Abstracts for the IMA Preprint Series
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September - December 1982 Series
1-7 |
1 Statistical mechanics, dynamical systems, and turbulence
Abstracts
We present here abstracts of some lecture series in the areas of statistical
mechanics, dynamical systems, and turbulence together with reading lists in
the hope that they will provide a useful guide to others who wish to learn these
subjects.
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2 A simple proof of C. Siegel's center theorem
Raphael De laLlave
We give an elementary proof of a particular case of C. Siegel's center theorem,
based on a method of M. Herman. Even if the proof has less generality than the
standard one, it is simpler and provides sharper bounds.
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3 On copositive matrices and strong ellipticity for
isotropic elastic materials
H. Simpson and S. Spector
In this paper we establish necessary and sufficient conditions for the strong-ellipticity
of the equations governing an isotropic (compressible) nonlinerly elastic material
at equilibrium. Our work extends results of Knowles and Sternberg [5] who obtained
such conditions for both ordinary and strong ellipticity in the special case
when the underlying deformations are plane.
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4 Vector fields in the vicinity of a compact invariant
manifold
George R. Sell
Let us consider two vector fields
(1) X' = F(X)
(2) Y' = F(Y)
defined on a give Euclidean space E where F and G are of class CN+1.
Furthermore, assume that there is a smooth compact manifold M smoothly imbedded
in E and that M is invariant for both vector fields. Also that F and G agree
on M, i.e. F|M = G|M.
We wish to study the question of CS-conjugacies between (1) and (2).
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5 Non-linear stability of asymptotic suction
Milan Miklavcic
A flow over a plane y = 0 in R3 given by
U(x,y,z) = (1 - e-y, -1/R, 0)
is called an asymptotic suction velocity profile [12]. R>0 is the Reynolds
number. U satisfies the Navier-Stokes equation
ðv / ðt + (v ·
) v = -
p0 + 1/R v
div v = 0
with p0 = 0. In the present paper it is proved that the stability
of U for small perturbations which initially decay exponentially in the y direction
and are periodic in the x and z direction is governed by the eigenvalues of
the classical Orr-Sommerfeld equation [1, 8, 12]. For precise statements see
Theorems 4, 5, 9, and 15.
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6 A simple system with a continuum of stable inhomogeneous
steady states
Hans Weinberger
The system
ut = {(1 + v)}xx
+ (R1 - au - bv)u
vt = (R2
- bu - av)v
{(1 + u)}xx
= 0 at x = 0 and x = 1
with
1/2 (a/b + b/a) < R1/R2
< a/b
and
> a(a2 - b2) / 2abR1 - (a2 +
b2) R2
was considered by M. Mimura [2] as a model for the population densities of two
competing species, one of which increases its migration rate in response to
crowding by the other species. It is a special case of the model of N. Shigesada,
K. Kawasaki, and E. Teramoto [3].
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7 Period 3 bifurcation for the logistic mapping
Bau-Sen Du
In the context of continuous mappings of the interval, one of the most striking
features may be Sharkovsky's theorem [6] which, among other thing, shows that
the existence of a period 3 point implies the existence of periodic points of
every period (see also [2, 5]). Therefore, for a one-parameter family of interval
mappings, the determination of period 3 bifurcation points may be interesting.
In recent years, the logistic mapping f (x)
= 1 - x2 has been entensively
studied ([1, 4]). By using computer simulation for this family f (x),
as the parameter is increased from 0,
we can observe the Feigenbaum "cascades" [3]. That is, stable periodic
points of double periods accumulate in a geometric and universal way. As the
parameter is approximately equal to
1.7498 ([1, p.129]), there seems to be a period 3 bifurcation. In this note,
we show that this family f (x)
does have a period 3 bifurcation exactly at
= 7/4.
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January - December 1983 Series
8-50 |
8 Optimal Numerical Approximation of a Linear Operator
Hans Weinberger
Many linear problems of numerical analysis can be formulated in the following
way: One is given a set of n linear data Nu =
and a bound for the norm ||u||B of an otherwise unknown element of
u of a hilbert space B. One wishes to find a best approximation to the element
Su, where S is a bounded linear operator from B to another Hilbert space .
For example, Su may be the solution of an ordinary or partial differential equation
with right-hand side, initial data, or boundary data u.
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9 Three component ionic microemulsions
L.R. Angel, D.F. Evans, and B. Ninham
Necessary design features of microemulsions formed from cationic surfactant
without any requirement for cosurfactant are illustrated by a study of microemulsions
formed from didodecyldimethylammonium bromide in various oils. Ease of purification,
preparation and manipulation give this and related systems a considerable advantage
over conventional systems in enhancing our understanding of microemulsions and
emulsion behavior.
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10 Surfactant diffusion; new results and interpretations
D.F. Evans, D. Mitchell, S. Mukherjee, and B. Ninham
Data for surfactant diffusion are reproted for sodium dodecylsulfate at 25°
and tetradecyltrimethylammonium bromide at 25°, 90°, and 135°C,
as measured by Taylor tube dispersion. These data are analyzed in terms of two
limiting forms of theory, one appropriate to "slow" reaction rates,
the other to "fast" rates. It is shown that the usual extrapolation
to the critical micelle concentration to infer intrinsic diffusion constants
is not permissible. The data is explicable if transport occurs by a process
wherein ionic micelles disassociate, diffuse as monomers and reassemble into
micelles. This is directly contrary to current ideas on diffusion of surfactants.
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11 Remark about the final aperiodic regime for maps
on the interval
Leif Arkeryd
We consider families of maps on the interval with one maximum, and prove the
geometric convergence of the bifurcation parameter for the case of superstable
periodic orbits converging towards the final aperiodic regime.
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12 Manifolds of global solutions of functional differential
equations
Luis T. Magalhães
This paper consider smooth invariant manifolds of global solutions of retarded
Functional Differential Equations in Rn. The persistence, under small
perturbations, of such manifolds where the flow is given by an Ordinary Differential
Equation in Rn is studied. The novelty of the present approach lies
on the use of the dynamics of the flow on the manifolds, instead of their attractivity
properties.
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13 Tori in resonance
Kenneth Meyer
This paper gives three examples of ordinary differential equations which depend
on one or more parameters and which admit invariant tori for some values of
the parameters. These examples illustrate how invariant tori evolve as the parameters
are changed; in particular how they disappear, bifurcate and lose smoothness.
The equations presented are choosen to be as simple as possible in order to
clearly show the interesting phenomenon without unnecessary details. However,
the theory of normal forms and unfoldings was used to select typical examples,
but no attempt will be made to define precisely the universe of discourse where
these examples are generic. The unfolding of invariant tori would consist of
a mutitude of cases not all of which are that interesting.
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14 Surface models with nonlocal potentials: Upper
bounds
C. Eugene Wayne
The behavior of fluctuations in a class of surface models with exponentially
decaying nonlocal potentials is studied. Combining a Mayer expansion with a
duality transformation we demonstrate the equivalence of these models to a class
of two dimensional spin systems with nonlocal interactions. The expansions give
sufficient control over the potentials to allow the fluctuations to be bounded
from above by the means of complex translations in the spin representation of
the model.
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15 On stability and uniqueness of fluid flow through
a rigid porous medium
K.A. Pericak-Spector
We study a set of equations describing the flow of an incompressible viscous
fluid through a rigid porous medium. Existence, uniqueness and stability results
are established for the case of a region impregnated with fluid, and uniqueness
for an unsaturated region.
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16 Smooth linearization near a
fixed point
George R. Sell
In this paper we extend a theorem of Sternberg and Bileckii. We study a vector
field, or a diffeomorphism, in the vicinity of a hyperbolic fixed point. We
show that if the eigenvalues of the linear part (at the fixed point) satisfy
2N-algebraic conditions (where N > 1), then there is a CN-linearization
in the vicinity of this fixed point. If the fixed point is stable, then the
CN-linearization theorem follows when only (N + 1)-algebraic conditions
are satisfied. Examples are given which show that the first of these results
is sharp. An application to celestial mechanics is included.
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17 A nonlinear stability analysis of a model equation
for alloy solidification
David Wollkind
Controlled plane front solidification of alloys and other binary substances
under an imposed temperature gradient is used in practice to grow single crystals,
refine materials (e.g., zone refining), and obtain uniform or non-uniform composition
within the material grown [1]. The most important industrial applications of
this type of solidification are for growth of crystals for metal oxide semiconductors
(MOS's) [1]. Growth of oxide crystals for jewels is another, much older commercial
application of single crystal growth [1]. Another important application is in
growth of oxides for laser systems and other optical devices [1]. Further industrial
applications arise in ingot casting and in the steel and glass industries [2].
For all of these solidification situations involving binary materials, quantitative
predictions of interfacial cellular morphology, including information on cell
size and intracellular solute distribution, prove to be extremely valuable and
are of a particular aid to industrial researchers.
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18 Local
conjugacy on the Julia set for some holomorphic perturbations of
Pierre Collet
We consider holomorphic perturbations f of f0, f0(z)
= z2, which are small in a neighborhood of the unit circle (the Julia
set of f0). We show that if the C1 conjugacy invariants
of f and f0 are identical, then f and f0 are
conjugate on their part of the Julia set which remains near the unit circle.
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19 On the modified Bessel functions of the first
kind (1st paper); and On barrelling for a material in finite elasticity
(2nd paper)
Henry C. Simpson, Scott J. Spector
A. On the modified Bessel functions of the first kind: We consider
the functions v (t)
t I (t) / I
+ 1 (t) where I are
the modified Bessel functions of the first kind of order
0. We prove that v
is strictly monotone and strictly convex on R+. These results have
application in finite elasticity.
B. On barrelling for a material in finite elasticity: In this paper we
investigate the question of stability for a solid circular cylinder, composed
of a particular homogeneous isotropic (compressible) nonlinearly elastic material,
that is subjected to compressive end forces in the direction of its axis (so
as to give fixed axial displacements at the ends).
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20 Linearization and global dynamics
George R. Sell
In this paper we show how the spectral theory of linear skew-product flows
may be used to study the following three questions in the qualitative theory
of dynamical systems: (1) when is an -limit
set or an attractor a manifold?
(2) Under which conditions will a dynamical system undergo a Hopf-Landau bifurcation
from a k-dimensional torus to a (k + 1)-dimensional torus?
(3) When is a vector field i the vicinity of a compact invariant manifold smoothly
conjugate to the linearized vector field and how smooth is the conjugacy?
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21 Global Lyapunov exponents, Kaplan-Yorke formulas
and the dimension of the attractors for 2D Navier-Stokes equations
P. Constantin and C. Foias
We study the fractal and Hausforff dimensions of the universal attractor for
the Navier-Stokes equations in two space dimensions. The finite dimensionality
of the attractors for the Navier-Stokes equation was first implicitly proven
in [16] and explicitely in [10]. The subject has been investigated recently
by several authors.
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22 Stability for semilinear parabolic equations
with noninvertible linear operator
Milan Miklavcic
Suppose that
x'(t) + Ax(t) = f(t, x(t)),
t ≥ 0
is a semilinear parabolic equation, e-At is bounded and f satisfies
the usual continuity condition. If for some 0 <
≤ 1, 0 < < 1,
p > 1, > 1
||t
Ae-At|| ≤ C, t ≥ 1
||f(t, x)|| ≤ C(||A
x|| p + (1 + t)- ),
t ≥ 0
whenever ||A x|| + ||x|| is
small enough, then for small initial data there exist stable global solutions.
Moreover, if the space is reflexive then their limit states exist. Some theorems
that are useful for obtaining the above bounds and some examples are also presented.
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23 Perturbations of geodesic flows on surfaces of
constant negative curvature and their mixing properties
P. Collet, H. Epstein, and G. Gallavotti
We consider one parameter analytic Hamiltonian perturbations of the geodesic
flows on surfaces of constant negative curvature. We find two different necessary
and sufficient conditions for the canonical equivalence of the perturbed flows
and the non perturbed ones. One condition says that the "Hamilton-Jacobi"
(introduced in this work) for the conjugation problem should admit a solution
as a formal power series (not necessarily convergent) in the perturbation parameter.
The alternative condition is based on the identification of a complete set of
invariants for the canonical conjugation problem. The relation with the similar
problems arising in the KAM theory of the perturbations of quasi periodic Hamiltonian
motions is briefly discussed. As a byproduct of our analysis we obtain some
results on the Livscic, Guillemin, Kazhdan equation and on the Fourier series
for the SL(2, R) group. We also prove that the analytic functions on the phase
space for the eodesic flow of unit speed have a mixing property (with respect
to the geodesic flow and to the invariant volume measure) which is exponential
with a universal exponent, independent on the particular function, equal to
the curvature of the surface divided by 2. This result is contrasted with the
slow mixing rates that the same functions show under the horocyclic flow: in
this case we find that the decay rate is the inverse of the time ("up to
logarithms").
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24 On the thermodynamics of interstitial working
J.E. Dunn and J. Serrin
In order to model fluid capillarity effects, the Dutch physicist Korteweg
formulated in 1901 a constitutive equation for the Cauchy stress that included
density gradients. Specifically, Koretweg proposed for study a compressible
fluid model in which the "elastic" or "equilibrium" portion of the Cauchy stress
tensor T is given by
T = $hat T$ ( ,
, grad ,
grad2 )
= (-p +
+ |grad |2)
1 + grad
grad
+ grad2 ,
where = (x,
t) is the density of the fluid at the place x at time t, where grad
and grad2 are, respectively,
the first and second (spatial) gradients of
with respect to x (with = tr (grad2 )
= the Laplacian of ), and where p, ,
, ,
and are material functions of
and the temperature . To model viscous
effects in the dynamic response of his fluids, Korteweg added to the right hand
side of (1.1) the classic form of Cauchy and Poisson, i.e., (tr
D) 1 + 2 D, where D is the usual stretching
tensor of hydrodynamics, and where
and are the usual viscosity coefficients
and may depend on and .
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25 On the absence of bifurcation for elastic bars
in uniaxial tension
Scott J. Spector
We prove that an elastic bar undergoing uniaxial tension will not neck before
the axial load on the bar attains a (local) maximum. Further, if the bar is
in a hard loading device we show that necking is delayed until after maximum
load is achieved. The key ingredient in the latter result is a generalized Korn
inequality.
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26 Maps
of an interval
W. A. Coppel
(There are three expository lectures in this preprint)
26-1 Motivation and elementary properties
26-2 Peiodic orbits, topological dynamics, chaos
26-3 Quadratic maps, qualitative and quantitative universality
27 Phase transitions in the Ising model with traverse
field
James Kirkwood
The Ising model perturbed by a small transverse field is shown to have a phase
transition by two methods. With the first method, using a Peierls' contour argument,
we are only able to show that spontaneous magnetization occurs with the transverse
field goint to 0 as -1/3.
With the second method, which used reflection positivity, long range order is
shown to occur for a small transverse field independent of temperature.
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28 The asymptotics of solutions of singularly perturbed
functional differential equations: distributed and concentrated delays are different
Luis Magalhães
This paper illustrated the differences between systems with distributed delays
and systems having only concentrated delays in what concerns the asymptotic
rates of solutions of singularly perturbed linear retarded functional differential
equations. An example of a system with distributed delays shows that the introduction
of a ``slow" variable coupled with the ``fast" variable may decrease the asymptotic
rates of solutions observed when the perturbation parameter is close to zero.
Such a situation cannot happen for ordinary differential equations, or even
for differential-difference equations.
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29 Homoclinic orbits for flow in R3
Charles Tresser
We propose a rough classification for volume contracting flows in R3
with chaotic behavior. In the simplest cases, one looks at the nature of a homoclinic
loop for the flow. Most configurations have been studied at length in the literature;
here we examine briefly the ``forgotten" case.
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30 About some theorems by L.P. Sil'nikov
Charles Tresser
Some theorems by L.P. Sil'nikov, which describe the dynamics in the neighborhood
of homoclinic orbits, bi-asymptotic to a saddle focus, and initially proved
for real analytic vector fields are collected here. Recent results in dynamical
systems theory allow us to precise some of the conclusions and to generalize
these theorems to the C1,1 class. Certain heteroclinic loops involving
a saddle focus are also considered.
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31 On the renormalized coupling constant and the
susceptibility in 44
field theory and the Ising model in four dimensions
Michael Aizenmann
We discuss the Euclidean 44
field theory, and the critical behavior in ferromagnetic systems in four dimensions.
It is rigorously shown that there are at most logarithmic corrections to the
mean field law in the behavior of the magnetic susceptibility
= 44 S2
(0, x). Furthermore, if any such corrections are present in a continuum limit
which is used to construct a 44
field theory the limiting theory would be non-interacting. Our analysis extends
to ferromagnetic systems of variables which belong to the Simon-Griffiths class.
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32 The KAM theory of systems with short range interactions
I
C. Eugene Wayne
The Kolmogorov, Arnol'd, Moser (KAM) theory [15, 1, 16] proves that ``small"
perturbations of integrable Hamiltonian systems possess ``large" sets of initial
conditions for which the trajectories remain quasiperiodic. In this paper we
discuss how the ``strength" of the allowed perturbation varies with the number
of degrees of freedom, N, in the system.
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33 Temporal and spatial chaos in a Van der Waals
fluid due to periodic thermal fluctuations
M. Slemrod and J.E. Marsden
This paper applies the Mel'nikov technique to prove the existence of deterministic
chaos in two problems for a Van der Waals fluid. The first problem shows that
temporal chaos results as a result of small time periodic fluctuations about
a subcritical temperature when the fluid is initially quenched in the unstable
spinoidal region. The second problem shows that spatial chaos arises from small
spatially periodic flunctions in an infinite tube of fluid if the ambient pressure
is appropriately chosen.
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34 Percolation in continuous systems
James R. Kirkwood and C. Eugene Wayne
A rigorous proof of the existence of a percolation phase transition in a system
of noninteracting discs in the plane is presented. In addition, bounds on the
critical density and critical area fraction are derived. The lower bound makes
use of Halperin's idea of a self-avoiding walk of discs. The upper bound is
proved by relating the continuum model to the site percolation problem on a
triangular lattice, whose critical probability is exactly known.
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35 Invariant manifolds for Functional Differential
Equations close to ordinary differential equations
Luis T. Magalhães
This paper considers invariant manifolds of global trajectories of retarded
Functional Differential Equations in Rn. The persistence, smoothness
and stability of such manifolds where the flow is given by an Ordinary Differential
Equation (ODE) in Rn is studied for small perturbations of ODEs.
The novelty of the present approach lies in the use of the dynamics of the flow
on the manifolds, instead of their attractivity properties.
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36 The KAM theory of systems with short range interactions,
II
C. Eugene Wayne
The proof of the results on the KAM theory of systems with short range interactions,
stated in [4] is completed. Estimates on the decay of the interactions generated
by the iterative procedure in the KAM theorem are proved, as well as the modification
of the theorems of [1-3] needed for our results.
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37 Passive quasi-free states of the noninteracting
Fermi gas
Jean De Cannière
The passive quasi-free states of the noninteracting Fermi gas with continuous
one-particle Hamiltonian H are computed. They turn out to be the well known
Fermi-Dirac states, or limits thereof. This still holds true if the spectrum
of H has both a continuous and a discrete part, except for the appearance of
a class of "ground state-like" states showing a local random excitation of the
point spectrum in a neighborhood of the Fermi energy. When H has only pure point
spectrum, the requirement that a state be passive and quasi-free is no longer
sufficient to characterize the Fermi-Dirac distributions.
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38 Maxwell and van der Waals
revisited
Elias C. Aifantis
We utilize a modern continuum mechanic framework to reconsider an old problem
for fluid interfaces, also addressed by Maxwell and van der Waals. We prove
that their results need not be valid necessarily. This conclusion is arrived
at as a consequence of questioning the existence of thermodynamic potentials
and the validity of usual thermodynamic relations within unstable (spinodal)
regions. One central result is that Maxwell's equal area rule needs not be valid
and certain statistical models are shown to be internally inconsistent. Prescise
conditions for the validity of Maxwell's rule and the variational theory of
van der Waals established in terms of the coefficients defining the interfacial
stress.
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39 On the mechanics of modulated structures
Elias C. Aifantis
The purpose of this lecture is to illustrate the appropriateness and potential
of the methods of continuum mechanics in modeling modulated structures. Modulations
are viewed, in general, as occurrences which may involve one or more properties
of a system and extend from a submicroscopic to a macroscopic scale. They are
also viewed as capable of possessing wave lengths and amplitudes which may vary
from very small to very large values.
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40 The strong
topology on symmetric sequence spaces
William H. Ruckle
Let S be a linear space of real sequences written in functional notation s=(s(j))=(s(1),
s(2),...). There is a natural duality between S and the space
of sequences which are eventually 0 given by the equation
<s,t> = j
s(j) t(j) s S, t
.
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41 A characterization of Borda's rule via optimization
Charles R. Johnson
It is shown that Borda's social welfare rule coincides with a social welfare
function resulting from a well-defined optimization principle applied to a collection
of individual binary preferences.
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42
The spatial homogeneity of stable equilibria of some reaction-diffusion systems
on convex domains
Kazuo Kishimoto and Hans F. Weinberger
43 On work and constraints in mixtures
K.A. Pericak-Spector and W.O. Williams
In recent years workers in mixture theory have become aware of the central
role that volume-fraction, the parameter describing the relative proportion
of the volume occupied by a constituent, must play in that theory. In particular,
the rate of change of volume-fraction, which we here call the chority, must
appear in a working term as contributing to the energy, in order to avoid various
inconsistencies. This is true both in theories in which volume-fraction appears
as a parameter of microstructure and in complete mixture theories.
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44 Some remarks on deformations of minimal surfaces
Harold Rosenberg and Eric Toubiana
We consider complete minimal surfaces (c.m.s.'s) in R3 and their
deformations. M1 is an
deformation of M0 if M1 is a graph over M0
in an tubular neighborhood of M1
and M1 is - C1
close to M0. A c.m.s. M0 is isolated if all minimal surfaces
M1, which are sufficiently small deformations of M0, are
congruent to M0. Many of the classical minimal surfaces in R3
are known to be isolated [2]; however, no example was known of a nonisolated
minimal surface.
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45 The duration of transients
S. Pelikan
Imagine a particle moving in a box and making elastic collisions with the
sides. Suppose there is a small hole in one side of the box. For many initial
conditions the particle will bounce around for a long time and then leave the
box. These trajectories are examples of transients. In this paper we investigate
the average duration of transients for a certain class of transformations T.
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46 Random fluctuations of the duration of harvest
V. Capasso, K.L. Cooke, and M. Witten
In this report, we wish to discuss models of harvesting of a population when
the duration of the harvest interval is subject to random fluctuations. This
kind of situation arises, for example, if the harvestor or predator can harvest
only when weather conditions are favorable. Clearly, the length of the favorable
period will be subject to random variations.
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47 The Lp-intergrability of Green's functions
and fundamental solutions for elliptic and parabolic equations
E. Fabes and D.W. Stroock
Given d ≥ 1 and in (0,1) denote
by Ad( ) the class of smooth,
symmetric, d X d matrix-valued functions a
(aij (x)) on Rd which satisfy
I ≤ a(x) ≤ 1/
I x in Rd
in the sense of nonnegative definiteness. Set
La u = i,j=1d
aij (x) ð2 u / ðxi ðxj
(x)
and let
La* v = i,j=1d
ð2 / ðyi ðyj (aij(y)
v(y))
denote the adjoint of L.
In the first part of this paper we study the interior behavior of nonnegative
solutions, v, of the adjoint equation, La* v = 0, in a
domain of Rd. Our main result
is the establishment of an interior "backward Hölder inequality" for such
solutions.
In the second part we will use the estimate
supx
supa Ad ( )
 Ga (x,y) q
dy <
to study the integrability properties of the fundamental solution,
a(t,x,y), (t,x,y)
(0, ) X Rd X Rd,
to the parabolic initial-value problem:
ðu / ðt (t,x) = La u(t,x),
u(0,x) = f(x) (La u =
i,j=1d aij (x) ð2
/ ðxi ðxj).
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48 Semilinear equations in RN without
conditions at infinity
Haïm Brezis
The purpose of this paper is to point out that some nonlinear elliptic (and
parabolic) problems are well-posed in all of RN without conditions
at infinity.
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49 Lax-Friedrichs and the viscosity-capillarity
criterion
M. Slemrod
It has been shown by Lax some time ago that for hyperbolic conversation laws
solutions obtained as limits of the Lax-Friedrichs finite difference scheme
will actually satisfy an "entropy" admissibility criterion. The goal of this
paper is to attempt to extend Lax's idea to a form which is amenable to mixed
problems as well, e.g. the dynamics of a van der Waals fluid. Specifically,
we compare shocks obtained by the Lax-Friedrichs scheme with those permitted
by the viscosity-capillarity criterion of [2, 3]. We show that for isothermal
motion it is expected that shocks produced by Lax-Friedrichs will satisfy the
viscosity-capillarity criterion.
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50 Spanning tree extensions of the Hadamard-Fischer
inequalities
Charles R. Johnson and Wayne W. Barrett
All possible graph theoretic generalizations of a certain sort for the Hadamard-Fischer
determinantal inequalities are determined. These involve ratios of products
of principal minors which dominate the determinant. Furthermore, the cases of
equality in these inequalities are characterized, and equality is possible for
every set of values which can occur for the relevant minors. This relates recent
work of the authors on positive definite completions and determinantal identities.
When applied to the same collections of principal minors, earlier generalizations
give poorer, more difficult to compute bounds than the present inequalities.
Thus, this work extends, and in certain sense completes, a series of generalizations
of Hadamard-Fischer begun in the 1960's.
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January - December 1984 Series
51-125 |
51 Revelation and implementation under differential
information
Andrew Postlewaite and David Schmeidler
Our goal in this pape is to merge several central ideas in economic theory;
strategic behavior (incentive compatibility), differential (or incomplete) information,
and the Arrow-Debreu model of general equilibrium. By strategic behavior we
refer to the literature which models economic institutions as games in strategic
form and uses Nash equilibrium as the solution concept. This literature, motivated
by informational decentralization questions, deals not with a single economic
environment and a single game, but rather considers a class of environments
and a strategic outcome function (game form) which is applied uniformly to this
class. The concept of differential information is that of Bayesian equilibrium
as it has been applied in the literature on implicit contracts, principal-agent
problems and bidding and auction models.
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52 Complex analytic dynamics on the Riemann sphere
Paul Blanchard
Holomorphic, non-invertible dynamical systems of the Riemann sphere are surprisingly
intricate and beautiful. Often the indecomposable, completely invariant sets
are fractals (a la Mandelbrot [M1]) because, in fact, they are quasi-self-similar
(see Sullivan [S3] and (8.5)). Sometimes they are nowhere differentiable Jordan
curves whose Hausdorff dimension is greater than one (Sullivan [S4] and Ruelle
[R]). Yet these sets are determined by a single analytic function zn+1
= R(zn).
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53 Topology and differentiability of labyrinths
in the disc and annulus
Gilbert Levitt and Harold Rosenberg
The study of differential equations in the plane which are locally of the
form ðy / ðx =F(x,y), gives rise to labyrinths. They are limit sets
of bounded solutions to this equation. This is made precise in [Ro], where the
singularities considered are thorns and tripods. In part I of this paper, we
shall extend the results of [Ro] to differential equations with n-prong singularities,
in the disc and annulus. For the disc, the story is not essentially different
from the previous case. However, for the annulus, the study is quite different
and more complicated. In both cases, we obtain a topological structure theorem
for solutions of the equation.
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54 Symmetry of constant mean curvature hypersurfaces
in hyperbolic space
Gilbert Levitt and Harold Rosenberg
In a recent paper, M. Do Carmo and B. Lawson studied hypersurfaces M of constant
mean curvature in hyperbolic space [2]. They use the Alexandrov reflection technique
to study M given the asymptotic boundary ð M.
For example, one of their theorems says M is a horoshpere when ð M
reduces to a point. They also prove a Bernstein type theorem for minimal graphs.
In this paper we shall extend their results to other boundary conditions. We
prove an embedded M, of constant mean curvature, with ð M
a subset of a codimension one sphere S, either is invariant by reflection in
the hyperbolic hyperplane containg S or is a hypersphere. In the former case
M is a "bigraph" over H: it meets any geodesic orthogonal to H either not at
all or transversaly in two points (one on each side of H) or tangentially on
H.
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55 Analysis of a dynamic, decentralized exchange
economy
Ennio Stacchetti
A dynamic exchange economy model is presented. Similarly to the Walrasian
equilibrium problem, each consumer is characterized by a feasible set and by
an instantaneous demand function, that depends on the price vector, time, and
the commodity holding. The commodity holding of each consumer varies according
to his instantaneous demand function at each moment. We show that the market
can choose prices that will lead the commodity holding of each consumer to remain
in his consumption set while the aggregate commodity holding satisfies the scarcity
constraints of the market.
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56 On failure of the complementing condition and
nonuniqueness in linear elastostatics
Henry Simpson and Scott J. Spector
Consider a homogeneous, isotropic body composed of a compressible linearly
elastic material and assume that the body is at equilibrium in a state of plane
strain. The traction problem for such a body (in the absence of body forces
and surface tractions) consists of finding a displacement U=(u1,u2)
that satisfies (cf., e.g., Gurtin [4])
(1) U
+ ( + )
div U = 0 in R.
(2) [ ( U
+ UT) +
(div U) I] n = 0 on ðR.
Here R R2 is a regular region,
n the outward unit normal to the boundary, ðR, and ,
and are the (constant) Lamé
moduli.
It is well-known that (1) and (2) have a unique solution, modulo an infinitesimal
rigid deformation, provided that ≠ 0,
+
≠ 0, and 2 +
≠ 0.
The purpose of this note is to demonstrate that the above mentioned uniqueness
result fails when = - .
In fact we show that (1) and (2) have an infinite number of linearly independent
solutions (in spite of the ellipticity of the equations). The reason for this
unusual (for an elliptic system) behavior is that the boundary conditions fail
to satisfy the complementing (or Lopatinsky-Shapiro) conditions.
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57 Complete integrability in statistical mechanics
and the Yang-Baxter equations
Craig Tracy
In this paper we give a differential formulation of the Yang-Baxter equations.
This formulation leads to the introduction of the Yang-Baxter ideal IYB,
the basic geometric object in this formulation. These ideas are illustrated
in the context of the Baxter model and the general eight-vertex model.
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58 Boundedness of solutions of Duffing's equation
Tongren Ding
J. Littlewood, L. Markus, and J. Moser proposed independently the boundedness
problem for solutions of Duffing's equation: x+g(x)=p(t), where p(t) is continuous
and periodic and g(x) is superlinear at infinity. The purpose of this paper
is to prove that all solutions of the above-mentioned Duffing's equation are
bounded for t R when p(t) is even (or when
p(t) is odd and g(x) is odd).
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59 Workshop on price adjustment, quantity adjustment,
and business cycles
Abstract
The workshop dealt with economic models in which time plays an essential role,
and both the description of adjustment to a static equilibrium and the description
of equilibrium paths were considered. From a mathematical point of view, discrete
dynamical systems and the dynamics of ordinary and partial differential equations
played a major role.
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60 The Coase theorem - An informational perspective
Rafael Rob
It is common knowledge these days that environmental policy plays a crucial
role in a society characterized by a rapidly developing technology. While a
world of highly mechanized productions methods offers its inhabitants a larger
supply of goods and services, it raises at the same time serious questions about
the ecological price that has to be paid for this increased abundance. The public
concern expressed through the media, and governmental responses to this concern
via budgetary provisions testify to the importance of the issue.
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61 Approximate Newton methods and homotopy for stationary
operator equations
Joseph W. Jerome
A quadratically convergent algorithm, based upon a Newton-type iteration,
is defined to approximate roots of operator equations in Banach spaces. Fréchet
derivative operator invertibility is not required; approximate right inverses
are used in a neighborhood of the root. This result, which requires an initially
small residual, is sufficiently robust to yield existence; it may be viewed
as a generalized version of the Kantorovich theorem. A second algorithm, based
on continuation via single, Euler-predictor/Newton-corrector iterates, is also
presented. It has the merit of controlling the residual until the homotopy terminates,
at which point the first algorithm applies. This method is capable of yielding
existence of a solution curve as well. An application is given for operators
described by compact perturbations of the identity.
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62 A note on competitive bidding with asymmetric
information
Rafael Robz
An interesting case of competitive bidding with an asymmetrical knowledge
about the true value of the auctioned object is examined by R. Wilson [4]. The
primary motivation for his study is the insight it provides about the value
of information, or, more specifically, about the relative gains of the informed
bidder vs. the uninformed bidder. As a by-product one can learn something about
the ability of the seller to appropriate or realize the value of the item he
offers for sale and about the identiy of the buyer. His analysis tells us, in
short, about allocations and imputation under conditions of uncertainty and
symmetric market positions - a fundamental question in economic theory. The
purpose of this paper is expositional. By means of two alternative approaches,
I will derive the equilibrium strategies and outcomes of the bidding game formulated
by Wilson. A few flaws in his analysis will be corrected thererby. Additional
examples illustrating the results will be offered. To be self-sufficient, let
me start out by presenting the real-life situtation we wish to investigate and
the model corresponding to it.
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63 Equilibrium price distributions
Rafael Rob
Equilibrium price distributions (for a homogeneous product) consistent with
individual incentives are investigated. They arise in informationally imperfect
markets in which the only primitive datum is the distribution of search costs.
It is shown that single, multi- and continuous price distributions are all viable
long-run phenomena depending on the nature of search costs. A method for computing
equilibrium price distributions is also provided.
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64 The linearizing projection, global theories
William H. Ruckle
A linearizing operator or projection is a device which converts nonlinear
information into linear form. A well-known example of a linearizing projection
is the Shapley value, both in the descrete case (Shapley, 1953) and the continuous
case (Aumann and Shapley, 1974). A linearizing projection usually satisfies
certain axioms of rationality which insure that it is the "unique, fair" allocation
or distribution. Thus it is an admiriable bookkeeping device because bookkeeping
must be linear.
In Ruckle (1982) a first attempt was made to treat the Aumann-Shapley theory
of values in the setting of functionals defined in an arbitrary Banach space
E.
This paper continues the effort begun in Ruckle (1982) by constructing three
global theories of linearizing projections (or x0-value). These theories
are called "global" because they refer to spaces of functionals which are defined
on the entire Banach space E. In Section 6 we shall describe what we mean by
a "local" theory and explain why such theories are needed.
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65 Ergodic properties of linear dynamical systems
Russell Johnson, Kenneth Palmer, and George R. Sell
The Multiplicative Ergodic Theorem give information about the dynamical structure
of a cocycle , or a linear skew product
flow , over a suitable base space M. In
typical applications the base space M is either an attractor; a compact invariant
set; or the space of coefficients for a diffeomorphism, a differential equation,
or a vector field. This theorem asserts that for every invariant probability
measure on M there is a measurable decomposition
of the vector bundle over M into invariant measurable subbundles, and that every
solution with initial conditions in any of these subbundles has strong Lyapunov
exponets. These exponents, or growth rates, depend on the measure ,
and when is ergodic, they are constant
(almost everywhere) on M and form a finite set meas ( ), the measurable (Millionscikov-Oseledec) spectrum.
The main objective in this paper is to study the connection between the measurable
spectrum meas ( ) and the dynamical spectrum dyn
introduced by Sacker and Sell (1975, 1978, 1980). (Also see Daletskii and Krein
(1974), as well as Selgrade (1975). The dynamical spectrum dyn
consists of those values
R for which the shifted flow
fails to have an exponential dichotomy over M. It follows from the Spectral
Theorem, Sacker and Sell (1978), that the dynamical spectrum is the finite union
of disjoint compact intervals when M is compact and dynamically connected.
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66 How a network of processors can schedule its
work
Stanley Reiter
The problem addressed in this paper is to design a method by which a network
of processors confronted with a flow of tasks may distribute the computing to
be done among the processors so as to make effective use of them to perform
the required computations. The method, and its variants, presented in this paper
gives weight to the objectives of carrying out the prescribed tasks in short
time, and to the relative urgencies associated with those tasks. This problem
is reminiscent of the problem of scheduling the flow of jobs through a machine
shop. The methods presented here are adapted from a method developed for that
problem which were described in [1].
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67 Linear subdivision is strictly a polynomial phenomenon
R.N. Goldman and D.C. Heath
In this paper we give an elementary proof that polynomial curves are the only
differentiable curves which permit subdivision by standard linear techniques.
Subdivision methods for rational polynomial curves are also discussed.
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69 Realization and Nash implementation: Two aspects
of mechanism design
Steven R. Williams
In this paper we will show how a message process which "realizes" (or computes)
a given social choice rule F can be used to construct a game which implements
F in Nash equilibrium. Any efficient encoding of information that occurs in
the message process causes a corresponding reduction in the size of the strategy
space of the game which we will construct to implement F.
Necessary and (stronger) sufficient conditions on the message process will be
given for this construction.
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70
Sufficient Conditions for Nash Implementation
Steven R. Williams
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71
Equilibria in Banach lattices without ordered preferences
Nicholas C. Yannelis and William R. Zame
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72
The reciprocals of solutions of linear ordinary differential equations
William A. Harris, Jr. and Yasutaka Sibuya
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73
A dynamical meaning of fractal dimension
Steve Pelikan
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74
Continuous-time portfolio management: Minimizing the expected time to reach
a goal
David C. Heath and William D. Sudderth
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75
Information flows intrinsic to the stability of economic equilibrium
J.S. Jordan
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84
Subjective
probability and expected utility without additivity
David Schmeidler
86
State
categories, closed categories, and the existence semi-continuous entropy functions
F. William Lawvere
87
Functional
Remarks on the General Concept of Chaos
F. William Lawvere
101
The
derivative of a tensor-valued function of a tensor
Donald E. Carlson and Anne Hoger
113
On
the derivatives of the principal invariants of a second-order tensor
D. Carlson and A. Hoger
January 1985 - December 1985
Series
126-205 |
171
On
Hadamard stability in finite elasticity
H.C. Simpson and S.J. Spector
January 1986 - December 1986
Series
206-285 |
239
Interaction of Shallow-Water Waves and Bottom Topography
B. Boczar-Karaki, J.L. Bona, and D.L. Cohen
January 1987 - December 1987
Series
286-388 |
286
Finite difference methods for the transient behavior of a semiconductor device
Jim Douglas, Jr. and Yuan Yirang
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287
The extrapolation for boundary finite elements
Li Kaitai and Yan Ningning
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288
Stochastic growth models
R. Durrett and R. Schonmann
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289
Remarks about equilibrium configurations of crystals
David Kinderlehrer
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290
Eventual C -regularity
and concavity for flows in one-dimensional porous media
D.G. Aronson and J.L. Vazquez
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291
Distributed data structures for scientific computation
L.R. Scott, J.M. Boyle, and B. Bagheri
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292
Simulation of flow in naturally fractured petroleum reservoirs
Jim Douglas, Jr., Paulo J. Paes Leme, Todd Arbogast,
and Tânia Schmitt
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293
Optimal regularity for one-dimensional porous medium flow
D.G. Aronson and L.A. Caffarelli
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294
Liquid crystals and energy estimates for -valued M maps
Haim Brezis
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295
Analysis of the simulation of single phase flow through a naturally fractured
reservoir
Todd Arbogast
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296
The coupling method of finite elements and boundary elements for radiation
problems
He Yinnian and Li Kaitai
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297
Nonlinear effects in wave equation with a cubic restoring force
T. Cazenave, A. Haraux, L. Vazquez, and F.B. Weissler
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298
Some blow-up results for a nonlinear parabolic equation with a gradient term
M. Chipot and F.B. Weissler
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299
Perturbation solutions of simple and double bifurcation problems for Navier-Stokes
equations
Li Kaitai
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300
The convergence on the multigrid algorithm for Navier-Stokes equations
Chen Zhangxin and Li Kaitai
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301
Martingale approach for modeling DNA synthesis
A. Gerardi and G. Nappo
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302
Regular inversion of the divergence operator with Dirichlet boundary conditions
on a polygon
Douglas N. Arnold, L. Ridgway Scott, and Michael Vogelius
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303
Error analysis in ,
for mixed definite element methods for linear and quasi-linear ^M elliptic problems
Ricardo G. Duran
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304
An efficient linear scheme to approximate parabolic free boundary problems:
Error estimates and implementation
Ricardo Nochetto and Claudio Verdi
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305
Nonuniqueness for a hyperbolic system: Cavitation in nonlinear elastodynamics
K.A. Pericak-Spector and Scott J. Spector
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306
q-series and orthogonal polynomials associated with Barnes' first Lemma
E.G. Kalnins and Willard Miller, Jr.
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307
A uniformly accurate finite element method for Mindlin-Reissner plate
Douglas N. Arnold and Richard S. Falk
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308
TVD properties of a class of modified ENO schemes for scalar conservation
laws
Chi-Wang Shu
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309
A random boundary value problem modeling spatial variability in porous media
flow
Edmund Dikow and Ulrich Hornung
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310
Compact attractors and singular perturbations
Jack K. Hale
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311
The
TVD-projection method for solving implicit numeric schemes for scalar conservation
laws: A numerical study of a simple case
A. Bourgeat and B. Cockburn
312
Navier-Stokes computation of transonic vortices over a round leading edge
delta wing
Bernhard Muller and Arthur Rizzi
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313
On the accuracy of vortex methods at large times
J. Thomas Beale
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314
Decomposition methods for adherence problems in finite elasticity
P. Le Tallec and A. Lotfi
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315
Approximation of waves in composite media
Jim Douglas, Jr. and Juan E. Santos
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316
The double porosity model for single phase flow in naturally fractured reservoirs
Todd Arbogast
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317
Two-phase immiscible flow in naturally fractured Reservoirs
Todd Arbogast, Jim Douglas, Jr., and Juan E. Santos
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318
Numerical simulation of immiscible flow in porous media based on combining
the method of characteristics with mixed finite element procedures
Jim Douglas, Jr. and Y. Yirang
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319
Sharp maximum norm error estimates for finite element approximations Of the
Stokes problem in 2-D
R. Durán, R.H. Nochetto, and J. Wan
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320
A phase transition for a system of branching random walks in a random environment
Andreas Greven
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321
Brownian models of open queueing networks with homogeneous customer populations
J.M. Harrison and R.J. Williams
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322
Solutions et mesures invariantes pour des equations d'evolution Stochastiques
du type Navier-Stokes
Ana Bela Cruzeiro
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323
Solutions et mesures invariantes pour des equations d'evolution Stochastiques
du type Navier-Stokes
Ana Bela Cruzeiro
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324
Typical cluster size for 2-dim percolation processes (revised)
Bao Gia Nguyen
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325
Stable defects of minimizers of constrained variational principles
Robert Hardt, David Kinderlehrer, and Fang-Hua Lin
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326
Equilibrium configurations of crystals
Michel Chipot and David Kinderlehrer
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327
Malliavin's C functionals
of a centered Gaussian system
Kiyosi Itô
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328
Derivation of the hydrodynamical equation for one-dimensional Ginzburg-Landau
model
Tadahisa Funaki
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329
Schauder expansion by some quadratic base function
Masaya Yamaguti
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330
Stabilized mixed methods for the Stokes problem
Franco Brezzi and Jim Douglas, Jr.
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331
Inertial manifolds for reaction diffusion equations in higher space dimensions
J. Mallet-Paret and G.R. Sell
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332
Relaxation methods for liquid crystal problems
San-Yih Lin and Mitchell Luskin
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388
The
Runge-Kutta Local Projection P1-Discontinuous-Galerkin Finite Element
Method for Scalar Conservation Laws
Bernardo Cockburn and Chi-Wang Shu
January 1988 - December 1988
Series
389-473 |
460
A quantitative model for lifespan curves
Matthew Witten
January 1989 - December 1989
Series
474-598 |
531
On
the Semilinear Elliptic Equation
in
Jong-Shenq Guo
February 1990 Series
599-624 |
633
Numerical approximation of the solutions of delay differential equations
on an infinite interval using piecewise constant arguments
K.L. Cooke and I. Györi
September 1990 Series
681-708 |
November 1990 Series
709-732 |
December 1990 Series
733-758 |
February 1991 Series
759-783 |
772
Computing centre conditions for certain cubic systems
N.G. Lloyd and J.M. Pearson
March 1991 Series
784 - 791 |
May 1991 Series
792 - 817 |
June 1991 Series
818 - 835 |
August 1991 Series
836 - 872 |
860
Quantum holography and neurocomputer architectures
Walter Schempp
October 1991 Series
873 - 891 |
December 1991 Series
892 - 911 |
February 1992 Series
912 - 932 |
April 1992 Series
933 - 964 |
May 1992 Series
965 - 986 |
July 1992 Series
987 - 1003 |
987
Numerical methods for the regularization of descriptor systems by output
feedback
Angelika Bunse-Gerstner, Volker Mehrmann and Nancy
K. Nichols
August 1992 Series
1004 - 1020 |
September 1992 Series
1021 - 1042 |
November 1992 Series
1043 - 1065 |
1043
Protocol verification using discrete-event systems
Karen Rudie and W. Murray Wonham
1044
Nucleation, kinetics and admissibility criteria for propagating phase boundaries
Rohan Abeyaratne and James K. Knowles
1048
On the computation of suboptimal controllers for unstable infinite dimensional
systems
Onur Toker and Hitay Özbay
1051
A free boundary problem arising in the modeling of interanl oxidation of
binary alloys
Bei Hu and Jianhua Zhang
1055
Multiphase averaging for generalized flows on manifolds
H.S. Dumas, F. Golse, and P. Lochak
1056
Global solutions and quenching to a class of quasilinear parabolic equations
Bei Hu and Hong-Ming Yin
1063
Maximum principle for state-constrained optimal control problems governed
by quasilinear elliptic equations
Eduardo Casas and Jiongmin Yong
1064
Optimal control for degenerate parabolic equations with logistic growth
Suzanne M. Lenhart and Jiongmin Yong
December 1992 Series
1066 - 1093 |
1084
Fluids of differential type: Critical review and thermodynamic analysis
J.E. Dunn and K.R. Rajagopal
January 1993 Series
1094 - 1104 |
March 1993 Series
1105 - 1127 |
April 1993 Series
1128 - 1138 |
June 1993 Series
1139 - 1151 |
July 1993 Series
1152 - 1165 |
September 1993 Series
1166 - 1174 |
October 1993 Series
1175 - 1180 |
November 1993 Series
1181 - 1194 |
1231
Entropy maximization
K.B. Athreya
September 1994
1248 - 1253 |
December 1994
1270 - 1283 |
February 1995
1284 - 1297 |
1316
Soliton's rebuilding in one-dimensional Schrödinger model with polynominal
nonlinearity
Valery E. Grikurov
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1317
On self-similar solutions of the Navier-Stokes equations
J. Necas, M. Ruzicka, and V. Sverák
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1318
Remarks on W2,p-solutions of bilateral obstacle problems
Srdjan Stojanovic
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1319
Pseudospectral vs. finite difference methods of initial value-problems with discontinuous
coeffcients
Erding Luo and Heinz-Otto Kreiss
Download
1320 Soliton's
rebuilding in one-dimensional Schrödinger model with polynominal nonlinearity
Valery E. Grikurov
Download
1321 A multiclass
closed queueing network with unconventional heavy traffic behavior
J.M. Harrison and R.J. Williams
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1322 Microlocal
analysis on Morrey spaces
Michael E. Taylor
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1323 Homogenization
of biharmonic equations in domains perforated with tiny holes
Chaocheng Huang
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1324
An inverse obstacle problem: A uniqueness
theorem for spheres
Changmei Liu
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1325 Approximation
of a laminated microstructure for a rotationally invariant, double well energy
density
Mitchell Luskin
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1326
Haplotyping algorithms
Eric Sobel, Kenneth Lange, Jeffrey R. O'Connell, and
Daniel E. Weeks
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1327
Haplotyping algorithms
Eric Sobel, Kenneth Lange, Jeffrey R. O'Connell, and
Daniel E. Weeks
Download
1328 Haplotyping
algorithms
Eric Sobel, Kenneth Lange, Jeffrey R. O'Connell, and
Daniel E. Weeks
Download
1329 Estimating
the number of asymptotic degrees of freedom for nonlinear dissipative systems
Bernardo Cockburn, Don A. Jones, and Edriss S. Titi
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1330
Inverse Schrödinger scattering on the line with partial knowledge of the
potential
Tuncay Aktosun
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1331 Partition
of the potential of the one-dimensional Schrödinger equation
Tuncay Aktosun and Cornelis van der
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1332
Convergence of the multigrid method with a wavelet coarse grid operator
Bjorn Engquist and Erding Luo
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1333
Ergodic properties of the spin-boson system
V. Jaksic and C.-A. Pillet
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1334 Recursive
solution for diffuse tomographic systems of arbitrary size
S.K. Patch
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1335
Ergodic properties of the spin-boson system
V. Jaksic and C.-A. Pillet
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1336
Bitangential structured interpolation
theory
Juan C. Cockburn
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1337
The blow-up problem for exponential nonlinearities
Satyanad Kichenassamy
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1338 How many
parameters can one solve for in diffuse tomography?
F.A. Grünbaum and S.K. Patch
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1339
Reciprocal relations, bounds and size effects for composites with highly conducting
interface
Robert Lipton
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1340 A global
nonexistence theorem for quasilinear evolution equations with dissipation
Howard A. Levine and James Serrin
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1341 The conjugate
operator meth |