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.
It was shown by Vinogradov (see Theorem 7, Chapter 4 of [18]) that, for ε > 0, there are infinitely many solutions in primes p of the inequality
where {x} denotes the fractional part of x and y = 0.1. The value of γ was improved to
by Kaufman [9]. On the Riemann Hypothesis he showed that one can take γ =¼ The method used actually shows that, for any real β and any δ with 0 < 8 > 1, the number of primes p ≤ x satisfying
is
where π(x) denotes the number of primes not exceeding x. The sequence √p is, of course, a subsequence of the sequence n½ whose distribution modulo one has also been investigated (see Chapter 2, Section 3 of [10]: the argument for sequences nσ (0 < σ < 1) is entirely elementary). It is useful in this context to define the discrepancy (modulo one) of a sequence an by
One of the oldest questions concerning primitive roots is that of the actual order df magnitude of the least positive primitive root m(p) to a large prime modulus p. During the last sixty years the interest of several mathematicians has been attracted by this problem. The history of the major results is too well known to need elaboration. The best known bound for m(p) is due to Wang [8] and Burgess [1] who independently obtained
Let ℱ be a set of m subsets of X = {1,2,…, n}. We study the maximum number λ of containments Y ⊂ Z with Y, Z ∊ ℱ. Theorem 9. , if, and only if, ml/n → 1. When n is large and members of ℱ have cardinality k or k–1 we determine λ. For this we bound (ΔN)/N where ΔN is the shadow of Kruskal's k-cascade for the integer N. Roughly, if m ∼ N + ΔN, then λ ∼ kN with infinitely many cases of equality. A by-product is Theorem 7 of LYM posets.
Let be a smooth projective, geometrically irreducible curve over a finite field . We fix a rational point ∞on , and consider the ring A of functions on regular away from ∞. We set k to be the function field of and k∞ its completion at ∞. After taking algebraic closure we obtain the field whose elements will be called “numbers”.
A linear second order partial differential equation with variable coefficients is considered. The equation is relevant in a number of physical situations. Simple general solutions are obtained subject to the coefficients satisfying certain constraints.
We shall give a simple new proof of the following known theorem [1, 2].
Theorem. The upper density of a packing of translates of a convex disc cannot exceed the density of the densest lattice-packing of these discs.
In [] and [2] this theorem is proved for centrally symmetric discs. The general case can be reduced to this one by applying to the discs the known construction of central symmetrization. Our proof goes in a reverse way. We shall give a direct proof for a special family of asymmetric discs whose centrally symmetric images exhaust the family of centrally symmetric convex discs. Using the properties of the symmetrization, this implies the validity of the theorem for all centrally symmetric discs, and consequently for all convex discs. This procedure of going from a special case to the general one, by applying the symmetrization twice, is illustrated by the following example. The validity of the theorem for a Reuleaux triangle implies its validity for a circle, which implies its validity for any disc of constant width.
Ergodic theory today is a large and rapidly developing subject. The aim of this book is to introduce the reader first to the fundamentals of the ergodic theory of point transformations and then to several advanced topics which are currently undergoing intense research. By selecting one or more of these topics to focus on, a student can quickly approach the specialized literature and indeed the frontier of the area of interest.
Of course the number of interesting topics that we have neglected is necessarily far greater than that of those we have been able to include. Thus we have to refer the reader elsewhere for discussions of, for example, operator ergodic theory, the existence of invariant measures, nonsingular transformations, orbit equivalence, differentiable dynamics, subadditive ergodic theorems, etc. Unfortunately, there do not exist coherent expositions of all of these topics; I invite those of my colleagues who are more expert than I in the areas I have omitted to do some more expository writing.
It should also be understood that, even for the advanced topics that we do discuss, their treatment here cannot be more than an entryway to the rapidly expanding specialized literature. Thus our presentations of multiple recurrence and the Ornstein theory, to mention two examples, are intended as introductions to the books of Furstenberg (1981) and Ornstein (1974), respectively.
Without going into the details (to which the rest of the book is devoted), we mention some of the basic questions, examples, and constructions of ergodic theory, in order to provide an indication of the content and flavor of the subject as well as to establish reference points for terminology and notation. The final section presents a few facts from measure theory and functional analysis that will be used repeatedly.
The basic questions of ergodic theory
Ergodic theory is the mathematical study of the long-term average behavior of systems. The collection of all states of a system forms a space X. The evolution of the system is represented by a transformation T: X → X, where Tx is taken as the state at time 1 of a system which at time 0 is in state x. If one prefers a continuous variable for the time, he can consider a one-parameter family {Tt: t ∈ ℝ} of maps of X into itself. When the laws governing the behavior of the system do not change with time, it is natural to suppose that Ts + t = TsTt so that {Tt: t ∈ ℝ} is a flow, or group action of U on X. A single (invertible) transformation T: X → X also determines the action of a group, namely the integers ℤ, on X.
This chapter presents several further topics concerning recurrence and mixing. First is a direct construction (based on the theory of almost periodic functions) of eigenfunctions for m.p.t.s which are not weakly mixing. The second section presents the purely topological analogues of recurrence, ergodicity, and weak and strong mixing, and the third introduces Furstenberg's theory of multiple recurrence and his proof of the Szemeredi Theorem. In 4.4 we give the Jewett–Bellow–Furstenberg proof of the existence of uniquely ergodic topological representations of ergodic m.p.t.s. The final section examines two examples of weakly mixing m.p.t.s which are not strongly mixing: an example of Kakutani (which we show is not even topologically strongly mixing), and one of Chacon, which is also prime (i.e. without proper invariant sub-σ-algebras). as was discovered by del Junco.
Construction of eigenfunctions
We will give now a more direct proof of the existence of eigenfunctions for m.p.t.s which are not weakly mixing. The idea, apparently due to Varadhan, Furstenberg, and Katznelson, is to reduce the statement to the existence of nontrivial characters on compact abelian groups. However, since this is itself usually proved with the help of the Spectral Theorem for compact operators, we will complete the argument by means of an elementary proof, which also introduces some important ideas from topological dynamics and the theory of almost periodic functions.
This chapter treats several topics in entropy theory that are somewhat beyond the basics. We begin by computing the entropies of automorphisms of the torus, skew products, and induced transformations. The following sections discuss convergence of the information per unit time (Shannon–McMillan–Breiman Theorem) and the topological version of entropy for cascades. We give an introduction to the Ornstein Isomorphism Theorem, which says that two Bernoulli schemes are isomorphic if and only if they have the same entropy. Ornstein's associated theory of sufficient conditions for m.p.t.s to be isomorphic to Bernoulli shifts has produced a surprising list of examples, including classical ones like geodesic maps and automorphisms of the torus, that are metrically indistinguishable from repeated independent random experiments. In the final section we present the Keane–Smorodinsky construction of the isomorphism whose existence is implied by Ornstein's theorem. Their work actually strengthens Ornstein's result, since they are able to construct the isomorphism explicitly, and the map is finitary: each coordinate of the image of a point can be calculated from knowledge of only a finite piece of the history of that point. (Alternatively, the map is a homeomorphism once a set of measure 0 has been deleted). This means that in principle such a coding can actually be carried out mechanically.