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The method of upper and lower solutions for a Lidstone boundary value problem

Yanping Guo, Ying Gao (2005)

Czechoslovak Mathematical Journal

In this paper we develop the monotone method in the presence of upper and lower solutions for the 2 nd order Lidstone boundary value problem u ( 2 n ) ( t ) = f ( t , u ( t ) , u ' ' ( t ) , , u ( 2 ( n - 1 ) ) ( t ) ) , 0 < t < 1 , u ( 2 i ) ( 0 ) = u ( 2 i ) ( 1 ) = 0 , 0 i n - 1 , where f [ 0 , 1 ] × n is continuous. We obtain sufficient conditions on f to guarantee the existence of solutions between a lower solution and an upper solution for the higher order boundary value problem.

The method of upper and lower solutions for partial hyperbolic fractional order differential inclusions with impulses

Saïd Abbas, Mouffak Benchohra (2010)

Discussiones Mathematicae, Differential Inclusions, Control and Optimization

In this paper we use the upper and lower solutions method to investigate the existence of solutions of a class of impulsive partial hyperbolic differential inclusions at fixed moments of impulse involving the Caputo fractional derivative. These results are obtained upon suitable fixed point theorems.

The method of upper and lower solutions for perturbed nth order differential inclusions

Bupurao C. Dhage, Adrian Petruşel (2006)

Discussiones Mathematicae, Differential Inclusions, Control and Optimization

In this paper, an existence theorem for nth order perturbed differential inclusion is proved under the mixed Lipschitz and Carathéodory conditions. The existence of extremal solutions is also obtained under certain monotonicity conditions on the multi-functions involved in the inclusion. Our results extend the existence results of Dhage et al. [7,8] and Agarwal et al. [1].

The microstructure of Lipschitz solutions for a one-dimensional logarithmic diffusion equation

Nicole Schadewaldt (2011)

Commentationes Mathematicae Universitatis Carolinae

We consider the initial-boundary-value problem for the one-dimensional fast diffusion equation u t = [ sign ( u x ) log | u x | ] x on Q T = [ 0 , T ] × [ 0 , l ] . For monotone initial data the existence of classical solutions is known. The case of non-monotone initial data is delicate since the equation is singular at u x = 0 . We ‘explicitly’ construct infinitely many weak Lipschitz solutions to non-monotone initial data following an approach to the Perona-Malik equation. For this construction we rephrase the problem as a differential inclusion which enables us...

The monotone iterative technique for periodic boundary value problems of second order impulsive differential equations

Eduardo Liz, Juan J. Nieto (1993)

Commentationes Mathematicae Universitatis Carolinae

In this paper, we develop monotone iterative technique to obtain the extremal solutions of a second order periodic boundary value problem (PBVP) with impulsive effects. We present a maximum principle for ``impulsive functions'' and then we use it to develop the monotone iterative method. Finally, we consider the monotone iterates as orbits of a (discrete) dynamical system.

The Montgomery model revisited

B. Helffer (2010)

Colloquium Mathematicae

We discuss the spectral properties of the operator ( α ) : = - d ² / d t ² + ( 1 / 2 t ² - α ) ² on the line. We first briefly describe how this operator appears in various problems in the analysis of operators on nilpotent Lie groups, in the spectral properties of a Schrödinger operator with magnetic field and in superconductivity. We then give a new proof that the minimum over α of the groundstate energy is attained at a unique point and also prove that the minimum is non-degenerate. Our study can also be seen as a refinement for a specific...

The moving frames for differential equations. I. The change of independent variable

Václav Tryhuk, Oldřich Dlouhý (2003)

Archivum Mathematicum

The article concerns the symmetries of differential equations with short digressions to the underdetermined case and the relevant differential equations with delay. It may be regarded as an introduction into the method of moving frames relieved of the geometrical aspects: the stress is made on the technique of calculations employing only the most fundamental properties of differential forms. The present Part I is devoted to a single ordinary differential equation subjected to the change of the independent...

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