Constructive Approximation

, Volume 42, Issue 1, pp 93–128 | Cite as

The Hardy Space \(H^1\) in the Rational Dunkl Setting

  • Jean-Philippe Anker
  • Néjib Ben Salem
  • Jacek Dziubański
  • Nabila Hamda
Open Access
Article

Abstract

This paper is perhaps the first attempt at a study of the Hardy space \(H^1\) in the rational Dunkl setting. Following Uchiyama’s approach, we characterize \(H^1\) atomically and by means of the heat maximal operator. We also obtain a Fourier multiplier theorem for \(H^1\). These results are proved here in the one-dimensional case and in the product case.

Keywords

Dunkl theory Heat kernel Hardy space Maximal operator  Atomic decomposition Multiplier 

Mathematics Subject Classification

Primary: 42B30 Secondary: 33C52 33C67 33D67 33D80 35K08 42B25 42C05 

1 Introduction

Dunkl theory is a far reaching generalization of Euclidean Fourier analysis which includes most special functions related to root systems, such as spherical functions on Riemannian symmetric spaces. It started in the late 1980s with Dunkl’s seminal article [7] and developed extensively afterwards. We refer to the lecture notes [18] for the rational Dunkl theory, to the lecture notes [15] for the trigonometric Dunkl theory, and to the books [4, 11] for the generalized quantum theories.

The theory of classical real Hardy spaces in \({\mathbb {R}}^n\) originates from the study of holomorphic functions of one variable in the upper half-plane. We refer the reader to the original works of Stein and Weiss [22], Burkholder et al. [3], and Fefferman and Stein [9]. An important contribution to this theory lies in the atomic decomposition introduced by Coifman [5] and extended to spaces of homogeneous type by Coifman and Weiss [6] (see also [12]). More information can be found in the book [21] and references therein.

This paper deals with the real Hardy space \(H^1\) in the rational Dunkl setting, where the underlying space is of homogeneous type in the sense of Coifman and Weiss. In such a setting, the theory of Hardy spaces goes back to the 1970s [6, 12]. Here we follow Uchiyama’s approach [25], and we characterize the Hardy space \(H^1\) in two ways, by means of the heat maximal operator and atomically. The first characterization, which requires precise heat kernel estimates, has led us to a seemingly new observation, namely that the heat kernel has a rather slow decay in certain directions and is in particular not Gaussian in the present setting (see Remark 2.4). The second characterization is used to prove a Fourier multiplier theorem for \(H^1\).

Throughout the paper, we shall restrict our considerations to the one-dimensional case and to the product case. This restriction is due to our present lack of knowledge in general about the behavior of the Dunkl kernel on the one hand and about generalized translations on the other hand.

Let us introduce some notation and state our main results. On \(\mathbb {R}^n\) we consider the Dunkl operators
$$\begin{aligned} D_jf(\mathbf{x})=\frac{\partial }{\partial x_j} f(\mathbf{x}) +\frac{k_j}{x_j}\left[ f(\mathbf{x})-f(\sigma _j\mathbf{x})\right] \qquad (j\!=\!1,2,\ldots ,n) \end{aligned}$$
associated with the reflections
$$\begin{aligned} \sigma _j(x_1,x_2,\ldots ,x_j,\ldots ,x_n)=(x_1,x_2,\ldots ,-x_j,\ldots ,x_n) \end{aligned}$$
(1.1)
and the multiplicities \(k_j\!\ge 0\). Their joint eigenfunctions constitute the Dunkl kernel
$$\begin{aligned} \mathbf{E}(\mathbf{x},\mathbf{y}) =\prod \nolimits _{j=1}^{\,n}E_{k_j}(x_j,y_j)\,, \end{aligned}$$
(1.2)
where
$$\begin{aligned} E_k(x,y)&= \frac{\Gamma \left( k+\frac{1}{2}\right) }{\Gamma (k)\,\Gamma \left( \frac{1}{2}\right) } \int _{-1}^{+1}\mathrm{d}u\,(1\!-u)^{k-1}(1\!+u)^k\,e^{\,xyu}\nonumber \\&= e^{\,xy} \underbrace{ \frac{\Gamma (2k+1)}{\Gamma (k)\,\Gamma (k+1)}\int _{0}^{\,1}\!\mathrm{d}v v^{k-1}(1\!-v)^k\,e^{-2xyv} }_{{_1F}_{{1}(k;2k+\!1;-2\,xy)}} \end{aligned}$$
(1.3)
(see for instance [18, p. 107, Example 2.1]). Here  \({{}_1}{F_{1}}(a;b;z)\)  is the confluent hypergeometric function which is also known as the Kummer function and denoted by \(M(a,b,z)\). Notice that  \(\mathbf{E}(\mathbf{x},\mathbf{y})=e^{\langle \mathbf{x},\mathbf{y}\rangle }\) if all multiplicities \(k_j\) vanish.
Let us first define the Hardy space \(H^1\) by means of the heat maximal operator. The Dunkl Laplacian
$$\begin{aligned} \mathbf{L}f(\mathbf{x})\!=\!\sum \nolimits _{j=1}^{\,n}D_j^{2}f(\mathbf{x})\!=\!\sum \nolimits _{j=1}^{\,n}\left\{ \!\left( \frac{\partial }{\partial x_j}\!\right) ^2f(\mathbf{x})\!+\!\frac{2k_j}{x_j}\frac{\partial }{\partial x_j}f(\mathbf{x})\!-\!\frac{k_j}{x_j^2}\!\left[ f(\mathbf{x})\!-\!f(\sigma _j\mathbf{x})\!\right] \right\} \end{aligned}$$
is the infinitesimal generator of the heat semigroup
$$\begin{aligned} e^{\,t\,\mathbf{L}}\qquad (t\!>\!0), \end{aligned}$$
which acts by linear self-adjoint operators on \(L^2(\mathbb {R}^n,\mathrm{d}\varvec{\mu })\) and by linear contractions on \(L^p(\mathbb {R}^n,\mathrm{d}\varvec{\mu })\), for every \(1\le p\le \infty \), where
$$\begin{aligned} \mathrm{d}\varvec{\mu }(\mathbf{x}) =\mathrm{d}\mu _1(x_1)\cdots \,\mathrm{d}\mu _n(x_n) =|x_1|^{2k_1}\cdots \,|x_n|^{2k_n}\, \mathrm{d}x_1\cdots \mathrm{d}x_n. \end{aligned}$$
(1.4)
The heat semigroup consists of integral operators
$$\begin{aligned} e^{\,t\mathbf{L}}f(\mathbf{x}) =\int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{y})\, \mathbf{h}_{t}(\mathbf{x},\mathbf{y})\,f(\mathbf{y})\, \end{aligned}$$
associated with the heat kernel
$$\begin{aligned} \mathbf{h}_{t}(\mathbf{x},\mathbf{y})= \mathbf{c}_{\mathbf{k}}^{-1}\,t^{-\frac{\mathbf{N}}{2}}\, e^{-\frac{|\mathbf{x}|^2+|\mathbf{y}|^2}{4\,t}}\, \mathbf{E}\left( \frac{\mathbf{x}}{\sqrt{2t}}, \frac{\mathbf{y}}{\sqrt{2t}}\right) \!\!, \end{aligned}$$
(1.5)
see, e.g., [17], where
$$\begin{aligned} \mathbf{N}=n+\sum \nolimits _{j=1}^{\,n}2\,k_j \end{aligned}$$
(1.6)
is the homogeneous dimension and
$$\begin{aligned} \mathbf{c}_{\mathbf{k}}=\,2^{\frac{\mathbf{N}}{2}}\int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\,e^{-\frac{|\mathbf{x}|^2}{2}}=\,2^{\mathbf{N}}\,\prod \nolimits _{j=1}^{\,n}\Gamma \left( k_j\!+\!\frac{1}{2}\right) . \end{aligned}$$
From this point of view, the Hardy space \(H^1_{\text {max}}\) consists of all functions \(f\!\in \!L^1(\mathbb {R}^n,\mathrm{d}\varvec{\mu })\) whose maximal heat transform
$$\begin{aligned} \mathbf{h}_{*}f(\mathbf{x}) =\sup \nolimits _{\,t>0}\, \left| \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{y})\, \mathbf{h}_{t}(\mathbf{x},\mathbf{y})\,f(\mathbf{y})\right| \end{aligned}$$
(1.7)
belongs to \(L^1(\mathbb {R}^n,\mathrm{d}\varvec{\mu })\) and the norm is given by
$$\begin{aligned} \Vert f\Vert _{H^1_{\text {max}}}=\Vert \mathbf{h}_{*}f\Vert _{L^1(\mathrm{d}\varvec{\mu })}. \end{aligned}$$
Let us turn next to the atomic definition of the Hardy space \(H^1\). Notice that \(\mathbb {R}^n\), equipped with the Euclidean distance \(d(\mathbf{x},\mathbf{y})=|\mathbf{x}\!-\!\mathbf{y}|\) and with the measure \(\varvec{\mu }\), is a space of homogeneous type in the sense of Coifman and Weiss (see Appendix 1). Recall that an atom is a measurable function  \(a:\mathbb {R}^n\!\rightarrow \mathbb {C}\)  such that
  • \(\;a\) is supported in a ball \(\mathbf{B}\),

  • \(\;\Vert a\Vert _{L^\infty }\!\lesssim \varvec{\mu }(\mathbf{B})^{-1}\),

  • \(\;\displaystyle \int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{x})\,a(\mathbf{x})=0\).

By definition, the atomic Hardy space \(H^1_{\text {atom}}\) consists of all functions \(f\!\in \!L^1(\mathbb {R}^n,\mathrm{d}\varvec{\mu })\) that can be written as \(f=\sum _{\ell }\lambda _{\ell }\,a_{\ell }\), where the \(a_\ell \)’s are atoms, the \(\lambda _{\ell }\)’s are complex numbers such that \(\sum _{\ell }|\lambda _{\ell }|\!<\!+\infty \), and the norm is given by
$$\begin{aligned} \Vert f\Vert _{H^1_\text {atom}}=\,\inf \,\sum \nolimits _{\ell }|\lambda _\ell |\,, \end{aligned}$$
where the infimum is taken over all atomic decompositions of \(f\).

Our first main result is the following theorem.

Theorem 1.8

The spaces \(H^1_{\mathrm{max}}\) and \(H^1_{\mathrm{atom}}\) coincide and their norms are equivalent, i.e., there exists a constant  \(C\!>\!0\) such that
$$\begin{aligned} C^{-1}\,\Vert f\Vert _{H^1_{\mathrm{max}}}\le \Vert f\Vert _{H^1_{\mathrm{atom}}}\! \le C\,\Vert f\Vert _{H^1_{\mathrm{max}}}. \end{aligned}$$
The Fourier transform in the Dunkl setting is given by
$$\begin{aligned} {\mathcal {F}}f(\varvec{\xi }) =\mathbf{c}_{\mathbf{k}}^{-1}\! \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\,f(\mathbf{x})\, \mathbf{E}(\mathbf{x},-i\varvec{\xi })\,. \end{aligned}$$
(1.9)
It is an isometric isomorphism of \(L^2(\mathbb {R}^n,\mathrm{d}\varvec{\mu })\) onto itself and the inversion formula reads
$$\begin{aligned} f(\mathbf{x})={\mathcal {F}}^{2}f(-\mathbf{x})\,. \end{aligned}$$
Notice that, if all multiplicities \(k_j\) vanish, then (1.9) boils down to the classical Fourier transform
$$\begin{aligned} \widehat{f}(\varvec{\xi }) =(2\pi )^{-\frac{n}{2}}\!\int _{\mathbb {R}^n}\!\mathrm{d}\mathbf{x}\,f(\mathbf{x})\, e^{-i\langle \mathbf{x},\varvec{\xi }\rangle }\,. \end{aligned}$$
Our second main result is the following Hörmander type multiplier theorem (see [10] for the original multiplier theorem on \(L^p\) spaces).

Theorem 1.10

Let  \(\chi =\chi (\varvec{\xi })\) be a smooth radial function on  \(\mathbb {R}^n\) such that
$$\begin{aligned} \chi (\varvec{\xi })={\left\{ \begin{array}{ll} \,1&{}\text {if }\;|\varvec{\xi }|\!\in \!\left[ \frac{1}{2},2\right] ,\\ \,0&{}\text{ if } \; |\varvec{\xi }|\!\notin \!\left( \frac{1}{4},4\right) .\\ \end{array}\right. } \end{aligned}$$
If a function \(m=m(\varvec{\xi })\) on  \(\mathbb {R}^n\) satisfies
$$\begin{aligned} M=\,\sup \nolimits _{\,t>0}\, \Vert \,\chi \,m(t\,.\,)\Vert _{W_{2}^{\mathbf{N}/2+\epsilon }} <+\infty \end{aligned}$$
for some  \(\epsilon \!>\!0\), then the multiplier operator
$$\begin{aligned} {\mathcal {T}}_{m}f ={\mathcal {F}}^{-1}\{m\,({\mathcal {F}}f)\} \end{aligned}$$
is bounded on the Hardy space \(H^1\) and
$$\begin{aligned} \Vert \,{\mathcal {T}}_{m}\,\Vert _{H^1\rightarrow H^1}\lesssim \,M. \end{aligned}$$
Here \(W_{2}^{\sigma }(\mathbb {R}^n)\) denotes the classical \(L^2\) Sobolev space on \(\mathbb {R}^n\), whose norm is given by
$$\begin{aligned} \Vert g\Vert _{W_{2}^{\sigma }} =\left\{ \,\int _{\mathbb {R}^n}\mathrm{d}\mathbf{x}\, (1\!+\!|\mathbf{x}|^2)^\sigma \,|\widehat{g}(\mathbf{x})|^2\,\right\} ^{1/2}\,. \end{aligned}$$
Notice that the multiplier \(m\) is continuous and bounded, as  \(\frac{\mathbf{N}}{2}+\epsilon >\frac{n}{2}\).

Our paper is organized as follows. Section 2 is devoted to the heat kernel in dimension \(1\). There we analyze its behavior thoroughly, and we remove a small part of it, in order to get Gaussian estimates similar to those in the Euclidean setting. These results are extended to the product case in Sect. 3. Section 4 is devoted to the proof of Theorem 1.8 and Sect. 5 to the proof of Theorem 1.10. Section  consists of three appendices. Appendix 1 contains information about the measure of balls, which is used throughout the paper. Appendices 2 and 3 are devoted to so-called folklore results in connection with Uchiyama’s theorem, which have been used for instance in [8].

This paper results from two independent research projects, which were carried out by the first and third authors and by the second and fourth authors, respectively, and which have been merged into a joint article.

2 Heat Kernel Estimates in Dimension \(1\)

Consider first the one-dimensional Dunkl kernel \(E(x,y)=E_k(x,y)\). As the case \(k=0\) is trivial, we may assume that \(k>0\).

Lemma 2.1

  1. (a)

    \(E(x,y)\) is a holomorphic function of \((x,y)\!\in \!\mathbb {C}^2\).

     
  2. (b)

    \(E(x,y)>0\)  for every  \(x,y\!\in \!\mathbb {R}\).

     
  3. (c)
    \(E(x,y)\) has the following symmetry and rescaling properties :
    $$\begin{aligned} {\left\{ \begin{array}{ll} \,E(x,y)=E(y,x) \qquad \forall \;x,y\!\in \!\mathbb {C},\\ \,E(\lambda x,y)=E(x,\lambda y) \qquad \forall \;\lambda ,x,y\!\in \!\mathbb {C}.\\ \end{array}\right. } \end{aligned}$$
     
  4. (d)
    For every  \(y\!\in \!\mathbb {C}\),  \(x\mapsto E(x,y)\) is an eigenfunction of the Dunkl operator
    $$\begin{aligned} Df(x)=f^{\prime }(x)+\frac{k}{x}\,\{f(x)\!-\!f(-x)\} \end{aligned}$$
    and of the Dunkl Laplacian
    $$\begin{aligned} Lf(x)=D^{2}f(x) =f^{\prime \prime }(x) +\frac{2k}{x}f^{\prime }(x) -\frac{k}{x^2}\,\{f(x)\!-\!f(-x)\}\,. \end{aligned}$$
    More precisely,
    $$\begin{aligned} D_xE(x,y)=y\,E(x,y) \quad \text {and}\quad L_xE(x,y)=y^{2}E(x,y)\,. \end{aligned}$$
     
  5. (e)
    As  \(xy\rightarrow 0\),
    $$\begin{aligned} E(x,y)=1+\mathrm{O}\left( |xy|\right) \,. \end{aligned}$$
     
  6. (f)
    As  \(xy\rightarrow +\infty \),
    $$\begin{aligned} E(x,y)=\frac{2^{k}\,\Gamma (k+\frac{1}{2})}{\sqrt{\pi }}\, e^{xy}\,(xy)^{-k}\, \left\{ 1-\frac{k^2}{2}\frac{1}{xy}+\mathrm{O}\left( \frac{1}{x^2y^2}\right) \right\} \!. \end{aligned}$$
     
  7. (g)
    As  \(xy\rightarrow -\infty \),
    $$\begin{aligned} E(x,y)=\frac{2^{k-1}k\,\Gamma (k+\frac{1}{2})}{\sqrt{\pi }}\, e^{-xy}\,(-xy)^{-k-1}\, \left\{ 1+\frac{k^2-1}{2}\frac{1}{xy}+\mathrm{O}\left( \frac{1}{x^2y^2}\right) \right\} \!. \end{aligned}$$
     

Proof

The first four properties are known to hold in general. In dimension \(1\), they can also be deduced from the explicit expression (1.3), as can (e). As already observed in [20, Section 2] (see also [18, Example 5.1]), the asymptotics of \(E(x,y)\) at infinity follow from the asymptotics of the confluent hypergeometric function which read, let us say for \(0<a<b\),
$$\begin{aligned} {{}_1}{F_{1}}(a;b;z)\sim \frac{\Gamma (b)}{\Gamma (a)}\;e^{\,z}\,z^{a-b}\, \sum \limits _{\ell =0}^{+\infty }\frac{(1-a)_\ell (b-a)_\ell }{\ell \,!}\,z^{-\ell } \end{aligned}$$
as \(z\rightarrow +\infty \) and
$$\begin{aligned} {{}_1}{F_{1}}(a;b;z)\sim \frac{\Gamma (b)}{\Gamma (b-a)}\,|z|^{-a}\, \sum \limits _{\ell =0}^{+\infty }\frac{(a)_\ell (a-b+1)_\ell }{\ell \,!}\,|z|^{-\ell } \end{aligned}$$
as \(z\rightarrow -\infty \) (see for instance [1], (13.5.1)] or [14], (13.7.2)]). \(\square \)
Consider next the one-dimensional heat kernel
$$\begin{aligned} h_{t}(x,y) =\,&c_{k}^{-1}\,t^{-k-\frac{1}{2}}\,e^{-\frac{x^2+y^2}{4t}}E\left( \frac{x}{\sqrt{2t}},\frac{y}{\sqrt{2t}}\right) \nonumber \\ =\,&c_{k}^{-1}\,t^{-k-\frac{1}{2}}\,e^{-\frac{(x-y)^2}{4t}}{{}_1}{F_{1}}\left( k;2k+\!1;-\frac{xy}{t}\right) , \end{aligned}$$
(2.2)
where  \(c_{k}=2^{2k+1}\Gamma \left( k\!+\!\frac{1}{2}\right) \).

Proposition 2.3

  1. (a)

    \(h_{t}(x,y)\) is a  \(C^\infty \) function of  \((t,x,y)\!\in \!(0,+\infty )\!\times \mathbb {R}^2\).

     
  2. (b)

    \(h_{t}(x,y)>0\)  for every  \(t\!>\!0\) and  \(x,y\!\in \!\mathbb {R}\).

     
  3. (c)
    \(h_{t}(x,y)\) has the following symmetry and rescaling properties :
    $$\begin{aligned} {\left\{ \begin{array}{ll} \;h_{t}(x,y)=h_{t}(y,x) \qquad \forall \;x,y\!\in \!\mathbb {R},\\ \;h_{\lambda ^2t}(\lambda x,\lambda y) =|\lambda |^{-2k-1}\,h_{t}(x,y) \qquad \forall \;\lambda \!\in \!\mathbb {R}^*,\,\forall \;t\!>\!0,\,\forall \;x,y\!\in \!\mathbb {R}.\\ \end{array}\right. } \end{aligned}$$
     
  4. (d)
    \(h_{t}(x,y)\) satisfies the heat equation
    $$\begin{aligned} {\left\{ \begin{array}{ll} \;\partial _{t}h_{t}(x,y)=L_yh_{t}(x,y),\\ \;\lim _{\,t\searrow 0}h_{t}(x,y)\,|y|^{2k}dy=\delta _x(y).\\ \end{array}\right. } \end{aligned}$$
     
  5. (e)
    The heat kernel has the following global behavior :
    $$\begin{aligned} h_{t}(x,y)\,\asymp \,{\left\{ \begin{array}{ll} \;t^{-k-\frac{1}{2}}\, e^{-\frac{x^2+y^2}{4t}} &{}\text {if}\;|xy|\!\le t,\\ \;t^{-\frac{1}{2}}\,(xy)^{-k}\, e^{-\frac{(x-y)^2}{4t}} &{}\text {if }\;xy\ge t,\\ \;t^{\frac{1}{2}}\,(-xy)^{-k-1}\, e^{-\frac{(x+y)^2}{4t}} &{}\text {if }\,-xy\ge t,\\ \end{array}\right. } \end{aligned}$$
    and the following asymptotics :
    $$\begin{aligned} h_{t}(x,y)\!=\!{\left\{ \begin{array}{ll} \;c_{k}^{-1}\,t^{-k-\frac{1}{2}}\, e^{-\frac{x^2+y^2}{4t}}\, \left\{ 1+\mathrm{O}\left( \frac{|xy|}{t}\right) \right\} &{}\text {if }\; \frac{xy}{t}\!\rightarrow 0,\\ \;\frac{1}{2\sqrt{\pi }}\;e^{-\frac{(x-y)^2}{4t}}\, t^{-\frac{1}{2}}\,(xy)^{-k}\, \left\{ 1-k^2\frac{t}{xy}+\mathrm{O}\left( \frac{t^2}{x^2y^2}\right) \right\} &{}\text {if}\; \frac{xy}{t}\!\rightarrow \!+\infty ,\\ \;\frac{k}{2\sqrt{\pi }}\;e^{-\frac{(x+y)^2}{4t}}\, t^{\frac{1}{2}}\,(-xy)^{-k-1}\, \left\{ 1+\mathrm{O}\left( -\frac{t}{xy}\right) \right\} &{}\text {if} \; \frac{xy}{t}\!\rightarrow \!-\infty . \end{array}\right. } \end{aligned}$$
     
  6. (f)
    The following gradient estimates hold for the heat kernel :
    $$\begin{aligned}&\left| \frac{\partial }{\partial y}h_{t}(x,y)\right| \\&\lesssim \,{\left\{ \begin{array}{ll} \;t^{-k-\frac{3}{2}}\left( |x|\!+\!|y|\right) \, e^{-\frac{x^2+y^2}{4t}} &{}\text {if }\; |xy|\!\le t,\\ \,\left\{ t^{-\frac{3}{2}}|x\!-\!y| +t^{-\frac{1}{2}}|y|^{-1}\right\} \, (xy)^{-k}\,e^{-\frac{(x-y)^2}{4t}} &{}\text {if }\; xy\ge t,\\ \,\left\{ t^{-\frac{1}{2}}|x\!+\!y| +t^{\frac{1}{2}}(|x|^{-1}\!+|y|^{-1})\right\} \, (-xy)^{-k-1}\, e^{-\frac{(x+y)^2}{4t}} &{}\text {if} \, -xy\ge t.\\ \end{array}\right. } \end{aligned}$$
     

Proof

The first five properties follow from the expression (2.2) and from Lemma 2.1. Let us turn to the proof of (f). By differentiating (2.2) with respect to \(y\) and by using the well-known formula
$$\begin{aligned} \frac{d}{{d}z}{{}_1}{F_{1}}(a;b;z) =\frac{a}{b}{{}_1}{F_{1}}(a+\!1;b+\!1;z) \end{aligned}$$
(see for instance [1], (13.4.8)] or [14], (13.3.15)]), we get
$$\begin{aligned} \frac{\partial }{\partial y}h_{t}(x,y)&= c_{k}^{-1}\,t^{-k-\frac{1}{2}}\,e^{-\frac{(x-y)^2}{4t}}\left\{ \frac{x-y}{2\,t}\,{{}_1}{F_{1}}(k;2k+\!1;-\frac{xy}{t})\right. \\&\left. \qquad \qquad -\frac{k}{2k+1}\frac{x}{t}\, {{}_1}{F_{1}}\left( k+\!1;2k+2;-\frac{xy}{t}\right) \right\} . \end{aligned}$$
We conclude by using again the behavior of the confluent hypergeometric function. \(\square \)

Remark 2.4

It follows from Proposition 2.3(e) and Appendix 1 that
$$\begin{aligned} h_{t}(x,x)\asymp \mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1} \quad \text {and}\quad \,h_{t}(x,-x)\asymp \mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1}\frac{t}{t\,+\,x^2} \end{aligned}$$
for every  \(t\!>\!0\) and  \(x\!\in \!\mathbb {R}\). Observe in particular that the heat kernel has no global Gaussian behavior and decays rather slowly in certain directions. This phenomenon is even more striking in the product case (3.1), where
$$\begin{aligned} \mathbf{h}_{t}(\mathbf{x},{\mathbf{y}})\asymp \varvec{\mu }\big (\mathbf{B}\big (\mathbf{x},\sqrt{t\,}\big )\big )^{-1}\frac{t}{t\;+\,|\mathbf{x}-\mathbf{y}|^2} \end{aligned}$$
if  \(t\!>\!0\), \(\mathbf{x}\!\in \!\mathbb {R}^n\), and  \(\mathbf{y}=(-x_1,x_2,\ldots ,x_n)\).
Let us introduce a variant of the heat kernel with a Gaussian behavior. Given two smooth bump functions \(\chi _1\) and \(\chi _2\) on \(\mathbb {R}\) such that
$$\begin{aligned} {\left\{ \begin{array}{ll} \,0\le \chi _1\!\le \!1,\\ \,\chi _1\!=\!1\text { on }\left[ -1,+\frac{1}{2}\right] ,\\ \,\mathrm{supp }\chi _1\!\subset \!\left[ -2,+\frac{2}{3}\right] , \end{array}\right. } \quad \text {and}\qquad {\left\{ \begin{array}{ll} \,0\le \chi _2\!\le \!1,\\ \,\chi _2\!=\!1\text { on }\left[ 0,+\frac{1}{2}\right] ,\\ \,\mathrm{supp }\chi _2\subset \!\left[ -1,+1\right] , \end{array}\right. } \end{aligned}$$
consider the smooth cutoff function
$$\begin{aligned} \chi _t(x,y)={\left\{ \begin{array}{ll}\, \chi _1\left( \frac{x+y}{x}\right) \,\chi _2\left( \frac{t}{x^2}\right) &{}\text {if }\; x\!\ne \!0\,,\\ 0 &{}\text {if }\; x\!=\!0\,,\\ \end{array}\right. }\end{aligned}$$
and the truncated heat kernel
$$\begin{aligned} H_t(x,y)=\{1-\chi _t(x,y)\}\,h_{t}(x,y), \qquad \forall \;t\!>\!0,\,\forall \;x,y\!\in \!\mathbb {R}. \end{aligned}$$

Remark 2.5

The truncated heat kernel  \(H_t(x,y)\) inherits the following properties of the heat kernel  \(h_{t}(x,y)\) :
  1. (a)

    Smoothness : \(H_{t}(x,y)\) is a  \(C^\infty \) function of  \((t,x,y)\!\in \!(0,+\infty )\!\times \mathbb {R}^2\).

     
  2. (b)

    Nonnegativity : \(H_{t}(x,y)\ge 0\)  for every  \(t\!>\!0\) and  \(x,y\!\in \!\mathbb {R}\).

     
  3. (c)

    Rescaling : \(H_{\lambda ^2t}(\lambda x,\lambda y)=|\lambda |^{-2k-1}H_t(x,y)\)  for every  \(\lambda \!\in \!\mathbb {R}^*\), \(t\!>\!0,\) and  \(x,y\!\in \!\mathbb {R}\).

     
  4. (d)

    Approximation of identity :  \(\lim _{\,t\searrow 0}H_{t}(x,y)\,|y|^{2k}\mathrm{d}y=\delta _x(y)\)  for every  \(x,y\!\in \!\mathbb {R}\).

     

Theorem 2.6

The following estimates hold for the truncated heat kernel  \(H_t(x,y)\).
  1. (a)
    On-diagonal estimate :
    $$\begin{aligned} H_t(x,x)\asymp \mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1} \qquad \forall \;t\!>\!0,\,\forall \;x\!\in \!\mathbb {R}. \end{aligned}$$
     
  2. (b)
    Off-diagonal Gaussian estimate :
    $$\begin{aligned} 0\le H_t(x,y)\lesssim \mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(x-y)^2}{c\,t}} \qquad \forall \;t\!>\!0,\,\forall \;x,y\!\in \!\mathbb {R}. \end{aligned}$$
     
  3. (c)
    Gradient estimate :
    $$\begin{aligned} \left| \frac{\partial }{\partial y}H_t(x,y)\right| \lesssim t^{-\frac{1}{2}}\,\mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(x-y)^2}{c\,t}} \qquad \forall \;t\!>\!0,\,\forall \;x,y\!\in \!\mathbb {R}. \end{aligned}$$
     
  4. (d)
    Lipschitz estimates :
    $$\begin{aligned}\textstyle |H_t(x,y)-H_t(x,y^{\prime })| \lesssim \mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1}\, \frac{|y-y^{\prime }|}{\sqrt{t\,}} \qquad \forall \;t\!>\!0,\,\forall \;x,y,y^{\prime }\in \!\mathbb {R}, \end{aligned}$$
    with the following improvement, if  \(|y\!-\!y^{\prime }|\le \frac{1}{2}\,|x\!-\!y|\) :
    $$\begin{aligned}\textstyle |H_t(x,y)-H_t(x,y^{\prime })| \lesssim \mu \big (B\big (x,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(x-y)^2}{c\,t}}\, \frac{|y-y^{\prime }|}{\sqrt{t\,}}. \end{aligned}$$
     
Here  \(c\) denotes some positive constant and the ball measure has the following behavior, according to Appendix 1 :
$$\begin{aligned} \mu \big (B\big (x,\sqrt{t\,}\big )\big )\asymp {\left\{ \begin{array}{ll} \;t^{\,k+\frac{1}{2}} &{}\text {if} \, |x|\le \!\sqrt{t\,},\\ \,|x|^{2k}\sqrt{t\,} &{}\text {if }\, |x|\ge \!\sqrt{t\,}.\\ \end{array}\right. }\end{aligned}$$
Fig. 1

Cases and subcases considered in the proof of Theorem 2.6(b)

Proof

As far as (a), (b), (c) are concerned, the case \(x=0\) follows immediately from the previous heat kernel estimates. Thus we may assume that \(x\ne 0\) and reduce furthermore to \(x=1\) by rescaling.

(a) is immediate:
$$\begin{aligned} H_t(1,1)=h_{t}(1,1) \asymp \left\{ \begin{matrix} t^{-\frac{1}{2}} &{}\text {if } \, t\le \!1\,\\ \,t^{-k-\frac{1}{2}} &{}\text {if } \, t\ge \!1\,\\ \end{matrix}\right\} \asymp \mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}. \end{aligned}$$
Let us next prove (b) (Fig. 1).
  • Case 1. Assume that \(|y|\!\le t\).

    \(\circ \)  Subcase 1.1. Assume that \(t\) is bounded above, say \(t\le \!\frac{1}{2}\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{-k-\frac{1}{2}}\,e^{-\frac{1+y^2}{4t}}\! =t^{-\frac{1}{2}}\,e^{-\frac{(1-y)^2}{8t}}\, t^{-k}\,e^{-\frac{1+y^2}{8t}}\,e^{-\frac{y}{4t}} \end{aligned}$$
    is bounded above by
    $$\begin{aligned} \mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1} \,e^{-\frac{(1-y)^2}{8t}} \end{aligned}$$
    as  \(t^{\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\),  \(t^{-k}\lesssim e^{\frac{1}{8t}}\le e^{\frac{1+y^2}{8t}}\), and \(e^{\frac{y}{4t}}\asymp 1\). \(\circ \)  Subcase 1.2. Assume that \(t\) is bounded below, say \(t\ge \!\frac{1}{2}\). Then
    $$\begin{aligned} H_t(1,y) \le h_{t}(1,y) \asymp t^{-k-\frac{1}{2}}\,e^{-\frac{1+y^2}{4t}}\! =t^{-k-\frac{1}{2}}\,e^{-\frac{(1-y)^2}{4t}}\,e^{-\frac{y}{2t}} \end{aligned}$$
    with  \(t^{k+\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\) and  \(e^{\frac{y}{2t}}\asymp 1\).
  •  Case 2. Assume that \(y\) is close to \(-x=\!-1\), say \(-2\le y\le \!-\frac{1}{2}\).

    \(\circ \)  Subcase 2.1. If \(t\le \!\frac{1}{2}(\le \!-y)\), then
    $$\begin{aligned} H_t(1,y)=0\,. \end{aligned}$$
    \(\circ \)  Subcase 2.2. If \(t\) is bounded below, say \(t\ge \!\frac{1}{2}\), we argue as in Subcase 1.2.
  •  Case 3. Assume that \(y\ge t\).

    \(\circ \)  Subcase 3.1. Assume that t is bounded below, say \((y\!\ge )t\!\ge \!\frac{1}{2}\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{-\frac{1}{2}}\,y^{-k}\,e^{-\frac{(1-y)^2}{4t}}\le t^{-k-\frac{1}{2}}\,e^{-\frac{(1-y)^2}{4t}} \end{aligned}$$
    with  \(t^{k+\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\).
    \(\circ \)  Subcase 3.2. Assume that \(y\ge \!\frac{1}{2}\!\ge t\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{-\frac{1}{2}}\,y^{-k}\,e^{-\frac{(1-y)^2}{4t}}\lesssim t^{-\frac{1}{2}}\,e^{-\frac{(1-y)^2}{4t}} \end{aligned}$$
    with  \(t^{\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\).
    \(\circ \)  Subcase 3.3. Assume that \(t\le y\le \!\frac{1}{2}\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{-\frac{1}{2}}\,y^{-k}\,e^{-\frac{(1-y)^2}{4t}} \end{aligned}$$
    is bounded above by
    $$\begin{aligned} \mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1} \,e^{-\frac{(1-y)^2}{8t}} \end{aligned}$$
    as  \(t^{\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\) and  \(y^{-k}\le t^{-k}\lesssim e^{\frac{1}{32\,t}}\le e^{\frac{(1-y)^2}{8t}}\).
  •  Case 4. Assume that \(y\le \!-t\,(<\!0)\) and that \(y\) stays away from \(-1\), say \(y\!\notin \!\left( -2, -\frac{1}{2}\right) \). Notice that \((1\!+\!y)^2\!\ge \!\frac{(1-\,y)^2}{9}\)  if and only if  \(y\!\notin \!\left( -2, -\frac{1}{2}\right) \).

    \(\circ \)  Subcase 4.1. Assume that \(2\le t\le \!-y\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{\frac{1}{2}}\,(-y)^{-k-1}\,e^{-\frac{(1+y)^2}{4t}}\! \le t^{-k-\frac{1}{2}}\,e^{-\frac{(1-y)^2}{36\,t}} \end{aligned}$$
    with  \(t^{k+\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\).
    \(\circ \)  Subcase 4.2. Assume that \(t\le 2\le \!-y\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{\frac{1}{2}}\,(-y)^{-k-1}\,e^{-\frac{(1+y)^2}{4t}}\! \lesssim t^{-\frac{1}{2}}\,e^{-\frac{(1-y)^2}{36\,t}} \end{aligned}$$
    with  \(t^{\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\).
    \(\circ \)  Subcase 4.3. Assume that \(t\le \!-y\le \frac{1}{2}\). Then
    $$\begin{aligned} H_t(1,y)\le h_{t}(1,y)\asymp t^{\frac{1}{2}}\,(-y)^{-k-1}\,e^{-\frac{(1+y)^2}{4t}}\! \le t^{-k-\frac{1}{2}}\,e^{-\frac{(1+y)^2}{8t}}\,e^{-\frac{(1-y)^2}{72\,t}} \end{aligned}$$
    is bounded above by
    $$\begin{aligned} \mu (B(1,\sqrt{t\,}))^{-1}\,e^{-\frac{(1-y)^2}{72\,t}} \end{aligned}$$
    as  \(t^{\frac{1}{2}}\asymp \mu (B(1,\sqrt{t\,}))\) and  \(t^{-k}\lesssim e^{\frac{1}{32\,t}}\le e^{\frac{(1+y)^2}{8t}}\).
The proof of (c) follows the same pattern. To begin with, observe that the derivative
$$\begin{aligned}\textstyle \frac{\partial }{\partial y}\bigl \{1\!-\underbrace{ \chi _1(1\!+y)\,\chi _2(t) }_{\chi _{t}(1,y)}\bigr \} =-\,\chi _1^{\prime }(1\!+y)\,\chi _2(t) \end{aligned}$$
of the cut-off is bounded and vanishes unless  \(y\in \!\left( -3,-2\right) \cup \left( -\frac{1}{2},0\right) \)  and  \(t\le \!1\). According to the subcases 1.1, 4.2, and 4.3 above, the contribution of  \(\frac{\partial }{\partial y}\left\{ 1-\chi _{t}(1,y)\right\} \, h_{t}(1,y)\) to \(\frac{\partial }{\partial y}H_t(1,y)\) is bounded by
$$\begin{aligned} \mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{c\,t}} \le t^{-\frac{1}{2}}\,\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{c\,t}}. \end{aligned}$$
Thus it remains to estimate the contribution of  \(\{1-\chi _{t}(1,y)\} \,\frac{\partial }{\partial y}h_{t}(1,y)\).
  •  Case 1. Assume that \(|y|\!\le t\).

    \(\circ \)  Subcase 1.1. Assume that \(t\le \!\frac{1}{2}\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim t^{-k-\frac{3}{2}}(1\!+\!|y|)\,e^{-\frac{1+y^2}{4t}}\!\\&\lesssim \overbrace{ t^{-k-\frac{1}{2}}e^{-\frac{1+y^2}{8t}}e^{-\frac{y}{4t}} }^{\text {bounded}}t^{-1}e^{-\frac{(1-y)^2}{8t}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{8t}}. \end{aligned}$$
    \(\circ \)  Subcase 1.2. Assume that \(t\ge \!\frac{1}{2}\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim t^{-k-\frac{3}{2}}(1\!+|y|)\, e^{-\frac{1+y^2}{4t}}\\&\!\lesssim t^{-k-1}e^{-\frac{(1-y)^2}{8t}} \overbrace{ \left( \frac{1+y^2}{t}\right) ^{\frac{1}{2}}e^{-\frac{1+y^2}{8t}}e^{-\frac{y}{4t}} }^{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{8t}}. \end{aligned}$$
  •  Case 2. Assume that \(-2\le y\le \!-\frac{1}{2}\).

    \(\circ \)  Subcase 2.1. If \(t\le \!\frac{1}{2}(\le \!-y)\), then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \frac{\partial }{\partial y}h_{t}(1,y)=0\,. \end{aligned}$$

    \(\circ \)  Subcase 2.2. If \(t\) is bounded below, say \(t\ge \!\frac{1}{2}\), we argue as in Subcase 1.2.

  •  Case 3. Assume that \(y\ge t\).

    \(\circ \)  Subcase 3.1. Assume that \((y\!\ge )t\!\ge \!\frac{1}{2}\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim \left\{ t^{-\frac{3}{2}}|1-\!y|+t^{-\frac{1}{2}}y^{-1}\right\} \,y^{-k}\,e^{-\frac{(1-y)^2}{4t}}\\&\lesssim t^{-k-1}\,e^{-\frac{(1-y)^2}{8t}} \underbrace{\left\{ 1+\frac{|1-y|}{\sqrt{t\,}}\,e^{-\frac{(1-y)^2}{8t}} \right\} }_{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{8t}}. \end{aligned}$$
    \(\circ \)  Subcase 3.2. Assume that \(y\ge \!\frac{1}{2}\!\ge t\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim \left\{ t^{-\frac{3}{2}}|1-\!y|+t^{-\frac{1}{2}}y^{-1}\right\} \,y^{-k}\,e^{-\frac{(1-y)^2}{4t}}\\&\lesssim t^{-1}\,e^{-\frac{(1-y)^2}{8t}} \underbrace{\left\{ \sqrt{t\,}\! +\frac{|1-y|}{\sqrt{t\,}}\,e^{-\frac{(1-y)^2}{8t}} \right\} }_{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{8t}}. \end{aligned}$$
    \(\circ \)  Subcase 3.3. Assume that \(t\le y\le \!\frac{1}{2}\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim \left\{ t^{-\frac{3}{2}}|1-\!y|+t^{-\frac{1}{2}}y^{-1}\right\} \,y^{-k}\,e^{-\frac{(1-y)^2}{4t}}\\&\lesssim t^{-1}\,e^{-\frac{(1-y)^2}{8t}} \underbrace{ t^{-k-\frac{1}{2}}\,e^{-\frac{1}{32t}} }_{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{8t}}. \end{aligned}$$
  •  Case 4. Assume that \(y\le \!-t\,(<\!0)\) and that \(y\!\notin \!\left( -2, -\frac{1}{2}\right) \). Recall that \((1\!+\!y)^2\!\ge \!\frac{(1-\,y)^2}{9}\)  if and only if  \(y\!\notin \!\left( -2, -\frac{1}{2}\right) \).

    \(\circ \)  Subcase 4.1. Assume that \(2\le t\le \!-y\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim \left\{ t^{-\frac{1}{2}}|1+\!y|+t^{\frac{1}{2}}\frac{1+|y|}{|y|}\right\} \, |y|^{-k-1}\,e^{-\frac{(1+y)^2}{4t}}\\&\lesssim t^{-k-1}\,e^{-\frac{(1+y)^2}{8t}} \underbrace{\frac{|1+y|}{\sqrt{t\,}}\, e^{-\frac{(1+y)^2}{8t}}}_{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{72\,t}}. \end{aligned}$$
    \(\circ \)  Subcase 4.2. Assume that \(t\le 2\le \!-y\). Then
    $$\begin{aligned} \{1-\chi _{t}(1,y)\}\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim \left\{ t^{-\frac{1}{2}}|1+\!y|+t^{\frac{1}{2}}\frac{1+|y|}{|y|}\right\} \, |y|^{-k-1}\,e^{-\frac{(1+y)^2}{4t}}\\&\lesssim t^{-1}\,e^{-\frac{(1+y)^2}{8t}} \underbrace{\left\{ \frac{|1+y|}{\sqrt{t\,}}\,e^{-\frac{(1+y)^2}{8t}}\! +\sqrt{t}\right\} }_{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{72\,t}}. \end{aligned}$$
    \(\circ \)  Subcase 4.3. Assume that \(t\le \!-y\le \frac{1}{2}\). Then
    $$\begin{aligned} \chi _{t}(1,y)\, \left| \frac{\partial }{\partial y}h_{t}(1,y)\right|&\lesssim \left\{ t^{-\frac{1}{2}}|1+\!y|+t^{\frac{1}{2}}\frac{1+|y|}{|y|}\right\} \, |y|^{-k-1}\,e^{-\frac{(1+y)^2}{4t}}\\&\lesssim t^{-1}\,e^{-\frac{(1+y)^2}{8t}} \underbrace{ t^{-k-\frac{1}{2}}\,e^{-\frac{1}{32t}} }_{\text {bounded}}\\&\lesssim t^{-\frac{1}{2}}\mu \big (B\big (1,\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{(1-y)^2}{72\,t}}. \end{aligned}$$
Finally, (d) is an immediate consequence of (c). For every \(y^{\prime \prime }\in \![\,y,y^{\prime }]\), we have indeed
$$\begin{aligned} e^{-\frac{(x-y^{\prime \prime })^2}{c\,t}}\le 1\,. \end{aligned}$$
Moreover, if \(|y\!-\!y^{\prime }|\!\le \!\frac{1}{2}|x\!-\!y|\), then \(|x\!-\!y^{\prime \prime }|\ge |x\!-\!y|-|y\!-\!y^{\prime \prime }|\ge |x\!-\!y|-|y\!-\!y^{\prime }|\ge \frac{1}{2}|x\!-\!y|\), hence
$$\begin{aligned} e^{-\frac{(x-y^{\prime \prime })^2}{ct}} \le e^{-\frac{(x-y)^2}{4ct}}\,. \end{aligned}$$
\(\square \)

Remark 2.7

Contrarily to \(h_{t}(x,y)\), \(H_t(x,y)\) is not symmetric in the space variables \(x,y\). Nevertheless, according to the following result, we may replace \(\mu (B(x,\sqrt{t\,}))\) by \(\mu (B(y,\sqrt{t\,}))\) in the estimates (b), (c) and in the second estimate (d).

Lemma 2.8

For every \(\varepsilon \!>\!0\), there exists \(C\!>\!0\) such that
$$\begin{aligned} \frac{\mu \big (B\big (x,\sqrt{t}\big )\big )}{\mu \big (B\big (y,\sqrt{t}\big )\big )}\le C\,e^{\,\varepsilon \frac{(x-y)^2}{t}}, \qquad \forall \;x,y\!\in \!\mathbb {R}, \,\forall \;t\!>\!0. \end{aligned}$$

Proof

By rescaling (see Appendix 1), we can reduce to the case \(t=\!1\). The estimate
$$\begin{aligned} \frac{\mu (B(x,1))}{\mu (B(y,1))}\lesssim \,e^{\varepsilon (x-y)^2} \end{aligned}$$
is obvious if \(x\) and \(y\) are bounded or if \(|x|/|y|\) is bounded from above. In the remaining case, let us say, when \(|x|\!\ge \!1\!+2|y|\), we have \(|x|\le |x\!-\!y|+|y|\le |x\!-\!y|+\frac{1}{2}\left| x\right| \), hence \(|x|\le 2\,|x\!-\!y|\). Furthermore, as \(|x\!-\!y|\ge |x|-|y|\ge 1\), we have \(|x|\le 2\,(x\!-\!y)^2\). Thus
$$\begin{aligned} \frac{\mu (B(x,1))}{\mu (B(y,1))}\lesssim \mu (B(x,1))\asymp (|x|\!+\!1)^{2k}\lesssim \,e^{\,\frac{\varepsilon }{2}|x|} \lesssim \,e^{\,\varepsilon (x-y)^2}. \end{aligned}$$
\(\square \)

The next proposition, which will be used in the proof of Theorem 1.8, shows that the truncated heat kernel \(H_t(x,y)\) captures the main features of the heat kernel \(h_{t}(x,y)\).

Proposition 2.9

The maximal operator
$$\begin{aligned} Q_*f(x)=\sup \nolimits _{t>0}\, \left| \int _{\mathbb {R}}\mathrm{d}\mu (y)\,Q_t(x,y)\,f(y)\right| , \end{aligned}$$
associated with the error
$$\begin{aligned} Q_t(x,y) =h_{t}(x,y)-H_t(x,y) =\chi _{t}(x,y)\,h_{t}(x,y) \ge 0\,, \end{aligned}$$
is bounded from \(L^1(\mathbb {R},\mathrm{d}\mu )\) into itself.

Proof

It suffices to check that
$$\begin{aligned} \sup \nolimits _{\,y\in \mathbb {R}}\int _{\mathbb {R}}\mathrm{d}\mu (x)\, \sup \nolimits _{\,t>0}Q_t(x,y)<+\infty \,. \end{aligned}$$
The case \(y=0\) is trivial, as \(\chi _{t}(x,0)\) and hence \(Q_t(x,0)\) vanish, for every \(t\!>\!0\) and \(x\!\in \!\mathbb {R}\). Consider next the case \(y\!\in \!\mathbb {R}^*\), which reduces to \(y=1\) by rescaling. Then \(\chi _{t}(x,1)\) and \(Q_t(x,1)\) vanish, unless  \(t\!<\!9\) and \(-3\!<\!x\!<\!-\frac{1}{3}\), and in this range (see Proposition 2.3)
$$\begin{aligned} h_{t}(x,1)\asymp t^{\frac{1}{2}}\,e^{-\frac{(x+1)^2}{4t}} \end{aligned}$$
is bounded. Hence
$$\begin{aligned} \int _{\mathbb {R}}\mathrm{d}\mu (x)\,\sup \nolimits _{\,t>0}Q_t(x,1) \lesssim \int _{-3}^{-\frac{1}{3}}\mathrm{d}x\, \sup \nolimits _{\,0<t<9}h_{t}(x,1) <+\infty \,. \end{aligned}$$
\(\square \)

3 Heat Kernel Estimates in the Product Case

According to (1.5) and (1.2), the heat kernel in the product case splits up into one-dimensional heat kernels:
$$\begin{aligned} {\mathbf{h}}_{t}(\mathbf{x},{\mathbf{y}}) =\prod \nolimits _{j=1}^{\,n}h_{\,t}^{(j)}(x_j,y_j)\,. \end{aligned}$$
(3.1)
By expanding
$$\begin{aligned} h_{\,t}^{(j)}(x_j,y_j)=\,\underbrace{ \{1\!-\chi _{t}(x_j,y_j)\}\,h_{\,t}^{(j)}(x_j,y_j) }_{H_{\,t}^{(j)}(x_j,\,y_j)}\, +\,\underbrace{ \chi _{t}(x_j,y_j)\,h_{\,t}^{(j)}(x_j,y_j) }_{Q_{\,t}^{(j)}(x_j,\,y_j)}\,, \end{aligned}$$
we get
$$\begin{aligned} {\mathbf{h}}_{t}(\mathbf{x},{\mathbf{y}}) ={\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}}) +{\mathbf{P}}_{t}(\mathbf{x},{\mathbf{y}}). \end{aligned}$$
Here
$$\begin{aligned} {\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}}) =\prod \nolimits _{j=1}^{\,n}H_{\,t}^{(j)}(x_j,y_j) \end{aligned}$$
and \({\mathbf{P}}_{t}(\mathbf{x},{\mathbf{y}})\) is the sum of all possible products
$$\begin{aligned} \widetilde{\mathbf{P}}_{t}(\mathbf{x},{\mathbf{y}}) =\prod \nolimits _{j=1}^{\,n}p_{\,t}^{(j)}(x_j,y_j)\,, \end{aligned}$$
where each factor \(p_{\,t}^{(j)}(x_j,y_j)\) is equal to \(H_{\,t}^{(j)}(x_j,y_j)\) or \(Q_{\,t}^{(j)}(x_j,y_j)\), and at least one factor \(p_{\,t}^{(j)}(x_j,y_j)\) is equal to \(Q_{\,t}^{(j)}(x_j,y_j)\). Notice the rescaling property
$$\begin{aligned} {\mathbf{h}}_{\lambda ^2t}(\lambda \mathbf{x},\lambda {\mathbf{y}}) =|\lambda |^{-\mathbf{N}}\,{\mathbf{h}}_{t}(\mathbf{x},{\mathbf{y}}) \qquad \forall \;\lambda \!\in \!\mathbb {R}^*,\,\forall \;t\!>\!0, \,\forall \;\mathbf{x},\mathbf{y}\!\in \!\mathbb {R}^n, \end{aligned}$$
and similarly for the other product kernels. The following estimates follow from the one-dimensional case (see Theorem 2.6 and Remark 2.7).

Theorem 3.2

  1. (a)
    On-diagonal estimate :
    $$\begin{aligned} {\mathbf{H}}_{t}(\mathbf{x},\mathbf{x})\asymp \varvec{\mu }\big (\mathbf{B}\big (\mathbf{x},\sqrt{t\,}\big )\big )^{-1}, \qquad \forall \;t\!>\!0,\,\forall \;\mathbf{x}\!\in \!\mathbb {R}^n. \end{aligned}$$
     
  2. (b)
    Off-diagonal Gaussian estimate :
    $$\begin{aligned} 0\le {\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}}) \lesssim \varvec{\max }\left\{ \varvec{\mu }\big (\mathbf{B}\big (\mathbf{x},\sqrt{t\,}\big )\big ), \varvec{\mu }\big (\mathbf{B}\big ({\mathbf{y}},\sqrt{t\,}\big )\big )\right\} ^{-1}\, e^{-\frac{|\mathbf{x}-{\mathbf{y}}|^2}{c\,t}} \end{aligned}$$
    for every  \(t\!>\!0\) and for every  \(\mathbf{x},\mathbf{y}\!\in \!\mathbb {R}^n\).
     
  3. (c)
    Gradient estimate :
    $$\begin{aligned} |\nabla _{\mathbf{y}} {\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}})| \lesssim t^{-\frac{1}{2}}\, \varvec{\max }\left\{ \varvec{\mu }\big (\mathbf{B}\big (\mathbf{x},\sqrt{t\,}\big )\big ), \varvec{\mu }\big (\mathbf{B}\big ({\mathbf{y}},\sqrt{t\,}\big )\big )\right\} ^{-1}\, e^{-\frac{|\mathbf{x}-{\mathbf{y}}|^2}{c\,t}} \end{aligned}$$
    for every  \(t\!>\!0\) and  \(\mathbf{x},\mathbf{y}\!\in \!\mathbb {R}^n\).
     
  4. (d)
    Lipschitz estimates :
    $$\begin{aligned} |{\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}})-{\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}}^{\prime })| \lesssim \varvec{\mu }\big (\mathbf{B}\big (\mathbf{x},\sqrt{t\,}\big )\big )^{-1}\, \frac{|{\mathbf{y}}-{\mathbf{y}}^{\varvec{\prime }}|}{\sqrt{t\,}}\,, \end{aligned}$$
    for every  \(t\!>\!0\) and  \(\mathbf{x},\mathbf{y},\mathbf{y}^{\varvec{\prime }}\in \!\mathbb {R}^n\), with the following improvement, if  \(|{\mathbf{y}}\!-\!{\mathbf{y}}^{\varvec{\prime }}|\le \frac{1}{2}\,|\mathbf{x}\!-\!{\mathbf{y}}|\) :
    $$\begin{aligned} |{\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}})-{\mathbf{H}}_{t}(\mathbf{x},{\mathbf{y}}^{\varvec{\prime }})| \lesssim \varvec{\max }\left\{ \varvec{\mu }\big (\mathbf{B}\big (\mathbf{x},\sqrt{t\,}\big )\big ), \varvec{\mu }\big (\mathbf{B}\big ({\mathbf{y}},\sqrt{t\,}\big )\big )\right\} ^{-1} e^{-\frac{|\mathbf{x}-{\mathbf{y}}|^2}{c\,t}} \frac{|{\mathbf{y}}-{\mathbf{y}}^{\varvec{\prime }}|}{\sqrt{t\,}}. \end{aligned}$$
     

Let us turn to the analog of Proposition 2.9 in the product case.

Proposition 3.3

The maximal operator
$$\begin{aligned} {\mathbf{P}}_{*}f(\mathbf{x}) =\sup \nolimits _{t>0}\, \left| \int _{\mathbb {R}^n}\!\mathrm{d}{\varvec{\mu }}({\mathbf{y}})\, {\mathbf{P}}_t(\mathbf{x},{\mathbf{y}})\,f({\mathbf{y}})\,\right| \end{aligned}$$
is bounded from \(L^1(\mathbb {R}^n,\mathrm{d}{\varvec{\mu }})\) into itself.

Proof

We will show again that
$$\begin{aligned} \sup \nolimits _{\,{\mathbf{y}}\in \mathbb {R}^n} \int _{\mathbb {R}^n}\!\mathrm{d}{\varvec{\mu }}(\mathbf{x})\, \sup \nolimits _{\,t>0}{\mathbf{P}}_{t}(\mathbf{x},{\mathbf{y}})\, <\,+\infty \,, \end{aligned}$$
but the proof will be more involved in the product case than in the one-dimensional case. Let us begin with some observations. First of all, by using the symmetries
$$\begin{aligned} H_{\,t}^{(j)}(x_j,y_j)=H_{\,t}^{(j)}(-x_j,-y_j) \quad \text {and}\quad Q_{\,t}^{(j)}(x_j,y_j)=Q_{\,t}^{(j)}(-x_j,-y_j) \end{aligned}$$
and by interchanging variables, we may reduce to products of the form
$$\begin{aligned} \widetilde{\mathbf{P}}_{t}(\mathbf{x},{\mathbf{y}}) =\underbrace{Q_{\,t}^{(1)}(x_1,y_1)\cdots \, Q_{\,t}^{(n^{\prime })}(x_{n^{\prime }},y_{n^{\prime }}) }_{{\mathbf{Q}}_{t}^{\prime } (\mathbf{x}^{\prime },{\mathbf{y}}^{\prime })} \underbrace{ H_{\,t}^{(n^{\prime }+1)} (x_{n^{\prime }+1},y_{n^{\prime }+1}) \cdots \,H_{\,t}^{(n)}(x_n,y_n) }_{{\mathbf{H}}_{t}^{\prime \prime } (\mathbf{x}^{\prime \prime },{\mathbf{y}}^{\prime \prime })}, \end{aligned}$$
where \(1\le n^{\prime }\!\le n\) and \(0\le y_1\!\le {\cdots }\le y_{n^{\prime }}\). Next we may assume that, for every \(1\le j\le n^{\prime }\),
$$\begin{aligned} y_j\!>0\,,\quad -3y_j\!<x_j\!<\!-\frac{1}{3}y_j \quad \text {and}\quad x_j^2>t, \end{aligned}$$
because otherwise \(\chi _{t}(x_j,y_j)\) and hence \(Q_{\,t}^{(j)}(x_j,y_j)\) vanish. By rescaling, we may reduce to the case \(y_1\!=\!1\). Consequently, \(t\) is bounded by \(x_1^{2}\!<9\,y_1^{2}\!=9\) and each factor \(Q_{\,t}^{(j)}(x_j,y_j)\) is bounded by
$$\begin{aligned} t^\frac{1}{2}\,(-x_jy_j)^{-k_j-1}\,e^{-\frac{(x_j+y_j)^2}{4\,t}}\, \mathrm{1}\mathrm{I}_{\,\left( -3y_j,-\frac{1}{3}y_j\right) }(x_j)\, \lesssim \,t^\frac{1}{2}\,y_j^{-2k_j-2}\, \mathrm{1}\mathrm{I}_{\,\left( -3y_j,-\frac{1}{3}y_j\right) }(x_j)\,. \end{aligned}$$
Thus, on the one hand, the integral
$$\begin{aligned}\begin{aligned} {\mathbf{I}}^{\prime }({\mathbf{y}}^{\prime })&=\int _{\mathbb {R}^{n^\prime }}\! \mathrm{d}{\varvec{\mu }}^{\prime }(\mathbf{x}^{\prime })\, \sup \nolimits _{\,t>0}t^{-\frac{n'}{2}}{\mathbf{Q}}_{\,t}^{\prime } (\mathbf{x}^{\prime },{\mathbf{y}}^{\prime })\\&\lesssim \int _{-3}^{-\frac{1}{3}}\mathrm{d}\mu _1(x_1)\, y_2^{-2k_2-2}\! \int _{-3y_2}^{-\frac{1}{3}y_2} d\mu _2(x_2)\;\cdots \; y_{n^{\prime }}^{-2k_{n^\prime }-2}\! \int _{-3y_{n^{\prime }}}^{-\frac{1}{3}y_{n^{\prime }}} \mathrm{d}\mu _{ n^{\prime }}(x_{n^{\prime }}) \end{aligned}\end{aligned}$$
is bounded, uniformly in \({\mathbf{y}}^{\prime }\). On the other hand, let us prove the uniform boundedness of
$$\begin{aligned} {\mathbf{I}}^{\prime \prime }({\mathbf{y}}^{\prime \prime })=\int _{\mathbb {R}^{n^{\prime \prime }}} \mathrm{d}{\varvec{\mu }}^{\prime \prime }(\mathbf{x}^{\prime \prime })\, \sup \nolimits _{\,0<t<9} t^{\frac{n^\prime }{2}}\,{\mathbf{H}}_{\,t}^{\prime \prime } (\mathbf{x}^{\prime \prime },{\mathbf{y}}^{\prime \prime })\,, \end{aligned}$$
when \(n^{\prime \prime }\!=n-n^{\prime }\!>\!0\). For this purpose, let us deduce from the Gaussian estimate
$$\begin{aligned} {\mathbf{H}}_{\,t}^{\prime \prime } \left( \mathbf{x}^{\prime \prime }\!,{\mathbf{y}}^{\prime \prime }\right) \lesssim \varvec{\mu }^{\prime \prime }\big (\mathbf{B}\big ({\mathbf{y}}^{\prime \prime },\sqrt{t\,}\big )\big )^{-1}\, e^{-\frac{|\mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }|^2}{c\,t}} \end{aligned}$$
that
$$\begin{aligned} \sup \nolimits _{\,0<t<9\,} t^{\frac{n^\prime }{2}}\,{\mathbf{H}}_{\,t}^{\prime \prime } \left( \mathbf{x}^{\prime \prime },{\mathbf{y}}^{\prime \prime }\right) \lesssim \, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \; \varvec{\mu }^{\prime \prime }\big (\mathbf{B} \big ({\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \big )\big )^{-1}\, e^{-\frac{|\mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }|^2}{18\,c}}. \end{aligned}$$
Assume first that \(\left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \ge \!\sqrt{t}\) with \(0\!<\!t\!<\!9\). Then, by using (6.2),
$$\begin{aligned}&t^{\frac{n^\prime }{2}}\,{\mathbf{H}}_{\,t}^{\prime \prime } \left( \mathbf{x}^{\prime \prime },{\mathbf{y}}^{\prime \prime }\right) \lesssim t^{\frac{n^\prime }{2}}\frac{\varvec{\mu }^{\prime \prime } \big (\mathbf{B}\big ({\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| \big )\big )}{\varvec{\mu }^{\prime \prime } \big (\mathbf{B}\big ({\mathbf{y}}^{\prime \prime },\sqrt{t}\big )\big )}\, \varvec{\mu }^{\prime \prime } \big (\mathbf{B}\big ({\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \big )\big )^{-1}\, e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{c\,t}}\\&\qquad \lesssim \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \underbrace{\left( \frac{\left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| }{\sqrt{t\,}} \right) ^{\mathbf{N}^{\prime \prime }}e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{2\,c\,t}}}_{\lesssim \,1} \varvec{\mu }^{\prime \prime } \big (\mathbf{B}\big ({\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \big )\big )^{-1} e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{18\,c}}. \end{aligned}$$
Assume next that \(0<|\mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }| \le \!\sqrt{t}\,(\le 3)\). Then, by using (6.2) again,
$$\begin{aligned}&t^{\frac{n^\prime }{2}}\,{\mathbf{H}}_{\,t}^{\prime \prime } \left( \mathbf{x}^{\prime \prime },{\mathbf{y}}^{\prime \prime }\right) \lesssim t^{\frac{n^\prime }{2}} \overbrace{\frac{\varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| \right) \right) }{\varvec{\mu }^{\prime \prime }\left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime },\sqrt{t}\right) \right) } }^{\lesssim \;\left( \frac{\left| \mathbf{x}^{\prime \prime } \!-{\mathbf{y}}^{\prime \prime }\right| }{\sqrt{t\,}}\right) ^{n^{\prime \prime }}}\varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \right) \right) ^{-1} \overbrace{ e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{c\,t}} }^{\asymp \;1}\\&\qquad \lesssim \underbrace{ t^{\frac{n^\prime \!-1}{2}} }_{\lesssim \;1}\underbrace{ \left( \frac{\left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| }{\sqrt{t\,}}\right) ^{n^{\prime \prime }-1} }_{\lesssim \;1}\left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \; \varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \right) \right) ^{-1}\underbrace{ e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{18\,c}} }_{\asymp \;1}. \end{aligned}$$
Now that we have estimated \(t^{\frac{n^\prime }{2}}{\mathbf{H}}_{\,t}^{\prime \prime } \left( \mathbf{x}^{\prime \prime }, {\mathbf{y}}^{\prime \prime }\right) \), let us split up the integral
$$\begin{aligned} {\mathbf{I}}^{\prime \prime }({\mathbf{y}}^{\prime \prime }) =\sum \nolimits _{j\in \mathbb {Z}}{\mathbf{I}}_{j}^{\prime \prime } \left( {\mathbf{y}}^{\prime \prime }\right) \end{aligned}$$
according to the decomposition  \(\mathbb {R}^{n^{\prime \prime }}\backslash \!\{0\}\!=\!\bigsqcup _{\,j\in \mathbb {Z}}\underbrace{ \left\{ \mathbf{x}^{\prime \prime }\!\in \!\mathbb {R}^{n^{\prime \prime }}| \,\,2^{\,j-\frac{1}{2}}\!\!\le \!|\mathbf{x}^{\prime \prime }\!-\!\mathbf{y}^{\prime \prime }| \!<\!2^{\,j+\frac{1}{2}}\right\} }_{\Omega _j}\). Let us show that
$$\begin{aligned} |\,{\mathbf{I}}_{j}^{\prime \prime } ({\mathbf{y}}^{\prime \prime })| \lesssim 2^{-|j|}\,. \end{aligned}$$
If  \(j\ge 0\), we have indeed
$$\begin{aligned} {\mathbf{I}}_{j}^{\prime \prime } \left( {\mathbf{y}}^{\prime \prime }\right)&\lesssim \int _{\Omega _j} \mathrm{d}{\varvec{\mu }}^{\prime \prime }\left( \mathbf{x}^{\prime \prime }\right) \underbrace{ \varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \right) \right) ^{-1} }_{\asymp \;\varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime }, 2^{j}\right) \right) ^{-1}} \underbrace{ \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \, e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{18\,c}} }_{\lesssim \;2^{-j}}\\&\lesssim \underbrace{\frac{\varvec{\mu }^{\prime \prime }\left( \Omega _j\right) }{\varvec{\mu }^{\prime \prime }\left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime },2^{j}\right) \right) } }_{\lesssim \;1}2^{-j}, \end{aligned}$$
and, if  \(j\le 0\),
$$\begin{aligned} {\mathbf{I}}_{j}^{\prime \prime } \left( {\mathbf{y}}^{\prime \prime }\right)&\lesssim \int _{\Omega _j} \mathrm{d}{\varvec{\mu }}^{\prime \prime }\left( \mathbf{x}^{\prime \prime }\right) \underbrace{ \varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime }, \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| \right) \right) ^{-1} }_{\asymp \;\varvec{\mu }^{\prime \prime } \left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime },2^{j}\right) \right) ^{-1}} \underbrace{ \left| \mathbf{x}^{\prime \prime } -{\mathbf{y}}^{\prime \prime }\right| }_{\lesssim \;2^{j}} \underbrace{ e^{-\frac{\left| \mathbf{x}^{\prime \prime }-{\mathbf{y}}^{\prime \prime }\right| ^2}{18\,c}} }_{\lesssim \;1}\\&\lesssim \underbrace{\frac{\varvec{\mu }^{\prime \prime }\left( \Omega _j\right) }{\varvec{\mu }^{\prime \prime }\left( \mathbf{B}\left( {\mathbf{y}}^{\prime \prime },2^{j}\right) \right) } }_{\lesssim \;1}2^{\,j}. \end{aligned}$$
By summing up over \(j\!\in \!\mathbb {Z}\), we obtain the uniform boundedness of \({\mathbf{I}}^{\prime \prime } \left( {\mathbf{y}}^{\prime \prime }\right) \). \(\square \)

4 Proof of Theorem 1.8

Theorem 1.8 relies on the following result due to Uchiyama [25].

Theorem 4.1

Assume that a set  \(X\) is equipped with
  • a quasi-distance \(\widetilde{d}\), i.e., a distance except that the triangular inequality is replaced by the weaker condition
    $$\begin{aligned} \widetilde{d}(x,y)\le A\,\{\widetilde{d}(x,z)+\widetilde{d}(z,y)\} \qquad \forall \;x,y,z\!\in \!X, \end{aligned}$$
  • a measure  \(\mu \) whose values on quasi-balls satisfy
    $$\begin{aligned} \frac{r}{A}\le \mu \left( \widetilde{B}(x,r)\right) \le r \qquad \forall \;x\!\in \!X,\,\forall \;r\!>\!0\,, \end{aligned}$$
  • a continuous kernel  \(K_r(x,y)\!\ge \!0\) such that, for every  \(r\!>\!0\) and  \(x,y,y^{\prime }\in \!X\),

  • \(\circ \)\(K_r(x,x)\ge \frac{1}{Ar}\) ,

  • \(\circ \)\(K_r(x,y)\le r^{-1}\left( 1+\frac{\widetilde{d}(x,y)}{r} \right) ^{-1-\delta }\) ,

  • \(\circ \)\(\left| K_r(x,y)-K_r(x,y^{\prime })\right| \le r^{-1}\left( 1+\frac{\widetilde{d}(x,y)}{r}\right) ^{-1-2\delta }\left( \frac{\widetilde{d}(y,y^{\prime })}{r}\right) ^{\delta }\) when  \(\widetilde{d}(y,y^{\prime })\! \le \!\frac{r+\widetilde{d}(x,y)}{4A}\) .

Here  \(A\!\ge \!1\) and  \(\delta \!>\!0\). Let us introduce the following definitions :
  • an atom is a measurable function  \(a:X\!\rightarrow \mathbb {C}\) such that
    $$\begin{aligned} a \; is\; supported \; in \; a \; quasi{\text{- }}ball \,\widetilde{B} , \,\Vert a\Vert _{L^\infty (X,\, \mathrm{d}\mu )}\lesssim \mu (\widetilde{B})^{-1} and \, \displaystyle \int _Xd\mu a=0, \end{aligned}$$
  • the atomic Hardy space \(H^1_\mathrm{atom}(X,\mu ,\widetilde{d}\,)\) consists of all functions  \(f\!\in \!L^1(X,\mathrm{d}\mu )\) which can be written as
    $$\begin{aligned} f=\sum \nolimits _{\ell }\lambda _{\ell }\,a_{\ell }\,, \end{aligned}$$
    (4.2)
    where the \(a_{\ell }\)’s are atoms and the \(\lambda _{\ell }\)’s are complex numbers such that \(\sum _{\ell }|\lambda _{\ell }|\!<\!+\infty \),
  • the atomic norm is given by
    $$\begin{aligned} \Vert f\Vert _{H^1_\mathrm{atom}(X,\mu ,\widetilde{d}\,)} =\,\inf \;\sum \nolimits _{\ell }|\lambda _{\ell }|\,, \end{aligned}$$
    (4.3)
    where the infimum is taken over all representations (4.2),
  • the maximal Hardy space \(H^1_\mathrm{max}(X,\mu ,K_r)\) consists of all functions  \(f\!\in \!L^1(X,\mathrm{d}\mu )\) such that
    $$\begin{aligned} K_*f(x)=\sup \nolimits _{\,r>0}\, \left| {\displaystyle \int _X}\mathrm{d}\mu (y)\,K_r(x,y)\,f(y)\,\right| \end{aligned}$$
    belongs to \(L^1(X,\mathrm{d}\mu )\).
Then  \(H^1_\mathrm{atom}(X,\mu ,\widetilde{d}\,)\) coincides with  \(H^1_\mathrm{max}(X,\mu ,K_r)\), and (4.3) is comparable to the maximal norm \(\Vert K_*f\Vert _{L^1(X,\, d\mu )}\).
We now adapt Uchiyama’s Theorem to our setting. For \(X\!=\mathbb {R}^n\), equipped with the Euclidean distance  \(d(\mathbf{x},\mathbf{y})=|\mathbf{x}-\mathbf{y}|\) and the measure (1.4), set
$$\begin{aligned} \widetilde{d}(\mathbf{x},\mathbf{y}) =\inf \varvec{\mu }(\mathbf{B}) \qquad \forall \;\mathbf{x},\mathbf{y}\!\in \!\mathbb {R}^n, \end{aligned}$$
where the infimum is taken over all closed balls  \(\mathbf{B}\) containing \(\mathbf{x}\) and \(\mathbf{y}\), and
$$\begin{aligned} K_r(\mathbf{x},\mathbf{y}) =\mathbf{H}_{t}(\mathbf{x},\mathbf{y}), \qquad \forall \;r\!>\!0,\,\forall \;\mathbf{x},\mathbf{y}\!\in \!\mathbb {R}^n, \end{aligned}$$
(4.4)
where  \(t=t(\mathbf{x},r)\) is defined by \(\varvec{\mu }\left( \mathbf{B}\left( \mathbf{x},\sqrt{t}\right) \right) =r\). In Appendices 2 and 3, we check that \(\left( X,\varvec{\mu }, \widetilde{d}, K_r\right) \) satisfy the assumptions of Uchiyama’s theorem with  \(\delta =\frac{1}{\mathbf{N}}\). Actually the conditions in Theorem 4.1 are obtained up to constants, and they can be achieved by considering suitable multiples of \(\varvec{\mu }\) and \(K_r(\mathbf{x},\mathbf{y})\). Thus the conclusion of Uchiyama’s theorem holds for the quasi-distance \(\widetilde{d}\) and for the maximal operator \(K_*\).
On the one hand, \(d\) and \(\widetilde{d}\) define the same atomic Hardy space \(H^1_\mathrm{atom}\), with equivalent norms, as balls and quasi-balls are comparable. Let us elaborate. For every \(\mathbf{x},\mathbf{y}\!\in \!\mathbb {R}^n\) and \(t\!>\!0\), we have
$$\begin{aligned} |\mathbf{x}-\mathbf{y}|\le \sqrt{t\,} \quad \Longrightarrow \quad \widetilde{d}(\mathbf{x},\mathbf{y})\le r \quad \Longrightarrow \quad |\mathbf{x}-\mathbf{y}|\lesssim \sqrt{t\,}\,, \end{aligned}$$
where \(r=\varvec{\mu }\left( \mathbf{B}\left( \mathbf{x},\sqrt{t\,}\right) \right) \). The first implication is an immediate consequence of the definition of \(\widetilde{d}\) and the second one is obtained by combining Lemma 6.4(b) in Appendix 2 with (6.2) in Appendix 1. Hence, there exists a constant \(c\!>\!0\) such that
$$\begin{aligned} \mathbf{B}(\mathbf{x},\sqrt{t\,}) \subset \widetilde{\mathbf{B}}(\mathbf{x},r) \subset \mathbf{B}(\mathbf{x},c\sqrt{t\,}), \end{aligned}$$
and these sets have comparable measures, according to Appendix 1.
On the other hand, the maximal operators \(K_*\) and \(\mathbf{H}_{*}\) coincide, and they define the same maximal Hardy space \(H^1_\mathrm{max}\), with equivalent norms, as the heat maximal operator \(\mathbf{h}_{*}\)  (see (1.7)), according to Propositions 2.9 and 3.3. Indeed, for every \(f\!\in \!L^1(\mathbb {R}^n,d\varvec{\mu })\), the integrals
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\;\mathbf{h}_{*}f(\mathbf{x}) \quad \text {and}\quad \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\;\mathbf{H}_{*}f(\mathbf{x}) \end{aligned}$$
differ at most by a multiple of  \(\Vert f\Vert _{L^1({\mathbb {R}}^n,\, d\varvec{\mu })}\), which is itself controlled by either integral above, as  \(\mathbf{h}_{t}(\mathbf{x},\mathbf{y})\,\mathrm{d}\varvec{\mu }(\mathbf{y})\) and \(\mathbf{H}_{t}(\mathbf{x},\mathbf{y})\,\mathrm{d}\varvec{\mu }(\mathbf{y})\) are approximations of the identity.

In conclusion, the atomic Hardy space \(H^1_\mathrm{atom}\) associated with Euclidean balls coincides with the Hardy space \(H^1_\mathrm{max}\) defined by the heat maximal operator \(\mathbf{h}_{*}\). \(\square \)

5 Proof of Theorem 1.10

The proof of Theorem 1.10 requires some weighted estimates in Dunkl analysis, which are well-known in the Euclidean setting corresponding to \(\mathbf{k}=\mathbf{0}\). Let us first prove a weak analog of the Euclidean estimate
$$\begin{aligned} \Vert (1\!+\!|\varvec{\xi }|)^\sigma \widehat{f}(\varvec{\xi })\Vert _{L^1(d\varvec{\xi })}\lesssim \Vert f\Vert _{W_{2}^{\sigma +n/2+\epsilon }}\,. \end{aligned}$$

Lemma 5.1

For every  \(\ell \!\in \!\mathbb {N}\) and  \(r\!>\!0\), there is a constant  \(C=C_{\ell ,r}\!>\!0\) such that
$$\begin{aligned} \sup \nolimits _{\,\varvec{\xi }\in \mathbb {R}^n}(1\!+\!|\varvec{\xi }|)^\ell \,|{\mathcal {F}}f(\varvec{\xi })| \le C\,\Vert f\Vert _{C^\ell } \end{aligned}$$
for every  \(f\!\in \!C^\ell (\mathbb {R}^n)\) with  \(\mathrm{supp }f\!\subset \mathbf{B}(0,r)\).

Proof

By using the Riemann–Lebesgue lemma for the Fourier transform (1.9), we get
$$\begin{aligned} \sup \nolimits _{\,\varvec{\xi }\in \mathbb {R}^n}(1\!+\!|\varvec{\xi }|)^\ell \,|{\mathcal {F}}f(\varvec{\xi })|&\lesssim \,\sup \nolimits _{\,\varvec{\xi }\in \mathbb {R}^n} \left( 1+\sum \nolimits _{j=1}^{\,n}|\xi _j|^\ell \right) \, |{\mathcal {F}}f(\varvec{\xi })|\\&\le \,\Vert f\Vert _{L^1(\mathrm{d}\varvec{\mu })}+\sum \nolimits _{j=1}^{\,n} \Vert D_j^{\ell }f\Vert _{L^1(\mathrm{d}\varvec{\mu })}\,. \end{aligned}$$
The last expression is bounded by \(\Vert f\Vert _{C^\ell }\) as, by induction on \(\ell \), \(\mathrm{supp }( D_j^{\ell }f)\!\subset \!B(0,r)\) and \(\Vert D_j^{\ell }f\Vert _{L^\infty }\! \lesssim \Vert f\Vert _{C^\ell }.\)\(\square \)

Corollary 5.2

For every  \(\ell \!\in \!\mathbb {N}\), \(r\!>\!0\), and  \(\epsilon \!>\!0\), there is a constant  \(C=C_{\ell ,r,\epsilon }\!>\!0\) such that
$$\begin{aligned} \Vert (1\!+\!|\varvec{\xi }|)^{\ell -\mathbf{N}/2-\epsilon } {\mathcal {F}}f(\varvec{\xi })\Vert _{L^2(\mathrm{d}\varvec{\mu }(\varvec{\xi }))}\le C\,\Vert f\Vert _{W_{2}^{\ell +n/2+\epsilon }}\,, \end{aligned}$$
for every  \(f\!\in \!W_{2}^{\ell +n/2+\epsilon }(\mathbb {R}^n)\) with  \(\mathrm{supp }f\!\subset \mathbf{B}(0,r)\), where  \(\mathbf{N}\) denotes the homogeneous dimension (1.6).

Proof

This result is deduced from Lemma 5.1, by using on the left-hand side the finiteness of the integral
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\varvec{\xi })\, (1\!+\!|\varvec{\xi }|)^{-\mathbf{N}-2\epsilon } \end{aligned}$$
and on the right-hand side the Euclidean Sobolev embedding theorem. \(\square \)

Proposition 5.3

For every  \(\sigma \!>\!0\), \(r\!>\!0\), and  \(\epsilon \!>\!0\), there is a constant  \(C=C_{\sigma ,r,\epsilon }\!>\!0\) such that
$$\begin{aligned} \Vert (1\!+\!|\varvec{\xi }|)^\sigma {\mathcal {F}}f(\varvec{\xi })\Vert _{L^2(\mathrm{d}\varvec{\mu }(\varvec{\xi }))}\le C\,\Vert f\Vert _{W_{2}^{\sigma +\epsilon }} \end{aligned}$$
for every  \(f\!\in \!W_{2}^{\sigma +\epsilon }(\mathbb {R}^n)\) with  \(\mathrm{supp }f\!\subset \mathbf{B}(0,r)\).

Proof

Let \(\chi \!\in \!C_c^\infty (\mathbb {R}^n)\). Following an argument due to Mauceri and Meda [13], this result is obtained by interpolation between the \(L^2\) estimate
$$\begin{aligned} \Vert {\mathcal {F}}(\chi f)\Vert _{L^2(\mathrm{d}\varvec{\mu })}=\mathrm{const. }\Vert \chi f\Vert _{L^2(\mathrm{d}\varvec{\mu })} \lesssim \Vert f\Vert _{L^2(\mathrm{d}\mathbf{x})}, \end{aligned}$$
which is deduced from Plancherel’s formula, and the following estimate for \(\ell \!\in \!\mathbb {N}\) large, which is deduced from Corollary 5.2:
$$\begin{aligned} \Vert (1\!+\!|\varvec{\xi }| )^{\ell -\mathbf{N}/2-\epsilon ^{\prime }}{\mathcal {F}}(\chi f)(\varvec{\xi })\Vert _{L^2(\mathrm{d}\varvec{\mu }(\varvec{\xi }))} \lesssim \Vert \chi f\Vert _{ W_{2}^{\ell +n/2+\epsilon ^{\prime }}} \lesssim \Vert f\Vert _{ W_{2}^{\ell +n/2+\epsilon ^{\prime }}}. \end{aligned}$$
\(\square \)

By using the Cauchy–Schwarz inequality, we deduce finally the following result.

Corollary 5.4

For every  \(\sigma \!>\!0\), \(r\!>\!0\), and  \(\epsilon \!>\!0\), there is a constant  \(C=C_{\sigma ,r,\epsilon }\!>\!0\) such that
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\varvec{\xi })\, (1\!+\!|\varvec{\xi }|)^\sigma \,|{\mathcal {F}}f(\varvec{\xi })| \le C\,\Vert f\Vert _{ W_{2}^{\sigma +\mathbf{N}/2+\epsilon }} \end{aligned}$$
for every  \(f\!\in \! W_{2}^{\sigma +\mathbf{N}/2+\epsilon }(\mathbb {R}^n)\) with  \(\mathrm{supp }f\!\subset \mathbf{B}(0,r)\).
Let us next prove analogs in the Dunkl setting of the Euclidean estimates
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\mathbf{x}\, (1\!+\!|\mathbf{x}|)^\delta \,|f*g(\mathbf{x})|\, \le \int _{\mathbb {R}^n}\!\mathrm{d}\mathbf{z}\, (1\!+\!|\mathbf{z}|)^\delta \,|f(\mathbf{z})|\, \int _{\mathbb {R}^n}\!\mathrm{d}\mathbf{y}\, (1\!+\!|\mathbf{y}|)^\delta \,|g(\mathbf{y})| \end{aligned}$$
and
$$\begin{aligned} \int _{\mathbb {R}^n\backslash \mathbf{B}(\mathbf{y},r)}\mathrm{d}\mathbf{x}\, |f(\mathbf{x}\!-\!\mathbf{y})|\,\lesssim \,r^{-\delta }\; \Vert (1\!+\!|\mathbf{x}|)^\delta f(\mathbf{x})\Vert _{L^1(\mathrm{d}\mathbf{x})}\,. \end{aligned}$$
Recall that Dunkl translations are defined via the Fourier transform (1.9) by
$$\begin{aligned} (\tau _{\mathbf{y}}f)(\mathbf{x}) =\mathbf{c}_{\mathbf{k}}^{-1}\! \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\varvec{\xi })\,{\mathcal {F}}f(\mathbf{\varvec{\xi }})\, \mathbf{E}(\mathbf{x},i\varvec{\xi })\, \mathbf{E}(\mathbf{y},i\varvec{\xi }) \end{aligned}$$
(see [17, 19, 23, 24]) and have an explicit integral representation
$$\begin{aligned} (\tau _{\mathbf{y}}f)(\mathbf{x})=\int _{\mathbb {R}^n} \mathrm{d}\varvec{\nu }_{\mathbf{x},\mathbf{y}}(\mathbf{z})\, f(\mathbf{z}) \end{aligned}$$
in dimension \(1\) (see [2, 16, 23]) and hence in the product case. Specifically,
$$\begin{aligned} \mathrm{d}\varvec{\nu }_{\mathbf{x},\mathbf{y}}(\mathbf{z}) =d\nu _{x_1,y_1}^{(1)}(z_1)\cdots \, \mathrm{d}\nu _{x_n,y_n}^{(n)}(z_n)\,, \end{aligned}$$
where
$$\begin{aligned} \mathrm{d}\nu _{x_j,y_j}^{(j)}(z_j)\, =\,{\left\{ \begin{array}{ll} \,\nu _j(x_j,y_j,z_j)\,|z_j|^{2k_j}\mathrm{d}z_j &{}\text {if }\, x_j,y_j\!\in \mathbb {R}^*,\\ \,\mathrm{d}\delta _{y_j}(z_j) &{}\text {if }\, x_j\!=0,\\ \,\mathrm{d}\delta _{x_j}(z_j) &{}\text {if} \, y_j\!=0, \end{array}\right. } \end{aligned}$$
and
$$\begin{aligned}\begin{aligned} \nu _j(x_j,y_j,z_j)\,&=\frac{\Gamma (k_j+\frac{1}{2})}{\sqrt{\pi }\,2^{2k_j}\Gamma (k_j)}\, \frac{(x_j+y_j+z_j)(-x_j+y_j+z_j)(x_j-y_j+z_j)}{x_jy_jz_j}\\&\quad \times \tfrac{\left\{ \left( |x_j|+|y_j|+|z_j|\right) \left( -|x_j|+|y_j|+|z_j|\right) \left( |x_j|-|y_j|+|z_j|\right) \left( |x_j|+|y_j|-|z_j|\right) \right\} ^{k_j-1}}{|x_jy_jz_j|^{2k_j-1}}\\&\quad \times \mathrm{1}\mathrm{I}_{\,\left[ \left| |x_j|-|y_j|\right| , |x_j|+|y_j|\right] }(|z_j|) \,. \end{aligned}\end{aligned}$$
Thus  \(\varvec{\nu }_{\mathbf{x},\mathbf{y}}\) is a signed measure which is supported in the product
$$\begin{aligned} \varvec{{\mathcal {I}}}_{\mathbf{x},\mathbf{y}} ={\mathcal {I}}_{x_1,y_1} \times \cdots \times \, {\mathcal {I}}_{x_n,y_n} \end{aligned}$$
of the one-dimensional sets
$$\begin{aligned} {\mathcal {I}}_{x_j,y_j}&=\left\{ z_j\!\in \!\mathbb {R}\,| \left| |x_j|-|y_j|\right| \le |z_j|\le |x_j|+|y_j|\right\} \\&=\left[ -|x_j|\!-\!|y_j|,-\left| |x_j|\!-\!|y_j|\right| \right] \cup \left[ \left| |x_j|\!-\!|y_j|\right| ,|x_j|\!+\!|y_j|\right] \end{aligned}$$
and which is generically given by
$$\begin{aligned} \mathrm{d}\varvec{\nu }_{\mathbf{x},\mathbf{y}}(\mathbf{z}) =\underbrace{\nu _1(x_1,y_1,z_1)\cdots \,\nu _n(x_n,y_n,z_n)}_{ \varvec{\nu }(\mathbf{x},\mathbf{y},\mathbf{z})}\, \mathrm{d}\varvec{\mu }(\mathbf{z})\,. \end{aligned}$$
Moreover, it is known (see [2, 16, 23]) that
$$\begin{aligned} \sup \nolimits _{\,\mathbf{x},\mathbf{y}\in \mathbb {R}^n}|\varvec{\nu }_{\mathbf{x},\mathbf{y}}|(\mathbb {R}^n) <+\infty \,. \end{aligned}$$

Lemma 5.5

For every  \(\delta \ge 0\), \(L^1((1\!+\!|\mathbf{x}|)^\delta \mathrm{d}\varvec{\mu }(\mathbf{x}))\) is an algebra with respect to the Dunkl convolution product
$$\begin{aligned} f*g(\mathbf{x}) =\!\int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{y})\, (\tau _{-\mathbf{y}}f)(\mathbf{x})\,g(\mathbf{y}). \end{aligned}$$

Proof

By using the symmetries
$$\begin{aligned} \varvec{\nu }(\mathbf{x},-\mathbf{y},\mathbf{z}) =\varvec{\nu }(-\mathbf{z},-\mathbf{y},-\mathbf{x}) =\varvec{\nu }(\mathbf{z},\mathbf{y},\mathbf{x})\,, \end{aligned}$$
we have
$$\begin{aligned} f*g(\mathbf{x}) =\!\int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{z})\,f(\mathbf{z}) \int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{y})\,g(\mathbf{y})\, \varvec{\nu }(\mathbf{z},\mathbf{y},\mathbf{x})\,. \end{aligned}$$
We conclude by estimating
$$\begin{aligned} \int _{\varvec{{\mathcal {I}}}_{\mathbf{z},\mathbf{y}}} \mathrm{d}\varvec{\mu }(\mathbf{x})\,\left( 1\!+\!\left| \mathbf{x}\right| \right) ^\delta \, \left| \varvec{\nu }(\mathbf{z},\mathbf{y},\mathbf{x})\right| \lesssim \left( 1\!+\!\left| \mathbf{z}\right| \right) ^\delta \left( 1\!+\!\left| \mathbf{y}\right| \right) ^\delta . \end{aligned}$$
\(\square \)

Lemma 5.6

For every  \(\delta \!>\!0\), there is a constant  \(C\!>\!0\) such that, for every  \(\mathbf{y}\in \mathbb {R}^n\) and  \(r\!>\!0\),
$$\begin{aligned} \int _{\mathbb {R}^n\backslash \mathcal {O}(\mathbf{y},r)}\mathrm{d}\varvec{\mu }(\mathbf{x}) \left| (\tau _{-\mathbf{y}}f)(\mathbf{x})\right| \le C\,r^{-\delta }\,\left\| f\right\| _{L^1((1+|\mathbf{x}|)^\delta \mathrm{d}\varvec{\mu }(\mathbf{x}))}\!, \end{aligned}$$
where
$$\begin{aligned} \mathcal {O}(\mathbf{y},r) =\big \{\,\mathbf{x}\!\in \!\mathbb {R}^n\,|\;\big ||x_j|-|y_j|\big |\le r, \forall \;1\le j\le n\,\big \} \end{aligned}$$
is the orbit of the cube \(\mathbf Q(\mathbf{y},r)=\prod _{j=1}^nB(y_j,r)\) under the group generated by the reflections (1.1).

Proof

As  \(\mathbb {R}^n\!\backslash \!\mathcal {O}(\mathbf{y},r)\) is contained in the union of the sets
$$\begin{aligned} A_j=\big \{\,\mathbf{x}\!\in \!\mathbb {R}^n\,|\;\big ||x_j|-|y_j|\big |>r\,\big \} \qquad (j=1,\ldots ,n), \end{aligned}$$
we have
$$\begin{aligned} \int _{\mathbb {R}^n\backslash \mathcal {O}(\mathbf{y},r)}\mathrm{d}\varvec{\mu }(\mathbf{x}) \left| (\tau _{-\mathbf{y}}f)(\mathbf{x})\right| \le \,\sum \nolimits _{j=1}^{\,n} \int _{A_j}\mathrm{d}\varvec{\mu }(\mathbf{x}) \int _{\varvec{{\mathcal {I}}}_{\mathbf{x},\mathbf{y}}} \mathrm{d}\varvec{\mu }(\mathbf{z}) \,\left| \varvec{\nu }(\mathbf{x},-\mathbf{y},\mathbf{z})\right| \,\left| f(\mathbf{z})\right| . \end{aligned}$$
As
$$\begin{aligned} |\mathbf{z}|\ge |z_j|\ge \big ||x_j|-|y_j|\big |>r \end{aligned}$$
when \(\mathbf{x}\!\in \!A_j\) and \(\mathbf{z}\!\in \!{\mathcal {I}}_{\mathbf{x},\mathbf{y}}\), the latter expression is bounded above by
$$\begin{aligned} r^{-\delta } \int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{z})\, \left| \mathbf{z}\right| ^\delta \,|f(\mathbf{z})| \int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{x}) \,|\varvec{\nu }(\mathbf{x},-\mathbf{y},\mathbf{z})|\,. \end{aligned}$$
We conclude by using the uniform estimate
$$\begin{aligned} \int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{x}) \,|\varvec{\nu }(\mathbf{x},-\mathbf{y},\mathbf{z})| =\int _{\mathbb {R}^n}\mathrm{d}\varvec{\mu }(\mathbf{x}) \,|\varvec{\nu }(\mathbf{z},\mathbf{y},\mathbf{x})| \le C. \end{aligned}$$
\(\square \)
Let us turn to the proof of Theorem 1.10, which consists in estimating
$$\begin{aligned} \Vert \mathbf{h}_{*}({\mathcal {T}}_{m}a)\Vert _{L^1(d\varvec{\mu })} \lesssim M\end{aligned}$$
(5.7)
for every atom \(a\) in the Hardy space \(H^1\!=H^1_\mathrm{atom}\). By rescaling, it suffices to prove (5.7) for any atom \(a\) associated with a unit ball  \(\mathbf{B}(\mathbf{z},1)\). As \(\mathbf{h}_{*}\) and \({\mathcal {T}}_{m}\) are bounded on \(L^2(\mathbb {R}^n,d\varvec{\mu })\), we have
$$\begin{aligned} \left\| \mathbf{h}_{*}({\mathcal {T}}_{m}a)\right\| _{L^1(\mathcal {O}(\mathbf{z},2),\mathrm{d}\varvec{\mu })} \lesssim M. \end{aligned}$$
Thus it remains to show that
$$\begin{aligned} \Vert \mathbf{h}_{*}({\mathcal {T}}_{m}a)\Vert _{L^1(\mathbb {R}^n\backslash \mathcal {O}(\mathbf{z},2),\mathrm{d}\varvec{\mu })}\lesssim M. \end{aligned}$$
(5.8)
For this purpose, let us introduce a dyadic partition of unity on the Dunkl transform side. More precisely, given a smooth radial function \(\psi \) on \(\mathbb {R}^n\) such that
$$\begin{aligned} \mathrm{supp }\psi \subset \{\,\varvec{\xi }\!\in \!\mathbb {R}^n\,|\,\frac{1}{2}\le |\varvec{\xi }|\le 2\,\} \quad \text {and}\quad \sum \nolimits _{\ell \in \mathbb {Z}}\psi (2^{-\ell }\varvec{\xi })^2=1, \quad \forall \;\varvec{\xi }\!\in \!\mathbb {R}^n\!\backslash \!\{0\}\,, \end{aligned}$$
let us split up
$$\begin{aligned} e^{-t|\varvec{\xi }|^2}m(\varvec{\xi }) =\sum \nolimits _{\ell \in \mathbb {Z}} \psi (2^{-\ell }\varvec{\xi })\,e^{-t|\varvec{\xi }|^2}\psi (2^{-\ell }\varvec{\xi })\,m(\varvec{\xi })\,. \end{aligned}$$
Set
$$\begin{aligned} m_{t,\ell }(\varvec{\xi }) =\overbrace{ \psi (\varvec{\xi })\,e^{-t|2^{\ell }\varvec{\xi }|^2} }^{\psi _{t,\ell }(\varvec{\xi })} \overbrace{ \psi (\varvec{\xi })\,m(2^{\ell }\varvec{\xi }) }^{m_\ell (\varvec{\xi })},\\ f_{t,\ell }={\mathcal {F}}^{-1}(m_{t,\ell }) =\underbrace{{\mathcal {F}}^{-1}(\psi _{t,\ell })}_{g_{t,\ell }}*\underbrace{{\mathcal {F}}^{-1}(m_\ell )}_{w_\ell }. \end{aligned}$$
Then  \(e^{-t|\varvec{\xi }|^2}m(\varvec{\xi })={\displaystyle \sum \nolimits _{\ell \in \mathbb {Z}}}m_{t,\ell }(2^{-\ell }\varvec{\xi })\). Consider the convolution kernel
$$\begin{aligned} F_{t,\ell }(\mathbf{x},\mathbf{y})= \tau _{-\mathbf{y}}\,{\mathcal {F}}^{-1}\left\{ m_{t,\ell }(2^{-\ell }.)\right\} (\mathbf x) =2^{\mathbf{N}\ell }(\tau _{-2^{\ell }\mathbf{y}}f_{t,\ell })(2^{\ell }\mathbf{x})\end{aligned}$$
of the multiplier operator \(\mathcal T_{m_{t,\ell } (2^{-\ell }. )}\).

Lemma 5.9

  1. (a)
    On the one hand, for every  \(0\!\le \!\delta \!<\!\epsilon \), we have
    $$\begin{aligned} \int _{\mathbb {R}^n\backslash \mathcal {O}(\mathbf{z},2)} \mathrm{d}\varvec{\mu }(\mathbf{x})\, \sup _{t>0}|F_{t,\ell }(\mathbf{x},\mathbf{y})|\, \lesssim \,M\,2^{-\delta \ell }, \quad \forall \;\ell \!\in \!\mathbb {Z}, \,\forall \,\mathbf{z}\in \!\mathbb {R}^n, \;\forall \;\mathbf{y}\!\in \!\mathcal {O}(\mathbf{z},1). \end{aligned}$$
     
  2. (b)
    On the other hand,
    $$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\,\sup _{t>0}|F_{t,\ell }(\mathbf{x},\mathbf{y})-F_{t,\ell }(\mathbf{x},\mathbf{y}^{\prime })|\, \lesssim \,M\,2^{\ell }|\mathbf{y}\!-\!\mathbf{y}^{\prime }|\, , \quad \forall \;\ell \!\in \!\mathbb {Z},\; \forall \;\mathbf{y},\mathbf{y}^{\prime }\in \!\mathbb {R}^n. \end{aligned}$$
     

Proof

On the one hand, as
$$\begin{aligned} \left| \partial _{\varvec{\xi }}^{\varvec{\alpha }} \left( \psi (\varvec{\xi })e^{-t|\varvec{\xi }|^2}\right) \right| \le C_{\varvec{\alpha }}, \qquad \forall \;t\!>\!0,\;\forall \,\varvec{\xi }\!\in \!\mathbb {R}^n, \end{aligned}$$
Lemma 5.1 yields the estimate
$$\begin{aligned} |g_{t,\ell }(\mathbf{x})|\le C_d\,(1\!+\!|\mathbf{x}|)^{-d}, \qquad \forall \,\mathbf{x}\!\in \!\mathbb {R}^n, \end{aligned}$$
which holds for any \(d\!\in \!\mathbb {N}\) and which is uniform in \(t\!>\!0\) and \(\ell \!\in \!\mathbb {Z}\). On the other hand, Corollary 5.4 yields the estimate
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\,(1\!+\!|\mathbf{x}|)^\delta \, |w_\ell (\mathbf{x})|\lesssim M, \end{aligned}$$
which holds uniformly in \(\ell \!\in \!\mathbb {Z}\). By resuming the proof of Lemma 5.5, we deduce that
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\,(1\!+\!|\mathbf{x}|)^\delta \sup _{t>0}|f_{t,\ell }(\mathbf{x})|\lesssim M. \end{aligned}$$
(5.10)
We reach our first conclusion by rescaling and by using Lemma 5.6:
$$\begin{aligned}&\int _{\mathbb {R}^n\backslash \mathcal {O}(\mathbf{z},2)} \mathrm{d}\varvec{\mu }(\mathbf{x})\, \sup _{t>0}|F_{t,\ell }(\mathbf{x},\mathbf{y})|\, \le \int _{\mathbb {R}^n\backslash \mathcal {O}(\mathbf{y},1)} \mathrm{d}\varvec{\mu }(\mathbf{x})\, \sup _{t>0}|F_{t,\ell }(\mathbf{x},\mathbf{y})|\\&=\int _{\mathbb {R}^n\backslash \mathcal {O}(2^{\ell }\mathbf{y},2^{\ell })} \mathrm{d}\varvec{\mu }(\mathbf{x})\, \sup _{t>0}|(\tau _{-2^{\ell }\mathbf{y}}f_{t,\ell })(\mathbf{x})|\, \lesssim \,M\,2^{-\delta \ell }. \end{aligned}$$
Let us turn to the proof of (b). This time we factorize
$$\begin{aligned} m_{t,\ell }(\varvec{\xi }) =\underbrace{\overbrace{ \psi (\varvec{\xi })\, e^{|\varvec{\xi }|^2}e^{-t|2^{\ell }\varvec{\xi }|^2} }^{\widetilde{\psi }_{t,\ell }(\varvec{\xi })} \overbrace{ \psi (\varvec{\xi })\, m(2^{\ell }\varvec{\xi }) }^{m_\ell (\varvec{\xi })} }_{\widetilde{m}_{t,\ell }(\varvec{\xi })}\, e^{-|\varvec{\xi }|^2},\\ \end{aligned}$$
and accordingly
$$\begin{aligned} f_{t,\ell } ={\mathcal {F}}^{-1}(m_{t,\ell })=\,\underbrace{ {\mathcal {F}}^{-1}(\widetilde{m}_{t,\ell }) }_{\widetilde{f}_{t,\ell }}\, *\,\underbrace{ {\mathcal {F}}^{-1}(e^{-|\varvec{\xi }|^2}) }_{h}\,. \end{aligned}$$
On the one hand, by resuming the proof of (5.10), we get
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\, \sup _{t>0}|\widetilde{f}_{t,\ell }(\mathbf{x})|\lesssim M. \end{aligned}$$
On the other hand, \(\mathbf{h}(\mathbf{x},\mathbf{y})=(\tau _{-\mathbf{y}}h)(\mathbf{x})\) is the heat kernel at time \(t=1\), which satisfies
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu } (\mathbf{x})\, |\mathbf{h}(\mathbf{x},\mathbf{y})-\mathbf{h}(\mathbf{x},\mathbf{y}^{\prime })| \lesssim |\mathbf{y}-\mathbf{y}^{\prime }|, \qquad \forall \;\mathbf{y},\mathbf{y}^{\prime }\in \!\mathbb {R}^n, \end{aligned}$$
according to the next lemma. After rescaling, we reach our second conclusion:
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu }(\mathbf{x})\,\sup _{t>0}|F_{t,\ell }(\mathbf{x},\mathbf{y})-F_{t,\ell }(\mathbf{x},\mathbf{y}^{\prime })|\lesssim M\,2^{\ell }\,|\mathbf{y}-\mathbf{y}^{\prime }|\,. \end{aligned}$$
\(\square \)

Lemma 5.11

The following gradient estimate holds for the heat kernel:
$$\begin{aligned} \int _{\mathbb {R}^n}\!\mathrm{d}\varvec{\mu } (\mathbf{x})\, |\nabla _{\mathbf{y}}\mathbf{h}_{t}(\mathbf{x},\mathbf{y})|\, \lesssim \,t^{-\frac{1}{2}}, \qquad \forall \;t\!>\!0,\;\forall \;\mathbf{y}\!\in \!\mathbb {R}^n. \end{aligned}$$

Proof

We can reduce to the one-dimensional case and moreover to \(t=\!1\) by rescaling. It follows from our gradient estimates for the heat kernel in dimension \(1\) (see Proposition 2.3) that
$$\begin{aligned} \left| \frac{\partial }{\partial y}h_1(x,y)\right| \lesssim \frac{1}{1+\,|xy|^k}\,e^{-\frac{1}{8}(|x|-|y|)^2}. \end{aligned}$$
  • Case 1: Assume that  \(|y|\le 2\). Then \(|\partial _{y}h_1(x,y)|\lesssim e^{-x^2/16}\), hence
    $$\begin{aligned} \int _{-\infty }^{+\infty }\mathrm{d}x\,|x|^{2k}\, \left| \frac{\partial }{\partial y}h_1(x,y)\right| \,\lesssim \,1\,. \end{aligned}$$
  • Case 2: Assume that  \(|y|\ge 2\). Then \(|x|/|y|\le 1+\frac{1}{2}\left| |x|-|y|\right| \), hence
    $$\begin{aligned}&|x|^{2k}\,\left| \frac{\partial }{\partial y}h_1(x,y)\right| \lesssim \left( \frac{|x|}{|y|}\right) ^{k}\, e^{-\frac{1}{8}(|x|-|y|)^2}\\&\qquad \lesssim \left( 1+\left| |x|-|y|\right| \right) ^{k}\, e^{-\frac{1}{8}(|x|-|y|)^2} \lesssim e^{-\frac{1}{16}(|x|-|y|)^2} \end{aligned}$$
    and
    $$\begin{aligned} \int _{-\infty }^{+\infty }\mathrm{d}x\,|x|^{2k}\, \left| \frac{\partial }{\partial y}h_1(x,y)\right| \, \lesssim \int _{\,0}^{+\infty }\mathrm{d}x\,e^{-\frac{1}{16}(x-|y|)^2} \lesssim \int _{-\infty }^{+\infty }\mathrm{d}z\,e^{-\frac{1}{16}z^2} \lesssim \,1\,. \end{aligned}$$

Conclusion of proof of Theorem 1.10

Let us split up and estimate
$$\begin{aligned} |\mathbf{h}_{*}({\mathcal {T}}_{m}a)(\mathbf{x})|&\le \sum \nolimits _{\ell \ge 0}|\mathbf{h}_{*} ({\mathcal {T}}_{\psi (2^{-\ell }.)^2m}a)(\mathbf{x})| +\sum \nolimits _{\ell <0}|\mathbf{h}_{*} ({\mathcal {T}}_{\psi (2^{-\ell }.)^2m}a)(\mathbf{x})|\\&=\sum \nolimits _{\ell \ge 0}\sup \nolimits _{t>0}\, \left| \,\int _{\mathbf{B}(\mathbf{z},1)} \mathrm{d}\varvec{\mu }(\mathbf{y})\, F_{t,\ell }(\mathbf{x},\mathbf{y})\,a(\mathbf{y})\,\right| \\&+\sum \nolimits _{\ell <0}\sup \nolimits _{t>0}\, \left| \,\int _{\mathbf{B}(\mathbf{z},1)} \mathrm{d}\varvec{\mu }(\mathbf{y})\, \left\{ F_{t,\ell }(\mathbf{x},\mathbf{y})\!-\!F_{t,\ell }(\mathbf{x},\mathbf{z})\right\} \, a(\mathbf{y})\,\right| \\&\le \sum \nolimits _{\ell \ge 0} \int _{\mathbf{B}(\mathbf{z},1)} \mathrm{d}\varvec{\mu }(\mathbf{y})\;|a(\mathbf{y})|\, \sup \nolimits _{t>0}\,\left| F_{t,\ell }(\mathbf{x},\mathbf{y})\right| \\&+\sum \nolimits _{\ell <0} \int _{\mathbf{B}(\mathbf{z},1)} \mathrm{d}\varvec{\mu }(\mathbf{y})\;|a(\mathbf{y})|\, \sup \nolimits _{t>0}\, \left| F_{t,\ell }(\mathbf{x},\mathbf{y})-F_{t,\ell }(\mathbf{x},\mathbf{z})\right| \,. \end{aligned}$$
Then (5.8) follows from Lemma 5.9. \(\square \)

Example 5.1

The Riesz transforms  \({\mathcal {R}}_j=D_j(-\mathbf L)^{-1\slash 2}\) in the Dunkl setting correspond to the multipliers \(\xi _j/|\varvec{\xi }|\), up to a constant. Hence, by Theorem 1.10, they are bounded operators on the Hardy space \(H^1\).

Notes

Acknowledgments

JPA and JD were partially supported by the European Commission (European program ToK HANAP 2005–2009, Polish doctoral program SSDNM 2010–2013) and by a French–Polish cooperation program (PHC Polonium 22529RF 2010–2011). JPA, NBS, NH partially supported by a French–Tunisian cooperation program (PHC Utique / CMCU 10G1503 2010–2013). JD was supported by the Polish National Science Centre (Narodowe Centrum Nauki, Grant DEC-2012/05/B/ST1/00672) and by the University of Orléans. The third author wishes to thank Paweł Głowacki and Jacek Zienkiewicz for conversations on the subject of the paper.

References

  1. 1.
    Abramowitz, M., Stegun, I.A.: Handbook of Mathematical Functions (with Formulas, Graphs, and Mathematical Tables). Dover Publications, Mineola (1972)MATHGoogle Scholar
  2. 2.
    Amri, B., Anker, J-Ph, Sifi, M.: Three results in Dunkl analysis. Colloq. Math. 118(1), 299–312 (2010)MATHMathSciNetCrossRefGoogle Scholar
  3. 3.
    Burkholder, D.L., Gundy, R.F., Silverstein, M.L.: A maximal function characterisation of the class \(H^p\). Trans. Am. Math. Soc. 157, 137–153 (1971)MATHMathSciNetGoogle Scholar
  4. 4.
    Cherednik, I.: Double Affine Hecke Algebras. London Mathematical Society Lecture Note Series, vol. 319. Cambridge University Press, Cambridge (2005)MATHCrossRefGoogle Scholar
  5. 5.
    Coifman, R.R.: A real variable characterization of \(H^p\). Stud. Math. 51, 269–274 (1974)MATHMathSciNetGoogle Scholar
  6. 6.
    Coifman, R.R., Weiss, G.L.: Extensions of Hardy spaces and their use in analysis. Bull. Am. Math. Soc. 83, 569–615 (1977)MATHMathSciNetCrossRefGoogle Scholar
  7. 7.
    Dunkl, C.F.: Differential-difference operators associated to reflection groups. Trans. Am. Math. 311(1), 167–183 (1989)MATHMathSciNetCrossRefGoogle Scholar
  8. 8.
    Dziubański, J., Preisner, M., Wróbel, B.: Multivariate Hörmander-type multiplier theorem for the Hankel transform. J. Fourier Anal. Appl. 19, 417–437 (2013)MATHMathSciNetCrossRefGoogle Scholar
  9. 9.
    Fefferman, C., Stein, E.M.: \(H^p\) spaces of several variables. Acta Math. 129, 137–193 (1972)MATHMathSciNetCrossRefGoogle Scholar
  10. 10.
    Hörmander, L.: Estimates for translation invariant operators in \(L^p\) spaces. Acta Math. 104, 93–140 (1960)MATHMathSciNetCrossRefGoogle Scholar
  11. 11.
    Macdonald, I.G.: Affine Hecke Algebras and Orthogonal Polynomials. Cambridge Tracts in Mathematics, vol. 157. Cambridge University Press, Cambridge (2003)MATHCrossRefGoogle Scholar
  12. 12.
    Macías, R.A., Segovia, C.: A decomposition into atoms of distributions on spaces of homogeneous type. Adv. Math. 33, 271–309 (1979)MATHCrossRefGoogle Scholar
  13. 13.
    Mauceri, G., Meda, S.: Vector-valued multipliers on stratified groups. Rev. Mat. Iberoamericana 6(3–4), 141–154 (1990)MATHMathSciNetCrossRefGoogle Scholar
  14. 14.
    NIST Digital Library of Mathematical Functions. http://dlmf.nist.gov
  15. 15.
    Opdam, E.M.: Lecture notes on Dunkl operators for real and complex reflection groups. Math. Soc. Jpn Mem. 8 (2000)Google Scholar
  16. 16.
    Rösler, M.: Bessel-type signed hypergroup on \(\mathbb{R}\). In: Heyer, H. (ed.) Probability Measures on Groups and Related Structures XI (Oberwolfach, 1994), pp. 292–304. World Science Publisher, Singapore (1995)Google Scholar
  17. 17.
    Rösler, M.: Generalized Hermite polynomials and the heat equation for Dunkl operators. Commun. Math. Phys. 192, 519–542 (1998)MATHCrossRefGoogle Scholar
  18. 18.
    Rösler, M.: Dunkl operators (theory and applications). In: Koelink, E., Van Assche, W. (eds.) Orthogonal Polynomials and Special Functions (Leuven, 2002). Lecture Notes in Mathematics, vol. 1817, pp. 93–135. Springer, New York (2003)Google Scholar
  19. 19.
    Rösler, M.: A positive radial product formula for the Dunkl kernel. Trans. Am. Math. Soc. 355(6), 2413–2438 (2003)MATHCrossRefGoogle Scholar
  20. 20.
    Rösler, M., de Jeu, M.: Asymptotic analysis for the Dunkl kernel. J. Approx. Theory 119, 110–126 (2002)MATHMathSciNetCrossRefGoogle Scholar
  21. 21.
    Stein, E.M.: Harmonic Analysis (Real-Variable Methods, Orthogonality, and Oscillatory Integrals). Princeton Mathematics Series, vol. 43. Princeton University Press, Princeton (1993)MATHGoogle Scholar
  22. 22.
    Stein, E.M., Weiss, G.L.: On the theory of harmonic functions of several variables I (the theory of \(H^p\) spaces). Acta Math. 103, 25–62 (1960)MATHMathSciNetCrossRefGoogle Scholar
  23. 23.
    Thangavelu, S., Xu, Y.: Convolution operator and maximal function for the Dunkl transform. J. Anal. Math. 97, 25–56 (2005)MathSciNetCrossRefGoogle Scholar
  24. 24.
    Trimeche, K.: Paley–Wiener theorems for the Dunkl transform and Dunkl translation operators. Integr. Transforms Spec. Funct. 13(1), 17–38 (2002)MATHMathSciNetCrossRefGoogle Scholar
  25. 25.
    Uchiyama, A.: A maximal function characterization of \(H^p\) on the space of homogeneous type. Trans. Am. Math. Soc. 262(2), 579–592 (1980)MATHMathSciNetGoogle Scholar

Copyright information

© The Author(s) 2014

Open AccessThis article is distributed under the terms of the Creative Commons Attribution License which permits any use, distribution, and reproduction in any medium, provided the original author(s) and the source are credited.

Authors and Affiliations

  • Jean-Philippe Anker
    • 1
  • Néjib Ben Salem
    • 2
  • Jacek Dziubański
    • 3
  • Nabila Hamda
    • 2
  1. 1.Fédération Denis Poisson (FR 2964) & Laboratoire MAPMO (UMR 7349)Université d’Orléans & CNRSOrléans Cedex 2France
  2. 2.Faculté des Sciences de TunisUniversité de Tunis El Manar, LR11ES11 Analyse Mathématiques et ApplicationsTunisTunisia
  3. 3.Instytut MatematycznyUniwersytet WrocławskiWrocławPoland

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