QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES. Citation Journal of Evolution Equations. 4(3.

Size: px
Start display at page:

Download "QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES. Citation Journal of Evolution Equations. 4(3."

Transcription

1 Title QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES Author() Favini, Angelo; Yagi, Atuhi Citation Journal of Evolution Equation. 4(3 Iue 24-9 Date Text Verion publiher URL DOI 1.17/ Right Oaka Univerity

2 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) Abtract. The quailinear degenerate evolution equation of parabolic type d(mv) + L(Mv)v = F (Mv), < t T conidered in a Banach pace X i dt written, putting Mv = u, in the form du + A(u)u F (u), < t T, where dt A(u) = L(u)M 1 are multivalued linear operator in X for u K, K being a bounded ball u Z < R in another Banach pace Z continuouly embedded in X. Exitence and uniquene of the local olution for the related Cauchy problem are given. The reult are applied to quailinear elliptic-parabolic equation and ytem. 1. Introduction We are concerned with the Cauchy problem of a degenerate abtract evolution equation of parabolic type dmv + L(Mv)v = F (Mv), < t T, (D.E) dt Mv() = u in a Banach pace X. Here, L(u) are cloed linear operator in X with ome contant domain D(L(u)) D L for u K = {u Z; u Z R}, R >, where Z i another Banach pace uch that Z X with continuou embedding. M i a cloed linear operator in X with the domain D(M) D L uch that M(D L ) Z. F ( ) i a nonlinear operator from K into X. u K i an initial value. v = v(t) i an unknown function. Cauchy problem of many concrete equation are formulated a thoe of abtract equation of the form (D.E), uch a elliptic-parabolic equation, elliptic-parabolic ytem, nonlinear equation of Sobolev type [14], emiconductor equation [15], and o on. Like in our previou paper [3] (cf. alo [11]) for linear problem, we rewrite the degenerate equation in (D.E) in the form du dt + A(u)u F (u) by changing unknown function from v = v(t) to u = M v(t) and introducing multivalued linear operator A(u) = L(u)M 1, u K, which act in X with a contant domain D(A(u)) = M(D L ). In thi way we have the Cauchy problem for a quailinear (*) Partially upported M. I. U. R. (Fund ex 6 % ) and by Univerity of Bologna Fund for elected reearch topic, the author i a menber of G. N. A. M. P. A. of INdAM. (**) Partially upported by Grant-in-Aid for Scientific Reearch (No ) by Japan Society for the Promotion of Science. 1

3 2 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) multivalued equation but of nondegenerate type du + A(u)u F (u), < t T, (E) dt u() = u. Sobolevkii [8] (cf. alo [12, Part 2] and [17]) ha firt tudied uch an abtract problem in the cae where the coefficient operator A(u) are all ingle valued and are the generator of analytic emigroup, that i A(u) atify (1.1) (λ A(u)) 1 L(X) C ( λ + 1) 1 κ, λ Σ, u K with the optimal exponent κ = and with ome ectorial domain Σ = {λ C; arg λ < φ}, < φ < π 2. He in fact contructed, under uitable aumption on A(u), F (u) and u, a unique X-valued C 1 local olution. We remark however that even if L(u) are the generator of analytic emigroup, A(u) = L(u)M 1 do not necearily atify (1.1) with κ =. The firt half of thi paper i then devoted to tudying the problem (E) with multivalued operator atifying (1.1). We hall prove exitence and uniquene of X-valued C 1 local olution by generalizing Sobolevkii reult on the bai of the previou work on multivalued linear evolution equation in [3]. In the econd half we hall apply our abtract reult to elliptic-parabolic equation and elliptic-parabolic ytem. There i an enormou literature on the ubject. We refer to the recent monograph by Showalter [16], ee alo [1]. In fact, mot available reult until now develop the baic approach by Brezi [2], where one ee the left hand ide of (D.E) a the um of two operator, the former being linear, the latter being (poibly nonlinear) monotone, and further aumption allow to apply the theory by Bardo and Brezi [1]. On the other hand, uch an approach force to tudy the equation in ome particular functional etting a L p (, T ; W ), where W i either the dual pace of a reflexive Banach pace or a weighted pace (depending on the operator M), 1 p + 1 p = 1, p 2. The mot recent main reult on quailinear degenerate evolution equation in [16, pp ] (ee in particular Corollary 6.2 and Corollary 6.3) are concerned with the equation d (S) (Bu) + A(t, u) = f(t), a. e. t (, T ). dt It i uppoed that B i a continuou, linear, ymmetric and monotone operator from the reflexive eparable Banach pace V to it dual V and A : [, T ] V V atifie ome appropriate continuity, monotonicity and coercivity aumption ([16, p. 129]). The application of thee reult to quailinear elliptic-parabolic equation i detailed in [16, Example 6.3]. For other reult, we quote Kuttler [5] and [6], too. Here it will be hown that our approach allow to conider problem of thi type having a nonlinearity (in u) in the right hand ide of (S), too, with a bit more retrictive aumption on the data, due to the greater regularity in time of our olution.

4 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 3 The plan of the paper i a follow. In Section 2 we recall baic reult on multivalued linear operator depending on time from [3] and [11], and prove new etimate for the evolution operator to be ued in the ubequent ection. Section 3 i devoted to the problem (E). Some condition given there are inpired by [8] and [9] too, and they guarantee the exitence and uniquene of the olution to (E). In ection 4 we apply uch reult to olve (D.E). Of coure, if L(u) L i independent of u, we can olve a emilinear degenerate differential equation. Section 5 and 6 contain example from partial differential equation of ellipticparabolic type to which our abtract theory applie. It i to be oberved that unlike all previou literature, where the ambient pace i a Sobolev pace of negative exponent, here we can take X = L 2 (Ω) (or, a hown in [4], L p (Ω), 1 < p < ), when Ω i a bounded region in R n with a mooth boundary. Notation. Throughout the paper, X denote a complex Banach pace whoe norm i denoted by X. If Y i another Banach pace, L(X, Y ) i the pace of all bounded linear operator from X to Y and L(X,Y ) denote the uniform operator norm. L(X) i ued for intead of L(X, X). An operator A : X 2 Y having the two propertie: Au + Av A(u + v), u, v X and λau A(λu), λ C, u X i called a multivalued linear operator from D(A) = {u X; Au } to Y. For u D(A), Au X = inf{ f Y ; f Au}. If A : D(A) Y i a multivalued linear operator, a ingle valued operator A : D(A) Y uch that A A in the graph ene i called a ection of A. With an arbitrary ection A, it hold that Au = A + A u, u D(A). If I i a nonempty interval in R and k i a nonnegative integer, C k (I; X) denote the pace of all k-time continuouly differentiable function with value in X defined on I, where C (I; X) = C(I; X). For < µ < 1, C µ (I; X) i the pace of µ-hölder continuou function with value in X defined on I. B(I; X) denote the pace of all bounded function on I with value in X. 2. Multivalued linear equation We conider a family of multivalued linear operator A(t), t T, acting in a Banach pace X which have a domain D(A(t)) D independent of t. In the previou paper [3], we have already contructed the evolution operator U(t, ) under the Aumption (L.A.i,ii) and (L.Ex) below. The purpoe of thi ection i then to review the baic propertie of U(t, ) and verify more refined one which will be required in tudying the multivalued quailinear equation. We make the following aumption. For every t T, the pectral et σ(a(t)) of A(t) i contained in a fixed open ectorial domain Σ, σ(a(t)) Σ = {λ C; arg λ < φ}, where < φ < π 2. And the reolvent atifie the etimate (L.A.i) (λ A(t)) 1 L(X) M, λ Σ, t T, ( λ + 1) 1 κ

5 4 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) with ome exponent κ < 1 and a contant M >. A( ) atifie a Hölder condition of the form (L.A.ii) A(t){A(t) 1 A() 1 }f X N t µ f X, f X,, t T with ome exponent < µ 1 and a contant N >. The exponent atify the relation (L.Ex) 3κ < µ 1. Before introducing the evolution operator, let u firt notice that (L.A.i) and (L.A.ii) imply the etimate (2.1) A(t) (λ A(t)) 1 {A(t) 1 A() 1 }f X Here, MN t µ ( λ + 1) 1 κ f X, λ Σ, f X. A(t) (λ A(t)) 1 = λ(λ A(t)) 1 1 A(t)(λ A(t)) 1 denote the linear ection of A(t)(λ A(t)) 1 introduced in [3, Theorem 2.7]. It i known that A(t) (λ A(t)) 1 = (λ A(t)) 1 A(t) on D, where A(t) in the right hand ide denote an arbitrary ection of A(t) not necearily linear. In fact, (2.1) i verified a follow. For f X, A(t) (λ A(t)) 1 {A(t) 1 A() 1 }f = (λ A(t)) 1 A(t) {A(t) 1 A() 1 }f. In addition, ince (λ A(t)) 1 A(t) {A(t) 1 A() 1 }f = (λ A(t)) 1 g with any g A(t){A(t) 1 A() 1 }f, it follow that (2.2) (λ A(t)) 1 A(t) {A(t) 1 A() 1 }f X (λ A(t)) 1 L(X) A(t){A(t) 1 A() 1 }f X, f X. Therefore, (L.A.i) and (L.A.ii) imply (2.1). In thi theory we hall make an eential ue of the Yoida approximation A n (t) = A(t) J n (t) = n{1 J n (t)}, n = 1, 2, 3,..., J n (t) = (1 + n 1 A(t)) 1 of A(t). A n (t) are ingle valued bounded linear operator on X with A n (t) L(X) Cn 1+κ. Since A n (t) 1 = A(t) 1 + n 1, we have A n (t){a n (t) 1 A n () 1 }f = J n (t)a(t) {A(t) 1 A() 1 }f. Therefore, by (2.2), A n (t){a n (t) 1 A n () 1 }f X N J n (t) L(X) t µ f X, f X. Thi how that, a J n (t) L(X) Cn κ, the Hölder condition (L.A.ii) may not imply that of the Yoida approximation in any uniform ene. Such a difficulty i

6 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 5 however overcome by the fact that (2.1) implie the ame one for A n (t). In fact, ince A n (t)(λ A n (t)) 1 {A n (t) 1 A n () 1 }f (2.1) yield that = n n λ ( n n λ A(t) (2.3) A n (t)(λ A n (t)) 1 {A n (t) 1 A n () 1 } L(X) ) 1 A(t) {A(t) 1 A() 1 }f, C t µ, λ Σ, ( λ + 1) 1 κ ee alo [3, (4.8)]. We hall alo ue the fractional power of A(t). For θ > κ, the fractional power A(t) θ i defined by the Dunford integral A(t) θ = 1 2πi Γ λ θ (λ A(t)) 1 dλ in L(X), where Γ i an integral contour lying in C σ(a(t)). A(t) θ, θ > κ, i then a multivalued linear operator in X. In particular, A(t) 1 = A(t). A n, A n (t) θ converge to A(t) θ in L(X). (L.A.i) yield that for each t T, A(t) generate an infinitely differential emigroup e τa(t), τ, on X, ee [3, Section 3]. For θ, a bounded linear operator on X given by the integral {A(t) θ } e τa(t) = 1 2πi Γ λ θ e τλ (λ A(t)) 1 dλ, τ >, i introduced. Obviouly, thi operator i alo obtained a a limit of A n (t) θ e τa n(t) alo. The following etimate (2.4) A n (t) θ e τa n(t) J n (t) k L(X) C θ τ θ κ, τ >, k =, 1, {A(t) θ } e τa(t) L(X) C θ τ θ κ, τ >, are verified. If θ > κ, {A(t) θ } e τa(t) i really a linear ection of the multivalued operator A(t) θ e τa(t). For θ > κ, τ (2.5) {e τa(t) 1}A(t) θ L(X) = A(t) e σa(t) dσa(t) θ L(X) τ = {A(t) 1 θ } e σa(t) dσ C θ τ θ κ, τ >. L(X) According to [3, Theorem 4.1] (cf. alo [11, Section 4.1]), under (L.A.i), (2.1), and (L.Ex), there exit an evolution operator U(t, ), t T, for A(t). U(t, ) i in fact obtained a a limit of U n (t, ), where U n (t, ) i an evolution operator for A n (t). Moreover, U n (t, )J n () ha the ame limit a U n (t, ), that i,

7 6 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) U n (t, )J n () alo converge to U(t, ). The etimate U n (t, )J n () k L(X) C(t ) κ, < t T, k =, 1, U(t, ) L(X) C(t ) κ, < t T hold. The convergence of A n (t)u n (t, ) i alo etablihed, it limit being denoted by A(t) U(t, ). A(t) U(t, ) i a linear ection of A(t)U(t, ). The etimate A n (t)u n (t, ) L(X) C(t ) 1 κ, < t T, A(t) U(t, ) L(X) C(t ) 1 κ, < t T hold. Similarly, for < θ < 1, a bounded linear operator {A(t) θ } U(t, ) i defined a a limit of A n (t) θ U n (t, ). The etimate (2.6) A n (t) θ U n (t, ) L(X) C(t ) θ κ, < t T, θ 1, {A(t) θ } U(t, ) L(X) C(t ) θ κ, < t T, θ 1 are verified by the moment inequality of the fractional power. In addition, it i verified that (2.7) A n (t) θ U n (t, )J n () L(X) A n (t) θ U n (t, t+ 2 ) L(X) U n ( t+ 2, )J n() L(X) C(t ) θ 2κ, < t T, < θ 1. To obtain (2.8) below, we notice from [3, (4.1)] that U n (t, )A n () θ = A n () θ e (t )A n() + U n (t, τ)a n (τ){a n (τ) 1 A n () 1 }A n () θ+1 e (τ )A n() dτ. By the ame argument a for (2.2), we oberve that U n (t, τ)a n (τ){a n (τ) 1 A n () 1 }f X Hence, for θ < µ κ, = U n (t, τ)j n (τ)a(τ) {A(τ) 1 A() 1 }f X U n (t, τ)j n (τ) L(X) A(τ){A(τ) 1 A() 1 }f X, f X. (2.8) U n (t, )A n () θ L(X) C(t ) θ κ + C (t τ) κ (τ ) θ 1 κ+µ dτ C θ (t ) θ κ, < t T. We now prove ome new etimate of U n (t, ) and U(t, ). Propoition 2.1. For κ < ϕ 1, (2.9) A n (t)u n (t, )A n () ϕ L(X) C ϕ (t ) ϕ 1 κ, < t T, A(t) U(t, )A() ϕ L(X) C ϕ (t ) ϕ 1 κ, < t T.

8 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 7 Proof. From U n (t, ) = e (t )An(t) it follow that e (t τ)a n(t) A n (t){a n (t) 1 A n (τ) 1 }A n (τ)u n (τ, )dτ, (2.1) A n (t)u n (t, )A n () ϕ = A n (t)e (t )An(t) A n () ϕ A n (t)e (t τ)a n(t) J n (t)a(t) {A(t) 1 A(τ) 1 }A n (τ)u n (τ, )A n () ϕ dτ with any ection A(t) A(t). We here how the following lemma. Lemma 2.1. For θ 1 and κ < ϕ 1, {A n (t) θ e τan(t) A n () θ e τan() }A n () ϕ L(X) CΓ(θ ϕ + 2κ)τ ϕ θ 2κ t µ, if ϕ < θ + 2κ, C{log(τ 1 + 1) + 1} t µ, if ϕ = θ + 2κ, C(ϕ θ 2κ) 1 t µ, if ϕ > θ + 2κ, where Γ( ) denote the gamma function. Letting n, the ame etimate are verified for the family A(t), too. Proof. We ee that {A n (t) θ e τan(t) A n () θ e τan() }A n () ϕ = 1 λ θ e τλ {(λ A n (t)) 1 (λ A n ()) 1 }A n () ϕ dλ 2πi Γ = 1 λ θ e τλ A n (t)(λ A n (t)) 1 {A n (t) 1 A n ()) 1 } 2πi Γ A n () 1 ϕ (λ A n ()) 1 dλ, where Γ i an integral contour: λ = ρe ±φi, ρ <. Therefore, by (2.3), it follow that {A n (t) θ e τan(t) A n () θ e τan() }A n () ϕ L(X) C ( λ + 1) θ ϕ+2κ 1 e τreλ dλ t µ. If ϕ < θ + 2κ, then ( λ + 1) θ ϕ+2κ 1 e τreλ dλ Γ C Γ ρ θ ϕ+2κ 1 e τρ co φ dρ Cτ ϕ θ 2κ ρ θ ϕ+2κ 1 e ρ dρ.

9 8 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) If ϕ = θ + 2κ, then ( λ + 1) θ ϕ+2κ 1 e τreλ dλ C Γ C τ 1 (ρ + 1) 1 e τρ co φ dρ (ρ + 1) 1 dρ + C ρ 1 e τρ co φ dρ. τ 1 Hence the deired etimate i obtained. Similarly, if ϕ > θ + 2κ, then ( λ + 1) θ ϕ+2κ 1 e τreλ dλ C (ρ + 1) θ ϕ+2κ 1 dρ. Γ Uing thi lemma with θ = 1, we have A n (t)e (t )An(t) A n () ϕ L(X) A n () 1 ϕ e (t )An() L(X) + {A n (t)e (t )A n(t) A n ()e (t )A n() }A n () ϕ L(X) C ϕ [(t ) ϕ κ 1 + log{(t ) 1 + 1}(t ) ϕ 2κ+µ 1 ] C ϕ (t ) ϕ κ 1. Then, from (2.1), the following integral inequality A n (t)u n (t, )A n () ϕ L(X) C ϕ (t ) ϕ 1 κ + C (t τ) µ 1 κ A n (τ)u n (τ, )A n () ϕ L(X) dτ i obtained, which implie the firt etimate (2.9). Obviouly the econd etimate i an immediate conequence of the firt one. Hence the proof of the propoition ha been accomplihed. Propoition 2.2. For θ < 1 κ and θ + κ < ϕ 1, A n (t) θ U n (t, )A n () ϕ L(X) C θ,ϕ, < t T, {A(t) θ } U(t, )A() ϕ L(X) C θ,ϕ, < t T. Proof. From (2.1) we can write that A n (t) θ U n (t, )A n () ϕ = A n (t) θ e (t )An(t) A n () ϕ A n (t) θ e (t τ)an(t) J n (t)a(t) {A(t) 1 A(τ) 1 }A n (τ)u n (τ, )A n () ϕ dτ. In addition, by (L.Ex), (2.5) and Lemma 2.1, we can oberve that A n (t) θ e (t )An(t) A n () ϕ L(X) {A n (t) θ e (t )An(t) A n () θ e (t )An() }A n () ϕ L(X) + {e (t )An() 1}A n () θ ϕ L(X) + A n () θ ϕ L(X) C θ,ϕ.

10 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 9 Therefore, in view of (L.Ex), (2.4) and (2.9), we obtain that A n (t) θ U n (t, )A n () ϕ L(X) C θ,ϕ {1 + } (t τ) µ θ κ (τ ) ϕ κ 1 dτ C θ,ϕ {1 + (t ) ϕ θ 2κ+µ } C θ,ϕ. The econd etimate i an immediate conequence of thi. A to the difference of the evolution operator and the emigroup, we verify the following reult. Propoition 2.3. For θ < 1 2κ and κ < ϕ 1, A n (t) θ {U n (t, ) e (t )A n() }A n () ϕ L(X) For κ < θ < 1 2κ and κ < ϕ 1, A(t) θ {U(t, ) e (t )A() }A() ϕ f X Proof. Uing [3, (4.1)] with ρ = 1, we ee that (2.11) A n (t) θ {U n (t, ) e (t )An() }A n () ϕ = C θ,ϕ (t ) ϕ θ 3κ+µ, < t T. C θ,ϕ (t ) ϕ θ 3κ+µ f X, < t T, f X. A n (t) θ U n (t, τ)j n (τ)a(τ) {A(τ) 1 A() 1 }A n () 1 ϕ e (t )A n() dτ. Then, by (2.7) and (2.9), the norm of the right hand ide i etimated by C θ,ϕ (t τ) θ 2κ (τ ) ϕ 1 κ+µ dτ C θ,ϕ (t ) ϕ θ 3κ+µ. Let κ < θ < 1 2κ. Operating A n (t) θ to (2.11) and letting n in the reulting equality, we obtain that {U(t, ) e (t )A() }A() ϕ = A(t) θ {A(t) θ } U(t, τ)a(τ) {A(τ) 1 A() 1 }A() 1 ϕ e (t )A() dτ. From thi the econd etimate of the propoition i obtained. We finally how a formula which give a olution to the Cauchy problem of a multivalued linear equation du + A(t)u F (t), < t T, (L.E ) dt u() = u

11 1 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) in X. [, T ) i a fixed initial time. F i a given Hölder continuou function on [, T ] uch that (L.F) F C σ ([, T ]; X), σ > κ. u i an initial value in X uch that (L.In) u D(A() γ ), κ < γ 1. A proved by [3, Theorem 4.1], there exit a unique olution to (L.E ) in the function pace: u C([, T ]; X) C 1 1+κ γ du ((, T ]; X), (t ) dt B((, T ]; X). u i in fact given by u(t) = U(t, )u + U(t, τ)f (τ)dτ, t T. Moreover, we can verify the following etimate A (2.12) n(t) U n (t, τ)f (τ)dτ C σ (t ) κ F C σ ([,T ];X), < t T, X A(t) (2.13) U(t, τ)f (τ)dτ C σ (t ) κ F Cσ ([,T ];X), < t T. X Indeed, (2.14) A n (t) + U n (t, τ)f (τ)dτ = A n (t)u n (t, τ){f (τ) F (t)}dτ {A n (t)u n (t, τ) A n (t)e (t τ)an(t) }F (t)dτ + {1 e (t )An(t) }F (t). Uing the integral equation [3, (4.12)], it i een that A n (t)u n (t, ) A n (t)e (t )A n(t) L(X) C(t ) 1 3κ+µ, < t T. Then (2.12) i obtained directly from (2.14). Operating A n (t) 1 to (2.14) and letting n in the reulting equation, we obtain that U(t, τ)f (τ)dτ = A(t) 1[ A(t) U(t, τ){f (τ) F (t)}dτ + ] {A(t) U(t, τ) A(t) e (t τ)a(t) }F (t)dτ + {1 e (t )A(t) }F (t). From thi the etimate (2.13) i verified.

12 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES Quailinear evolution equation Let X be a Banach pace. We conider the Cauchy problem of a multivalued abtract evolution equation du + A(u)u F (u), < t T, (E) dt u() = u in X. Let Z be a econd Banach pace continuouly embedded in X and let K be an open ball of Z uch that K = {u Z; u Z < R}, < R <. For each u K, A(u) i a multivalued linear operator of X with domain D(A(u)) D which i contant in u. F i a nonlinear operator from K to X. u i an initial value in K. We make the following aumption. The pectral et σ(a(u)) i contained in a fixed open ectorial region σ(a(u)) Σ = {λ C; arg λ < φ}, where < φ < π 2, and the reolvent atifie (A.i) (λ A(u)) 1 M L(X) ( λ + 1) 1 κ, λ Σ, u K with ome exponent κ < 1 and a contant M > which are independent of u. A( ) atifie a Lipchitz condition of the form (Aii) A(u){A(u) 1 A(v) 1 }f X N u v Z f X, f X, u, v K with a contant N >. F atifie the Lipchitz condition (F) F (u) F (v) X L u v Z, u, v K with a contant L >. The pace X and Z are a follow (Sp.i) Z X with continuou embedding. There i ome exponent β (κ, 1) uch that, for every u K, D(A(u) β ) Z with the etimate (Sp.ii) ũ Z D A(u) β ũ X, ũ D(A(u) β ), u K, D > being ome contant. u K atifie a compatibility condition of the form (In) u D(A(u ) γ ) with ome exponent γ uch that β < γ 1. Finally, the exponent atify the relation (Ex) κ < β < γ 1 and 5κ + β < γ. A a matter of fact, (Ex) how that κ mut be le than 1 6. Then, the following reult i proved.

13 12 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) Theorem 3.1. Under (A.i,ii), (F), (Sp.i,ii), (In), and (Ex), there exit a unique local olution to (E) in the function pace: { u(t) D(A(u(t)) for < t Tu and u C([, T u ]; Z), (3.1) u C 1 1+κ γ du ((, T u ]; X) and t dt B((, T u ]; X), where T u > i determined by the norm u Z and A(u ) γ u X. Proof. The proof conit of everal tep. C denote a univeral contant which i determined by the exponent and the initial contant. f tand for an arbitrary element in A(u ) γ u. Step 1. For S uch that < S T, we et a Banach pace Z(S) = C([, S]; Z) and a ubet of Z(S) uch that K(S) = {u C µ ([, S]; Z); u() = u, u(t) u() up Z t 1 and up u(t) <t S µ Z D u }. t S Here, µ i ome fixed exponent o that 3κ < µ < γ β 2κ, (Ex) how that uch a µ really exit. The contant D u i fixed o that (3.2) u Z < D u < R. Clearly, K(S) i a nonempty cloed ubet of Z(S). Step 2. For each v K(S), let u conider a linear problem du (3.3) dt + A v(t)u F v (t), < t S, u() = u, where A v (t) = A(v(t)) and F v (t) = F (v(t)) for t S. It i eay to oberve that A v (t) atifie (L.A.i,ii) and (L.Ex) in Section 2 and that F v C µ ([, S]; X) and u atify (L.F) and (L.In), repectively. Therefore, there exit a unique olution to (3.3) in the pace u C([, S]; X) C 1 1+κ γ du ((, S]; X), t dt B((, S]; X), and the olution u i given by u(t) = U v (t, )u + U v (t, )F v ()d, t S, where U v (t, ) denote the evolution operator for the family of multivalued linear operator A v (t) = A(v(t)). We then arrive at defining a correpondence Φ from K(S) to Z(S) by etting Φ(v)(t) = u(t), t S, for each v K(S). Step 3. If S > i ufficiently mall, then Φ map the et K(S) into itelf. Indeed, for u = Φ(v), we write that u(t) = u + {e ta(u) 1}u + {U v (t, ) e tav() }u + U v (t, )F v ()d.

14 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 13 Then, ince u = A(u ) γ f, it i een by (2,5) that {e ta(u ) 1}u Z D A(u ) β {e ta(u ) 1}A(u ) γ f X Similarly, by Propoition 2.3, C {e ta(u ) 1}A(u ) β γ f X Ct γ β κ f X. {U v (t, ) e ta v() }u Z D A v (t) β {U v (t, ) e ta v() } Finally, by (2.6), U v (t, )F v ()d D Z Therefore we obtain by definition (3.2) that A v () γ f X Ct γ β 3κ+µ f X. {A v (t) β } U v (t, )F v ()d Ct 1 β κ. X u(t) Z u Z + C(S γ β 3κ+µ + S 1 β κ )( A(u ) γ u X + 1) D u, provided that S > i ufficiently mall. Note that f denote an arbitrary element of A(u ) γ u. We next fix an exponent ϕ o that and notice that β + 3κ < β + κ + µ < ϕ < γ κ 1 κ, A v (t) ϕ u(t) {A v (t) ϕ } U v (t, )A v () γ f + {A v (t) ϕ } U v (t, )F v ()d = g v (t). By (2.6) and Propoition 2.2, g v (t) i hown to be uniformly bounded with (3.4) g v (t) X C ϕ ( A(u ) γ u X + 1), t S. Uing g v (), we can write that u(t) u() = {U v (t, ) 1}u() + U v (t, τ)f v (τ)dτ = [ {U v (t, ) e (t )Av() }A v () ϕ + {e (t )Av() 1}A v () ϕ] g v () Then, by Propoition 2.3, it i een that + U v (t, τ)f v (τ)dτ, < t S. {A v (t) β } {U v (t, ) e (t )Av() }A v () ϕ L(X) C ϕ (t ) ϕ β 3κ+µ. Similarly, by (2.5) and (2.6), A v () β {e (t )Av() 1}A v () ϕ L(X) C ϕ (t ) ϕ β κ, {A v (t) β } U v (t, τ)f v (τ)dτ C(t ) 1 β κ. X

15 14 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) Therefore, in view of (3.4), we oberve that u(t) u() Z C ϕ (S ϕ β 3κ + S ϕ β κ µ + S 1 β κ µ )( A(u ) γ u ) X + 1)(t ) µ. Therefore, in view of the definition of ϕ, we conclude that u(t) u() Z (t ) µ, provided S > i ufficiently mall. Step 4. If S > i ufficiently mall, then the mapping Φ : K(S) K(S) i a contraction with repect to the norm Z(S). Indeed, for u i = Φ(v i ), v i K(S), i = 1, 2, we have u 1 (t) u 2 (t) = {U v1 (t, ) U v2 (t, )}u + {U v1 (t, ) U v2 (t, )}F v2 ()d + Here we etablih the following lemma. Lemma 3.1. We have A v1 (t) β {U v1 (t, ) U v2 (t, )}u X U v1 (t, ){F v1 () F v2 ()}d. Ct γ β 3κ A(u ) γ u X v 1 v 2 Z(S), t S, and A v 1 (t) β {U v1 (t, ) U v2 (t, )}F v2 ()d X Ct 1 β 3κ F v2 C µ ([,t]; X) v 1 v 2 Z(S), t S. Proof. In order to verify thee fundamental reult, we have to employ the evolution operator U vi,n(t, ) (i = 1, 2) for the familie of the Yoida approximation A vi,n(t) (i = 1, 2) of A vi (t). Indeed we oberve that (3.5) A v1,n(t) β {U v1,n(t, ) U v2,n(t, )}A v2,n() γ = A v1,n(t) β U v1,n(t, ) A v1,n(){a v1,n() 1 A v2,n() 1 }A v2,n()u v2,n(, )A v2,n() γ d. By the ame argument a for (2.2), we can how by (2.7) that A v1,n(t) β U v1,n(t, )J v1,n()a v1 () {A v1 () 1 A v2 () 1 }f X C A v1,n(t) β U v1,n(t, )J v1,n() L(X) A v1 (){A v1 () 1 A v2 () 1 f X C(t ) β 2κ v 1 () v 2 () Z f X, f X. where A v1 () A v1 () i an arbitrary ection. Therefore, (3.6) {A v1 (t) β } U v1 (t, )A v1 () {A v1 () 1 A v2 () 1 }f X C(t ) β 2κ v 1 () v 2 () Z f X, f X.

16 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 15 Operating A v1,n(t) β to (3.5) and letting n in the reulting equality, we obtain that {U v1 (t, ) U v2 (t, )}u = A v1 (t) β {A v1 (t) β } U v1 (t, ) Thi yield that A v1 () {A v1 () 1 A v2 () 1 }A v2 ()U v2 (, )A v2 () γ f d. A v1 (t) β {U v1 (t, ) U v2 (t, )}u X C (t ) β 2κ γ 1 κ d v 1 v 2 Z(S) f X. Since f A(u ) γ u i arbitrary, we obtain the firt etimation. Next, we can write that A v1,n(t) β {U v1,n(t, ) U v2,n(t, )}F v2 ()d = A v1,n(t) β U v1,n(t, τ) A v1,n(τ){a v1,n(τ) 1 A v2,n(τ) 1 }A v2,n(τ)u v2,n(τ, )F v2 ()dτd = A v1,n(t) β U v1,n(t, τ)a v1,n(τ){a v1,n(τ) 1 A v2,n(τ) 1 } A v2,n(τ) τ U v2,n(τ, )F v2 ()ddτ. From (2.12), A τ v2,n(τ) U v 2,n(τ, )F v2 ()d atifie the uniform etimate τ A v 2,n(τ) U v2,n(τ, )F v2 ()d Cτ κ F v2 C µ ([,S]; X), X and converge a n to a continuou function g(τ) on (, S]. Then, we obtain in the ame way a above that {U v1 (t, ) U v2 (t, )}F v2 ()d = A v1 (t) β {A v1 (t) β } U v1 (t, τ)a v1 (τ) {A v1 (τ) 1 A v2 (τ) 1 }g(τ)dτ. Therefore, A v 1 (t) β {U v1 (t, ) U v2 (t, )}F v2 ()d C X Hence we verify the econd etimate of the lemma. (t τ) β 2κ τ κ dτ F v2 Cµ ([,S]; X) v 1 v 2 Z(S). Let u now complete the proof of thi Step. It i eay to ee that A v 1 (t) β U v1 (t, ){F v1 () F v2 ()}d Ct 1 β κ v 1 v 2 Z(S). X

17 16 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) Thi together with the lemma then yield that u 1 (t) u 2 (t) Z CS γ β 3κ ( A(u ) γ u X + 1) v 1 v 2 Z(S), t S. Hence, we have verified that Φ i a contraction, provided S > i ufficiently mall. Step 5. Take a T u = S > in uch a way that the reult of Step 3 and 4 are valid. Then, there exit a unique fixed point u K(S) of Φ. Since u atifie the formula u(t) = U u (t, )u + U u (t, )F u ()d, t S, u i hown to be a olution to (E) which belong to the pace (3.1). Step 6. Finally we verify the uniquene of olution. Let u be the olution contructed above. We conider the Yoida approximation A u,n (t) of the operator A u (t) and the evolution operator U u,n (t, ) correponding to A u,n (t). Let ũ be any other olution to (E) in the pace (3.1). Then, for < t < S ( T u ), U u,n(t, )ũ() = U u,n (t, ){A u,n ()ũ() g()} + U u,n (t, )Fũ(), < < t, where g() Aũ()ũ() with dũ d + g() = F ũ(). Integrating thi identity in (, t) and operating A u,n (t) β to the reulting one yield that A u,n (t) β {ũ(t) u n (t)} = A u,n (t) β U u,n (t, ) A u,n (){Aũ() 1 A u,n () 1 } g()d + A u,n (t) β U u,n (t, ){Fũ() F u ()}d, where u n (t) = U u,n (t, )u + U u,n(t, )F u ()d. We are concerned with the limit a n. By the ame method a in Step 4, it i in fact verified that (3.7) ũ(t) u(t) = A u (t) β[ {A u (t) β } U u (t, )A u () {Aũ() 1 A u () 1 } g()d + Moreover, we oberve the following fact. ] {A u (t) β } U u (t, ){Fũ() F u ()}d lim n n 1 U u,n (t, )A u,n () g()d. Lemma 3.2. lim n n 1 U u,n (t, )A u,n () g()d =.

18 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 17 Proof. For any ρ (, µ κ), we have by (2.8) that U u,n (t, )A u,n () L(X) U u,n (t, )A u,n () ρ L(X) A u,n () 1 ρ L(X) C ρ (t ) ρ κ A u,n () 1 ρ L(X) C ρn (1+κ)(1 ρ) (t ) ρ κ. In addition, from (3.1), g atifie that g() X Cũ γ κ 1. Therefore, U u,n (t, )A u,n () g()d C ρ Cũn (1+κ)(1 ρ) X (t ) ρ κ γ κ 1 d C ρ Cũn (1+κ)(1 ρ) t γ ρ 2κ. κ It then uffice to take a ρ o that 1+κ < ρ < µ κ. Since κ 1+κ + κ 3κ (< µ) for κ < 1 6, it i clearly poible to take uch a ρ. In view of (3.6), we verify from (3.7) that A u (t) β {ũ(t) u(t)} X CũS γ β 3κ ũ u Z(S), t S. Thi in turn how that ũ(t) = u(t) for all t [, S] if S > i ufficiently mall. A a matter of fact, we have hown by thi argument that the et {S (, T U ]; ũ(t) = u(t) for all t [, S]} i nonempty and open in (, T U ]. On the other hand, it i clear that the et i cloed. Therefore, ũ(t) = u(t) for all t [, T U ]. Remark 3.1. A hown in the proof, T u i determined by the norm A(u ) γ u X = inf{ f X ; f A(u ) γ u }. Thi then mean that the global exitence of olution to (E) will be etablihed if we can verify a priori etimate u(t) Z < R and A(u(t)) γ u(t) X C for every local olution. 4. Degenerate Abtract Evolution Equation We conider the Cauchy problem of a degenerate abtract evolution equation dmv + L(Mv)v = F (Mv), < t T, (D.E) dt Mv() = u in a Banach pace X. Let Z X be the econd Banach pace continuouly embedded in X and K be a bounded ubet of Z uch that K = {u Z; u Z < R}, < R <. For each u K, L(u) i a denely defined cloed linear operator of X with contant domain D(L(u)) D L. M i a cloed linear operator of X with domain D(M) D L, and M map D L into Z. F i a nonlinear operator from K into X. u K i an initial value of the problem. v = v(t) i the unknown function.

19 18 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) We make the following aumption. For every u K, the M-modified pectral et σ M (L(u)) i contained in a fixed open ectorial region σ M (L(u)) Σ = {λ C; arg λ < φ}, where < φ < π 2, and the M-modified reolvent atifie (D.A.i) M(λM L(u)) 1 C L(X) ( λ + 1) 1 κ, λ Σ, u K with ome exponent κ < 1 and a contant C > which are independent of u. The M-modified reolvent alo atifie (D.A.ii) M(λM L(u)) 1 C L(X,Z) ( λ + 1) 1 ρ, λ, u K with ome exponent κ ρ < 1 and a contant C > independent of u. L(u) atifie the Lipchitz condition (D.A.iii) L(u){L(u) 1 L(ũ) 1 } L(X) C u ũ Z, u, ũ K with ome contant C >. F alo atifie the Lipchitz condition (D.F) F (u) F (ũ) X C u ũ Z, u, ũ K with ome contant C >. We et u(t) = Mv(t) and rewrite (D.E) in the form du (4.1) dt + L(u)M 1 u F (u), < t T, u() = u. Here, L(u)M 1 = A(u) i a multivalued linear operator defined for u K with the contant domain D(A(u)) = M(D L ). Our goal i then to apply the Theorem 3.1 to the preent Cauchy problem. According to [3, Theorem1.14], if λ σ M (L(u)), then λ σ(a(u)), and it hold that M(λM L(u)) 1 = (λ A(u)) 1, λ σ M (L(u)). Therefore, (D.A.i) yield that For u, ũ K, (λ A(u)) 1 L(X) C, λ Σ. ( λ + 1) 1 κ {A(u) 1 A(ũ) 1 }f = M{L(u) 1 L(ũ) 1 }f D(A(u)), f X. In addition, L(u){L(u) 1 L(ũ) 1 }f A(u){A(u) 1 A(ũ) 1 }f. Therefore, it follow from (D.A.iii) that A(u){A(u) 1 A(ũ) 1 }f X L(u){L(u) 1 L(ũ) 1 }f X C u ũ Z f X, f X. Hence, (A.i,ii) in the preceding ection have been verified.

20 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 19 For κ < β < 1 it i known that A(u) β f = From (D.A.ii) it i een that in πβ π (λ + A(u)) 1 L(X,Z) Therefore, for any β uch that ρ < β < 1, A(u) β f Z 1 π Setting ũ = A(u) β f, we oberve that λ β (λ + A(u)) 1 fdλ, f X. C, λ. (λ + 1) 1 ρ λ β (λ + 1) ρ 1 dλ f X C f X. ũ Z C f X. For a given ũ D(A(u) β ), thi i true for any f A(u) β ũ. Hence, (Sp.ii) i fulfilled with any β (ρ, 1). For (In), we aume that u K and u atifie a compatibility condition of the form (D.In) u D({L(u )M 1 } γ ) with ome exponent < γ 1. For the exponent we aume the relation (D.Ex) κ ρ < γ 1 and 5κ + ρ < γ. It i then poible to take the exponent β in uch a way that (Sp.ii) and (Ex) hold. We have thu found out the condition to be aumed to apply Theorem 3.1 and obtained the main reult of the paper. Theorem 4.1. Under (D.A.i,ii,iii), (D.F), (D.Ex), and (D.In), there exit a unique local olution to (D.E) in the function pace { Mv C([, Tu ]; Z) C 1 ((, T u ]; X), v C((, T u ]; D L ), t 1+κ γ L(Mv)v B((, T u ]; X), where T u > i determined by the norm u Z and {L(u )M 1 } γ u X. 5. Quailinear elliptic-parabolic equation A an application of our abtract reult, we hall conider the Cauchy problem of a quailinear elliptic-parabolic equation of the form m(x)v = {a(x, m(x)v) v} + f(x, m(x)v) in (, T ] Ω, t (5.1) v = on (, T ] Ω, m(x)v(x, ) = u (x) in Ω

21 2 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) in a bounded region Ω R n of C 2 cla. In thi paper we handle the cae where n = 1, 2, and 3. m(x) i a nonnegative function uch that (5.2) m(x) C 1 (Ω) when n = 1, m(x) C 2 (Ω) when n = 2, 3. a(x, u) i a real valued mooth function defined for (x, u) Ω (R + ir), and it i aumed for each < R < to atify (5.3) a(x, u) δ R > for all x Ω and u uch that u R with ome poitive contant δ R. f(x, u) i a mooth function of (x, u) Ω (R + ir). For the initial function, we aume that { H 1 (Ω) when n = 1, (5.4) u = m(x)v with ome v H 2 (Ω) H 1 (Ω) when n = 2, 3. Cae when n = 1. In thi cae we formulate (5.1) in the pace X = H 1 (Ω). We take a Z the Sobolev pace H 1 2 +ε (Ω), where ε i an exponent arbitrarily fixed o that ε (, 1 2 ). Let u Z and u Z < R <, then K i taken a K = {u Z; u Z < R}. By the embedding theorem, K i a bounded et of C(Ω). For u K, the equilinear form a(u; w 1, w 2 ) = a(x, u(x)) w 1 (x) w 2 (x) dx, w 1, w 2 H 1 (Ω) Ω i defined. According to the Lax-Milgram theorem (ee e. g. [13, Chap. 2,Thm. 9.1]), thi equilinear form determine under (5.3) a cloed linear operator L(u) in H 1 (Ω) with the domain D(L(u)) = H 1 (Ω) = D L which i in fact an iomorphim from D L to X. Implicitly, L(u) i the differential operator {a(x, u) w}. We define M a the multiplication operator of the function m(x), in view of (5.2), M i a bounded linear operator on both X and H 1 (Ω), that i M L(X) L(H 1 (Ω)). F (u) i defined by F (u) = f(x, u(x)), u K. In thi way, (5.1) i written a the Cauchy problem of an abtract equation of the form (D.E) in X. Let u now verify all the aumption (D.Ai,ii,iii) and (D.F) in Section 4. It i already known by [3, Example 6.3, (6.7)] that (D.A.i) i fulfilled with a uitable ectorial domain Σ and κ =. In order to verify (D.A.ii), we ue the interpolation property that H 1 2 +ε (Ω) = [L 2 (Ω), H 1 (Ω)] 1 2 +ε. Then, M(λM L(u)) 1 L(X,Z) C M(λM L(u)) ε L(X,H 1 ) M(λM L(u)) ε L(X,L 2 ). But, from [3, (6.6) and (6.8)] it i known that (λm L(u)) 1 L(X,H1 ) C, λ Σ, u K, M(λM L(u)) 1 C L(X,L 2 ), λ Σ, u K, ( λ + 1) 1 2

22 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 21 therefore we obtain that (5.5) M(λM L(u)) 1 L(X,Z) C( λ + 1) ε 2 1 4, λ Σ, u K. Thi how that (D.A.ii) i valid with ρ = ε 2. Verification of (D.A.iii) i very eay. Indeed, we have L(u){L(u) 1 L(ũ) 1 }f, w H 1 H 1 = {L(ũ) L(u)}L(ũ) 1 f, w H 1 H 1 = {a(x, ũ(x)) a(x, u(x))} L(ũ) 1 f w dx, f X, w D L. Therefore, ince Ω a(x, ũ) a(x, u) C C ũ u C C ũ u Z, ũ, u K, (D.A.iii) follow immediately. Verification of (D.F) i alo very eay. Finally, (5.4) implie that u belong to D(L(u )M 1 ), that i u atifie (D.In) with γ = 1. (D.Ex) i then fulfilled with κ =, ρ = ε 2, and γ = 1. We have thu hown that, under (5.2), (5.3) and (5.4), we can apply the Theorem 4.1 to the problem (5.1). Cae when n = 2, 3. In thi cae, we take a X the pace L 2 (Ω) and a Z the Sobolev pace H n 2 +ε (Ω), where ε i an exponent arbitrarily fixed o that ε (, 1 2 ). Let u Z and u Z < R <. Then K i taken a K = {u Z; u Z < R}. K i a bounded et of C(Ω). For u K, the linear operator L(u) i defined by L(u)w = {a(x, u(x)) w} + cw with D(L(u)) = H 2 (Ω) H 1 (Ω), where c i ome ufficiently large contant for which all the argument below are true. L(u) i a poitive definite elf-adjoint operator of X, the domain D(L(u)) D L being independent of u. The following etimate alo hold w H 2 C L(u)w L 2, w D L, u K. M i a multiplication operator of m(x); in view of (5.2), M i een to be a bounded linear operator on both X and H 2 (Ω). F (u) i defined by F (u) = cu+f(x, u), u K. Then (5.1) i formulated a the Cauchy problem of an abtract equation of the form (D.E) in X. In the preent cae we have to aume in addition to (5.2) the following order condition (5.6) m(x) Cm(x) ζ, x Ω with ome uitable exponent ζ [, 1) which will be pecified below. A hown in [3, Example 6.3], condition (5.6) yield that M(λM L(u)) 1 L(X) C( λ + 1) 1 2 ζ, λ Σ, u K with ome uitable ectorial domain Σ, < φ < π 1 ζ 2. Therefore, with κ = 2 ζ, (5.7) (5.8) M(λM L(U)) 1 L(X) C( λ + 1) κ 1, λ Σ, u K, (λm L(u)) 1 L(X,H 2 ) C( λ + 1) κ, λ Σ, u K.

23 22 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) By the interpolation property that Z = H n 2 +ε (Ω) = [L 2 (Ω), H 2 (Ω)] n 4 + ε 2, it follow that M(λM L(u)) 1 L(X,Z) (5.7) and (5.8) yield that C M(λM L(u)) 1 1 n 4 ε 2 L(X,X) M(λM L(u)) 1 n 4 + ε 2 L(X,H 2 ). M(λM L(u)) 1 L(X,Z) C( λ + 1) 1+ n 4 + ε 2 +κ, λ Σ, u K. Therefore, (D.A.ii) i fulfilled with ρ = n 4 + ε 2 + κ. (D.A.iii) i verified directly from L(u){L(u) 1 L(ũ) 1 }f = {L(ũ) L(u)}L(ũ) 1 f = {a(x, u) a(x, ũ)} L(ũ) 1 f + {a(x, u) a(x, ũ)} L(ũ) 1 f. Note that the following etimate a(x, u) a(x, ũ) Z C u ũ Z, u, ũ K i verified by uing the theory of Sobolev pace (cf. [7]). (D.F) i alo verified immediately. (5.4) implie that u D(L(u )M 1 ), that i (D.In) i valid with γ = 1. Therefore, by imple calculation, (D.Ex) i hown to be valid, provided that (5.9) 16+2n+4ε 2+n+2ε < ζ < 1, n = 2, 3. Thu, under (5.2), (5.3), (5.4), (5.6), and (5.9), Theorem 4.1 i applicable to the problem (5.1). Remark 5.1. According to Favini et al. [4], (D.A.i) i valid even in the pace L p (Ω), 1 < p <. If we utilize thee reult, it i equally poible to handle the problem (5.1) in L p pace. 6. Quailinear Elliptic-Parabolic Sytem In thi ection let u conider an elliptic-parabolic ytem of the form u t = { a(x, u) } u + b(x, u) x x x v + f(x, u) in (, T ] Ω, (6.1) = { c(x, u) } u + d(x, u) x x x v + g(x, u) in (, T ] Ω, u = v = on (, T ] Ω, u(x, ) = u (x) in Ω in a bounded open interval Ω = (, l). a(x, u), b(x, u), c(x, u), and d(x, u) are all real valued mooth function of variable (x, u) Ω (R + ir). It i aumed that, for each < R <, there exit

24 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 23 ome poitive contant δ R > dependent on R uch that the following etimate hold: (6.2) a(x, u)ξ 2 + (b(x, u) + c(x, u))ξη + d(x, u)η 2 δ R (ξ 2 + η 2 ), ξ, η R for all x Ω and u uch that u R. f(x, u) and g(x, u) are given mooth function of variable (x, u) Ω (R + ir). Initial value u i aumed to atify (6.3) u H 1 (Ω). We intend to formulate the problem (6.1) in a product pace {( ) } f X = ; f, g H 1 (Ω). g A Z we take the pace Z = {( ) } u ; u H 1 2 +ε (Ω), where ε i an arbitrarily fixed exponent o that ε (, 1 2 ), in view of the fact that H 1 2 +ε (Ω) C(Ω). Then K i taken a K = {( u ) Z; u 1 H +ε 2 } < R with ome fixed < R < uch that u 1 H +ε 2 < R, K being a bounded ubet ( u of C(Ω). For U = K, a linear operator L(U) acting in X i defined by ) ( ) (ũ ) (ũ ) Dx {a(x, u)d L(U)V = x } D x {b(x, u)d x }, V =, D x {c(x, u)d x } D x {d(x, u)d x } ṽ ṽ where D x = x, with the domain F (U) : K X i defined by {(ũ D(L(U)) D L = ṽ F (U) = ( ) f(x, u), U = g(x, u) ) ; ũ, ṽ H 1 (Ω) ( ) u K. Finally, M i defined a the projection on X uch that ( ) ( ) ( ) f f f (6.4) M =, X. g g (6.5) }. Obviouly, M map D L into Z. In thi way we are led to the following abtract formulation of (6.1) + L(MV )V = F (MV ), < t T, dmv dt MV () = U = ( u )

25 24 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) in the pace X. Let u how that the Theorem 4.1 i applicable to thi Cauchy problem. In order to verify (D.A.i) we have to conider equilinear form on D L : { A λ (U; V 1, V 2 ) = a(x, u)dx ũ 1 D x ũ 2 + b(x, u)d x ṽ 1 D x ũ 2 where U = Ω } + c(x, u)d x ũ 1 D x ṽ 2 + d(x, u)d x ṽ 1 D x ṽ 2 dx ) ) (ũ1 (ũ2 λ ũ 1 ũ 2 dx, V 1 =, V 2 = D L, Ω ( ) u K and λ C. It i immediate to ee that (6.6) A λ (U; V 1, V 2 ) C( λ + 1) V 1 DL V 2 DL, V 1, V 2 D L. In addition, we verify that ReA λ (U; V, V ) = Reλ ũ 2 { dx + a(x, u) Dx ũ 2 + d(x, u) D x ṽ 2 Ω Ω + (b(x, u) + c(x, u))(red x ũ ReD x ṽ + ImD x ũ ImD x ṽ) } dx and ImA λ (U, V, V ) = Imλ ũ 2 dx Ω + (b(x, u) c(x, u))(red x ũ ImD x ṽ ImD x ũ ReD x ṽ)dx. Ω Then, by (6.2) there exit δ > uch that { ReA λ (U; V, V ) δ( Dx ũ 2 + D x ṽ 2 ) Reλ ũ 2} dx, V D L, Ω { ImA λ (U; V, V ) Imλ ũ 2 C R ( D x ũ 2 + D x ṽ 2 ) } dx, V D L, here C R denote a contant Ω C R = ṽ 1 up b(x, u(x)) c(x, u(x)). x Ω, U K Let u introduce a parameter < θ < 1, and oberve that A λ (U; V, V ) (1 θ)rea λ (U; V, V ) + θ ImA λ (U; V, V ) ((1 θ)δ θc R )( D x ũ 2 L 2 + D xṽ 2 L 2 + (θ Imλ (1 θ)reλ) ũ 2 L 2. Then, if θ > i ufficiently mall o that (1 θ)δ θc R δ 2, and if λ i taken in uch a way that λ Σ = {λ C; arg λ < φ}, Tan 1 1 θ < φ < π θ 2, then (6.7) A λ (U; V, V ) δ ( V 2 D L + λ MV 2 L 2), V D L, U K ṽ 2

26 QUASILINEAR DEGENERATE EVOLUTION EQUATIONS IN BANACH SPACES 25 with ome poitive contant δ >. Here we ued the Poincaré inequality ũ L 2 C D x ũ L 2, ũ H 1 (Ω). In view of (6.6) and (6.7), we can now apply the Lax-Milgram theorem (ee e. g. [13, Chap. 2,Thm. 9.1,Rem. 9.3]). Let λ Σ, then for a given F X, the problem A λ (U; V, W ) = F, W X DL, W D L ha a unique olution V D L with the etimate (6.8) (6.9) Since V DL (1/δ ) F X, λ 1 2 MV L 2 (1/δ ) F X. A λ (U; V, W ) = (λm L(U))V, W X DL, W D L, it follow that for a given F X, the problem (λm L(U))V = F ha a unique olution with the etimate (6.8) and (6.9). Thi then mean that λ ρ M (L(U)) and the reolvent atifie the etimate (6.1) (6.11) (λm L(U)) 1 F DL (1/δ ) F X, F X, λ 1 2 (λm L(U)) 1 F L 2 (1/δ ) F X, F X. In thi way we have verified that σ M (L(U)) Σ, U K. Therefore it uffice to verify the etimate (D.A.i). But by (6.1) it i now een that λm(λm L(U)) 1 F X = F + L(U)(λM L(U)) 1 F X F X + C (λm L(U)) 1 F DL C(1 + (1/δ )) F X, F X. Hence, (D.A.i) i fulfilled with the domain Σ determined above and κ =. To verify (D.A.ii) we ue the interpolation property that H 1 2 +ε (Ω) = [L 2 (Ω), H 1 (Ω)] 1 2 +ε. Then, by the ame argument a for (5.5), (6.1) and (6.11) yield that (λm L(U)) 1 L(X,Z) C( λ + 1) ε 2 1 4, λ Σ. Hence, (D.A.ii) i valid with ρ = ε 2. (D.A.iii) i verified directly a in the previou ection by uing the expreion L(U 1 ){L(U 1 ) 1 L(U 2 ) 1 } = {L(U 2 ) L(U 1 )}L(U 2 ) 1 ( ) Dx {[a(x, u = 1 ) a(x, u 2 )]D x } D x {[b(x, u 1 ) b(x, u 2 )]D x } L(U D x {[c(x, u 1 ) c(x, u 2 )]D x } D x {[d(x, u 1 ) d(x, u 2 )]D 2 ) 1, x } ( ) ui U i = K (i = 1, 2).

27 26 ANGELO FAVINI ( ) AND ATSUSHI YAGI ( ) (D.F) i alo verified directly. Since D(L(U )M 1 ) = M(D L ), (6.3) together with (6.4) implie that the initial value U in (6.5) belong to D(L(U )M 1 ). Hence, (D.In) i valid with γ = 1. (D.Ex) i alo fulfilled a well. In thi way we conclude that, under (6.2) and (6.3), Theorem 4.1 i applied to (6.5) to obtain the exitence and uniquene of local olution. Reference [1] C. Bardo and H. Brezi, Sur une clae de problème d évolution nonlinéaire, J. Diff. Eq. 6, 1969, [2] H. Brezi, On ome degenerate nonlinear parabolic equation, Nonlinear Functional Analyi, Proc. Symp. Pure Math. 18, 197, [3] A. Favini and A. Yagi, Multivalued linear operator and degenerate evolution equation, Ann. Mat. Pura. Appl. (IV) 163, 1993, [4] A.Favini, A. Lorenzi, H. Tanabe and A. Yagi, An L p -approach to ingular linear parabolic equation in bounded domain, Preprint. [5] A. Kuttler, A degenerate nonlinear Cauchy problem, Applicable Analyi 13, 1982, [6] A. Kuttler, Implicit evolution equation, Appl. An. 16, 1983, [7] K. Oaki, T. Tujikawa, A. Yagi and M. Mimura, Exponential attractor for a chemotaxigrowth ytem of equation, Nonlinear Analyi 51, 22, [8] P. E. Sobolevkii, Equation of parabolic type in Banach pace, Amer. Math. Soc. Tran. Ser. 2 49, 1966, [9] A. Yagi, Abtract quailinear evolution equation of parabolic type in Banach pace, Boll. Un. Mat. Ital. 5-B, 1991, [1] R. W. Carroll and R. E. Showalter, Singular and Degenerate Cauchy Problem, 1976, Academic Pre, London, New York. [11] A. Favini and A. Yagi, Degenerate Differential Equation in Banach Space, 1999, Marcel Dekker, New York. [12] A. Friedman, Partial Differential Equation, 1969, Holt, Rinehart and Winton, New York. [13] J. L. Lion et E. Magene, Problème aux limite non homogène et Application, vol. 1, 1968, Dunod, Pari. [14] Yu. N. Rabotnov, Polzuchet Elementov Kontruktii (Creep of contructional element), 1967, Nauka, Mocow. [15] W. Shockley, Electron and Hole in Semiconductor, 195, D. Van Notrand, Princeton, New Jerey. [16] R. E. Showalter, Monotone Operator in Banach Space and Nonlinear Partial Differential Equation, Math. Survey & Monograph 49, 1997, AMS, Providence. [17] H. Tanabe, Functional Analytic Method for Partial Differential Equation, 1997, Marcel Dekker, New York. (*) Department of Mathematic, Univerity of Bologna, Piazza di Porta S. Donato 5, 4126 Bologna, Italia (**) Department of Applied Phyic, Oaka Univerity, Suita, Oaka , Japan

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS Electronic Journal of Differential Equation, Vol. 206 (206), No. 204, pp. 8. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR

More information

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL

TRIPLE 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 information

On mild solutions of a semilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach spaces

On mild solutions of a semilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach spaces MAEMAIA, 16, Volume 3, Number, 133 14 c Penerbit UM Pre. All right reerved On mild olution of a emilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach pace

More information

Research Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation

Research 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 information

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS

FOURIER 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 information

Hyperbolic Partial Differential Equations

Hyperbolic 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 information

A 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 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 information

Research Article Existence for Nonoscillatory Solutions of Higher-Order Nonlinear Differential Equations

Research 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 information

General System of Nonconvex Variational Inequalities and Parallel Projection Method

General 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 information

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES

TAYLOR 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 information

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS

ON 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 information

February 5, :53 WSPC/INSTRUCTION FILE Mild solution for quasilinear pde

February 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 information

Manprit Kaur and Arun Kumar

Manprit 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 information

STOCHASTIC EVOLUTION EQUATIONS WITH RANDOM GENERATORS. By Jorge A. León 1 and David Nualart 2 CINVESTAV-IPN and Universitat de Barcelona

STOCHASTIC 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 information

INFINITESIMAL GENERATORS OF INVERTIBLE EVOLUTION FAMILIES

INFINITESIMAL GENERATORS OF INVERTIBLE EVOLUTION FAMILIES Method of Functional Analyi and Topology Vol. 23 (207), no., pp. 26 36 INFINITESIMAL GENERATORS OF INVERTIBLE EVOLUTION FAMILIES YORITAKA IWATA Abtract. A logarithm repreentation of operator i introduced

More information

Unbounded solutions of second order discrete BVPs on infinite intervals

Unbounded 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 information

Convex Hulls of Curves Sam Burton

Convex 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 information

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation

IEOR 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 information

On Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces

On 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 information

Semilinear obstacle problem with measure data and generalized reflected BSDE

Semilinear obstacle problem with measure data and generalized reflected BSDE Semilinear obtacle problem with meaure data and generalized reflected BSDE Andrzej Rozkoz (joint work with T. Klimiak) Nicolau Copernicu Univerity (Toruń, Poland) 6th International Conference on Stochatic

More information

One Class of Splitting Iterative Schemes

One 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 information

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations Marquette Univerity e-publication@marquette Mathematic, Statitic and Computer Science Faculty Reearch and Publication Mathematic, Statitic and Computer Science, Department of 6-1-2014 Beta Burr XII OR

More information

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3

More information

arxiv: v1 [math.mg] 25 Aug 2011

arxiv: v1 [math.mg] 25 Aug 2011 ABSORBING ANGLES, STEINER MINIMAL TREES, AND ANTIPODALITY HORST MARTINI, KONRAD J. SWANEPOEL, AND P. OLOFF DE WET arxiv:08.5046v [math.mg] 25 Aug 20 Abtract. We give a new proof that a tar {op i : i =,...,

More information

Bogoliubov Transformation in Classical Mechanics

Bogoliubov 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 information

c 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

c 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 information

STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS

STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS Bulletin of Mathematical Analyi and Application ISSN: 1821-1291, URL: http://bmathaa.org Volume 1 Iue 2(218), Page 19-3. STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE

More information

UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE

UNIQUE 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 information

Multi-dimensional Fuzzy Euler Approximation

Multi-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 information

Explicit formulae for J pectral factor for well-poed linear ytem Ruth F. Curtain Amol J. Saane Department of Mathematic Department of Mathematic Univerity of Groningen Univerity of Twente P.O. Box 800

More information

Laplace Transformation

Laplace 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 information

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES Fixed Point Theory, 5(24, No. 2, 475-486 http://www.math.ubbcluj.ro/ nodeacj/fptcj.html MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

More information

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

7.2 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 information

A CATEGORICAL CONSTRUCTION OF MINIMAL MODEL

A 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 information

New bounds for Morse clusters

New bounds for Morse clusters New bound for More cluter Tamá Vinkó Advanced Concept Team, European Space Agency, ESTEC Keplerlaan 1, 2201 AZ Noordwijk, The Netherland Tama.Vinko@ea.int and Arnold Neumaier Fakultät für Mathematik, Univerität

More information

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004

Lecture 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 information

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas) Lecture 7: Analytic Function and Integral (See Chapter 4 in Boa) Thi i a good point to take a brief detour and expand on our previou dicuion of complex variable and complex function of complex variable.

More information

Linear System Fundamentals

Linear 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 information

arxiv: v2 [math.nt] 30 Apr 2015

arxiv: 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 information

Multicolor Sunflowers

Multicolor Sunflowers Multicolor Sunflower Dhruv Mubayi Lujia Wang October 19, 2017 Abtract A unflower i a collection of ditinct et uch that the interection of any two of them i the ame a the common interection C of all of

More information

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty IOSR Journal of Electrical and Electronic Engineering (IOSR-JEEE) ISSN: 78-676Volume, Iue 6 (Nov. - Dec. 0), PP 4-0 Simple Oberver Baed Synchronization of Lorenz Sytem with Parametric Uncertainty Manih

More information

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova МАТЕМАТИКА И МАТЕМАТИЧЕСКО ОБРАЗОВАНИЕ, 2006 MATHEMATICS AND EDUCATION IN MATHEMATICS, 2006 Proceeding of the Thirty Fifth Spring Conference of the Union of Bulgarian Mathematician Borovet, April 5 8,

More information

THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON

THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON Anal. Theory Appl. Vol. 28, No. (202), 27 37 THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON Chaoyi Zeng, Dehui Yuan (Hanhan Normal Univerity, China) Shaoyuan Xu (Gannan Normal Univerity,

More information

Chapter 4. The Laplace Transform Method

Chapter 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 information

QUENCHED LARGE DEVIATION FOR SUPER-BROWNIAN MOTION WITH RANDOM IMMIGRATION

QUENCHED 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 information

On the regularity to the solutions of the Navier Stokes equations via one velocity component

On the regularity to the solutions of the Navier Stokes equations via one velocity component On the regularity to the olution of the Navier Stoke equation via one velocity component Milan Pokorný and Yong Zhou. Mathematical Intitute of Charle Univerity, Sokolovká 83, 86 75 Praha 8, Czech Republic

More information

Advanced methods for ODEs and DAEs

Advanced methods for ODEs and DAEs Lecture : Implicit Runge Kutta method Bojana Roić, 9. April 7 What you need to know before thi lecture numerical integration: Lecture from ODE iterative olver: Lecture 5-8 from ODE 9. April 7 Bojana Roić

More information

Lecture 8: Period Finding: Simon s Problem over Z N

Lecture 8: Period Finding: Simon s Problem over Z N Quantum Computation (CMU 8-859BB, Fall 205) Lecture 8: Period Finding: Simon Problem over Z October 5, 205 Lecturer: John Wright Scribe: icola Rech Problem A mentioned previouly, period finding i a rephraing

More information

6. KALMAN-BUCY FILTER

6. 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 information

A THEOREM OF ROLEWICZ S TYPE FOR MEASURABLE EVOLUTION FAMILIES IN BANACH SPACES

A THEOREM OF ROLEWICZ S TYPE FOR MEASURABLE EVOLUTION FAMILIES IN BANACH SPACES Electronic Journal of Differential Equation, Vol. 21(21, No. 7, pp. 1 5. ISSN: 172-6691. URL: http://ejde.math.wt.edu or http://ejde.math.unt.edu ftp ejde.math.wt.edu (login: ftp A THEOREM OF ROLEWICZ

More information

Hilbert-Space Integration

Hilbert-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 information

Stochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions

Stochastic 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 information

2 where. x 1 θ = 1 θ = 0.6 x 2 θ = 0 θ = 0.2

2 where. x 1 θ = 1 θ = 0.6 x 2 θ = 0 θ = 0.2 Convex et I a ne and convex et I ome important example I operation that preerve convexity I eparating and upporting hyperplane I generalized inequalitie I dual cone and generalized inequalitie IOE 6: Nonlinear

More information

Primitive Digraphs with the Largest Scrambling Index

Primitive 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 information

Pacific Journal of Mathematics

Pacific Journal of Mathematics Pacific Journal of Mathematic OSCILLAION AND NONOSCILLAION OF FORCED SECOND ORDER DYNAMIC EQUAIONS MARIN BOHNER AND CHRISOPHER C. ISDELL Volume 230 No. March 2007 PACIFIC JOURNAL OF MAHEMAICS Vol. 230,

More information

List coloring hypergraphs

List 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 information

Asymptotic behavior of solutions of mixed problem for linear thermo-elastic systems with microtemperatures

Asymptotic 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 information

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem An Inequality for Nonnegative Matrice and the Invere Eigenvalue Problem Robert Ream Program in Mathematical Science The Univerity of Texa at Dalla Box 83688, Richardon, Texa 7583-688 Abtract We preent

More information

Lecture 3. January 9, 2018

Lecture 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 information

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria

ON 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 information

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1

NULL 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 information

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order

Computers 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 information

WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD

WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD JENNIFER RAE ANDERSON 1. Introduction A plama i a partially or completely ionized ga. Nearly all (approximately 99.9%) of the matter

More information

MATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.:

MATEMATIK 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 information

On the Unit Groups of a Class of Total Quotient Rings of Characteristic p k with k 3

On the Unit Groups of a Class of Total Quotient Rings of Characteristic p k with k 3 International Journal of Algebra, Vol, 207, no 3, 27-35 HIKARI Ltd, wwwm-hikaricom http://doiorg/02988/ija2076750 On the Unit Group of a Cla of Total Quotient Ring of Characteritic p k with k 3 Wanambii

More information

Michał Kisielewicz SOME OPTIMAL CONTROL PROBLEMS FOR PARTIAL DIFFERENTIAL INCLUSIONS

Michał Kisielewicz SOME OPTIMAL CONTROL PROBLEMS FOR PARTIAL DIFFERENTIAL INCLUSIONS Opucula Mathematica Vol. 28 No. 4 28 Dedicated to the memory of Profeor Andrzej Laota Michał Kiielewicz SOME OPTIMAL CONTROL PROBLEMS FOR PARTIAL DIFFERENTIAL INCLUSIONS Abtract. Partial differential incluion

More information

Online 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 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 information

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS

ON 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 information

arxiv: v1 [math.ca] 23 Sep 2017

arxiv: v1 [math.ca] 23 Sep 2017 arxiv:709.08048v [math.ca] 3 Sep 07 On the unit ditance problem A. Ioevich Abtract. The Erdő unit ditance conjecture in the plane ay that the number of pair of point from a point et of ize n eparated by

More information

Minimizing movements along a sequence of functionals and curves of maximal slope

Minimizing movements along a sequence of functionals and curves of maximal slope Minimizing movement along a equence of functional and curve of maximal lope Andrea Braide Dipartimento di Matematica, Univerità di Roma Tor Vergata via della ricerca cientifica 1, 133 Roma, Italy Maria

More information

in a circular cylindrical cavity K. Kakazu Department of Physics, University of the Ryukyus, Okinawa , Japan Y. S. Kim

in 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 information

L 2 -transforms for boundary value problems

L 2 -transforms for boundary value problems Computational Method for Differential Equation http://cmde.tabrizu.ac.ir Vol. 6, No., 8, pp. 76-85 L -tranform for boundary value problem Arman Aghili Department of applied mathematic, faculty of mathematical

More information

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value

Some 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 information

Singular perturbation theory

Singular 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 information

Research Article Triple Positive Solutions of a Nonlocal Boundary Value Problem for Singular Differential Equations with p-laplacian

Research Article Triple Positive Solutions of a Nonlocal Boundary Value Problem for Singular Differential Equations with p-laplacian Abtract and Applied Analyi Volume 23, Article ID 63672, 7 page http://dx.doi.org/.55/23/63672 Reearch Article Triple Poitive Solution of a Nonlocal Boundary Value Problem for Singular Differential Equation

More information

LECTURE 12: LAPLACE TRANSFORM

LECTURE 12: LAPLACE TRANSFORM LECTURE 12: LAPLACE TRANSFORM 1. Definition and Quetion The definition of the Laplace tranform could hardly be impler: For an appropriate function f(t), the Laplace tranform of f(t) i a function F () which

More information

Problem Set 8 Solutions

Problem 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 information

Robustness analysis for the boundary control of the string equation

Robustness 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 information

SOME RESULTS ON INFINITE POWER TOWERS

SOME 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 information

arxiv: v1 [math.ds] 29 Dec 2015

arxiv: v1 [math.ds] 29 Dec 2015 Non-mooth addle-node bifurcation III: trange attractor in continuou time G. Fuhrmann arxiv:1512.8763v1 [math.ds] 29 Dec 215 8th November 218 Non-mooth addle-node bifurcation give rie to minimal et of intereting

More information

ONLINE APPENDIX: TESTABLE IMPLICATIONS OF TRANSLATION INVARIANCE AND HOMOTHETICITY: VARIATIONAL, MAXMIN, CARA AND CRRA PREFERENCES

ONLINE APPENDIX: TESTABLE IMPLICATIONS OF TRANSLATION INVARIANCE AND HOMOTHETICITY: VARIATIONAL, MAXMIN, CARA AND CRRA PREFERENCES ONLINE APPENDIX: TESTABLE IMPLICATIONS OF TRANSLATION INVARIANCE AND HOMOTHETICITY: VARIATIONAL, MAXMIN, CARA AND CRRA PREFERENCES CHRISTOPHER P. CHAMBERS, FEDERICO ECHENIQUE, AND KOTA SAITO In thi online

More information

Approximate Analytical Solution for Quadratic Riccati Differential Equation

Approximate Analytical Solution for Quadratic Riccati Differential Equation Iranian J. of Numerical Analyi and Optimization Vol 3, No. 2, 2013), pp 21-31 Approximate Analytical Solution for Quadratic Riccati Differential Equation H. Aminikhah Abtract In thi paper, we introduce

More information

INITIAL VALUE PROBLEMS OF FRACTIONAL ORDER HADAMARD-TYPE FUNCTIONAL DIFFERENTIAL EQUATIONS

INITIAL VALUE PROBLEMS OF FRACTIONAL ORDER HADAMARD-TYPE FUNCTIONAL DIFFERENTIAL EQUATIONS Electronic Journal of Differential Equation, Vol. 205 205), No. 77, pp. 9. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu ftp ejde.math.txtate.edu INITIAL VALUE PROBLEMS OF

More information

Social Studies 201 Notes for November 14, 2003

Social 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 information

A new conjugate gradient method with the new Armijo search based on a modified secant equations

A new conjugate gradient method with the new Armijo search based on a modified secant equations ISSN: 35-38 Enineerin an echnoloy Vol 5 Iue 7 July 8 A new conjuate raient metho with the new Armijo earch bae on a moifie ecant equation Weijuan Shi Guohua Chen Zhibin Zhu Department of Mathematic & Applie

More information

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle

Flag-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 information

(3) A bilinear map B : S(R n ) S(R m ) B is continuous (for the product topology) if and only if there exist C, N and M such that

(3) A bilinear map B : S(R n ) S(R m ) B is continuous (for the product topology) if and only if there exist C, N and M such that The material here can be found in Hörmander Volume 1, Chapter VII but he ha already done almot all of ditribution theory by thi point(!) Johi and Friedlander Chapter 8. Recall that S( ) i a complete metric

More information

UNIT 15 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS

UNIT 15 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS UNIT 1 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS Structure 1.1 Introduction Objective 1.2 Redundancy 1.3 Reliability of k-out-of-n Sytem 1.4 Reliability of Standby Sytem 1. Summary 1.6 Solution/Anwer

More information

arxiv: v4 [math.co] 21 Sep 2014

arxiv: v4 [math.co] 21 Sep 2014 ASYMPTOTIC IMPROVEMENT OF THE SUNFLOWER BOUND arxiv:408.367v4 [math.co] 2 Sep 204 JUNICHIRO FUKUYAMA Abtract. A unflower with a core Y i a family B of et uch that U U Y for each two different element U

More information

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang

ON 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 information

Lecture 7: Testing Distributions

Lecture 7: Testing Distributions CSE 5: Sublinear (and Streaming) Algorithm Spring 014 Lecture 7: Teting Ditribution April 1, 014 Lecturer: Paul Beame Scribe: Paul Beame 1 Teting Uniformity of Ditribution We return today to property teting

More information

SECTION x2 x > 0, t > 0, (8.19a)

SECTION 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 information

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement

More information

EXISTENCE AND REGULARITY RESULTS FOR SOME NONLINEAR PARABOLIC EQUATIONS

EXISTENCE AND REGULARITY RESULTS FOR SOME NONLINEAR PARABOLIC EQUATIONS EXISTECE AD REGULARITY RESULTS FOR SOME OLIEAR PARABOLIC EUATIOS Lucio BOCCARDO 1 Andrea DALL AGLIO 2 Thierry GALLOUËT3 Luigi ORSIA 1 Abstract We prove summability results for the solutions of nonlinear

More information

1. Preliminaries. In [8] the following odd looking integral evaluation is obtained.

1. 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 information

Factor Analysis with Poisson Output

Factor 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 information

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL 98 CHAPTER DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL INTRODUCTION The deign of ytem uing tate pace model for the deign i called a modern control deign and it i

More information

Research Article Iterative Schemes for Zero Points of Maximal Monotone Operators and Fixed Points of Nonexpansive Mappings and Their Applications

Research Article Iterative Schemes for Zero Points of Maximal Monotone Operators and Fixed Points of Nonexpansive Mappings and Their Applications Hindawi Publihing Corporation Fixed Point Theory and Application Volume 2008, Article ID 168468, 12 page doi:10.1155/2008/168468 Reearch Article Iterative Scheme for Zero Point of Maximal Monotone Operator

More information

Riemann s Functional Equation is Not a Valid Function and Its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.

Riemann 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 information

696 Fu Jing-Li et al Vol. 12 form in generalized coordinate Q ffiq dt = 0 ( = 1; ;n): (3) For nonholonomic ytem, ffiq are not independent of

696 Fu Jing-Li et al Vol. 12 form in generalized coordinate Q  ffiq dt = 0 ( = 1; ;n): (3) For nonholonomic ytem, ffiq are not independent of Vol 12 No 7, July 2003 cfl 2003 Chin. Phy. Soc. 1009-1963/2003/12(07)/0695-05 Chinee Phyic and IOP Publihing Ltd Lie ymmetrie and conerved quantitie of controllable nonholonomic dynamical ytem Fu Jing-Li(ΛΠ±)

More information