 1. Approximate f by piece-wise constant left-continuous non-random functions f n such that (f(s) f n (s)) 2 ds 0. Advanced Financial Models Example shee 3 - Michaelmas 217 Michael Tehranchi Problem 1. Le f : [, R be a coninuous (non-random funcion and W a Brownian moion, and le σ 2 = f(s 2 ds and assume σ 2

More information

SOLUTIONS TO ECE 3084

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

More information

Introduction to Probability and Statistics Slides 4 Chapter 4

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

More information

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018 MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren

More information

Solutions to Assignment 1

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

More information

Question 1: Question 2: Topology Exercise Sheet 3

Question 1: Question 2: Topology Exercise Sheet 3 Topology Exercise Shee 3 Prof. Dr. Alessandro Siso Due o 14 March Quesions 1 and 6 are more concepual and should have prioriy. Quesions 4 and 5 admi a relaively shor soluion. Quesion 7 is harder, and you

More information

5. Stochastic processes (1)

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

More information

Sobolev-type Inequality for Spaces L p(x) (R N )

Sobolev-type Inequality for Spaces L p(x) (R N ) In. J. Conemp. Mah. Sciences, Vol. 2, 27, no. 9, 423-429 Sobolev-ype Inequaliy for Spaces L p(x ( R. Mashiyev and B. Çekiç Universiy of Dicle, Faculy of Sciences and Ars Deparmen of Mahemaics, 228-Diyarbakir,

More information

Undetermined coefficients for local fractional differential equations

Undetermined coefficients for local fractional differential equations Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani

More information

SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM

SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM FRANCISCO JAVIER GARCÍA-PACHECO, DANIELE PUGLISI, AND GUSTI VAN ZYL Absrac We give a new proof of he fac ha equivalen norms on subspaces can be exended

More information

SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990),

SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990), SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F Trench SIAM J Marix Anal Appl 11 (1990), 601-611 Absrac Le T n = ( i j ) n i,j=1 (n 3) be a real symmeric

More information

Research Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations

Research Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations Hindawi Publishing Corporaion Boundary Value Problems Volume 11, Aricle ID 19156, 11 pages doi:1.1155/11/19156 Research Aricle Exisence and Uniqueness of Periodic Soluion for Nonlinear Second-Order Ordinary

More information

A proof of Ito's formula using a di Title formula. Author(s) Fujita, Takahiko; Kawanishi, Yasuhi. Studia scientiarum mathematicarum H Citation

A proof of Ito's formula using a di Title formula. Author(s) Fujita, Takahiko; Kawanishi, Yasuhi. Studia scientiarum mathematicarum H Citation A proof of Io's formula using a di Tile formula Auhor(s) Fujia, Takahiko; Kawanishi, Yasuhi Sudia scieniarum mahemaicarum H Ciaion 15-134 Issue 8-3 Dae Type Journal Aricle Tex Version auhor URL hp://hdl.handle.ne/186/15878

More information

6. Stochastic calculus with jump processes

6. Stochastic calculus with jump processes A) Trading sraegies (1/3) Marke wih d asses S = (S 1,, S d ) A rading sraegy can be modelled wih a vecor φ describing he quaniies invesed in each asse a each insan : φ = (φ 1,, φ d ) The value a of a porfolio

More information

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria

More information

The Arcsine Distribution

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

More information

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

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

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Asymptotic instability of nonlinear differential equations

Asymptotic instability of nonlinear differential equations Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy

More information

A remark on the H -calculus

A remark on the H -calculus A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has

More information

Vehicle Arrival Models : Headway

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

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

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

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Hedgehogs are not colour blind

Hedgehogs are not colour blind Hedgehogs are no colour blind David Conlon Jacob Fox Vojěch Rödl Absrac We exhibi a family of 3-uniform hypergraphs wih he propery ha heir 2-colour Ramsey numbers grow polynomially in he number of verices,

More information

On a Fractional Stochastic Landau-Ginzburg Equation

On a Fractional Stochastic Landau-Ginzburg Equation Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn

More information

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien

More information

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,

More information

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i)

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i) A NOTE ON WRONSKIANS AND THE ABC THEOREM IN FUNCTION FIELDS OF RIME CHARACTERISTIC Julie Tzu-Yueh Wang Insiue of Mahemaics Academia Sinica Nankang, Taipei 11529 Taiwan, R.O.C. May 14, 1998 Absrac. We provide

More information

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

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

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a

More information

Lecture 10: The Poincaré Inequality in Euclidean space

Lecture 10: The Poincaré Inequality in Euclidean space Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?

More information

Some Ramsey results for the n-cube

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

More information

Approximation Algorithms for Unique Games via Orthogonal Separators

Approximation Algorithms for Unique Games via Orthogonal Separators Approximaion Algorihms for Unique Games via Orhogonal Separaors Lecure noes by Konsanin Makarychev. Lecure noes are based on he papers [CMM06a, CMM06b, LM4]. Unique Games In hese lecure noes, we define

More information

1 Solutions to selected problems

1 Solutions to selected problems 1 Soluions o seleced problems 1. Le A B R n. Show ha in A in B bu in general bd A bd B. Soluion. Le x in A. Then here is ɛ > 0 such ha B ɛ (x) A B. This shows x in B. If A = [0, 1] and B = [0, 2], hen

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

On Carlsson type orthogonality and characterization of inner product spaces

On Carlsson type orthogonality and characterization of inner product spaces Filoma 26:4 (212), 859 87 DOI 1.2298/FIL124859K Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Carlsson ype orhogonaliy and characerizaion

More information

Stability and Bifurcation in a Neural Network Model with Two Delays

Stability and Bifurcation in a Neural Network Model with Two Delays Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy

More information

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

t 2 B F x,t n dsdt t u x,t dxdt

t 2 B F x,t n dsdt t u x,t dxdt Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.

More information

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

More information

On some Properties of Conjugate Fourier-Stieltjes Series

On some Properties of Conjugate Fourier-Stieltjes Series Bullein of TICMI ol. 8, No., 24, 22 29 On some Properies of Conjugae Fourier-Sieljes Series Shalva Zviadadze I. Javakhishvili Tbilisi Sae Universiy, 3 Universiy S., 86, Tbilisi, Georgia (Received January

More information

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS MICHAEL DORFF AND J. SZYNAL Absrac. Differen mehods have been used in sudying he univalence of he inegral ) α ) f) ) J α, f)z) = f ) d, α,

More information

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004 ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform

More information

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

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

More information

arxiv: v1 [math.gm] 4 Nov 2018

arxiv: v1 [math.gm] 4 Nov 2018 Unpredicable Soluions of Linear Differenial Equaions Mara Akhme 1,, Mehme Onur Fen 2, Madina Tleubergenova 3,4, Akylbek Zhamanshin 3,4 1 Deparmen of Mahemaics, Middle Eas Technical Universiy, 06800, Ankara,

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS

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

More information

4.6 One Dimensional Kinematics and Integration

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

More information

On Oscillation of a Generalized Logistic Equation with Several Delays

On Oscillation of a Generalized Logistic Equation with Several Delays Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid

More information

556: MATHEMATICAL STATISTICS I

556: MATHEMATICAL STATISTICS I 556: MATHEMATICAL STATISTICS I INEQUALITIES 5.1 Concenraion and Tail Probabiliy Inequaliies Lemma (CHEBYCHEV S LEMMA) c > 0, If X is a random variable, hen for non-negaive funcion h, and P X [h(x) c] E

More information

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k Challenge Problems DIS 03 and 0 March 6, 05 Choose one of he following problems, and work on i in your group. Your goal is o convince me ha your answer is correc. Even if your answer isn compleely correc,

More information

A Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball

A Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball A Noe on Superlinear Ambrosei-Prodi Type Problem in a Ball by P. N. Srikanh 1, Sanjiban Sanra 2 Absrac Using a careful analysis of he Morse Indices of he soluions obained by using he Mounain Pass Theorem

More information

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS XUAN THINH DUONG, JI LI, AND ADAM SIKORA Absrac Le M be a manifold wih ends consruced in [2] and be he Laplace-Belrami operaor on M

More information