where 0,$"> and space dimensions . Assume that the initial data
where \frac{n}{2},$"> weighted Sobolev spaces are
Also we suppose that
where
Then we prove that there exists a positive such that the Cauchy problem above has a unique global solution satisfying the time decay property
for all 0,$"> where
and, for ,
- (i)
- a class of noncommutative holomorphic functions on the open unit ball of , generalizing the analytic functions on the open unit disc;
- (ii)
- the noncommutative disc algebra and the noncommutative analytic Toeplitz algebra ;
- (iii)
- a class of noncommutative selfadjoint harmonic functions on the open unit ball of , generalizing the real-valued harmonic functions on the open unit disc;
- (iv)
- the Cuntz-Toeplitz algebra , the reduced (resp. full) group -algebra (resp. ) of the free group with generators;
- (v)
- a class of analytic functions on the open unit ball of .
The classical Bohr inequality is shown to be a consequence of Fejér's inequality for the coefficients of positive trigonometric polynomials and Haager- up-de la Harpe inequality for nilpotent operators. Moreover, we provide an inequality which, for analytic polynomials on the open unit disc, is sharper than Bohr's inequality.
(1)
(2)
(3)
where is a bounded open set in with sufficiently smooth boundary. The problem (1)-(3) is first reduced to the analogous problem in the space with zero initial condition and
The resulting problem is then reduced to the problem where the operator satisfies Condition This reduction is based on a priori estimates which are developed herein for linear parabolic operators with coefficients in Sobolev spaces. The local and global solvability of the operator equation are achieved via topological methods developed by I. V. Skrypnik. Further applications are also given involving relevant coercive problems, as well as Galerkin approximations.
In this paper the zero reaction limit of the hyperbolic conservation law with stiff source term of monostable type
is studied. Solutions of Cauchy problems of the above equation with initial value are proved to converge, as , to piecewise constant functions. The constants are separated by either shocks determined by the Rankine-Hugoniot jump condition, or a non-shock jump discontinuity that moves with speed . The analytic tool used is the method of generalized characteristics. Sufficient conditions for the existence and non-existence of traveling waves of the above system with viscosity regularization are given. The reason for the failure to capture the correct shock speed by first order shock capturing schemes when underresolving 0$"> is found to originate from the behavior of traveling waves of the above system with viscosity regularization.
where and . Nonexistence of positive solutions is analyzed.
These bounds coincide with the first few terms of the well-known asymptotic expansion
as , being fixed, where is the -th negative zero of the Airy function , and so are ``best possible'.
acting on functions in . We prove uniqueness of the martingale problem for this degenerate operator under suitable nonnegativity and regularity conditions on and . In contrast to previous work, the need only be nonnegative on the boundary rather than strictly positive, at the expense of the and being Hölder continuous. Applications to super-Markov chains are given. The proof follows Stroock and Varadhan's perturbation argument, but the underlying function space is now a weighted Hölder space and each component of the constant coefficient process being perturbed is the square of a Bessel process.
This paper is concerned with the oscillatory behavior of first-order delay differential equations of the form
(1) |
where is non-decreasing, for and . Let the numbers and be defined by
It is proved here that when and all solutions of Eq. (1) oscillate in several cases in which the condition
holds, where is the smaller root of the equation .
where denote the Fourier coefficients of when considered as a function of period 1,
and where is the circle of length 1. Denote by the periodic eigenvalues of when considered on the interval with multiplicities and ordered so that We prove the following result. Theorem. For any bounded set there exist and so that for and , the eigenvalues are isolated pairs, satisfying (with
together with no-flux conditions at and , i.e.
Such a problem arises as a kinetic approximation to describe the evolution of the radiation distribution in a homogeneous plasma when radiation interacts with matter via Compton scattering. We shall prove that there exist solutions of , which develop singularities near in a finite time, regardless of how small the initial number of photons is. The nature of such singularities is then analyzed in detail. In particular, we show that the flux condition is lost at when the singularity unfolds. The corresponding blow-up pattern is shown to be asymptotically of a shock wave type. In rescaled variables, it consists in an imploding travelling wave solution of the Burgers equation near , that matches a suitable diffusive profile away from the shock. Finally, we also show that, on replacing near as determined by the manner of blow-up, such solutions can be continued for all times after the onset of the singularity.
and if the set of all global minima of the function has at least connected components, then, for each 0$"> small enough, the Neumann problem
admits at least strong solutions in .
- (i)
- There is a positive constant and a finite set such that for every and , either , or for some ,
- (ii)
- For every , there is an -formula , such that is precisely the set of with
where . We assume that the the potential depends only on the modulus of and vanishes along two concentric circles. We present a priori estimates for the solution , and, in the spatially radially symmetric case, we show rigorously that in the singular limit as , two phases are created. The interface separating the bulk phases evolves by its mean curvature, while evolves according to a harmonic map flow on the respective circles, coupled across the interfaces by a jump condition in the gradient.
In this paper, we are concerned with the boundedness of all the solutions and the existence of quasi-periodic solutions for second order differential equations
where the 1-periodic function is a smooth function and satisfies sublinearity: