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At the end of this chapter, we shall know almost everything about the heat kernel and the Sobolev inequalities associated to a family of Hörmander fields on a nilpotent Lie group.
Later we shall obtain related results in much wider settings. Local questions will be studied on manifolds in Chapter V. Global questions will be studied on unimodular groups (Chapters VI, VII and VIII). We shall, in Chapter IX, even consider non-unimodular Lie groups as far as Sobolev inequalities are concerned.
But it is pleasant to see right away how the semigroup machinery of Chapter II and the considerations of Chapter III about sublaplacians yield complete results in the particular setting of nilpotent groups; this is because, in some sense, the geometry of these groups is not too complicated.
In Section 1 we recall general properties of nilpotent Lie groups, and in Section 2, we give examples. Section 3 is simple, but essential: we obtain for free a powerful scaled Harnack inequality. In Section 4, we show how to estimate the heat kernel with respect to the volume growth, thanks to this Harnack inequality. An analysis of the Lie algebra gives in Section 5 an estimate from above and below of the volume of the ball of radius t. In Sections 6 and 7, we draw fairly complete consequences of all this, using Chapter II; we also introduce a device which yields L1 Sobolev inequalities and which we shall use again later.
This chapter and the next are not concerned with left invariant sublaplacians and their associated heat kernel ht on unimodular Lie groups. Nevertheless, the matters we shall treat are closely related to the main stream of this book. Indeed, in the previous chapter we investigated the behaviour of ||ht||∞ for 0 ≤ t ≤ 1. We would now like to study ||ht||infin; for t ≥ 1. This will be achieved in Chapter VIII, but we are going to attack this problem from a somewhat more general point of view.
Let F(k) be the kth convolution power of F ∈ L1 ∩ L∞. In order to find out the behaviour of ||ht||∞ for t ≥ 1, it suffices to look at hk = h(k), k = 1,2,… Moreover, the function h1 has a rapid decay at infinity since we know that h1(x) ≤ C exp(−cρ2(x)); see V.4.3. It is thus natural to address ourselves to the more general question of the behaviour of ||F(k)||∞, as k tends to infinity, for symmetric, positive compactly supported functions F of integral one.
Clearly enough, the Lie structure is no longer relevant here. Locally compact, unimodular groups which are compactly generated form the natural setting within which we will work. What we will eventually be able to show is that the decay of ||F(k)||∞ (with F as above) is governed by the volume growth of the group.
In this chapter we shall present some of the results which are central and for which we need the full thrust of our methods.
In this paper we obtain new results which relate the number of conjugacy classes of л-elements of a finite group and an arbitrary subgroup, which are analogous to some results about normal subgroups. We also prove some new results which show the relationship between class numbers and splitting theorems. Our proofs only involve elementary techniques.
Prime Malcev superalgebras over fields of characteristic not two and three have been studied by Shestakov [8]. He obtains the remarkable result that if these superalgebras have a nonzero odd part then they are Lie superalgebras. The main purpose of this note is to extend this result to fields of characteristic three. To this aim, it is enough to use adequately a result of Filippov [3]. Commutative and anticommutative superalgebras will be considered too, showing that they are prime, semiprime or simple as superalgebras if and only if they are as algebras. Finally, some conclusions for finite-dimensional semisimple Malcev superalgebras will be deduced. Any such superalgebra is the direct sum of a semisimple Lie superalgebra and a direct sum of simple non-Lie algebras.
We treat the problem of determining a crack inside a conductor when two pairs of current and voltage boundary measurements are given. We prove a theorem of continuous dependence from the data.
The paper is concerned with equations of the form x' = A(t)x +f(t, x), where A is a continuous matrix function defined on ℝ, f is a continuous vector-valued function of (t, x) with f(t, 0) = 0. It is proved that if x' = A(t)x has an exponential trichotomy, A is bounded and f satisfies the Lipschitz condition with coefficient sufficiently small, then these equations are topologically equivalent to the systems of equations of the form , where B, g satisfy the same conditions as A, f.
We give several results which extend our recent proof of the Payne-Pólya–Weinberger conjecture to ratios of higher eigenvalues. In particular, we show that for a bounded domain Ω⊂ℝn the eigenvalues of its Dirichlet Laplacian obey where λm denotes the mth eigenvalue and jp,k denotes the kth positive zero of the Bessel function Jp(x). Certain extensions of this result are given, the most general being the bound where k≧2 and l(m) denotes the number of nodal domains of an mth eigenfunction. Our results imply certain further conjectures of Payne, Pólya, and Weinberger concerning λ3/λ2 and λ4/λ3. In addition, we find a resonably good bound on λ4/λ1. We also briefly discuss extensions to Schrödinger operators and other elliptic eigenvalue problems.
Let B(ℤ)* be the Banach dual of the space of all bounded complex-valued functions on ℤ. For each n ε ℤ, let Ln be the translation operator on B(ℤ) and Tn be its adjoint operator on B(ℤ)*. This paper concerns itself with equations of the form