+ All Categories
Home > Documents > Strong solutions of abstract fractional differential equations

Strong solutions of abstract fractional differential equations

Date post: 07-Jan-2017
Category:
Upload: phungdiep
View: 239 times
Download: 1 times
Share this document with a friend
72
Transcript
Page 1: Strong solutions of abstract fractional differential equations
Page 2: Strong solutions of abstract fractional differential equations
Page 3: Strong solutions of abstract fractional differential equations

1

Welcome

The Department of Computation and Mathematics of the Faculdade de Filosofia, Ciências e Letrasde Ribeirão Preto of the Universidade de São Paulo (DCM-FFCLRP-USP) and the GAFEVOL groupwelcome you to the IX Conference GAFEVOL which will take place at the city of Ribeirão Preto, in thestate of São Paulo, Brazil, on September 16-18, 2014.

Organizing committee

Andréa Cristina Prokopczyk Arita (UNESP)

Eduardo Hernández de Morales (DCM/USP)

Jaqueline Godoy Mesquita (DCM/USP)

Kátia de Azevedo (DCM/USP)

Márcia Federson (ICMC/USP)

Michelle Pierri (DCM/USP)

Vanessa Rolnik (DCM/USP)

Scientific committee

Carlos Lizama (Universidade de Santiago de Chile)

Eduardo Hernandez de Morales (Universidade de São Paulo, Brazil)

Hernán Henríquez (Universidade de Santiago de Chile)

István Györi (University of Pannonia, Hungary)

Sergei Trofimchuk (Universidade de Talca, Chile)

Address

IX Conference GAFEVOL

Departamento de Computação e Matemática

Faculdade de Filosofia, Ciências e Letras de Ribeirão Preto

Universidade de São Paulo

Bandeirantes Avenue, 3900

CEP: 14040-901 - Ribeirão Preto - SP

Page 4: Strong solutions of abstract fractional differential equations

2

FAX: +55 (16) 3602-0429

e-mail: [email protected]

website: dcm.ffclrp.usp.br/gafevol

Facebook: https://www.facebook.com/groups/143660335644302/

Page 5: Strong solutions of abstract fractional differential equations

Contents

Map . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7

General Information . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11

Conference site . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13

Registration . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13

Financial support . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13

Social events . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13

Computer and wireless LAN use . . . . . . . . . . . . . . . . . . . . . . . . . 13

Meals and refreshments . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14

Health emergencies . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14

Money exchanges . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14

Taxis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15

Tourism . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15

Smoking . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 16

Programme . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17

Abstracts . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21

3

Page 6: Strong solutions of abstract fractional differential equations

4 CONTENTS

Semilinear fractional differential equations with critical nonlinearitiesBruno de Andrade . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23

Controllability for systems of neutral type with delayFernando Gomes de Andrade* and Andréa Cristina Prokopczyk Arita . . . . . . . . . . . . 24

Bifurcation of Periodic Solutions for Retarded Functional Differential Equations on ManifoldsPierluigi Benevieri*, Alessandro Calamai, Massimo Furi and

Maria Patrizia Pera . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25

On the Jack Hale’s problem for impulsive systemsEveraldo de Mello Bonotto . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26

Existence of solutions for abstract neutral nonlinear fractional differential degenerate equationsEduardo Hernández, Alejandro Caicedo Roque* and Donal O’Regan . . . . . . . . . . . . . 27

Pullback attractor and extremal complete trajectoriesÉrika Capelato* and Ricardo de Sá Teles . . . . . . . . . . . . . . . . . . . . . . . . . . . 28

An inverse problem in biological olfactory ciliumCarlos Conca . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29

Well-posedness and qualitative aspects of solutions with datum on Besov-Morrey spaces fora diffusion-wave equation

Marcelo Fernandes de Almeida . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 30

Cycles by interaction ofdamping and jumps of energy

Miguel V. S. Frasson*, Marta C. Gadotti, Selma H. J. Nicola and Plácido Z. Táboas . . . . 31

Dominant Solutions of Delay Differential EquationsIstván Györi . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33

Second Order Abstract Neutral Functional Differential EquationsHernán R. Henríquez* and Claudio Cuevas . . . . . . . . . . . . . . . . . . . . . . . . . . 34

A unified approach to discrete fractional calculus and applicationsSebastián Calzadillas, Carlos Lizama* and Jaqueline G. Mesquita . . . . . . . . . . . . . . 37

Almost automorphic solutions for evolutions equationsArlucio Viana, Bruno de Andrade and Eder Mateus* . . . . . . . . . . . . . . . . . . . . . 38

Continuous solutions for divergence-type PDEsLaurent Moonens . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40

Dengue: Model with human mobilityS. Oliva . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41

Dynamics of parabolic equations governed by the p-laplacian on unbounded thin domainsRicardo Parreira da Silva . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42

Thin domains and reactions concentrated on boundaryMarcone C. Pereira . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43

Page 7: Strong solutions of abstract fractional differential equations

CONTENTS 5

On a functional equation associated with a first order problem with finite delayCarlos Lizama and Felipe Poblete* . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44

Hölder continuous solutions for a fractional differential equationsRodrigo Ponce . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 48

Strong solutions of abstract fractional differential equationsJuan C. Pozo*, Hernán R. Henríquez and Verónica Poblete . . . . . . . . . . . . . . . . . 50

Existence of solutions for a fractional neutral integro-differential equation with unboundeddelay . . . . . . .

José Paulo Carvalho dos Santos . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 52

On evolutionary differential equations with state-dependent delayGiovana Siracusa* and Bruno de Andrade . . . . . . . . . . . . . . . . . . . . . . . . . . . 53

On a class of discontinuous dynamical systemsMiguel V. S. Frasson, Marta C. Gadotti, Selma H. J. Nicola and

Plácido Z. Táboas* . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 55

Stability results for measure neutral functional differential equations via GODEMárcia Federson and Patricia H. Tacuri* . . . . . . . . . . . . . . . . . . . . . . . . . . . 56

On a class of thermoelastic plates with p-LaplacianTo Fu Ma . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 57

Asymptotically almost automorphic and almost automorphic solutions of Volterra IntegralEquations on time scales

Eduard Toon . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 58

Soluciones Convergentes en Ecuaciones Diferenciales Impulsivas con AvanceManuel Pinto and Ricardo Torres N.* . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59

Asymptotic behaviour of the time-fractional telegraph equationVicente Vergara . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61

Acknowledgements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 62

Sponsors . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 66

Page 8: Strong solutions of abstract fractional differential equations
Page 9: Strong solutions of abstract fractional differential equations

7

Map

Page 10: Strong solutions of abstract fractional differential equations
Page 11: Strong solutions of abstract fractional differential equations

9

Legends of map

1. Department of Computation and Mathematics (DCM)

2. Didactic Building

3. Canteen

4. Parking

Page 12: Strong solutions of abstract fractional differential equations
Page 13: Strong solutions of abstract fractional differential equations

11

General Information

Page 14: Strong solutions of abstract fractional differential equations
Page 15: Strong solutions of abstract fractional differential equations

13

Conference site

The meeting will take place at Auditorium (Room DE-11) and also in the Coffee Area. The Auditoriumis at Didactic Building and the Coffee Area is at DCM. See the map on page 11.

Registration

The registrations will be made in the following schedule:

• Monday, September 15th From 14:00hs to 14:40hs in the lobby of Pousada Santa Rita.

• Monday, September 15th From 17:10hs to 17:50hs in the lobby of Pousada Santa Rita.

• Tuesday, September 16th From 8:00hs to 8:50hs in the DCM.

We will provide you a badge at registration. Please wear your badge at the event.

Financial support

The financial support payment is planned to be made on Wednesday, September 17th.

Social events

• Tuesday, September 16th: Photo of the meeting at 17:10 at DCM.

• Tuesday, September 16th: Music presentation at 17:50 at DCM.

• Tuesday, September 16th: Cocktail at 19:00 at DCM.

• Wednesday, September 17th: Conference Dinner at 20:30 at the Churrascaria Estância

Computer and wireless LAN use

There will be available computers for use at Informatics Laboratory (room 601 at DCM). Also, all theparticipants of the IX Conference GAFEVOL can use this laboratory during the days of the conferencefrom 8:00 a.m. to 18:00 p.m.

In order to access the wireless connection at the University you need to follow the steps:

1. Enable wireless on your device.

2. Join the USP-NET wireless network.

3. Open a browser and attempt to visit a website (for example your home page).

Page 16: Strong solutions of abstract fractional differential equations

14

4. Click on the button in the page to proceed.

5. You will be redirected to a login page. Enter the login and password which you will receive atthe registration day.

6. You may freely browse the internet after logging in. You may occasionally need to re-authenticateusing the above procedure.

Meals and refreshments

There is a canteen available at DCM where you can have snacks. Also, all the lunchs during theconference will be there. See the map on page 11.

Also, there are several restaurants and bars in the city. Some of them are:

• Pinguim Bar and Restaurant (regional beer and restaurant house)Address: Street General Osório, 389, Centro, Ribeirão PretoContact Number: (16) 3610-8258Website: http://www.pinguimochopp.com.br/

• Colorado Cervejarium (Regional beer house)Address: Av. Independência, 3.242, Ribeirão PretoContact Number: (16) 3911.4949Website: http://www.coloradocervejarium.com.br/

• Nelson Restaurant and BarAddress: Street Prudente de Morais, 1313, Centro, Ribeirão PretoContact Number: (16) 3625-6669Website: http://www.bardonelsonrp.com.br/

• Churrascaria EstânciaAddress: Av. Presidente Vargas, 1100, Alto da Boa Vista, Ribeirão PretoContact Number: ( 16) 3911-9513Website: http://www.estanciaribeirao.com.br/

The Conference Dinner will be at the Churrascaria Estância.

Health emergencies

In case of accidents or health emergencies call 192 (SAMU).

Page 17: Strong solutions of abstract fractional differential equations

15

Money exchanges

In case you need to exchange your money, we recommend you to look for the following agencies:

• Confidence Cambio ExchangeAddress 1: Av. Coronel Fernando Ferreira Leite, 1540, Jd. Califórnia, Ribeirão ShoppingAddress 2: Street São José, 933, Shopping Santa Úrsula.Contact Number: 4004 5700Website: http://www.confidencecambio.com.br/Open hours: Monday to Friday from 10:00 a.m. to 20:00 p.m. and Saturday from 10:00 a.m.to 16:00 p.m.

• Daycoval CambioAddress: Av. Presidente Vargas, 1617Contact Number: (16) 3620 2043 / 3621 0512Website: http://www.daycoval.com.br/Open Hours: Monday to Friday from 10:00 a.m. to 19:00 p.m

Taxis

In case you need to use a taxi, we recommend the following agencies:

• CoopertaxiContact number: (16) 3323-7000

• Aliança Rádio TáxiContact number: (16) 3911-3000

Tourism

We recommend some nice places to visit during your stay in Ribeirão Preto.

• Parks

1. Curupira Park (Park Prefeito Luiz Roberto Jábali)Address: Av. Costabile Romano, 337, Ribeirão Preto-SP

2. Municipal Park Raia (Municipal Park Dr. Luiz Carlos Raia)Address: Street Severino Amaro dos Santos, Ribeirão Preto-SP

3. Bosque and Zoo Fábio BarretoAddress: Street Liberdade s/n, Ribeirão Preto, Estado de São Paulo, BrasilContact Number: (16) 3636-2545 / 3636-2283Website: http://www.ribeiraopreto.sp.gov.br/turismo/zoologico/i71principal.php

Page 18: Strong solutions of abstract fractional differential equations

16

• Theater and Museum

1. Theater Pedro IIAddress: Street Álvares Cabral, 370, Ribeirão Preto-SPContact Number: (16) 3977 8111Website: http://www.theatropedro2.com.br/

2. Coffee Museum Francis SchmidtAddress: Av. Zeferino Vaz, s/n Campus da USP, Monte Alegre, Ribeirão Preto-SPContact Number: (16) 3633-1986

Smoking

Smoking is prohibited in any of the DCM buildings.

Page 19: Strong solutions of abstract fractional differential equations

17

Programme

Page 20: Strong solutions of abstract fractional differential equations
Page 21: Strong solutions of abstract fractional differential equations

19

!

!Monday!

Septem

ber,!15!

Tuesday!

Septem

ber,!16!

Wednesday!

Septem

ber,!17!

Thursday!

Septem

ber!18!

Chairm

an!

!Eduardo!Hernández!

Carlos!Lizam

a!Márcia!Federson!

8h10!–!8h50!

!Registration!

Miguel!Frasson!

István!Györi!

8h50!–!9h30!

!Opening!Cerem

ony!

Sergio!Oliva!

Plácido!Táboas!

9h30!–!10h10!

!Carlos!Lizam

a!Everaldo!Bonotto!

Pierluigi!Benevieri!

10h10!–10h40!

!CoffeeMbreak!

CoffeeMbreak!

CoffeeMbreak!

10h40!–11h20!

!Hernán!Henríquez!

Rodrigo!Ponce!

José!Paulo!dos!Santos!

11h20!–12h!

!Carlos!Conca!

Felipe!Poblete!

Alejandro!Caicedo!

12h!–!14h!

!Lunch!

Lunch!

Lunch!

Chairm

an!

!Hernán!Henríquez!

Kátia!Azevedo!

Rodrigo!Ponce!

14h!–!14h40!

Registration!at!

Pousada!Santa!Rita!

Ma!To!Fu!

Éder!Mateus!

Patrícia!Hilário!

14h40!–15h20!

!Marcone!Correa!

Marcelo!Fernandes!

Laurent!M

oonens!

15h20!–!16h!

!Ricardo!Parreira!

Eduard!Toon!

Fernando!de!Andrade!

16h!–!16h30!

!CoffeeMbreak!

CoffeeMbreak!

CoffeeMbreak!

16h30!–17h10!

!Érika!Capelato!

Giovana!Siracusa!

Bruno!de!Andrade!

17h10!–!17h50!

Registration!at!

Pousada!Santa!Rita!

Oficial!Photo!

Juan!Pozo!

Ricardo!Torres!

17h50!–!18h30!

!Music!Presentation!

Vicente!Vergara!

Closing!Ceremony!

19h!–!20h30!

!Cocktail!

!!

20h30!

!!

Conference!Dinner!

!

Page 22: Strong solutions of abstract fractional differential equations
Page 23: Strong solutions of abstract fractional differential equations

21

Abstracts

Page 24: Strong solutions of abstract fractional differential equations
Page 25: Strong solutions of abstract fractional differential equations

23

Semilinear fractional differential equations with criticalnonlinearities

Bruno de Andrade

Abstract

In this work we study existence of regular mild solutions to abstract fractional Cauchy problems oforder ↵ 2 (0, 1) with critical nonlinearities. Concretely, we analyze the existence of local regular mildsolutions for the problem, and its possible continuation to a maximal interval of existence. We applyour abstract results to fractional partial differential equations coming from heat conduction theory.

This is joint work with Alexandre Nolasco de Carvalho (ICMC-USP), Paulo Carvalho-Neto (IMECC-UNICAMP) and Pedro Marín-Rubio (EDAN-US).

Bibliography

[1] de Andrade, B. ; Carvalho, A. N. ; Carvalho-Neto, P. M. ; Marín-Rubio, P. . Semilinear fractionaldifferential equations: global solutions, critical nonlinearities and comparison results. TopologicalMethods in Nonlinear Analysis, 2014.

Partially supported by CNPq 100994/2011-3 and 478053/2013-4 , e-mail: [email protected], De-partament of Mathematics, Federal University of Sergipe, São Cristóvão-SE, Brazil.

Page 26: Strong solutions of abstract fractional differential equations

24

Controllability for systems of neutral type with delay

Fernando Gomes de Andrade* and Andréa Cristina Prokopczyk Arita

Abstract

This work is a study of the approximate controllability of a system of neutral type described byd

dt

⇣x(t) + F (t)(x

t

)⌘= Ax(t) + L(t)(x

t

) +Bu(t), t � 0, (0.0.1)

x0 = ' 2 C, (0.0.2)

where x(t) 2 X, u(t) 2 U , for all t � 0, X is the state space, U is the space of control, both areHilbert spaces, C = C([�r, 0], X) is the space of continuous functions from [�r, 0] to X, for each t,x

t

: [�r, 0] ! X is the history of x at t, i.e., xt

(✓) = x(t+✓), for all ✓ 2 [�r, 0], L : [0,1) ! L(C, X) isstrongly continuous, i.e., t 7! L(t) is continous for all 2 C fixed, furthermore, A : D(A) ⇢ X ! X

is the infnitesimal generator of analytic semigroup on X, B : U ! X

� is a boundend linear operator,where X

� = (D((�A)�), k ·k�

), for some � 2 ( 12 , 1), is a Banach space with kxk�

= k(�A)�xk, 8 x 2D((�A)�), and F : [0,+1) ! L(C, X�), is strongly continuous and satisfies the following Lipschitzcondition

k(�A)�F (t)( 1)� (�A)�F (s)( 2)k C0(|t� s|+ k 1 + 2kC),for all t, s 2 [0, ⌧ ], 1, 2 2 C and some constant C0 > 0.

Our aim is to use the ideas presented in [1] and [2] to compare the controllability of the linearsystem without delay

x

0(t) = Ax(t) +Bu(t), t � 0, (0.0.3)

x(0) = x

0 2 X. (0.0.4)

with the controllability of neutral system with delay (0.0.1)-(0.0.2).

Bibliography

[1] Hernández, E., Henríquez, H.R. Approximate controllability of second-order distributedimplicit functional systems. Nonlinear Analysis, 70, 1023-1039, 2009.

[2] Prokopczyk Arita, A. C. Controlabilidade e estabilizaaão de sistemas de controle hereditáriosdistribuídos lineares a tempo-variando. Tese (Doutorado em Matemática) - Programa de Pós-Graduação em Matemática - PPGM, ICMC - USP, 2009.

Partially supported by CAPES, Instituto de Ciências Matemáticas e de Computação, Universidade de SãoPaulo, São Carlos, Brasil, e-mail: [email protected]

Page 27: Strong solutions of abstract fractional differential equations

25

Bifurcation of Periodic Solutions for Retarded FunctionalDifferential Equations on Manifolds

Pierluigi Benevieri*, Alessandro Calamai, Massimo Furi andMaria Patrizia Pera

Abstract

We consider T -periodic parametrized retarded functional differential equations, with infinite delay, on(possibly) noncompact manifolds. Using a topological approach, based on the notions of degree of atangent vector field and of the fixed point index, we prove a global continuation result for T -periodicsolutions of such equations. As corollaries we obtain a Rabinowitz type global bifurcation result and acontinuation principle of Mawhin type.

Bibliography

[1] P. Benevieri, A. Calamai, M. Furi and M.P. Pera. Global continuation of periodic solutions forretarded functional differential equations on manifolds. Boundary value problems, 2013, 2013:21.

[2] P. Benevieri, A. Calamai, M. Furi and M.P. Pera. Global Continuation of Forced Oscillations ofRetarded Motion Equations on Manifolds. Preprint

Department of Mathematics, University of Sao Paulo, Sao Paulo, Brazil

Page 28: Strong solutions of abstract fractional differential equations

26

On the Jack Hale’s problem for impulsive systems

Everaldo de Mello Bonotto

Abstract

In this work, we study the Jack Hale’s problem for impulsive dynamical systems. In order to solve theproblem of Jack Hale, we use the concept of asymptotic compactness for impulsive systems.

Bibliography

[1] E. M. Bonotto, L. P. Gimenes and G. M. Souto, On the Jack Hale’s problem to impulsive semi-dynamical systems. Submitted.

[2] D. N. Cheban, Global attractors of non-autonomous dissipative dynamical systems, Interdiscip.Math. Sci., vol. 1, World Scientic Publishing, Hackensack, NJ, 2004.

Partially supported by FAPESP (2012/16709-6) and CNPq, Departament of Mathematics, University ofSão Paulo, São Carlos, Brazil, e-mail: [email protected]

Page 29: Strong solutions of abstract fractional differential equations

27

Existence of solutions for abstract neutral nonlinear fractionaldifferential degenerate equations

Eduardo Hernández, Alejandro Caicedo Roque* and Donal O’Regan

Abstract

In this work we continue the developments in [1] on abstract fractional differential equations. Specif-ically, we study the existence and qualitative properties of solutions for a class of abstract degenerateneutral differential equations with fractional temporal derivative of the form

D

c

(Lx(t) + g(t, xt

)) = Ax(t) + f(t, xt

), t 2 [0, a], (0.0.5)

x0 = ' 2 B = C([�p, 0];X), (0.0.6)

where 0 < ↵ < 1, D↵

c

denotes the ↵-fractional derivative in the Caputo sense, A : D(A) ⇢ X ! X isa sectorial operator, (X, k · k) is a Banach space, the history x

t

belongs to C([�p, 0];X) and f(·), g(·)are suitable continuous functions.

Bibliography

[1] Hernández, Eduardo., O’Regan, Donal. On a New Class of Abstract Neutral Differential Equations.J. Functional Analysis. 261 (2011), 12, 3457-3481.

[2] Kilbas, Anatoly A.; Srivastava, Hari M.; Trujillo, Juan J. Theory and applications of fractional dif-ferential equations. North-Holland Mathematics Studies, 204. Elsevier Science B.V., Amsterdam,2006.

[3] Lunardi, A. Analytic semigroups and optimal regularity in parabolic problems, PNLDE Vol. 16,Birkhäauser Verlag, Basel, 1995.

[4] J. Prüss. Evolutionary Integral Equations and Applications. Monographs Math., 87, BirkhäuserVerlag, 1993.

Suportado pela Fapesp, Grant 2012/01072-2, e-mail: [email protected], Departamento de MatematicaItabaiana, Universidade Federal de Sergipe, Itabaiana, Brazil

Page 30: Strong solutions of abstract fractional differential equations

28

Pullback attractor and extremal complete trajectories

Érika Capelato* and Ricardo de Sá Teles

Abstract

The subject of this paper is to analyze the asymptotic behavior of the nonlinear nonautonomous problem⇢

u

t

� div(|ru|p(x)�2ru) = B(t, u)u(⌧) = u0 2 L

2(⌦),(0.0.7)

where ⌦ is a bounded smooth domain in Rn

, n � 1, p(x) 2 C(⌦), 2 + � p(x) 3 � �, � > 0a.e. x 2 ⌦. We will suppose that B : R ⇥ L

2(⌦) ! L

2(⌦) is globally Lipschitz and increasing. Inthe Banach space, W 1,p(x)(⌦), defined by [1] we obtain an estimate for the solution of the problem(0.0.7) using results of the [3] and thus, we have proved the existence of the pullback attractor for thisproblem. To prove the existence of the extremal complete trajectories, that “delimitate” in a certainsense the pullback attractor, we observe that principal part of the problem is a maximal monotoneoperator and can also be seen as the subdifferential of a lower semicontinuous convex function (see [2])and furthermore, the process is monotonous.

Bibliography

[1] Fran, X., Zhao, D., On the spaces Lp(x)(⌦) and W

1,p(x)(⌦), J. Math. Anal. Appl. 263, 424-446,2001.

[2] Simsen, J., Simsen, M.S.,On p(x)-Laplacian parabolic problems. Nonlinear Studies, vol 18, no. 3,393-403, 2011.

[3] Simsen, J.,A global attractor for a p(x)-Laplacian parabolic problem, Nonlinear Analysis 73, 3278-3283, 2010.

Department of Economics - UNESP, Araraquara, Brazil, e-mail: [email protected]

Page 31: Strong solutions of abstract fractional differential equations

29

An inverse problem in biological olfactory cilium

Carlos Conca

Abstract

In this lecture we study a linear inverse problem with a biological interpretation, modelled by a Fredholmintegral equation of the first kind, where the kernel is represented by step functions. Based on differentassumptions, identifiability, stability and reconstruction results are obtained.

Partially supported by Basal-CMM project, Ecos-Conicyt C13E05, and Fondecyt 1140773,Department ofMathematical Engineering Center for Mathematical Modelling University of Chile Santiago, Chile, e-mail:[email protected]

Page 32: Strong solutions of abstract fractional differential equations

30

Well-posedness and qualitative aspects of solutions withdatum on Besov-Morrey spaces for a diffusion-wave equation

Marcelo Fernandes de Almeida

Abstract

This paper concerns with an interpolated Parabolic-Hyperbolic PDE arisen of time-fractional inte-grodifferential equations. Global existence in critical Besov-Morrey spaces N �

p,µ,1(Rn) (n � 1) andqualitative aspects, like symmetries and positivity of solutions, is showed. Moreover, asymptotic behav-ior of solutions is proved in the framework of scaling invariant Besov-Morrey spaces. Also, self-similarityof solutions is investigated.

Bibliography

[1] de Almeida, Marcelo, F. ; FERREIRA, L. C. F. . Self-similarity, symmetries and asymptotic behaviorin Morrey spaces for a fractional wave equation. Differential and Integral Equations, v. 25, p. 957-976, 2012.

[2] C.X. Miao, H. Yang, The self-similar solution to some nonlinear integro-differential equationscorresponding to fractional order time derivative. Acta Math. Sin. (Engl. Ser.) 21 (2005), no. 6,1337–1350.

Federal University of Sergipe, Department of Mathematics, Aracaju, Brazil, e-mail: [email protected]

Page 33: Strong solutions of abstract fractional differential equations

31

Cycles by interaction ofdamping and jumps of energy

Miguel V. S. Frasson*, Marta C. Gadotti, Selma H. J. Nicola and PlácidoZ. Táboas

Abstract

We consider a linear oscillator with damping combined with an autonomous impulsive condition inspired byMyshkis [3]. We adopt a different approach to extend some of his results and prove that there areasymptotically orbitally stable cycles and stable orbits arising from period doubling bifurcations.

Consider the discontinuous dynamical system on the plane xx arising from the damped linearoscillator

x+ 2↵x+ !

2x = 0,

and suppose that when the total energy reaches some critical level, the velocity undergoes a fixedinstantaneous increase. Without loss of generality we may consider the impulsive system

x = y,

y = �x� 2ay,x

2(t) + y

2(t) = 1 =) (x(t+), y(t+)) = (x(t), y(t) + v)

(0.0.8)

where 0 < a < 1 and v > 0 are parameters. The orbits of the linear system of ordinary equations spiralsclockwise about the origin with forward t, with (x(t), y(t)) ! 0 as t ! 1 and |(x(t), y(t))| ! 1 ast ! �1. The impulse condition depends only in the current state. We have therefora a autonomousimpulsive system.

Periodic solutions of (0.0.8) are called cycles and were studied in [3]. A simple cycle has just oneinstant of impulse within a minimal period. A simple cycle z(t) = (x(t), y(t)) is positive if x(t) > 0, 8t.The value � over which the impulse occurs is called a vertex. A global solution u of (0.0.8) is orbitallystable, (resp. orbitally asymptotically stable or orbitally unstable) if its orbit � = {u(t) | �1 < t < 1}is stable (resp. asymptotically stable or unstable) as a set. We identify S

1 with the real line thoughthe usual parametrization ✓ 7! e

i✓ without further comments.

Results

ICMC/USP São Carlos-SP, Brazil, [email protected]

Page 34: Strong solutions of abstract fractional differential equations

32

Proposition 0.1 (Existence of simple cycles) Fix 0 < a < 1. For each � 2 [�2⇡, 0) there existsa sequence (v

n

), n > 0 with v

n

> 0 such that (0.0.8) with v = v

n

has a simple cycle z(t) withvertex � = z(0). The simple cycles are distiguished by their indexes. Let v⇤

= v0. Furthermore if�3⇡/2 < � < 0, (respectively if �2⇡ 6 � 6 �3⇡/2) then we have cycle have minimal indexes forv = v

⇤�

, that is, ` = 0 (respectively ` = 1).

Theorem 0.2 A cycle � of (0.0.8) with vertex � 2 [�⇡, 0) given by Proposition 0.1 is orbitally unstablefor |�| sufficiently small and orbitally asymptotically stable for � in a neighborhood of �⇡/2.

Theorem 0.3 For a > 0 sufficiently small, there exists �⇤ such that for � < �

⇤ we have that the simplecycle of (0.0.8) with v = v

⇤�

is orbitally stable and as v crosses the bifurcation value v

⇤�

⇤ the cyclesundergo a period doubling bifurcation, that is, a branch of orbitally stable non-simple cycles arises withthe period of these cycles tending to the double of the simple cycle of v = v

⇤�

⇤ as v ! v

⇤�

⇤+.

Bibliography

[1] Frasson, M.V.S. & Gadotti, M.C. & Nicola, S.H.J. & Táboas, P.Z – Cycles byinteraction of damping and jumps of energy, 2014, preprint.

[2] M. Gadotti and P. Táboas, Oscillations of planar impulsive delay differential equations,Funkcialaj Ekvacioj, 48 (2005), pp. 33–47.

[3] Myshkis, A – On autonomous self-supporting impulsive-continuous system, World Sc. Series inApplied An.; Dynam. Syst. Appl., 4 (1995), pp. 541–548.

Page 35: Strong solutions of abstract fractional differential equations

33

Dominant Solutions of Delay Differential Equations

István Györi

Abstract

In this talk, we describe several situations in which all solutions of a delay differential equation canasymptotically be characterized by appropriate "dominant" solutions. The class of equations includelinear autonomous equations, quasilinear equations and nonautonomous equations with small delays.This is a joint work with my colleagues Ferenc Hartung and Mihály Pituk (University of Pannonia,Hungary).

Bibliography

[1] I. Györi and F. Hartung. Asymptotically Exponential Solutions in Nonlinear Integral and DifferentialEquations. J. Differential Equations, 249 (2010), pp. 1322–1352.

[2] I. Györi and M. Pituk. Asymptotically Ordinary Dealy Differential Equations. Func. Diff. Equa.,12 (2005), pp. 187–208.

Partially supported by Hungarian National Foundation for Scientific Research (OTKA) Grant No. K101217,Departament of Mathematics, University of Pannonia, Veszprém, Hungary, e-mail: [email protected]

Page 36: Strong solutions of abstract fractional differential equations

34

Second Order Abstract Neutral Functional DifferentialEquations

Hernán R. Henríquez* and Claudio Cuevas

Abstract

In this paper we are concerned with a class of second order abstract neutral functional differential equationswith finite delay in a Banach space. We establish the existence of mild and classical solutions for the nonlinear

equation, and we show that the map defined by the mild solutions of the linear equation is a stronglycontinuous semigroup of bounded linear operators on an appropriate space. We use this semigroup to establish

a variation of constants formula to solve the inhomogeneous linear equation.

IntroductionThe aim of this work is to develop the basic theory for a class of second-order abstract neutral

functional differential equations. In this work, X denotes a Banach space endowed with a norm k ·k. Moreover, for a fixed constant r > 0 that represents the delay of the equation, we denote byC([�r, 0], X) the space of continuous functions from [�r, 0] into X provided with the norm of uniformconvergence. We are concerned with the the semilinear abstract Cauchy problem

d

2

dt

2D(x

t

) = AD(xt

) + f(t, xt

, x

0t

), t � 0, (0.0.9)

x0 = '

0, x

00 =

0. (0.0.10)

where x(t) 2 X, the function x

t

: [�r, 0] ! X, that denotes the segment of x(·) at t, is given byx

t

(✓) = x(t + ✓). We assume that D : C([�r, 0], X) ! X is a bounded linear map, and f is anappropriate X-valued function.

ResultsTo study problem (0.0.9)-(0.0.10) we assume that A : D(A) ✓ X ! X is the infinitesimal generator

of a cosine function of bounded linear operators (C(t))t2R on X, with associated sine function S(t),

D : C([�r, 0], X) ! X is a bounded linear map, and f : I ⇥ C([�r, 0], X)⇥ C([�r, 0], X) ! X is afunction that satisfies the Carathéodory conditions. We assume that

D(') = '(0)� P ('), ' 2 C([�r, 0], X),

Partially supported by CONICYT, under Grant FONDECYT 1130144 and DICYT-USACH, Department ofMathematics, University of Santiago-USACH, Santiago, Chile, e-mail: [email protected]

Page 37: Strong solutions of abstract fractional differential equations

35

where P : C([�r, 0], X) ! X is a bounded linear map defined by

P (') =

Z 0

�r

[d✓

µ(✓)]'(✓), ' 2 C([�r, 0], X),

where µ : [�r, 0] ! L(X) is a map of bounded variation and non-atomic at zero.In this general framework, and assuming that the function f has different properties, we show that

the problem (0.0.9)-(0.0.10) admits a solution. We distinguish between mild solutions and classicalsolutions. In particular, we establish the linear equation

d

2

dt

2D(x

t

) = AD(xt

) + ⇤1(xt

) + ⇤2(x0t

) + h(t), t � 0, (0.0.11)

with initial condition (0.0.10), where ⇤1,⇤2 : C([�r, 0], X) ! X are bounded linear maps, and

h : [0,1) ! X is a locally integrable function, '0 2 C

1, 0 =d

d✓

'

0 and D('0) 2 E, admits a uniquesolution. We introduce the space

C

1D

= {' 2 C

1([�r, 0], X) : D(') 2 E}

provided with the norm

k|'k| = kD(')kE

+ k'k1 + k'0k1, ' 2 C

1D

,

where E is the Kisyński space. Initially we consider the homogeneous case, i. e. we take h(t) = 0 fort � 0. Let '0 2 C

1D

and x(·,'0) be the mild solution of problem (0.0.11)-(0.0.10). We define the map

U(t)'0 = x

t

(·,'0), t � 0.

Theorem 0.4 Under the above conditions, the family (U(t))t�0 is a strongly continuous semigroup of

bounded linear operators on C

1D

.

Using the semigroup U(t) we establish a type of variation of constant formula to solve the nonhomo-geneous problem (0.0.11)-(0.0.10). We define the bounded linear operator V (t) : C1

D

! C([�r, 0], X)by

V (t)'0 = v

t

, t � 0,

where v(t) = u

0(t) and u

t

= U(t)'0.

Corollary 0.5 Under the above conditions, let '0 2 C

1D

and 0 = d

d✓

'

0. If u(·) is the mild solutionof problem (0.0.11)-(0.0.10), and v = u

0, then

u

t

= U(t)'0 + lim�!1

Zt

0U(t� s)�[e�✓�(�)�1

h(s)]ds

v

t

= V (t)'0 + lim�!1

Zt

0V (t� s)�[e�✓�(�)�1

h(s)]ds.

For a proof of these results, we refer the reader to [1].

Page 38: Strong solutions of abstract fractional differential equations

36

Bibliography

[1] H. R. Henríquez, C. Cuevas, Second order abstract neutral functional differential equations, pre-print, 2014.

Page 39: Strong solutions of abstract fractional differential equations

37

A unified approach to discrete fractional calculus andapplications

Sebastián Calzadillas, Carlos Lizama* and Jaqueline G. Mesquita

Abstract

We present a unified treatment of several existing definitions of discrete fractional sums and differencesby means of the use of the operator of translation. We then formulate a standard notion of fractionalsum by finite convolution, and we state their main properties in the space of vector-valued sequencess(N0;X) where X is a Banach space. We introduce the notion of generalized Mittag-Leffler sequence bymeans of the complex inversion of the Z-transform, and use it to solve, for � 2 C the non-homogeneousproblem

�↵

u(n) = �u(n) + f(n)

where f 2 s(N0;X) and 0 < ↵ 2. Here, the fractional difference is defined both as the discreteanalogous to the Caputo fractional derivative as well as the Riemann-Liouville. We recover, improveand extend several notions and applications in the existing literature on the subject.

Keywords: Fractional sums; fractional differences; Z-transform; fractional difference equations;convolution; translation

MSC 2010 subject classification: 39A13; 34A08; 44A15; 44A35

Partially supported by FONDECYT grant number 1140258, Universidad de Santiago de Chile, Facultad deCiencias, Departamento de Matemática y Ciencia de la Computación, Casilla 307, Correo 2, Santiago, CHILE,e-mail: [email protected]

Page 40: Strong solutions of abstract fractional differential equations

38

Almost automorphic solutions for evolutions equations

Arlucio Viana, Bruno de Andrade and Eder Mateus*

Abstract

In recent years, the theory of almost automorphic functions has been developed extensively and con-sequently there has been a considerable interest in the existence of almost automorphic solutions ofvarious kinds of evolution equations, see for instance [4, 6, 8, 10] and the references therein. In thiswork, we study existence and uniqueness of almost automorphic mild solutions for a class of abstractdifferential equations described in the form

u

0(t) = Au(t) + f(t, u(t)), t 2 R, (0.0.12)

where A is an unbounded linear operator, assumed to be Hille-Yosida of negative type, with domainD(A) not necessarily dense on some Banach space X, f : R ⇥ X0 ! X is a continuous functionand X0 = D(A). We ensure sufficient conditions for existence and uniqueness of almost autmorphicsolutions to (0.0.12) with Stepanov almost autmorphic conditions. We apply our abstract results in theframework of transmission problems for the Bernoulli-Euler plate equation and heat conduction theory.

Bibliography

[1] B. Amir and L. Maniar, Composition of pseudo-almost periodic functions and Cauchy problemswith operator of non dense domain, Ann. Math. Blaise Pascal, 6 (1), (1999), 1-11.

[2] K. Ammari and G. Vodev, Boundary stabilization of the transmission problem for the Bernoulli-Euler plate equation, Cubo, 11 (2009), 39-49.

[3] S. Bochner, Continuous mapping of almost automorphic and almost periodic functions, Proc. nat.Acad. Sci. USA, 52 (1964), 907-910.

[4] S. Boulite, L. Maniar and G. N’guérékata. Almost automorphic solutions for hyperbolic semilinearevolution equations. Semigroup Forum 71 (2) (2005), 231-240.

[5] K.J. Engel and R. Nagel, One-parameter semigroups for linear evolution equations, in: GraduateTexts in Mathematics, Springer-Verlag, 2001, p. 194.

e-mail: [email protected],Departamento de Matematica-DMAI, Universidade Federal de Sergipe, Itaba-iana, Brasil.

Page 41: Strong solutions of abstract fractional differential equations

39

[6] G. A. Goldstein and G. M. N’guerekata, Almost automorphic solutions of semilinear evolutionequations, Pro c. Amer. Math. Soc. 133(8) (2005), 2401-2408.

[7] J. Liang, J. Zhang and T.J. Xiao, Composition of pseudo almost automorphic and asymptoticallyalmost automorphic functions, J. Math. Anal. Appl. 340 (2008), 1493-1499.

[8] J. Liu and X. Song, Almost automorphic and weighted pseudo almost automorphic solutions ofsemilinear evolution equations, Journal of Functional Analysis, 258 (2010), 196-207.

[9] R. Nagel and E. Sinestrari, Inhomogeneous Volterra Integrodifferential Equations for Hille-YosidaOperators, in: Lectures Notes Pure Appl. Math., Marcel Dekker, 1994, p. 150.

[10] G. M. N’guerekata. Almost Automorphic and Almost Periodic Functions in Abstract Spaces,KluwerAcad/Plenum, New York-Boston-Moscow-London, 2001.

[11] G. M. N’guerekata and A. Pankov, Stepanov-like almost automorphic functions and monotoneevolution equations, Nonlinear Analysis, 68 (2008), 2658-2667.

[12] A. Pazy, Semigroups of linear operators and applications to partial differential equations, Spinger,New York, 1983.

[13] G. da Prato and E. Sinestrari, Differential operators with non dense domain. Ann. Scuola Norm.Sup. Pisa Cl. Sci. (4) 14 (1989), no. 2, 285-344.

[14] G. da Prato and P. Grisvard, On extrapolation spaces. Atti Accad. Naz. Lincei Rend. Cl. Sci. Fis.Mat. Natur. (8) 72 (1982), no. 6, 330-332.

Page 42: Strong solutions of abstract fractional differential equations

40

Continuous solutions for divergence-type PDEs

Laurent Moonens

Abstract

It follows from a famous work by J. Bourgain and H. Brezis [1] that given F 2 L

n whose integralvanishes on the n-dimensional torus, there exists a continuous vector field v satisfying div v = F . Weshall review some necessary and sufficient conditions (obtained by T. De Pauw and W.F. Pfeffer [2]) ona distribution F in order that the equation div v = F has a continuous solution, and provide a similarresult on the existence of continuous solutions to the equation d! = F in the class of m-differentialforms (the latter part being a joint work with T. De Pauw and W.F. Pfeffer [3]).

Bibliography

[1] J. Bourgain and H. Brezis, On the equation div Y = f and application to control of phases, J.Amer. Math. Soc., 16 (2003), pp. 393-426.

[2] T. De Pauw and W.F. Pfeffer. Distributions for which div v = F has a continuous solution, Comm.Pure Appl. Math., 61(2), 2008, pp. 230-260.

[3] T. De Pauw, L. Moonens and W.F. Pfeffer. Charges in middle dimensions. J. Math. Pures Appl.,92(1), 2009, pp. 86-112.

Partially supported by ANR Project “Geometrya”, Laboratoire de Mathématique, Université Paris-Sud, 91405Orsay Cedex, France, e-mail: [email protected]

Page 43: Strong solutions of abstract fractional differential equations

41

Dengue: Model with human mobility

S. Oliva

Abstract

We present recent models dealing with the spread of infectious diseases, we start with the simpleSIS model and build it up to include human mobility. The understanding of human mobility and thedevelopment of qualitative and quantitative models are key to understand human infectious diseases.We fix , as an example, Dengue. We try to connect several dynamic models, from systems of ordinarydifferential equations to evolution equations with fractional powers of the Laplacian.

Departamento de Matemática Aplicada, Universidade de São Paulo, São Paulo, Brasil

Page 44: Strong solutions of abstract fractional differential equations

42

Dynamics of parabolic equations governed by the p-laplacianon unbounded thin domains

Ricardo Parreira da Silva

Abstract

We consider the asymptotic behavior of quasilinear parabolic equations posed in a family of unboundeddomains that degenerates onto a lower dimensional set. Considering an auxiliary family of weightedSobolev spaces we show the existence of global attractors and we analyze convergence properties of thesolutions as well of the attractors.

Bibliography

[1] Silva, R.P. Behavior of the p-laplacian on thin domains, International Journal of Differential Equa-tions, v. 2013, 210270, (2013).

[2] Silva, R.P. Upper semicontinuity of global attractors for parabolic equations governed by the p-laplacian on unbounded thin domains, submitted, (2013), (http://arxiv.org/abs/1311.3649)

Department of Mathematics, University of the State of Sao Paulo, Rio Claro, Brazil

Page 45: Strong solutions of abstract fractional differential equations

43

Thin domains and reactions concentrated on boundary

Marcone C. Pereira

Abstract

In this talk we discuss the behavior of a family of steady state solutions of a semilinear reaction-diffusionequation with homogeneous Neumann boundary condition posed in a two-dimensional thin domainwhen some reaction terms of the problem are concentrated in a narrow oscillating neighborhood of theboundary. We assume that the domain, and so, the oscillating neighborhood, degenerates to an intervalas a small parameter ✏ goes to zero.

Our main goal here is to show that this family of solutions converges to the solutions of an one-dimensional limit equation capturing the geometry and oscillatory behavior of the open sets where theproblem is established.

Indeed, we introduce a model combining these both singular situations in a more general featuring.Here we adapt methods and techniques developed in [1, 2, 3] and [4] dealing with a semilinear ellipticequation.

Bibliography

[1] J. K. Hale and G. Raugel, Reaction-diffusion equation on thin domains, J. Math. Pures et Appl.(9) 71 (1) (1992) 33-95.

[2] J. M. Arrieta, A. Jiménez-Casas and A. Rodríguez-Bernal, Flux terms and Robin boundary con-ditions as limit of reactions and potentials concentrating at the boundary, Revista MatemáticaIberoamericana 24 (1) (2008) 183-211.

[3] G. S. Aragão, A. L. Pereira and M. C. Pereira, A nonlinear elliptic problem with terms concentratingin the boundary, Math. Methods Appl. Sci. 35 (9) (2012) 1110-1116.

[4] J. M. Arrieta and S. M. Bruschi, Rapidly varying boundaries in equations with nonlinear boundaryconditions. The case of a Lipschitz deformation, Math. Models and Meth. in Appl. Sciences 17(10) (2007) 1555-1585.

Partially supported by CNPq 302847/2011-1 and 471210/2013-7, FAPESP 2008/53094-4 and 2013/22275-1, CAPES DGU 127/07, Brazil, Escola de Artes, Ciências e Humanidades, Universidade de São Paulo, São Paulo,Brazil, e-mail: [email protected]

Page 46: Strong solutions of abstract fractional differential equations

44

On a functional equation associated with a first orderproblem with finite delay

Carlos Lizama and Felipe Poblete*

Abstract

In this work, we study the functional equation

G(s)(1 ⇤G)(t)� (1 ⇤G)(t)� (1 ⇤ FGt)(1 ⇤G)(s) = G(t)(1 ⇤G)(s)� (1 ⇤G)(s)� (1 ⇤ FGs)(1 ⇤G)(t),

for bounded operator valued functions G(t) defined on the positive real line R+. We show that, under somenatural assumptions, the existence of solution of the functional equation characterizes the well posedness on

C

1(R+;X), in a mild sense, the following problem of first order with finite delay on a Banach space X

(I) :=

8><

>:

u

0(t) = Au(t) + Fut t > 0

u(0) = x

u(t) = �(t) �r < t < 0,

Functional equations arise in most parts of mathematics. Well known examples are Cauchy’sequation, the functional equations for the Riemann zeta function, the equation for entropy and numerousequations in combinatorics. Still other examples arise in probability theory, geometry and operator theory[1].

The theory of functional equations for bounded operators, emerged after the book of Hille andPhillips [2] in 1957. A strongly continuous semigroup T (t) of bounded and linear operators on aBanach space X, is defined by means of Abel’s functional equation:

⇢T (t)T (s) = T (t+ s), t � 0,T (0) = I,

which, in turn, characterizes the well posedness of the abstract Cauchy problem of first order:⇢

u

0(t) = Au(t), t � 0;u(0) = u0,

Departament of Mathematics, Universidad Austral de Chile, Puerto Montt, Chile, e-mail:[email protected]

Page 47: Strong solutions of abstract fractional differential equations

45

where Ax = limt!0+

T (t)x� x

t

is defined on the domain D(A) := {x 2 X : limt!0+

T (t)x� x

t

exists in X}. In 1966, Sova [5] introduces the concept of strongly continuous cosine operator functions,C(t), by means of D’Alembert’s functional equation:

⇢C(t+ s) + C(t� s) = 2C(t)C(s), t, s 2 R;C(0) = I.

which characterizes the well posedness of the abstract Cauchy problem of second order:8<

:

u

00(t) = Au(t), t � 0;u(0) = u0;u

0(0) = u1.

where now Ax = 2 limt!0+

C(t)x� x

t

2is defined on D(A) := {x 2 X : lim

t!0+

C(t)x� x

t

2exists in X}.

Let A be a linear operator defined on a Banach space X. In [4] Prüss proved that the Volterra equationof scalar type:

u(t) =

Zt

0a(t� s)Au(s)ds+ f(t), (0.0.13)

is well posed if and only if it admits a resolvent family, i.e. a strongly continuous family S(t) of boundedand linear operators which commutes with A and satisfies the so called resolvent equation [4, Definition1.3]:

S(t)x = x+

Zt

0a(t� s)AS(s)xds, t � 0, x 2 X.

Resolvent families of operators have been known for a long time. They have many applications inthe study of abstract differential and integral equations. We note that choosing the kernels a(t) ⌘ 1and a(t) = t corresponds to the above mentioned cases of strongly continuous semigroups and cosineoperator functions, respectively.

Recently, the authors in [3] studied a commutative and one parameter family of strongly continuousoperators R

a,k

(t), depending on two scalar kernels a(t) and k(t), satisfying R

a,k

(0) = k(0)I and thefunctional equation

R

a,k

(s)(a⇤Ra,k

)(t)�(a⇤Ra,k

)(s)Ra,k

(t) = k(s)(a⇤Ra,k

)(t)�k(t)(a⇤Ra,k

)(s), t, s � 0. (0.0.14)

In case k(t) ⌘ 1 and a(t) positive, one of their main results in [3] show that the functional equation(0.0.14) characterizes a resolvent family, and therefore the well-posedness of the Volterra equation(0.0.16). Moreover, the representation of the generator is given by

Ax = limt!0+

R

a,1(t)x� x

Zt

0a(s)ds

, (0.0.15)

Page 48: Strong solutions of abstract fractional differential equations

46

for all x 2 D(A) := {x 2 X : limt!0+

R

a,1(t)x� x

(1 ⇤ a)(t) exists in X}, which includes the case of semigroups,

cosine operator functions and resolvent families for a(t) = g

(t),↵ > 0.

Following the above ideas, in this work we will connect the existence of a conmmutative of stronglycontinuous family of operators {G(t)}

t�0 defined by 0 for �r t < 0 which satisfies the functionalequation (FE)

G(s)(1 ⇤G)(t)� (1 ⇤G)(t)� (1 ⇤FG

t

)(1 ⇤G)(s) = G(t)(1 ⇤G)(s)� (1 ⇤G)(s)� (1 ⇤FG

s

)(1 ⇤G)(t)

for all s, t � 0. with the well posedness on C

1(R+;X), in a mild sense, for the following problem offirst order with finite delay on a Banach space X

(I) :=

8<

:

u

0(t) = Au(t) + Fu

t

t > 0u(0) = x

u(t) = �(t) �r < t < 0,

where the initial conditions x 2 D(A) and � 2 C([�r, 0], D(A)). Here, A is a closed operator withdomain D(A) ✓ X and F is a bounded linear map defined on an appropriate space.

To conclude the above mentioned, we motivate by using the Laplace transform, one definition ofa retarded resolvent family {G(t)}

t�0 and their relation with the well posedness of the problem (I) ina mild sense. More precisely, we say that a strongly continuous family of linear and bounded operators{G(t)}

t�0, defined by 0 for �r t < 0, is a retarded resolvent with delay F if the following propertieshold:

(i) G(0) = I;

(ii) G(t)x 2 D(A) and G(t)Ax = AG(t)x for all x 2 D(A) and t � 0;

(iii) G(t)x = x+

Zt

0AG(s)xds+

Zt

0FG

s

xds, t � 0, x 2 D(A).

In such case we called A the generator of the retarded resolvent family {G(t)}t�0 with delay F . Finally,

we will give sufficient and necessary conditions on the retarded resolvent family {G(t)}t�0 to ensure

that (FE) is satisfied. Here

D(A) :=

⇢x 2 X : lim

t!0+

G(t)x� x� (1 ⇤ FG

t

)x

t

exists

andAx := lim

t!0+

G(t)x� x� (1 ⇤ FG

t

)x

t

x 2 D(A).

Bibliography

[1] J. Aczél. On history, applications and theory of functional equations. Functional equations: History,applications and theory, 312, Math. Appl., Reidel, Dordrecht, 1984.

Page 49: Strong solutions of abstract fractional differential equations

47

[2] E. Hille, R.S. Phillips.Functional analysis and semi-groups. American Mathematical Society Collo-quium Publications, 31. American Mathematical Society, Providence, R. I., 1957.

[3] C. Lizama, F. Poblete, On a functional equation associated with (a, k)-regularized resolvent fam-ilies. Abstr. Appl. Anal.23 pp. 2012

[4] J. Prüss. Evolutionary Integral Equations and Applications. Monographs Math., 87, BirkhäuserVerlag, 1993.

[5] M. Sova.Cosine operator functions. Rozprawy Mat. 49 (1966), 1-47.

Page 50: Strong solutions of abstract fractional differential equations

48

Hölder continuous solutions for a fractional differentialequations

Rodrigo Ponce

Abstract

We study the existence and uniqueness of solutions of an abstract fractional differential equation in Hölderspaces.

Using some results of Arendt, Batty and Bu [1], we study the existence and uniqueness of Höldercontinuous solutions to equation

D

u(t) = Au(t) + f(t), t 2 R, (0.0.16)

where A is a closed linear operator defined on a Banach space X, f 2 C

↵(R;X), 0 < ↵ < 1, and thefractional derivative for � > 0 is taken in the sense of Caputo. Existence of Hölder continuous solutionsto fractional differential equations in the form of (0.0.16) have been studied for example, by Clement,Gripenberg and Londen using the method of the sum of Da Prato and Grisvard [2].

For � > 0, let C

↵,�(R, X) be the Banach space of all u 2 C

n(R, X), n = d�e, such that D

u

exists and belongs to C

↵(R, X) equipped with the norm

kukC

↵,� = kD�

ukC

↵ +nX

j=1

kD��j

u(0)k.

Definition 0.6 We say that the equation (0.0.16) is C

-well posed if, for each f 2 C

↵(R;X), thereexists a unique function u 2 C

↵(R; [D(A)])\C↵,�(R;X), and the equation (0.0.16) holds for all t 2 R.

The following Theorem is the main result of this talk. Its prove is based in the theory of C

↵-multipliers introduced in [1].

Theorem 0.7 Let A : D(A) ✓ X ! X, be a linear closed operator defined on Banach space X.Then,the following assertions are equivalent

(i) The equation (0.0.16) is C

↵-well posed;(ii) (i⌘)� 2 ⇢(A) for all ⌘ 2 R and sup

⌘2R

���(i⌘)��(i⌘)� �A

��1��� < 1.

Partially supported by Fondecyt Iniciación #11130619, Instituto de Matemática y Física, Universidad deTalca, Talca, Chile, e-mail: [email protected]

Page 51: Strong solutions of abstract fractional differential equations

49

Applying the results in [4], we study the existence of Hölder continuous solutions to problem⇢

D

u(t, x) = �u(t, x) + f(t, x), t 2 R,u = 0 in R⇥ @⌦,

(0.0.17)

where 0 < � < 1, ⌦ is a bounded domain in Rn with a smooth boundary @⌦, introduced in physics byNigmatullin [3] to describe diffusion in special types of porous media.

Bibliography

[1] W. Arendt, C. Batty, S. Bu: Fourier multipliers for Hölder continuous functions and maximalregularity, Studia Math., 160, 23-51 (2004).

[2] Ph. Clément, G. Gripenberg, S. Londen, Hölder regularity for a linear fractional evolution equation,in Topics in nonlinear analysis, 69-82, Progr. Nonlinear Differential Equations Appl., 35, Birkhäuser,Basel, 1999.

[3] R. Nigmatullin, The realization of the generalized transfer equation in a medium with fractalgeometry, Phys. Stat. Sol. B 133 (1986), 425-230.

[4] R. Ponce, Hölder continuous solutions for fractional differential equations and maximal regularity,J. of Differential Equations, 255 (2013), 3284-3304.

Page 52: Strong solutions of abstract fractional differential equations

50

Strong solutions of abstract fractional differential equations

Juan C. Pozo*, Hernán R. Henríquez and Verónica Poblete

Abstract

In this work we establish the existence of strong solutions for abstract semi-linear fractional differentialequations. We consider the autonomous and non-autonomous case. Our approach relies on the existence of a

resolvent family with bounded semivariation for the homogeneous autonomous equation, and appropriateconditions on the forcing function.

In this work we study the existence of strong solution of abstract Cauchy problem of fractionalorder.

Let X be a Banach space and suppose that A(t) : D(A(t)) ✓ X ! X are closed linear operatorswith domain D(A(t)) = D for all t 2 [0, a], a > 0. We consider the following fractional differentialequation

D

t

u(t) = A(t)u(t) + f(t, u(t)), t 2 [0, a],u(0) = x,

u

0(0) = y.

9=

; (0.0.18)

where ↵ 2 (1, 2), and the fractional derivative D

t

is understood in the Caputo sense.If A(t) = A for all t 2 [0, a], the problem (0.0.18) is known in the literature by fractional abstract

Cauchy problem associated to A of order ↵. The existence of solutions of this problem is stronglyrelated with the concept of ↵-resolvent family {S

(t)}t>0, developed by Bazhlekova [2]. In fact, the

fractional differential equation (0.0.18) is well posed if and only if A is the infinitesimal generator of an↵-resolvent family {S

(t)}t>0. Assuming that A is the infinitesimal generator of an ↵-resolvent family

{S↵

(t)}t>0, is well known that a strong solution of the problem (0.0.18) verifies the formula

u(t) = S

(t)x+ (g1 ⇤ S↵

)(t)y + (g↵�1 ⇤ S↵

⇤ f)(t), t 2 [0, a], (0.0.19)

However, a continuous function u : [0, a] ! X described by the preceding formula is not necessarilya strong solution of problem (0.0.18). This fact motivates the introduction of a weaker concept ofsolution of the abstract fractional Cauchy problem. A continuous function u : [0, a] ! X is called mildsolution of the abstract fractional differential Cauchy problem if u satisfies the formula (0.0.19).

Partially supported by FONDECYT 3140103, e-mail: [email protected] Departamento de Matemáticas,Universidad de Santiago de Chile

Page 53: Strong solutions of abstract fractional differential equations

51

The existence of strong solutions of the problem (0.0.18) when f 2 C([0, a];X) has been analyzedby F. Li and M. Li ([5]). Specifically, they show that for all f 2 C([0, a];X) the corresponding mildsolution is a strong solution of the problem (0.0.18) if and only if the ↵-resolvent family has boundedsemivariation in the interval [0, a]. This result can also be derived as a particular case of the theorydeveloped by H. Thieme [6]. However, in both works, the authors do not exhibit an explicit example ofan unbounded operator A that generates an ↵-resolvent family of bounded semivariation. This subjectwas originally studied for the abstract Cauchy problem of first order in [1, 4, 7]. These authors establishthat there are C0-semigroups of bounded semivariation and generated by unbounded operators. Later,this same topic for the abstract Cauchy problem of second order was studied in [3]. In this case,the authors establish that a cosine function with bounded semivariation can only be generated by abounded operator. It remains open to decide if there exist ↵-resolvent families of bounded semivariationfor 1 < ↵ < 2. In our main results we construct a concrete example of an ↵-resolvent family of boundedsemivariation where its infinitesimal generator is an unbounded operator. Moreover, we will establishthe existence of strong solutions of problem (0.0.18) if f is a X�valued continuous function on [0, a].The results are based on the properties of ↵-resolvent families of bounded semivariation and appropriateconditions on f . We apply our results to study semilinear and non-autonomous fractional differentialequations.

Bibliography

[1] J. B. Baillon, Caractére borné de certains générateurs de semi-groupes linéaires dans lesespaces de Banach, C. R. Acad. Sci. Paris 290 (1980), 757-760.

[2] E. G. Bazhlekova, Fractional Evolution Equations in Banach Spaces, Eindhoven University ofTechnology, Eindhoven, 2001. Dissertation.

[3] D. Chyan, S. Shaw, S. Piskarev, On maximal regularity and semivariation of cosine operatorfunctions, J. London Mathematical Society 59 (3) (1999), 1023-1032.

[4] C. S. Hönig, Semigroups and semivariation, Proc. 14� Seminário Brasileiro de Análise, 1981,pp. 185-193.

[5] F. Li, M. Li, On maximal regularity and semivariation of ↵-times resolvent families, Advancesin Pure Mathematics 3 (2013), 680-684.

[6] H. Thieme, Differentiability of convolutions, integrated semigroups of bounded semi-variation,and the inhomogeneous Cauchy problem, J. Evol. Equ. 8 (2) (2008), 283-305.

[7] C. C. Travis, Differentiability of weak solutions to an abstract inhomogeneous differentialequation, Proc. Amer. Math. Soc. 82 (3) (1981), 425-430.

Page 54: Strong solutions of abstract fractional differential equations

52

Existence of solutions for a fractional neutralintegro-differential equation with unbounded delay

José Paulo Carvalho dos Santos

Abstract

In this talk, we study the existence of mild solutions for the neutral fractional integral evolutionaryequation

D

t

(x(t) + f(t, xt

)) = Ax(t) +

Zt

0B(t� s)x(s)ds+ g(t, x

t

), t > 0,

x0 = ', x

0(0) = 0,

where ↵ 2 (1, 2); A, (B(t))t�0 are closed linear operators defined on a common domain which is dense

in a Banach space X, D↵

t

h(t) represent the Caputo derivative of ↵ > 0 defined by

D

t

h(t) :=

Zt

0g

n�↵

(t� s)d

n

ds

n

h(s)ds,

where n is the smallest integer greater than or equal to ↵ and g

(t) := t

��1

�(�) , t > 0,� � 0. The historyx

t

: (�1, 0] ! X given by x

t

(✓) = x(t+ ✓) belongs to some abstract phase space B defined axiomati-cally and f, g : I⇥B ! X are appropriate functions. This talk is based on work with Bruno de Andrade.

Partially supported by FAPEMIG/Brazil, Instituto de Ciências Exatas, Universidade Federal de Alfenas,Alfenas, Brazil, e-mail: [email protected]

Page 55: Strong solutions of abstract fractional differential equations

53

On evolutionary differential equations with state-dependentdelay

Giovana Siracusa* and Bruno de Andrade

Abstract

The study of the topological structure of solution set of differential equations dates back to the beginningof the 20’s when H. Kneser (see [7]) proved that the Peano existence theorem could be reformulatedto ensure that the solution set of a ODE is, beyond nonempty, a compact and connected set. Thisproperty is known in the literature as the Kneser’s property. Almost 20 years later, N. Aronszajn (see[4]) improved the Knenser theorem showing that the set of all solutions of a ODE is an R

-set, thatis, an intersection of a decreasing sequence of compact absolute retracts sets. Evidently the Aronszajntheorem had a large impact on qualitative theory of differential equations and due to this the study oftopological structure of the solution set of differential equations has drawn attention of researchers inthe last years (see for instance [1, 2, 3, 5, 6, 8] and references therein).

In this work we study some topological properties of the solution set of differential equation withstate-dependent delay

⇢u

0(t) = Au(t) + f

�t, u

⇢(t,ut)

�, t 2 [0, b],

u0 = ' 2 B,

(0.0.20)

where A : D(A) ⇢ X ! X is infinitesimal generator of the semigroup of linear operators {S(t); t > 0}on a Banach space X and the history x

t

: (�1, 0] ! X, given by

x

t

(✓) = x(t+ ✓),

belongs to phase space B described axiomatically. The functions f : [0, b]⇥B ! X and ⇢ : [0, b]⇥B !(�1, b] are given functions.

Bibliography

[1] J. Andres, G. Gabor, L. Górniewicz, Boundary value problems on infinite intervals, Trans. Amer.Math. Soc., 351, 1999, 4861-4903.

Departamento de Matemática, Universidade Federal de Sergipe, São Cristóvão, Brasil, e-mail:[email protected]

Page 56: Strong solutions of abstract fractional differential equations

54

[2] J. Andres, L. Górniewicz, Topological Fixed Point Principles for Boundary Value Problems, Topol.Fixed Point Theory Appl., Kluwer, Dordrecht, 2003

[3] W. Arendt and J. Prüss, Vector-Valued Tauberian Theorems and Asymptotic Behavior of LinearVolterra Equations, SIAM J. Math. Anal., 23 (1992), 412-448.

[4] N. Aronszajn, Le Correspondant Topologique De L’Unicite Dans La Theorie Des Equations Dif-ferentielles, Ann. Math., 43 (4), 1942, 730-738.

[5] D. Bugajewski and G. N’Guérékata, On the topological structure of almost automorphic and asymp-totically almost automorphic solutions of differential and integral equations in abstract spaces,Nonlinear Anal. 59, 2004, 1333-1345.

[6] L. Górniewicz, Topological structure of solution sets: current results, Arch. Math., 36 (5), 2000,343-382.

[7] H. Kneser, Uber die Losungen eine system gewohnlicher differential Gleichungen, das der lips-chitzchen Bedingung nicht genugt, S. B. Preuss. Akad.Wiss. Phys. Math. Kl. 4, 1923, 171-174.

[8] D. Miklaszewski, The two-point problem for nonlinear ordinary differential equations and differen-tial inclusions, Univ. Iagel. Acta Math., 36, 1998, 127-132.

Page 57: Strong solutions of abstract fractional differential equations

55

On a class of discontinuous dynamical systems

Miguel V. S. Frasson, Marta C. Gadotti, Selma H. J. Nicola andPlácido Z. Táboas*

Abstract

The object of study are the so called impulsive differential equations, where the involved equationis autonomous and the impulses, previously unknown, are given by intrinsec causes. Therefore thewhole system is autonomous and define a discontinuous semi-group. We give some examples showingpeculiarities of these systems and that, even when the involved equations are simple linear equations,they can exhibit interesting dynamics. We present a topological approach to deal with this kind ofproblem.

Departamento de Matemática Aplicada e Estatística, Universidade de São Paulo, São Carlos, Brasil

Page 58: Strong solutions of abstract fractional differential equations

56

Stability results for measure neutral functional differentialequations via GODE

Márcia Federson and Patricia H. Tacuri*

Abstract

We consider a class of measure neutral functional differential equations whose integral form is given by

x(t)� x(0) =

Zt

0f(x

s

, s)dg(s) +

Z 0

�r

d

[µ(t, ✓)]x(t+ ✓)�Z 0

�r

d

[µ(0, ✓)]'(✓)

and we establish stability results using the correspondence between of solutions of this equation andsolutions of a generalized ordinary differential equations. We introduce the concept of regular stabilityof linear operators on a Banach space of Rn-valued regulated functions. We discuss the total stabilityfor a class of measure neutral functional differential equations.

Bibliography

[1] S. M. Afonso; E. M. Bonotto and M. Federson. On the exponential stability of functional differentialequations with impulsive perturbations, Submitted.

[2] M. Federson, M. Frasson, J. Mesquita and P. Tacuri, Measure neutral functional differential equa-tions as generalized ODEs. Submitted.

[3] J. K. Hale, M. A. Cruz Stability of functional differential equations of neutral type. J. DifferentialEquations 7 (1970) 334-355.

[4] Š. Schwabik, Variational stability for generalized ordinary differential equations, Casopis Pest. Mat.109(4), (1984), 389-420

Supported by FAPESP grant 2012/18559-1, Department of Mathematics and Computer Sciences, SãoPaulo State University “Júlio Mesquita Filho”, Presidente Prudente, Brazil, e-mail: [email protected]

Page 59: Strong solutions of abstract fractional differential equations

57

On a class of thermoelastic plates with p-Laplacian

To Fu Ma

Abstract

In recent years the class of vibrating plates with p-Laplacian

u

tt

+�2u��

p

u = {damping and forcing},

defined on bounded domains of Rn, was studied by several authors (see for instance [1,2,3,4] and thereferences therein). The present paper contains a first thermoelastic model of this class of problemsincluding both Fourier and non-Fourier heat laws. We discuss the modeling and the well-posedness ofthe problem.

Bibliography

[1] I. Chueshov and I. Lasiecka, Global attractors for Mindlin-Timoshenko plates and for their Kirchhofflimits, Milan J. Math. 74 (2006) 117-138.

[2] M. A. Jorge Silva and T. F. Ma, Long-time dynamics for a class of Kirchhoff models with memory,J. Math. Phys. 54, 021505 (2013) 15 pp.

[3] Liu Yacheng and Xu Runzhang, A class of fourth order wave equations with dissipative and nonlinearstrain terms, J. Differential Equations 244 (2008) 200-228.

[4] Yang Zhijian, Finite-dimensional attractors for the Kirchhoff models, J. Math. Phys. 51, 092703(2010) 25 pp.

Partially supported by FAPESP, Instituto de Ciências Matemáticas e de Computação, Universidade de SãoPaulo, São Carlos, SP, Brasil, e-mail: [email protected]

Page 60: Strong solutions of abstract fractional differential equations

58

Asymptotically almost automorphic and almost automorphicsolutions of Volterra Integral Equations on time scales

Eduard Toon

Abstract

This is a joint work with Carlos Lizama, Jaqueline G. Mesquita and Rodrigo Ponce. In this work, weinvestigate the existence and uniqueness of almost automorphic solutions of semilinear Volterra IntegralEquation on time scales given by:

u(t) =

Zt

�1a(t,�(s))[u(s) + f(s, u(s))]�s, (0.0.21)

where a : T⇥ T ! Rn⇥n is almost automorphic in both variables and f : T⇥ Rn ! Rn.We also show a characterization of asymptotically almost automorphic solution of the following

semilinear Volterra Integral Equation:

u(t) =

Zt

t0

a(t,�(s))[u(s) + f(s, u(s))]�s, (0.0.22)

with t0 2 T+, t > t0, where a : T+ ⇥ T+ ! Rn⇥n is almost automorphic on both variables andf : T+ ⇥ Rn ! Rn.

Bibliography

[1] M. Bohner and A. Peterson, Dynamic Equations on Time Scales: An Introduction with Applica-tions, Birkhauser, Boston, 2001.

[2] H-S. Ding, T-J. Xiao and J. Liang, Asymptotically almost automorphic solutions for some inte-grodifferential equations with nonlocal initial conditions, J. Math. Anal. Appl. 338 (2008) 141-151.

[3] C. Lizama and J. G. Mesquita, Almost automorphic solutions of dynamic equations on time scales,J. Funct. Analysis, 265 (2013), 2267-2311.

[4] C. Lizama and J. G. Mesquita, Asymptotically almost automorphic solutions of dynamic equationson time scales, submitted.

Departamento de Matemática, Universidade Federal de Juiz de Fora, Juiz de Fora, Brazil, e-mail:[email protected]

Page 61: Strong solutions of abstract fractional differential equations

59

Soluciones Convergentes en Ecuaciones DiferencialesImpulsivas con Avance

Manuel Pinto and Ricardo Torres N.*

Abstract

Las ecuaciones diferenciales con argumento constante a trozos (DEPCAG) tienen soluciones continuasy en los extremos de los intervalos de constancia generan una ley recursiva, una ecuación discreta,ver [9, 6, 7]. Al tener en estos puntos un salto, aparecen las ecuaciones diferenciales con argumentoconstante a trozos (IDEPCAG) con impulsos. Este tipo de ecuaciones corresponden al tipo híbridas, yaque combinan propiedades tanto de ecuaciones discretas como de continuas. Ver [1, 2, 8, 9]

En esta ocasión mostraremos la existencia y unicidad de soluciones del sistema impulsivo con argumentoconstante a trozos �

X

0(t) = A(t)X(t) +B(t)X(�(t)) + F (t), t 6= t

i

�X(t)|t=ti = C

i

X(t�i

) +D

i

, t = t

i

ayudados del análisis de los sistemas

X

0(t) = A(t)X(t), t 6= t

i

�X(t)|t=ti = C

i

X(t�i

), t = t

i

y

X

0(t) = A(t)X(t) +B(t)X(�(t)), t 6= t

i

�X(t)|t=ti = C

i

X(t�i

) +D

i

, t = t

i

con A(t), B(t) y F (t) funciones continuas a trozos localmente integrables, (ti

)i2N partición del intervalo

[t0,1) con t

i

< t

i+1, 8i 2 N, en donde se considera un avance discontinuo

�(t) = t

i+1, si t 2 [ti

, t

i+1], 8i 2 N.

En nuestros resultados tiene un rol fundamental la invertibilidad de la matriz

J(t, ti

) = I +

Zt

ti

�(ti

, s)B(s)ds, 8t 2 [ti

, t

i+1], 8i 2 Z

Partially supported by Fondecyt 1120709. Departamento de Matemática. Facultad de Ciencias, Universidadde Chile. Santiago, Chile, e-mail: [email protected]

Page 62: Strong solutions of abstract fractional differential equations

60

con � matriz fundamental del sistema homogéneo asociado.

Las ecuaciones discretas asociadas juegan un gran papel, ya que son una aproximación a las solucionesde la ecuación a tiempo continuo. También son ecuaciones con avance y sus soluciones convergentes,ver [2, 3]. La ecuacion diferencial es una aproximación de la ecuación diferencial ordinaria, en cuanto

� = supi2N

|ti+1 � t

i

| ,

sea pequeño. Ver [4, 5]

Se obtiene la fórmula de variación de parámetros asociada, cuya matriz fundamental es particularmenteespecial.Probamos que si los coeficientes son integrables, entonces la soluciones son convergentes.

Bibliography

[1] M. Akhmet: Nonlinear Hybrid Continuous/Discrete-Time Models. Atlantis Studies in Mathematicsfor Engineering and Science. Vol. 8, 2011.

[2] M. Akhmet, E. Yilmaz Impulsive Hopfield-type neural network system with piecewise constantargument, Nonlinear Analysis: Real World Applications, 11-4, 2584–2593. 2010

[3] H. Bereketoglu, G Oztepe. Convergence in an impulsive advanced differential equations with piece-wise constant argument. Bulletin of Mathematical Analysis and Applications, 4-3, 57-70. 2012,

[4] K.L Cooke, I. Györi, Numerical approximation of the solutions of delay differential equations on ainfinite interval, Comput. Math. Appl. 28, 81-94, 1994.

[5] I. Gyorï, On approximation of the solutions of delay differential equations by using piecewise constantarguments, Internat. J. Math and Math. Sciences 14, 111-126. 1991.

[6] M. Pinto, Cauchy and Green matrices type and stability in alternately advanced and delayed differ-ential systems. Journal of difference equations and applications, 17(2), 235-254, 2011.

[7] M. Pinto, Asymptotic equivalence of nonlinear and quasi lineal differential equations with piecewiseconstant arguments. Mathematical and Computer Modelling, 49, 1750-1758, 2009.

[8] A.M. Samoilenko, N.A. Perestyuk, Impulsive Differential Equations, Series on Nonlinear ScienceSeries A: Volume 14, World Scientific 1995.

[9] J. Wiener, Generalized Solutions of Functional Differential Equations. World Scientific. 1993.

Page 63: Strong solutions of abstract fractional differential equations

61

Asymptotic behaviour of the time-fractional telegraphequation

Vicente Vergara

Abstract

We obtain the long-time behaviour to the variance of the distribution process associated with thesolution of the telegraph equation. To this end, we use a version of the Karamata-Feller Tauberiantheorem.

Bibliography

[1] Feller, W. An introduction to probability theory and its applications, Vol. II, 2nd-edn. John Wiley,New York, 1971.

[2] Gripenberg, G., Londen, S.-O. and Staffans, O. Volterra integral and functional equations, 34,Cambridge University Press, Cambridge, 1990.

[3] Kilbas, A., Srivastava, H. and Trujillo, J. Theory and applications of fractional differential equa-tions, 204, North-Holland Mathematics Studies, Elsevier Science B.V., Amsterdam, 2006.

[4] Orsingher, E. and Beghin, L. Time-fractional telegraph equations and telegraph processes withBrownian time. Probability Theory and Related Fields 128, (1), 141–160, 2004.

[5] Prüss, J. Evolutionary Integral Equations and Applications. Monographs Math., 87, BirkhäuserVerlag, 1993.

Partially supported by FONDECYT grant 1110033, Department of Mathematics, University of La Serena,La Serena, Chile, e-mail: [email protected]

Page 64: Strong solutions of abstract fractional differential equations

62

Acknowledgements

Page 65: Strong solutions of abstract fractional differential equations
Page 66: Strong solutions of abstract fractional differential equations

64

Acknowledgements

We would like to thank all the employees from the Department of Computation and Mathematicsat University of São Paulo, campus Ribeirão Preto, for all their effort and help in the organization ofthe IX Conference GAFEVOL, specially the following ones:

1. Jalmei Andre Tomio

2. Daniela Curado Pilheri

3. Karina Katia da Silva

4. Helena Braga Lopes Ebert

5. Daniel Camargo da Silva

6. Tiago Beani Carrer

7. Mateus Tarcinalli Machado

Also, we would like to acknowledge all the participants of the IX Conference GAFEVOL and theScientific Committee. Moreover, we would like to acknowledge our department head Professor Dr.Evandro Eduardo Seron Ruiz and the director of FFCLRP-USP Professor Dr. Fernando Luis MedinaMantelatto for all their support for the organization of this conference. Finally, our thanks to all thesponsors.

Sincerely,

Organizing Committee.

Page 67: Strong solutions of abstract fractional differential equations
Page 68: Strong solutions of abstract fractional differential equations

66

Sponsors

Page 69: Strong solutions of abstract fractional differential equations
Page 70: Strong solutions of abstract fractional differential equations

68

The IX Conference GAFEVOL is grateful to the following organizations for providing the financialsupport:

USPUniversidade de São Paulowww.usp.br

Faculdade de Filosofia, Ciências e Letras deRibeirão Pretohttp://www.ffclrp.usp.br/

USACHUniversidade de Santiago de Chilehttp://www.usach.cl/

GAFEVOL grouphttp://gafevol.usach.cl/

ANESTOCCentro de Analisis Estocástico y Aplicacioneshttp://www.anestoc.cl/

Page 71: Strong solutions of abstract fractional differential equations

69

CAPESCoordenação de Aperfeiçoamento de Pessoal deNível Superiorwww.capes.gov.br

FAPESPFundação de Amparo à Pesquisa do Estado deSão Paulowww.fapesp.br

CONICYTComisión Nacional de Investigación Científica yTecnológicahttp://www.conicyt.cl/

Page 72: Strong solutions of abstract fractional differential equations

Recommended