To save content items to your account,
please confirm that you agree to abide by our usage policies.
If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account.
Find out more about saving content to .
To save content items to your Kindle, first ensure no-reply@cambridge.org
is added to your Approved Personal Document E-mail List under your Personal Document Settings
on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part
of your Kindle email address below.
Find out more about saving to your Kindle.
Note you can select to save to either the @free.kindle.com or @kindle.com variations.
‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi.
‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.
We study the spreading of characteristics for a class of one-dimensional scalar conservation laws for which the flux function has one point of inflection. It is well known that in the convex case the characteristic speed satisfies a one-sided Lipschitz estimate. Using Dafermos' theory of generalized characteristics, we show that the characteristic speed in the non-convex case satisfies an Hölder estimate. In addition, we give a one-sided Lipschitz estimate with an error term given by the decrease of the total variation of the solution.
We study a problem from nonlinear optics that leads to an integro-differential equation which can be written as the abstract bifurcation problem Au = λLu + ∇φ(u). For such a type of equation, a general theorem on the bifurcation of solutions from the essential spectrum is proved. The hypothesis that φ is non-negative (as is usually assumed) could be omitted and replaced by other conditions that allow us to use the results for the particular example. We also indicate applications to semilinear elliptic equations.
In a recent illuminating paper, June M. Parker [5] discussed Choquet integral representations of comonotonic additive functionals and related concepts. In our paper we provide a generalization of the Choquet integral and use this to obtain an integral representation for comonotonic additive operators.
Rings in which each right ideal is quasi-continuous (right π-rings) are shown to be a direct sum of semisimple artinian square full ring and a right square free ring. Among other results it is also shown that (i) a nonlocal right continuous indecomposable right π-ring is either simple artinian or a ring of matrices of a certain type, and (ii) an indecomposable non-local right continuous ring is both a right and a left π-ring if and only if it is a right q-ring. In particular, a non local indecomposable right q-ring is a left q-ring.
In Chapter X §1, we started with three assumptions – three perceptions – about a Brownian particle's trajectory: (i) its direction at any instant cannot be determined; (ii) displacements over disjoint time intervals are unrelated; (iii) ‘statistics’ of displacements over time intervals of equal length are the same. In a framework of probability theory, the strongest interpretation of these perceptions implies that a Brownian particle's position X(t) at time t ∈ [0,1] is Gaussian with mean 0 and variance ct. Specifically, we argued in Chapter X §1 that if Brownian displacements are statistically independent, symmetrically distributed random variables with distributions homogeneous in time, then {X(t) : t ∈ [0,1]} is necessarily a Wiener process (Definition X.1). A Wiener process, however, conveys an idealized view: while haphazard and difficult to predict, Brownian displacements are not, in reality, independent of one another. At the end of Chapter X, imagining Brownian motion to be a random walk, we departed from the classical model, and viewed statistical independence as the first and indeed simplest instance on a scale of stochastic complexity. This view – under assumptions of time-homogeneity, finite variance, and prescribed ‘randomness’ – led us to α-chaos processes. The case α = 1, exemplified by a Wiener process, is a continuous-time model for the simple random walk, and the case α > 1, exemplified for integer α by the Wiener homogeneous chaos, is a continuous-time model for walks that manifest greater levels of ‘randomness’.
The primary purpose of this paper is to provide general sufficient conditions for any real quadratic order to have a cyclic subgroup of order n∈ℕ in its ideal class group. This generalizes results in the literature, including some seminal classical works. This is done with a simpler approach via the interplay between the maximal order and the non-maximal orders, using the underlying infrastructure via the continued fraction algorithm. Numerous examples and a concluding criterion for non-trivial class numbers are also provided. The latter links class number one criteria with new prime-producing quadratic polynomials.
If A is an algebra and ϑ is a congruence on A then A is said to be ϑ-coherent provided that, for every subalgebra B of A, if B contains some ϑ-class then B is a union of ϑ-classes. An algebra A is said to be congruence coherent if it is ϑ-coherent for every ϑ∈>ConA. This notion was investigated by Beazer [2] in the context of de Morgan algebras. Specifically, he showed that a de Morgan algebra is congruence coherent if and only if it is boolean, or simple, or the 4-element de Morgan chain. He also showed that if an algebra in the Berman class K1,1 of Ockham algebras is congruence coherent then it is necessarily a de Morgan algebra; and that a p-algebra is congruence coherent if and only if it is boolean. This notion has also been considered in the context of distributive double p-algebras by Adams, Atallah and Beazer [1] who showed that particular examples of congruence coherent double p-algebras are those that are congruence regular (in the sense that if two congruences have a class in common then they coincide). In this paperNATO Collaborative Research Grant 960153 is gratefully acknowledged. we extend the results of Beazer to the class of double MS-algebras.
First we define the notion of k-Ricci curvature of a Riemannian n-manifold. Then we establish sharp relations between the k-Ricci curvature and the shape operator and also between the k-Ricci curvature and the squared mean curvature for a submanifold in a Riemannian space form with arbitrary codimension. Several applications of such relationships are also presented.
Mise en Scène: A Historical Backdrop and Heuristics
The Wiener process – a stochastic process with independent Gaussian increments – was originally conceived as a probabilistic model for Brownian movement, and has been, ever since, among the most influential mathematical constructs in the twentieth century. For our purposes, we used it in Chapter VI §2 to produce a canonical example of an F2-measure that cannot be extended to an F1-measure. In this chapter and the next, we examine and develop ideas underlying this example.
We begin here with some of the history and heuristics behind Brownian motion and the Wiener process. (In this book, ‘Brownian motion’ or ‘Brownian movement’ will refer always to a physical phenomenon, and the ‘Wiener process’ to Norbert Wiener's mathematical model of it.)
From Brown to Wiener
In the sciences at large, Brownian movement generically refers to haphazard, erratic, difficult-to-predict trajectories of particles. Such movements exhibited by tiny particles suspended in liquid first became known to naturalists in the seventeenth century, soon after the invention of the microscope, and for a long time were thought to be vital – always manifesting life. Refuting that ‘vitality’ was the cause, the botanist Robert Brown recorded in 1827 that erratic movements, such as those observed by his colleagues and predecessors, were in fact performed by inorganic as well as organic particles. He guessed these particles to be nature's most basic constituents, and referred to them as ‘active molecules’ [Br]. Brown almost got it right.
We give a method allowing the generalization of the description of trace spaces of certain classes of holomorphic functions on Carleson sequences to finite unions of Carleson sequences. We apply the result to different classes of spaces of holomorphic functions such as Hardy classes and Bergman type spaces.
We show that if R is a ring such that each minimal left ideal is essential in a (direct) summand of RR, then the dual of each simple right R-module is simple if and only if R is semiperfect with Soc(RR)=Soc(RR) and Soc(Re) is simple and essential for every local idempotent e of R. We also show that R is left CS and right Kasch if and only if R is a semiperfect left continuous ring with Soc(RR)⊆eRR. As a particular case of both results we obtain that R is a ring such that every (essential) closure of a minimal left ideal is summand (R is then said to be left strongly min-CS) and the dual of each simple right R-module is simple if and only if R is a semiperfect left continuous ring with Soc(RR)=Soc(RR)⊆eRR. Moreover, in this case R is also left Kasch, Soc(eR)≠0 for every local idempotent e of R, and R admits a (Nakayama) permutation of a basic set of primitive idempotents. As a consequence of this result we characterise left PF rings in terms of simple modules over the 2×2 matrix ring by showing that R is left PF if and only if M2(R) is a left strongly min-CS ring such that the dual of every simple right module is simple.
A recurring construct in previous chapters was based on this simple blueprint:
given sets E1,…,En and x1 ∈ E1,…,xn ∈ En, form products x1 ⊗ … ⊗xn, and consider the class E1 ⊗…⊗ En comprising all linear combinations of such products.
At the very outset, if nothing is known or assumed about the ‘building blocks’ x1,…,xn, then their product x1⊗…⊗xn is merely a formal object, and not much more can be said. If something is known about E1,…,En, then meaning could be ascribed to x1⊗ … ⊗xn, and analysis of E1 ⊗…⊗En would proceed accordingly. In our specific context, we considered Rademacher functions and their products. We considered the set of independent functions R = {rk} on Ω = {−1, 1}ℕ, and viewed the elements in the n-fold R⊗…⊗R as functions on Ωn. An underlying theme has been that Rademacher functions are basic objects from which all else is constructed, a notion that can be formulated effectively in a framework of harmonic analysis. And that is our purpose in this chapter: to learn and analyze this framework, as it is built from the ground up.
Loosely put, harmonic analysis is about representing general phenomena in terms of familiar phenomena. The subject's beginnings – in the mid-eighteenth century, about ninety years after the invention of the calculus – were rooted in the notion that arbitrary functions could be represented by series of sines and cosines.
We give the residue class, modulo a certain power of p, for the dimension of a primitive interior G-algebra in terms of the dimension of the source algebra. To illustrate, we improve a theorem of Brauer on the dimension of a block algebra.