Abstract
We study Hardy and BMO spaces associated with the Grushin operator. We first prove atomic and maximal functions characterizations of the Hardy space. Further we establish a version of Fefferman–Stein decomposition of BMO functions associated with the Grushin operator and then obtain a Riesz transforms characterization of the Hardy space.
Similar content being viewed by others
Avoid common mistakes on your manuscript.
1 Introduction and Statement of the Results
1.1 Grushin Operator
On \({\mathbb {R}}^{n+1}={\mathbb {R}}^n\times {\mathbb {R}}\) we consider the Grushin operator
where \({\mathbb {R}}^n\times {\mathbb {R}}\ni {\mathbf {x}}=(x',x'')\), \(x'=(x'_1,x'_2,\ldots ,x'_n)\in {\mathbb {R}}^n\), \(x''\in {\mathbb {R}}\). The operator \({\mathcal {L}}\) is homogeneous of degree 2 with respect to the dilations
that is, \({\mathcal {L}}(f\circ \delta _t)({\mathbf {x}})= t^2 ({\mathcal {LF}})(\delta _t{\mathbf {x}})\). It is well known \(\mathcal {L}\) is a hypoelliptic operator. It is related to the Heisenberg group \(\mathbb {H}_n\). Actually the Grushin operator \({\mathcal {L}}\) is the image of a sub-Laplacian L associated to \(\mathbb {H}_n\) under a representation \(\pi \) acting on functions on \(\mathbb {R}^{n+1}.\) In fact we make use of this relation to prove some crucial estimates on some kernels related to \({\mathcal {L}}\).
The control distance on \({\mathbb {R}}^{n+1}\) associated with \({\mathcal {L}}\) is defined by
where \({\mathcal {D}}=\{\psi \in W^{1,\infty }({\mathbb {R}}^{n+1}):\sum _{j=1}^n( |\partial _{x'_j} \psi |^2+|x_j'\partial _{x''}\psi |^2)\le 1\}\). It is homogeneous, that is,
and behaves like:
see, e.g., [18, 20] for details. Clearly,
Let \(B({\mathbf {x}}, r)=\{ {\mathbf {y}}\in {\mathbf {X}}: d({\mathbf {x}},{\mathbf {y}})<r\}\) denote the ball with center \({\mathbf {x}}\) and radius \(r>0\) in the metric \(d({\mathbf {x}},{\mathbf {y}})\) and \(|B({\mathbf {x}},r)|\) be its Lebesgue measure volume. Then
and, consequently,
The homogeneity of the distance d implies
The space \({\mathbf {X}}={\mathbb {R}}^n\times {\mathbb {R}}\) equipped with the Lebesgue measure \(d{\mathbf {x}}\) and the distance \(d({\mathbf {x}},{\mathbf {y}})\) is the space of homogeneous type in the sense of Coifman–Weiss [7]. It is well known (see e.g., [20]) that \(-{\mathcal {L}}\) generates a semigroup of self-adjoint linear operators \(e^{-t{\mathcal {L}}}\) on \(L^2({\mathbf {X}}) \) which has the form
where the heat kernel \(H_t({\mathbf {x}},{\mathbf {y}})\) satisfies the Gaussian upper bound estimates (see (2.13)).
1.2 Hardy Space \(H^1_{\mathcal L}\)
Let \({\mathcal {M}}_{{\mathcal {L}}}f(x)=\sup _{t>0} |e^{-t{\mathcal {L}}}f(x)|\) be the maximal function associated with the semigroup \(e^{-t{\mathcal {L}}}\). The upper Gaussian estimates (2.13) imply that \({\mathcal {M}}_{{\mathcal {L}}}\) is bounded on \(L^p({\mathbf {X}})\) for \(1<p\le \infty \) and of weak-type (1,1). We define the Hardy space
Now we define atoms associated to the homogeneous space \({\mathbf {X}}.\)
1.3 Atoms
Fix \(1<q\le \infty \). A function a is called a (1, q)-atom for the Hardy space \(H^1({\mathbf {X}})\) if there is a ball \(B=B({\mathbf {x}},r)=\{ {\mathbf {y}}: \ d({\mathbf {x}},{\mathbf {y}})<r\}\) such that
\(\text {supp}\, a\subset B\),
\(\Vert a\Vert _{L^q}\le |B|^{\frac{1}{q}-1}\) (\(\Vert a\Vert _{L^\infty }\le |B|^{-1}\) if \(q=\infty \)),
\(\int a({\mathbf {y}})\, d{\mathbf {y}}=0\).
The atomic norm is given by
where the infimum is taken over all decompositions \(f=\sum \lambda _j a_j\), \(\lambda _j\in {\mathbb {C}}\), \(a_j\) are (1, q)-atoms for \(H^1({\mathbf {X}})\).
We are now in a position to state our first result.
Theorem 1.1
For every \(q\in (1,\infty ]\) the space \(H^1_{{\mathcal {L}}}\) admits atomic decomposition and the norms \(\Vert f\Vert _{H^1_{\mathcal {L}}}\) and \(\Vert f\Vert _{H^1_{\mathrm{atom},\, q}({\mathbf {X}})}\) are equivalent.
1.4 Riesz Transforms
The system of Riesz transforms \({\mathcal {R}}_j\), \(j=1,2,\ldots ,2n\), associated with \({\mathcal {L}}\) is defined by
This formal definition has a precise meaning and the operators \({\mathcal {R}}_j\) are Calderón–Zygmund operators on \({\mathbf {X}}\). Moreover, \( {\mathcal {R}}_j\) are well-defined in the sense of distributions on \(L^1({\mathbf {X}})\) (see Sect. 4). Our second main result is the following theorem.
Theorem 1.2
An \(L^1({\mathbf {X}})\) function F belongs to \(H^1_{{\mathcal {L}}}\) if and only if \({\mathcal {R}}_jF\in L^1({\mathbf {X}})\) for \(j=1,2,\ldots ,2n\). Moreover, there is a constant \(C>0\) such that
The theory of the classical real Hardy spaces on \({\mathbb {R}}^n\) has its origin in studying holomorphic function of one variable. The reader is referred to the very original works: Stein and Weiss [23], Burkholder et al. [2], Fefferman and Stein [11], and Coifman [6]. The spaces are natural extensions of \(L^p\) spaces and many operators occurring in harmonic analysis, like convolution singular integral operators, are bounded on them. The theory was then extended to the spaces of homogeneous type (see [8, 17, 25]). More information about the classical real \(H^p\) spaces with their characterizations and historical remarks can be also found in [22]. In [13] the authors provide a very general approach to the theory of \(H^1\) spaces for semigroups of linear operators satisfying Davies–Gaffney estimates and in particular Gaussian bounds. Let us point out, that in the context of semigroups, the classical Hardy spaces can be thought as those associated with the Laplace operator on \({\mathbb {R}}^n\).
In the monograph [12] Folland and Stein study \(H^p\) spaces on homogeneous nilpotent Lie groups proving equivalence of their definitions by means of maximal functions, square functions, and atoms. Important contributions to the theory of Hardy spaces on homogeneous groups are their characterizations by Riesz transforms proved in Christ and Geller [5]. To this end the authors of [5] extended Uchiyama’s theorem (see [26]) about Fefferman–Stein decomposition of BMO functions on \({\mathbb {R}}^n\) to homogeneous nilpotent Lie groups. Let us emphasise that our proof of the Riesz transforms characterization of Hardy space \(H^1_{{\mathcal {L}}}\) associated with the Grushin operator (see Theorem 1.2) takes an inspiration from [5]. We make use of the relation between \(\mathcal {L}\) and L via the already mentioned representation \(\pi \) and transfer the methods of [5] into the space of homogeneous type \({\mathbf {X}}\).
Let us also remark that our proof of Theorem 1.1 is based on Uchiyama results [25] about characterization of Hardy spaces on spaces of homogeneous type by maximal functions and atomic decompositions.
The Grushin operator \({\mathcal {L}}\) we consider here is a special example of operators of the form \({\mathbf {L}}=-\Delta _{x'}-|x'|^2\Delta _{x''}\), \((x',x'')\in {\mathbb {R}}^{n}\times {\mathbb {R}}^{m}\). It seems likely the methods we present here combined with [5] and relation of \({\mathbf {L}}\) with the Heisenberg–Reiter groups (see, e.g., [18]) will allow to develop the theory of Hardy spaces for \({\mathbf {L}}\).
1.5 Organization of the Paper
In Sect. 2 we describe relation of the Grushin operator and the sub-Laplacian on the Heisenberg group via a unitary representation and derive estimates on the heat kernel of \(\exp (-t{\mathcal {L}})\). Section 3 is devoted to proving Theorem 1.1. In Sect. 4 we study properties of kernels which are obtained as images by the representation of some singular integral kernels on \({\mathbb {H}}_n\). The crucial theorem about decompositions of compactly supported BMO functions by means of singular integrals is stated in Sect. 5 and its proof is completed in Appendixes 1 and 2. The proof of the Riesz transforms characterization of the Hardy space \(H^1_{{\mathcal {L}}}\) is presented in Sect. 6.
2 Relation with the Heisenberg Group
In this section we describe relation between the Grushin operator \({\mathcal {L}}\) and the sub-Laplacian L on the Heisenberg group \({\mathbb {H}}_n\). As we will see \({\mathcal {L}}\) occurs as an image of L in a special unitary representation \(\pi \) of \({\mathbb {H}}_n\) (see [15, 19]). We start this section by recalling basic facts from the analysis on the Heisenberg group.
2.1 Heisenberg Group
The Heisenberg group \({\mathbb {H}}_n\) is a Lie group with the underlying manifold \({\mathbb {R}}^{2n+1}={\mathbb {R}}^n\times {\mathbb {R}}^n\times {\mathbb {R}}\) and the group multiplication
where \(x\cdot y\) is the standard inner product in \({\mathbb {R}}^n\). We shall also denote the elements of the Heisneberg group by \(\varvec{x}=(x,y,t)\). Then \(\varvec{x}^{-1}=-\varvec{x}=(-x,-y,-t)\). The Lebesgue measure \(d\varvec{x}\) on \({\mathbb {R}}^{2n+1}\) turns out to be the bi-invariant Haar measure on \({\mathbb {H}}_n\). Clearly, \({\mathbb {H}}_n\) is a homogeneous nilpotent Lie group with dilations \(\delta _s(x,y,t)=(sx,sy,s^2t)\). We fix a homogeneous norm on \({\mathbb {H}}_n\) to be so called Koranyi norm given by
The function \({\mathbb {H}}_n\ni \varvec{x} \mapsto |\varvec{x}|\in {\mathbb {R}}_+\cup \{0\}\) is smooth away from the origin, homogeneous of degree one, that is, \(|\delta _s \varvec{x}|=s|\varvec{x} |\), and symmetric \((|\varvec{x}|=|\varvec{-}\varvec{x}|)\). Moreover, \(|\varvec{x}\varvec{y}|\le |\varvec{x}|+|\varvec{y}|\). Clearly, \(|(x,y,t)|\sim |x|+|y|+ |t|^{1\slash 2}\). The homogeneous dimension of \({\mathbb {H}}_n\) is denoted by D and in our case \(D=2n+2\).
We choose the standard basis of the left-invariant vector fields:
and the corresponding right-invariant vector fields:
Obviously, for \(j=1,2,\ldots ,n\) we have
where \(w_j(\varvec{x})=w_j(x,y,t)=y_j\), \(w_{n+j}(\varvec{x})=w_{n+j}(x,y,t)=-x_j\).
We apply the usual notation for higher order derivatives (see [12]). If \(I=(i_1,i_2,\ldots ,i_{2n+1})\in ({\mathbb {N}}\cup \{0\})^{2n+1}\) is a multi-index, we set
Let \(L=-\sum _{k=1}^{2n} X_k^2\) denote the left-invariant sub-Laplacian on \({\mathbb {H}}_n\). It is well-known (see e.g., [27]) that the corresponding heat semigroup \(e^{-sL}\) is given by the convolution \(e^{-sL} f(x,y,t)=f*h_s(x,y,t)\) with a heat kernel \(h_s(x,y,t)=h_s(-x,-y,-t)\) which satisfies
2.2 Unitary Representation
We define the unitary representation of \({\mathbb {H}}_n\) on \(L^2({\mathbf {X}})\) by
(cf. Meyer [19]). It is easy to see that
Hence, \(\pi (L)={\mathcal {L}}\).
For a function \(F\in L^1({\mathbb {H}}_n)\) we set
where
Clearly, if \(F\in L^1({\mathbb {H}}_n)\), then
where here and subsequently \(F_s(x,y,t)=s^{-D\slash 2}F(\delta _{s^{-1\slash 2}}(x,y,t))\).
Further, for suitable functions F on \({\mathbb {H}}_n\) one has
Lemma 2.1
There is a constant \(C_1>0\) such that if \(F\in L^1({\mathbb {H}}_n)\), \(\mathrm{supp}\, F\subset B_{{\mathbb {H}}_n}((0,0,0), R)\subset {\mathbb {H}}_n\), then
Here \(B_{{\mathbb {H}}_n}((0,0,0), R)=\{(x,y,t)\in {\mathbb {H}}_n: |(x,y,t)|<R\}\) and |(x, y, t)| is the homogeneous norm in \({\mathbb {H}}_n\).
Proof
In the proof we will frequently use, without any comment, the formulas (2.1), (2.6), and (1.1). Assume that \(d({\mathbf {x}},{\mathbf {y}})>C_1R\) with \(C_1\) being large. If \(|x'-y'|>R\), then \(\pi (F)({\mathbf {x}},{\mathbf {y}})=0\). Thus for the remaining part of the proof we assume that \(|x'-y'|\le R\). We shall consider two cases.
Case 1: \(|x''-y''|^{1\slash 2}\le |x'|+|y'|\). Then \(|x''-y''|>CR(|x'|+|y'|)\), where C is large if \(C_1\) is chosen to be large. Consequently, \(|x''-y''|>(CR)^2\). Hence, for \(|z|<R\) we have
Thus \(\pi (F)({\mathbf {x}},{\mathbf {y}})=0\) if \(C_1\) is large and, consequently, so is C.
Case 2: \(|x''-y''|^{1\slash 2}>|x'|+|y'|\). Then \(|x''-y''|^{1\slash 2}>CR\) and, again C is large if \(C_1\) is chosen to be large. For \(|z|<R\) we have \(|\frac{1}{2}z\cdot (y'+x')|<R(|x'|+|y'|)\le R|x''-y''|^{1\slash 2}\). Therefore,
which implies \(\pi (F)({\mathbf {x}},{\mathbf {y}})=0\) if \(C_1\) is large enough. \(\square \)
Lemma 2.2
There is a constant \(C_2>0\) such that if F is a bounded function on \({\mathbb {H}}_n\), \(\mathrm{supp}\, F\subset B((0,0,0), R)\subset {\mathbb {H}}_n\), then
Proof
It suffices to prove the lemma for F being the characteristic function of the ball \(B_{{\mathbb {H}}_n}((0,0,0),R)\) for every \(R>0\). Then, by (2.6),
Assume that \(\pi (F)({\mathbf {x}},{\mathbf {y}})>0\). We consider two cases.
Case 1: \(R>|x'|\slash C\), where \(C>0\) is a large constant. Then, by (1.3), \(|B({\mathbf {x}}, R)|\sim R^{n+2}\) and, consequently, \(|\pi (F)({\mathbf {x}},{\mathbf {y}}) |\le 2C R^n\sim R^D|B({\mathbf {x}}, R)|^{-1}\).
Case 2: \(R\le |x'|\slash C\). Notice that \(|x'+y'|\sim |x'|+|y'|\sim |x'|\), since \(|x'-y'|<R\) and \(C>0\) is large. Hence, by (2.11),
\(\square \)
2.3 Heat kernel for \({\mathcal {L}}\)
The kernels of the semigroups \(e^{-s{\mathcal {L}}}\) and \(e^{-sL}\) are related by
Let us also note that thanks to the homogeneity of \({\mathcal {L}}\) one has
Proposition 2.3
(Gaussian bounds for \(H_s\)) There are constants \(c,C>0\) such that
Proof
The proposition is well-known. For the convenience of the reader we present a short proof based on estimates of the heat kernel for the sub-Laplacian L on the Heisenberg group combined with Lemmas 2.1 and 2.2. To this end from (2.4) we have
Using (2.12), Lemmas 2.1 and 2.2, we obtain
Applying (1.4), we get
\(\square \)
Lemma 2.4
There is a constant \(C>0\) such that
Proof
Fix \({\mathbf {y}}\in {\mathbf {X}}\) and \(s>0\) and set \(F({\mathbf {x}})=H_s({\mathbf {x}},{\mathbf {y}})\). Now, using (2.5) and the same arguments we have used in the proof of (2.13), we obtain
Finally, by the definition of the distance d, we have
\(\square \)
Corollary 2.5
(Hölder-type estimates for \(H_t\)) For \(0<\gamma <1\) there are constants \(C,c_0>0\) such that
with the improvement
Lemma 2.6
(On diagonal lower bound of \(H_s\)) There is a constant \(C>0\) such that
Proof
By the homogeneity it suffices to prove the estimate for \(s=1\). To this end
\(\square \)
3 Proof of Theorem 1.1
Proof
To prove the theorem we use Uchiyama’s results [25]. For this purpose we set
where the infimum is taken over all closed balls B containing \({\mathbf {x}}\) and \({\mathbf {y}}\). Then \( \rho \) is a quasi-distance such that \( \rho ({\mathbf {x}}, {\mathbf {y}})\asymp |B({\mathbf {x}},d({\mathbf {x}},{\mathbf {y}}))|\) for all \({\mathbf {x}}, {\mathbf {y}}\!\in \!{\mathbf {X}} \) and
where \(\,{B_\rho }({\mathbf {x}},r)\) denotes the closed quasi-ball with center \( {\mathbf {x}} \) and radius r (see, e.g. [1, Lemma 6.4] for the proof).
Define the new kernel \(K_r(\mathbf {x},\mathbf {y})\) by
where \(r=|B(\mathbf {x},\sqrt{t})|\). The kernel \(K_r(\mathbf {x},\mathbf {y})\) satisfies the following assumptions of Uchiyama’s theorem, which are stated in conditions (3.3)–(3.5) below. \(\square \)
-
The on-diagonal lower estimate:
$$\begin{aligned} K_r(\mathbf {x},\mathbf {x})\ge \tfrac{1}{Ar}. \end{aligned}$$(3.3)
-
Upper estimate: for every \(\delta \!>\!0\),
$$\begin{aligned} K_r(\mathbf {x},\mathbf {y})\le \tfrac{A}{r}\,\bigl (1+\tfrac{\rho (\mathbf {x},\mathbf {y})}{r}\bigr )^{-1-\delta }. \end{aligned}$$(3.4)
-
Hölder estimate: there exist \(C_3\!>\!0\), \(\delta \!>\!0\), such that
$$\begin{aligned} \bigl | K_r(\mathbf {x},\mathbf {y}) -K_r(\mathbf {x},\mathbf {z})\bigr |\le & {} \tfrac{A}{r}\bigl ( 1+\tfrac{\rho (\mathbf {x},\mathbf {y})}{r} \bigr )^{-1-2\delta } \bigl (\tfrac{\rho (\mathbf {y},\mathbf {z})}{r} \bigr )^{\delta } \text {if}\;\rho (\mathbf {y},\mathbf {z})\nonumber \\\le & {} C_3\max \,\{ r,\rho (\mathbf {x},\mathbf {y})\}. \end{aligned}$$(3.5)
The estimates (3.3)–(3.5) are consequences of (1.4), (2.21), (2.13), and Corollary 2.5 (see, e.g., [1, Appendix 3]).
Now we define the Hardy spaces \(H^1_{\text {max},K_r}\) as the set of all \(L^1({\mathbb {R}}^{n+1})\)-functions f such that \(\Vert f^{(+)}\Vert _{L^1({\mathbf {X}})}<\infty \), where \(f^{(+)}=\sup _{r>0} |\int K_r({\mathbf {x}},{\mathbf {y}}) f({\mathbf {y}})\, d{\mathbf {y}}|\).
The atomic Hardy space \(H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )\) is defined in the standard way. A function a is called an atom for \(H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )\), if there is a ball \(B_\rho ({\mathbf {x}}_0,r)\) such that \(\text {supp}\, a\subset B_\rho ({\mathbf {x}}_0, r)\), \(\Vert a\Vert _{L^\infty }\le |B_\rho ({\mathbf {x}}_0, r)|^{-1}\sim r^{-1}\), \(\int a=0\). Now a function f is an element of \(H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )\) if \(f({\mathbf {x}})=\sum _{k} \lambda _k a_k({\mathbf {x}})\), where \(a_k({\mathbf {x}})\) are atoms for \(H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )\) and \(\lambda _k\in {\mathbb {C}}\) with \(\sum _{k}|\lambda _k|<\infty \). For such f we set \(\Vert f\Vert _{H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )}=\inf \sum _{k}|\lambda _k|\), where infimum is taken over all such representations.
We are now in a position to state the following theorem of Uchiyama about atomic and maximal characterizations of Hardy spaces on a space of homogeneous type.
Theorem 3.1
[25, Corollary 1’] Assume that \(\rho ({\mathbf {x}},{\mathbf {y}})\) and \(K_r({\mathbf {x}},{\mathbf {y}})\) satisfy (3.1) and (3.3)–(3.5). Then the spaces \(H^1_{\text {max},K_r}\) and \(H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )\) coincide and the norms \(\Vert f^{(+)}\Vert _{L^1({\mathbf {X}})}\) and \(\Vert f\Vert _{H^1_{\text {atom},\, \infty }({\mathbf {X}}, \rho )}\) are equivalent.
It is easy to prove that there exists a constant \(c\ge 1\) such that if \(r= |B(\mathbf {x},\sqrt{t})|\), then
The above inclusions imply that the atomic Hardy spaces for \(d({\mathbf {x}},{\mathbf {y}})\) and \(\rho ({\mathbf {x}},{\mathbf {y}})\) coincide. Moreover, the maximal functions for the kernels \(K_r\) and \(H_t\) are equal. Hence, Theorem 1.1 follows from Theorem 3.1.
4 Farther Properties of \(\pi \)
4.1 Homogeneous Kernels
A tempered distribution S on \({\mathbb {H}}_n\) is said to be a regular kernel of order \(r\in {\mathbb {R}}\) if S coincides with a \(C^\infty \) function \(m(\varvec{x})\) away from the origin and satisfies
for any \(f\in {\mathcal {S}}({\mathbb {H}})\). Any regular kernel of order r gives rise to the convolution operator
which will be denoted by the same symbol S.
Any tempered distribution S on \({\mathbb {H}}_n\) which is a regular kernel of order 0 is of the form
where m is a \(C^\infty \) function away from the origin, \(m(\delta _s \varvec{x})=s^{-D} m(\varvec{x})\), \(\int _{\Sigma } m(\bar{\varvec{x}}) \, d\sigma (\bar{\varvec{x}})=0\) (see [3, Lemma 2.4]). Here \(\Sigma =\{ \bar{\varvec{x}}\in {\mathbb {H}}_n: |\bar{\varvec{x}}|=1\}\) is the unit sphere in \({\mathbb {H}}_n\) and \(d\sigma (\bar{\varvec{x}})\) is the Radon measure on \(\Sigma \) such that \(\int _{{\mathbb {H}}_n} f(\varvec{x})d\varvec{x} = \int _0^\infty \int _{\Sigma } f(\delta _s \bar{\varvec{x}}) s^{D-1}d\sigma (\bar{\varvec{x}})\, ds\) (see [12, Proposition 1.5]).
Let \(\varphi \) be a \(C^\infty \) function on \({\mathbb {H}}_n\) such that \(0\le \varphi \le 1\), \(\varphi (\varvec{x})=\varphi (\varvec{y})\) whenever \(|\varvec{x}|=|\varvec{y}|\), \(\text {supp}\, \varphi \subset \{\varvec{x}\in {\mathbb {H}}_n: \frac{1}{2}\le |\varvec{x}|\le 2\}\), \(\sum _{j=-\infty }^\infty \varphi (\delta _{2^{j}}\varvec{x})=1\) for \(\varvec{x}\ne 0\). Then any regular kernel S of order 0 can be written as
where \(m_j(\varvec{x})= \varphi (\delta _{2^j}\varvec{x}) m(\varvec{x})\). Clearly,
Let \(m_j^*(\varvec{x})=\overline{m_j(\varvec{x}^{-1})}=\overline{m_j(-\varvec{x})}\), \(\check{m}_j(\varvec{x})=m_j(-\varvec{x})\). It is not difficult to check that there are constants \(C,c>0\) such that
Thus, by the Cotlar–Stein lemma, \(Sf=f*\check{S}=c_1f+\sum _{j=-\infty }^\infty f*\check{m}_j\) defines a bounded operator on \(L^2({\mathbb {H}}_n)\) and, then on \(L^p({\mathbb {H}}_n)\), \(1<p<\infty \), since S is a Calderón–Zygmund operator on \({\mathbb {H}}_n\). Moreover, \(\Vert S f\Vert _{L^p({\mathbb {H}}_n)}\le (C_p \Vert m\varphi \Vert _{C^1}+c_1)\Vert f\Vert _{L^p({\mathbb {H}}_n)}\). The space of convolution operators with regular kernels of order 0 is an algebra with involution. Clearly,
Set \(\pi (S)f= c_1 f+\sum _{j=-\infty }^\infty \pi (m_j) f \). Then using the Coifman–Weiss transference principle [9] we have \(\Vert \pi (S)\Vert _{L^2({\mathbf {X}})\rightarrow L^2( {\mathbf {X}})}\le C\Vert S\Vert _{L^2({\mathbb {H}}_n)\rightarrow L^2({\mathbb {H}}_n)}\). Moreover, from (2.7), (2.9), (4.2), Lemmas 2.1 and 2.2 we conclude
Consequently, \(\pi (S)\) is a Calderón–Zygmund operator with the associated kernel
which satisfies
Lemma 4.1
There is a constant \(C>0\) such that for any regular kernel S of order 0 on \({\mathbb {H}}_n\) and for every function \(f\in C^1_c(B({\mathbf {x}}_0, r_0))\) we have
Proof
Note that (1.2) and (4.5) imply
and
Let \(j_0\) be such that \(2^{-j_0}<r_0\le 2^{-j_0+1}\). Clearly, by (4.3) and (4.4), we get
Observe that if \(B({\mathbf {x}}_0,r_0)\cap B({\mathbf {x}}, C_12^{-j+1})\ne \emptyset \) with \(j<j_0\), then \(|B({\mathbf {x}}, 2^{-j})|\sim |B({\mathbf {x}}_0, 2^{-j})|\). Hence, applying (4.10), (4.11) and (1.4) we obtain
To estimate \(J_2\) we use (1.2) together with (4.11) and get
\(\square \)
Thanks to Lemma 4.1 for \(f\in L^1({\mathbf {X}})\) and a regular kernel S of order 0 we define \(\pi (S)f\) in the sense of distribution setting
Lemma 4.2
There is a constant \(C>0\) such that for any regular kernel S of order 0 on \({\mathbb {H}}_n\) which has the form (4.1) we have
Proof
The proof is standard. For the sake of completeness we present its sketch. Without loss of generality we can assume that \(c_1=0\). Because \(\pi (S)\) maps continuously \(L^1({\mathbf {X}})\) to \({\mathcal {D}}'({\mathbb {R}}^{n+1})\), it suffices to prove that there is a constant \(C>0\) such that \(\Vert \pi (S)a\Vert _{H^1_{{\mathcal {L}}}}\le C\) for every atom \(a\in H^1_\mathrm{atom, \, \infty } ({\mathbf {X}})\). Fix a \((1,\infty )\)-atom a associated with a ball \(B({\mathbf {y}}_0, r_0)\). Since \(\sum _{j}\pi (m_j)a\) converges in \(L^2({\mathbf {X}})\), it converges in the \(L^1({\mathbf {X}})\) norm on \(B({\mathbf {y}}_0, 2r_0)\) as well. Note also that \(\pi (m_j)a({\mathbf {x}})=0\) for \(d({\mathbf {x}}, {\mathbf {y}}_0)>2C_1 2^{-j}+r_0\). If \(2r_0<d({\mathbf {x}},{\mathbf {y}}_0)\le 2C_1 2^{-j}+r_0\), then applying (1.2) and (4.5) we get
Hence, \(\sum _{j}\pi (m_j)a\) converges in \(L^1({\mathbf {X}})\) and \(L^2({\mathbf {X}})\) to \(\pi (S)a\) and \(\int \pi (S)a({\mathbf {x}})\, d{\mathbf {x}}=0\). Moreover,
So, \(\pi (S)a\) can be written as \(\pi (S)a=\sum _{j} \lambda _j a_j \) with \(a_j\) being (1, 2)-atoms and \(\sum _j |\lambda _j |\le C\). \(\square \)
Let \(\psi \) be a Schwartz class function on \([0,\infty ) \) and \(dE_{L}\) and \(dE_{{\mathcal {L}}}\) be the spectral measures for L and \({\mathcal {L}}\) respectively. It is well known that the operator
is a convolution operator with a Schwartz class function on \({\mathbb {H}}_n\) denoted by the same symbol \(\psi (L)(\varvec{x})\) , that is, \(\psi (L)f(\varvec{x})=f*\psi (L)(\varvec{x})\) (see, e.g., [14]). Moreover, for every multi-index I and \(M\ge 0\) there is \(N>0\) and a constant \(C_{I,M,N}>0\) such that
By homogeneity,
Clearly, the operator
is of the form
where
For detailed spectral properties of \({\mathcal {L}}\) we refer the reader to [19].
4.2 Riesz Transforms
The Riesz transforms \(R_j\), \(j=1,2,\ldots ,2n\), on the Heisenberg group \({\mathbb {H}}_n\) are defined by \(R_jf=X_jL^{-1\slash 2}f=\lim _{\varepsilon \rightarrow 0}c\int _{\varepsilon }^{\varepsilon ^{-1}} X_j e^{-tL}f \frac{dt}{\sqrt{t}}= \lim _{\varepsilon \rightarrow 0}f*(c\int _{\varepsilon }^{\varepsilon ^{-1}} X_j h_t \frac{dt}{\sqrt{t}}).\) By the Cotlar–Stein almost orthogonality principle the above limit defines a bounded operator on \(L^2({\mathbb {H}}_n)\). One can also prove that \(R_j\) are the principal valued convolution singular integral operators \(R_jf=f*\check{R}_j\), where \( R_j(\varvec{x})= -c\int _0^\infty Y_j h_t(\varvec{x})\frac{dt}{\sqrt{t}}\) are real-valued regular kernels of order 0.
Similarly the Riesz transforms \({\mathcal {R}}_j\) associated with the Grushin operator are defined by \({\mathcal {R}}_j=c\pi (X_j){\mathcal {L}}^{-1\slash 2}\), \(j=1,2,\ldots ,2n\). Clearly, \({\mathcal {R}}_j=\pi ( R_j)\). Thus \({\mathcal {R}}_j\) are Calderón–Zygmund operators on \({\mathbf {X}}\), which are bounded on \(L^p({\mathbf {X}})\), \(1<p<\infty \), and, by Lemma 4.2, bounded on \(H^1_{{\mathcal {L}}}\). For boundedness of \(\mathcal R_j\) on \(L^p(\mathbf X)\) see also [16].
5 \((\star )\) Property and Decomposition of \(BMO({\mathbf {X}})\)
Let \(\overrightarrow{S}=(S_1,S_2,\ldots ,S_d)\) be a system of regular kernels of order 0 on \({\mathbb {H}}_n\). We say that it fulfills condition \((\star )\) if for every unit vector \(\nu \in {\mathbb {R}}^d\) there are regular kernels \(T_j\) of order zero, \(\langle T_j,f\rangle =c_j f(0)+\mathrm{pv}\int _{{\mathbb {H}}_n} m^{\{j\}}(\varvec{x}) f(\varvec{x})\, d\varvec{x}\), \(j=1,2,\ldots ,d\), such that
Theorem 5.1
(Christ and Geller [5, Sect. 6]) The system of the regular kernels of order zero \(\{\delta _0,R_1,R_2,\ldots ,R_{2n}\}\) on the Heisenberg group \({\mathbb {H}}_n\) fulfils condition \((\star )\).
A locally integrable function f on \({\mathbf {X}}\) is said to be an element of \(BMO({\mathbf {X}})\) if
here \(f_{B({\mathbf {y}}, r)}=|B({\mathbf {y}},r)|^{-1}\int _{B({\mathbf {y}}, r)}f({\mathbf {x}})\, d{\mathbf {x}}\) denotes the mean value of f over \(B({\mathbf {y}},r)=\{ {\mathbf {x}}\in {\mathbf {X}}: d({\mathbf {y}}, {\mathbf {x}})<r\}\).
Our goal of this section is to prove the following theorem.
Theorem 5.2
Assume that \(S_j\), \(j=1,2,\ldots ,d\), is a system of operators satisfying \((\star )\). Then there is a constant \(C>0\) such that any compactly supported \(BMO({\mathbf {X}})\) function f can be written as
with
Moreover,
For the proof of the theorem we follow methods presented in Christ and Geller [5] about decompositions of BMO functions on homogeneous Lie groups (see also the original Uchiyama’s proof [26] of constructive Fefferman–Stein decomposition of BMO functions on the Euclidean spaces).
There is no loss of generality to assume that \(\Vert f\Vert _{BMO({\mathbf {X}})}= \varepsilon \) with \(\varepsilon >0\) very small to be determined latter on.
Let us also emphasize that for any \(t>0\) the mapping \(f\mapsto f\circ \delta _t\) is an isometry on \(L^\infty \) and \(BMO({\mathbf {X}})\).
The main step of the proof of Theorem 5.2 is the following theorem.
Theorem 5.3
Assume that \(S_j\), \(j=1,2,\ldots ,d\), is a system of operators satisfying \((\star )\). Then there are constants constant \(C_8, C_9, \varepsilon _0 >0\) such that any \(BMO({\mathbf {X}})\) function f supported in any ball \(B({\mathbf {z}}_B, r)\) with \(\Vert f\Vert _{BMO({\mathbf {X}})}=\varepsilon <\varepsilon _0\), can be written as
Moreover,
For the proof of Theorem 5.3 we adapt arguments of Christ and Geller [5]. For the convenience of the reader we present all the details in Appendixes 1 and 2.
Proof of Theorem 5.2
Fix \(0<\varepsilon <\varepsilon _0\) such that \(C_9\varepsilon <1\) and \(C_9C_8^{3\slash 2} \varepsilon <1\). Decompose f according to Theorem 5.3. If \(f_1=0\) we are done. Otherwise we apply Theorem 5.3 to the function \(\varepsilon \Vert f_1\Vert _{BMO({\mathbf {X}})}^{-1} f_1\) and obtain functions \(f_2\), \(\widetilde{g}_j^{\{1\}}\), \(j=0,1,\ldots ,d\), such that
Set \(\widetilde{g}_j^{\{0\}}=\widetilde{g}_j\), \(j=0,1,\ldots ,d\). Continuing this procedure we obtain sequences of functions \(\widetilde{g}^{\{n\}}_j\), \(j=0,1,\ldots ,d\), \(n=0,1,2,\ldots \), and \(f_n\) such that
Observe that
Putting \(\varvec{g}_j=\sum _{n=0}^\infty \widetilde{g}_j^{\{n\}}\) we obtain Theorem 5.2. \(\square \)
6 Proof of Theorem 1.2
Let \(VMO({\mathbf {X}})\) be the closure of the space of continuous functions with compact support in the BMO-norm. It is well-known (see [8, Theorem 4.1]) that \(VMO({\mathbf {X}})\) is a predual space to \(H^1_\mathrm{atom,\, \infty }({\mathbf {X}})\), that is, \(VMO({\mathbf {X}})^*=H^1_\mathrm{atom, \, \infty }({\mathbf {X}})\) in the sense that any functional \(\Phi \) on \(VMO({\mathbf {X}})\) is of the form \(\Phi (f)=\int f({\mathbf {x}})\overline{F({\mathbf {x}})}\, d{\mathbf {x}}\) for \(f\in C_c({\mathbf {X}})\), where \(F\in H^1_\mathrm{atom, \, \infty }({\mathbf {X}})\).
Assume firstly that \(F\in L^1({\mathbf {X}})\cap L^2({\mathbf {X}})\) and \({\mathcal {R}}_j F\in L^1({\mathbf {X}})\), \(j=1,2,\ldots ,2n\). If f is compactly supported continuous function on \({\mathbf {X}}\), then, according to Theorems 5.1 and 5.2, there are functions \(\varvec{g}_j \in L^\infty ({\mathbf {X}})\cap L^2({\mathbf {X}})\), \(j=0,1,2,\ldots ,2n\), such that \(\sum _{j=0}^{2n} \Vert \varvec{g}_j\Vert _\infty \le C \Vert f\Vert _{BMO({\mathbf {X}})}\) and \(f=\varvec{g}_0+\sum _{j=1}^{2n} {\mathcal {R}}_j^*\varvec{g}_j\). Hence,
Thus, the integral \(f\mapsto \int f({\mathbf {x}})\overline{F({\mathbf {x}})}\, d{\mathbf {x}}\) has the unique extension to a bounded functional on \(VMO({\mathbf {X}})\) and, consequently, \(F\in H^1_{\mathrm{atom,\, \infty }}({\mathbf {X}})\) with
We now relax the assumption \(F\in L^2({\mathbf {X}})\) assuming only that \(F\in L^1({\mathbf {X}})\) with \({\mathcal {R}}_j F\in L^1({\mathbf {X}})\).
Lemma 6.1
Let S be a regular kernel of order zero on \({\mathbb {H}}_n\). Then there is a constant \(C>0\) such that for every \(t>0\)
where \(\big [\pi ( S),e^{-t{\mathcal {L}}}\big ]= \pi ( S)e^{-t{\mathcal {L}}}- e^{-t{\mathcal {L}}}\pi ( S)\) is the commutator of \(\pi (S)\) and \(e^{-t{\mathcal {L}}}\).
We shall postpone the proof of the lemma to the end of the section.
Note that \(e^{-t{\mathcal {L}}} F\in L^2({\mathbf {X}})\) for \(F\in L^1({\mathbf {X}})\). Thus from Lemma 6.1 we conclude that
with a constant C independent of \(t>0\). The first part of the proof combined with (6.3) and Theorem 1.1 lead to
because \(e^{-t{\mathcal {L}}}\) is uniformly bounded on \(L^1({\mathbf {X}})\). Since \({\mathcal {M}}_{{\mathcal {L}}} (e^{-t_1{\mathcal {L}}} F)({\mathbf {x}})\le {\mathcal {M}}_{{\mathcal {L}}} (e^{-t_2{\mathcal {L}}} F)({\mathbf {x}})\) for \(0<t_2<t_1\), we deduce from the Lebesgue monotone convergence theorem that \({\mathcal {M}}_{{\mathcal {L}}} F\in L^1({\mathbf {X}})\) and
This completes the proof of the first inequality of (1.6).
The proof of the second inequality in (1.6) is standard and follows from the fact that \({\mathcal {R}}_j\) are Calderón–Zygmund operators (see Sect. 4). We omit the details.
Proof of Lemma 6.1
By the homogeneity it suffices to prove the lemma for \(t=1\). Recall that
where \(H_t({\mathbf {x}},{\mathbf {y}})\) denote the integral kernel for \(e^{-t{\mathcal {L}}}\). Let \(m_j\) be as in Sect. 4.1. Set
If \(j\le 0\), then
By (4.5), (1.2) and (2.13), we have
Using (4.4) and (2.13) and (4.5), we obtain
Similarly,
Again, applying (1.2), (4.5), (2.13) and the doubling property of the measure, we get
If \(d({\mathbf {x}},{\mathbf {y}}) > 8C_12^{-j}\) then \(\pi (m_j)({\mathbf {x}},{\mathbf {y}})=0\). Hence, thanks to (2.13) and (4.5), we have
If \(j>0\), then using (4.3) and Corollary 2.5 we arrive to
Finally, (6.4)–(6.8) imply \(\sum _{j=-\infty }^\infty M_j\le C<\infty \), which completes the proof of the Lemma. \(\square \)
References
Anker, J-Ph, Ben Salem, N., Dziubański, J., Hamba, N.: The Hardy space \(H^1\) in the rational Dunkl setting. Constr. Approx. 42, 93–128 (2015)
Burkholder, D.L., Gundy, R.F., Silverstein, M.L.: A maximal function characterization of the class \(H^p\). Trans. Am. Math. Soc. 157, 137–153 (1971)
Christ, M.: On regularity of inverses of singular integral operators Duke. Math. J. 57, 547–598 (1984)
Christ, M.: A \(T(b)\) theorem with remarks on analytic capacity and the Cauchy integral. Colloq. Math. 60(61), 601–628 (1990)
Christ, M., Geller, D.: Singular integral characterizations of Hardy spaces on homogeneous groups. Duke Math. J. 51, 547–598 (1984)
Coifman, R.: A real variable characterization of \(H^p\). Studia Math. 51, 269–274 (1974)
Coifman, R., Weiss, G.: Analyse Harmonique Non-commutative sur Certains Espaces Homogènes. Lecture Notes in Mathematics. Étude de certaines intégrales singulières, vol. 242. Springer, Berlin (1971)
Coifman, R., Weiss, G.: Extensions of Hardy spaces and their use in analysis. Bull. Am. Math. Soc. 83, 569–615 (1977)
Coifman, R., Weiss, G.: Transference Methods in Analysis. CBMS Regional Conference Series in Mathematics, vol. 31. AMS, Providence (1977)
Coulhon, T., Sikora, A.: Gaussian heat kernel upper bounds via Phragmen-Lindelof theorem. Proc. Lond. Math. Soc. (3) 96, 507–544 (2008)
Fefferman, C., Stein, E.M.: \(H^p\) spaces of several variables. Acta Math. 129, 137–193 (1972)
Folland, D.G., Stein, E.M.: Hardy Spaces on Homogeneous Groups. Princeton University Press, Princeton (1982)
Hofmann, S., Lu, G.Z., Mitrea, D., Mitrea, M., Yan, L.X.: Hardy Spaces Associated with Non-negative Self-adjoint Operators Satisfying Davies-Gafney Estimates. Memoirs of the American Mathematical Society 214, vol. 1007. American Mathematical Society, Providence (2011)
Hulanicki, A.: A functional calculus for Rockland operators on nilpotent Lie groups. Studia Math. 78, 253–266 (1984)
Jotsaroop, K.: Grushin Multiplier and Toeplitz Operators. PhD thesis, Department of Mathematics Indian Institute of Sciences, Bangalore (2012)
Jotsaroop, K., Sanjay, P.K., Thangavelu, S.: Riesz transforms and multipliers for the Grushin operator. J. Anal. Math. 119, 255–273 (2013)
Macías, R.A., Segovia, C.: A decomposition into atoms of distributions on spaces of homogeneous type. Adv. Math. 33, 271–309 (1979)
Martini, A., Sikora, A.: Weighted Plancherel estimates and sharp spectral multipliers for the Grushin operators. Math. Res. Lett. 19, 1075–1088 (2012)
Meyer, R.: \(L^p\) estimates for the wave equation associated to the Grushin operator. PhD thesis, Mathematisch-Naturwissenschaftlichen Fakultät, Christian-Albrechts-Universität, Kiel, Germany (2006)
Robinson, D.W., Sikora, A.: Analysis of degenerate elliptic operators of Grushin type. Math. Z. 260, 475–508 (2008)
Sikora, A.: Riesz transform, Gaussian bounds and the method of wave equation. Math. Z. 247, 643–662 (2004)
Stein, E.M.: Harmonic Analysis, Real-Variable Methods, Orthogonality, and Oscillatory Integrals. Princeton University Press, Princeton (1993)
Stein, E.M., Weiss, G.: On the theory of harmonic functions of several variables, I: the theory of \(H^p\) spaces. Acta Math. 103, 25–62 (1960)
Stromberg, J.-O., Torchinsky, A.: Weighted Hardy Spaces. Lecture Notes in Mathematics, vol. 1381. Springer, Berlin (1989)
Uchiyama, A.: A maximal function characterization of \(H^p\) on the space of homogeneous type. Trans. Am. Math. Soc. 262(2), 579–592 (1980)
Uchiyama, A.: A constructive proof of the Fefferman-Stein decomposition of BMO\(({\mathbb{R}}^n)\). Acta Math. 148, 215–241 (1982)
Varopoulos, NTh, Saloff-Coste, L., Coulhon, T.: Analysis and Geometry on Groups. Cambridge Univesrity Press, Cambridge (1992)
Acknowledgments
This research was initiated when the second author was visiting the Institute of Mathematics of the University of Wrocław in the spring of 2014; the financial support and kind hospitality are gratefully acknowledged. The authors want to thank the referee for her/his helpful comments which improved the presentation of the paper. The first author supported by the Polish National Science Center (Narodowe Centrum Nauki, Grant DEC-2012/05/B/ST1/00672).
Author information
Authors and Affiliations
Corresponding author
Additional information
Communicated by Hans G. Feichtinger.
Appendices
Appendix 1: Chang–Fefferman Decomposition
Our goal in this section is to prove a version of Chang–Fefferman decomposition of compactly supported \(BMO({\mathbf {X}})\) functions. Then we shall establish some properties of the decomposition. We borrow main ideas from [5].
1.1 Dyadic Sets
Theorem 7.1
(Christ [4]) There exist a collection \({\mathcal {B}}\) of open sets \(\{Q_\alpha ^k\subset {\mathbb {R}}^{n+1}: \ k\in {\mathbb {Z}}, \ \alpha \in I_k\}\), and constants \(\delta \in (0,1)\), \(1\ge a_0>0\), and \(C_3>0\) such that
Set \({\mathcal {B}}_k=\{ Q_\alpha ^k: \ \alpha \in I_k\}\) and \(\ell (Q)=\delta ^{k}\) if \(Q\in {\mathcal {B}}_k\). Fix a constant \(A_0>2\) such that for any \({\mathbf {x}}\in {\mathbf {X}}\) and \(k\in {\mathbb {Z}}\) there is \(Q\in {\mathcal {B}}_k\) such that \(B({\mathbf {x}}, 8\delta ^{k-1})\subset A_0B_Q\). Then for any ball \(B=B({\mathbf {x}}, r)\) denote \(A_0B=B({\mathbf {x}},A_0r)\) by \(\tilde{B}\).
1.2 Chang–Fefferman Decomposition
Lemma 7.2
Suppose that \(N_1\in {\mathbb {N}}\) is given. Then every \(f\in BMO({\mathbf {X}})\) with compact support can be decomposed to
where
where \(C_{I}\) and C are independent of f.
Remark 7.3
Let us emphasize that the condition (7.7) replaces the condition
in the Chang–Fefferman decomposition for the classical BMO spaces and for the BMO spaces on homogeneous Lie groups. Actually (7.7) implies (7.11) by the integration by parts, since \({\mathcal {L}}^{N_1} W({\mathbf {x}})=0\) for every polynomial W of homogeneous degree \(<2N_1\).
Proof of Lemma 7.2
For fixed \(N_1\) let \(\phi , \psi , \eta \in {\mathcal {S}}({\mathbb {R}})\) be real valued functions such that
Here \(\widehat{\phi }\) and \( \widehat{\eta }\) denote the Fourier transforms of \(\phi \) and \(\eta \) respectively. Then there are Schwartz class functions \(\phi (\sqrt{L})(\varvec{x})\) and \(\eta (\sqrt{L})(\varvec{x})\) on \({\mathbb {H}}_n\) such that \(\phi (t\sqrt{L}) f(\varvec{x})=f* \phi (t\sqrt{L})(\varvec{x})\), \(\phi (t\sqrt{L})(\varvec{x})=t^{-D}\phi (\sqrt{L})(\delta _t^{-1}\varvec{x})\). The same holds for \(\eta (t\sqrt{L})(\varvec{x})\). Moreover, it follows from (2.13), (7.13), and the finite propagation of the fundamental solution of the wave equation that the functions \(\phi (t\sqrt{L})(\varvec{x})\) and \(\eta (t\sqrt{L})(\varvec{x})\) are compactly supported, that is, there is a constant \(C'>0\) such that
see [10, 21] for details. Consequently, by Lemma 2.1,
Additionally,
with the same estimates on \( \pi (X^I)_{{\mathbf {x}}} \phi (t\sqrt{{\mathcal {L}}}) ({\mathbf {x}},{\mathbf {y}})\).
For \(f\in L^2({\mathbf {X}})\) we have
Set
Thus (7.6) and (7.7) hold. Now (7.8) follows from (7.4) and (7.15). Observe that \( |B({\mathbf {y}}, t)| \sim |Q_{\alpha }^k|\) for \(({\mathbf {y}}, t) \in Q_\alpha ^k\times (\delta ^{k}, \delta ^{k-1})\). Thus from (7.15) and (7.16) we conclude
which gives (7.9). Finally, for fixed \(Q\in {\mathcal {B}}\),
So to finish the proof of (7.10) it suffices to note that \(|\phi (t\sqrt{{\mathcal {L}}})f({\mathbf {x}})|^2\, d{\mathbf {x}}\frac{dt}{t}\) is a Carleson measure with the estimate
for any ball \(B\subset {\mathbf {X}}\). This fact has a standard proof, which for the reader convenience we present here. First from (7.12) and (2.7) one gets
Fix a ball B and decompose
where \(c=|C_6B|^{-1}\int _{C_6B} f({\mathbf {x}})\, d{\mathbf {x}}\), \(C_6=16(C_5+1)\). Applying (7.24) we have \(\phi (t\sqrt{{\mathcal {L}}})f=\phi (t\sqrt{{\mathcal {L}}})f_1+\phi (t\sqrt{{\mathcal {L}}})f_2\). By the John–Nirenberg inequality \(\Vert f_1\Vert _{L^2}^2\le C |B|\Vert f\Vert _{BMO({\mathbf {X}})}^2\) (see e.g., [24, Sect. III]). Consequently,
Further, thanks to (7.15), \(\phi (t\sqrt{{\mathcal {L}}})f_2({\mathbf {x}})=0\) for \({\mathbf {x}}\in B\) and \(0<t\le \mathrm{diam}\, B\). Thus (7.23) is proved. \(\square \)
Let us remark that for \(\lambda _Q\) defined in (7.18) we have
since \(|\phi (t\sqrt{{\mathcal {L}}})f({\mathbf {x}})|^2\, d{\mathbf {x}}\frac{dt}{t}\) is a Carleson measure.
Lemma 7.4
Let \(N\in {\mathbb {Z}}^+\) be given. Then there exist constants \(N_1\in {\mathbb {Z}}^+\) and \(C_{N}>0\) such that for any regular kernel S of order 0 of the form (4.1) and any \(a_Q\) satisfying (7.7)–(7.9) we have
Proof
Thanks to (7.7)–(7.9) without loss of generality we may assume that \(c_1=0\).
In order to prove (7.27) it suffices, by (7.7)–(7.9), (4.5) and Lemma 4.1, to consider \(d({\mathbf {x}},{\mathbf {z}}_Q)>16C_4a_0\ell (Q)\). Then, integration by parts leads to
where in the last inequality we have used (1.4). The proof of (7.27) is complete.
We now turn to prove (7.28). It suffices to consider \(d({\mathbf {x}},{\mathbf {x}}')\le \ell (Q)\), otherwise (7.28) follows from (7.27).
Assume first that \(d({\mathbf {x}},{\mathbf {z}}_Q)>16C_4a_0\ell (Q)\). Let \(g\in C_c^\infty ({\mathbf {X}})\) be such that \(g({\mathbf {x}})=g({\mathbf {x}}')=1\), \(\text {supp}\, g\in B({\mathbf {x}}, d({\mathbf {x}},{\mathbf {z}}_Q)\slash 4)\), \(\Vert \pi (X^I)g\Vert _\infty \le C_Id({\mathbf {x}}, {\mathbf {z}}_Q) ^{-d(I)}\). Then, integrating by parts and using (1.2) together with (4.8) and (7.9), we obtain
where in the last inequality we have applied (1.4).
Assume now that \(d({\mathbf {x}},{\mathbf {z}}_Q)\le 16C_4a_0\ell (Q)\). According to (1.2) it is enough to prove that
Consider j’s such that \(2^{-j} > \ell (Q)\). Then, by (4.5) and (7.7)–(7.9), we get
Therefore, \(\sum _{2^{-j}>\ell (Q)} | \pi (X_k) \pi (m_j)a_Q({\mathbf {x}})|\le C\Vert m_0\Vert _{C^1} \ell (Q)^{-1} \).
Consider \(2^{-j}\le \ell (Q)\). By (2.9) and (2.2), we have
Hence, integration by parts and use of (4.3) lead to
since \(|w_{k}m_j|\le C2^{-j} |m_j|\). So, \(\sum _{2^{-j}\le \ell (Q)} | \pi (X_k) \pi (m_j)a_Q({\mathbf {x}})|\le C\Vert m_0\Vert _\infty \ell (Q)^{-1} \).
Finally (7.29) is a direct consequence of Lemma 4.2, because \(a_Q\) is a multiple of a \((1,\infty )\)-atom for \(H^1({\mathbf {X}})\). \(\square \)
Corollary 7.5
Assume that for \(S_j\), \(j=1,\ldots ,d\), the condition \((\star )\) holds. Suppose that \(a_Q\) satisfies the conclusions (7.7)–(7.9) of the Chang–Fefferman decomposition. Then there is a constant \(C_{N}\) such that given any unit vector \(\nu \in {\mathbb {R}}^d\) there exists \(\overrightarrow{b}_Q\) such that
Proof
Define \(\overrightarrow{b}_Q=\pi (\overrightarrow{T}) (a_Q)\). Then (7.34), (7.35), and (7.37) follow directly from Lemma 7.4 and property \((\star )\). It suffices to prove (7.36). If \(d({\mathbf {x}},{\mathbf {y}})\le \ell (Q)\) or \(d({\mathbf {x}},{\mathbf {y}})\le 3 d({\mathbf {x}},{\mathbf {z}}_Q)\), then (7.36) is deduced easily from (7.28). Finally assume that \(d({\mathbf {x}},{\mathbf {y}})>\ell (Q)\) and \(3d({\mathbf {x}},{\mathbf {z}}_Q)<d({\mathbf {x}},{\mathbf {y}})\). Then \(d({\mathbf {x}},{\mathbf {z}}_Q)<d({\mathbf {z}}_Q, {\mathbf {y}})\) and, consequently, (7.34) implies (7.36). \(\square \)
1.3 Auxiliary Functions
Let \(N_0\) be a large integer. For a compactly supported \(f\in BMO({\mathbf {X}})\) define
where \(\lambda _Q\) are scalars from the Chang–Fefferman decomposition (see Lemma 7.2). Fix \(0<\kappa <1-\delta \), where \(\delta \) is from Theorem 7.1 and set
Then,
Easily, if \(N_0\) is sufficiently large, then
Indeed,
Because \(\sum _{\ell (P)=\delta ^k} \big (1+\delta ^{-k}d({\mathbf {z}}_P,{\mathbf {x}})\big )^{-N_0}\le C\) independently of k, provided \(N_0>3\).
Lemma 7.6
(Christ and Geller [5]) If \(N_0\) is sufficiently large, then for every compacty supported \(BMO({\mathbf {X}})\)-function f one has
Proof
The proof is same as of [5, Lemma 3.3].
Lemma 7.7
There is a constant C such that if \(f=\sum \lambda _Qa_Q\) is the Chang–Fefferman decomposition of a \(BMO({\mathbf {X}})\)-function f given by the proof of Lemma 7.2 such that \(\text {supp}\, f\subset B({\mathbf {x}}_0,1)\), then
Proof
There is a constant \(M_1\) such that for \(k\le 0\) the number of \(Q\in {\mathcal {B}}_k\) such that \(\lambda _Q\ne 0\) is bounded by \(M_1\) with \(M_1\) independent of \({\mathbf {x}}_0\). For such Q, \(|Q|\sim |B({\mathbf {x}}_0,\delta ^k)|\). So, by (7.18) and (7.16),
which implies the lemma. \(\square \)
Appendix 2: Proof of Theorem 5.3
Proof of Theorem 5.3
Using dilations we may assume without loss of generality that f is supported by \(B({\mathbf {z}}_B, 1)\). By the Chang–Fefferman decomposition given in the proof of Lemma 7.2 we have
It follows from Lemma 7.7 that
Thus, in farther consideration we shall deal with the function \(f_0=\sum _{\ell (Q)\le 1} \lambda _Qa_Q\) with \(\lambda _Q\), \(a_Q\) satisfying (7.7)–(7.10). Remark that there is a constant \(C_{10}\) independent of \({\mathbf {z}}_B\) such that that if \(\lambda _Q\ne 0\) in the decomposition of \(f_0\), then
Following [5] our task is to construct, by induction, for each integer \(l\ge -1\) functions \(\overrightarrow{h}_l\), \(\overrightarrow{g}_l\) and \(\overrightarrow{E}_l\) on \({\mathbf {X}}\) taking values in \({\mathbb {C}}^d\) such that
The proofs of the above will be based on the following (simultaneously established) properties of \(\overrightarrow{h}_l\), \(\overrightarrow{g}_l\), and \(\overrightarrow{E}_l\):
where \(A_0\) is a constant appearing in the definition of \(\tilde{B}\) and \(A_1>C_{11}(1-C_{11}C_{12}\varepsilon )^{-1}\).
We define \(\overrightarrow{g}_{-1}({\mathbf {x}})\equiv (1,0,\ldots ,0)\), \(\overrightarrow{E}_{-1}({\mathbf {x}})=\overrightarrow{h}_{-1}({\mathbf {x}})\equiv (0,\ldots ,0)\).
Assume that (8.3)–(8.6), (8.9)–(8.16) hold for all j such that \(j<l\). From Corollary 7.5 one can deduce that for Q with \(\ell (Q)=\delta ^l\) there exists \(\overrightarrow{b}_Q({\mathbf {x}})\) satisfying (8.10)–(8.13) such that \(a_Q({\mathbf {x}})=\overrightarrow{S^*}\cdot \overrightarrow{b}_Q({\mathbf {x}})\). Let \(\overrightarrow{h}_l({\mathbf {x}})\) be given by (8.9). Then, thanks to (8.10) and Lemma 7.6,
Define \(\overrightarrow{G}_l({\mathbf {x}})=\overrightarrow{g}_{l-1}({\mathbf {x}})+ \overrightarrow{h}_l({\mathbf {x}})\). Set \(C_{13}= C_{11}C_{12}\). Since \(|\overrightarrow{g}_{l-1}({\mathbf {x}})|\equiv 1\),
In other words \(|\overrightarrow{G}_l({\mathbf {x}})|\) is close to 1. Thanks to the orthogonality a better estimates is true:
To show (8.19) we estimate
where in the first inequality we have used (8.10) and (8.14). Recall that \(|\overrightarrow{g}_{l-1}({\mathbf {x}})|\equiv 1\). Hence,
where in the last inequality we have used (7.40). Thus (8.19) is established.
We define
Our task is to verify (8.14). Using (8.18) we have
Further,
By induction the first summand in (8.22) is dominated by
By (8.11) and (8.9) the second summand in (8.22) is bounded by
Recall that \(\delta (1-\kappa )^{-1}<1\). Take \(\varepsilon >0\) small enough so that
Recall also that \(A_1>C_{11}(1-C_{13}\varepsilon )^{-1}\). By the above
and (8.14) is established.
To obtain (8.15) note that that thanks to (8.19) we have
We now turn to prove (8.16). We start by showing that there is a constant \(C_{15}\) such that
Applying (8.9), (8.11) and Lemma 7.6 we obtain
since \(d({\mathbf {x}},{\mathbf {y}})\le A_0 \delta ^l\). To estimate \(J_2\) we use (8.17), (8.14), and Lemma 7.6 to obtain
In order to estimate \(J_3\) we apply (8.9) and (8.13) to write
Then utilizing (8.12) and (8.14) we have
where in the last inequality we have used Lemma 7.6. So the proof of (8.25) is complete.
We are now in a position to finish the proof of (8.16). By the definition of \(\overrightarrow{E}_{l}\) and (8.18),
where in the last inequality for the first summand we have used (8.23) while for the second one we have applied (8.25). Now from Lemma 7.6 we obtain (8.16).
Thus the construction of the functions \(\overrightarrow{h}_{l}\), \(\overrightarrow{g}_{l}\) and \(\overrightarrow{E}_{l}\) satisfying (8.3)–(8.5) and (8.9)–(8.16) is complete.
It remains to prove (8.6)–(8.8). First, (7.29) combined with (8.11) and (8.13) imply
Now for nonnegative integers \(s_1\le s_2\) let \({\mathcal {Q}}={\mathcal {Q}}_{s_1,s_2}=\bigcup _{l=s_1}^{s_2}{\mathcal {B}}_l\). In virtue of (8.26),
Applying two times the Cauchy–Schwarz inequality we obtain
Observe that for fixed integer \(k\ge 0\) and fixed \(Q\in {\mathcal {Q}}\),
so
It follows from (1.4) and Theorem 7.1 that there is a constant \(C>0\) such that for every \(j,k\ge 0\) and every \(P\in {\mathcal {Q}}\) the number of \(Q\in {\mathcal {Q}}\) such that \(\ell (P)=\delta ^{k}\ell (Q)\), \(d({\mathbf {z}}_Q,{\mathbf {z}}_P)\le 2^{j}\ell (Q)\) is bounded by \(C2^{3j}\). Therefore,
where in the last inequality we have used (7.18). From the spectral theorem we easily conclude that \(\Vert \sum _{l=s_1}^{s_2} \overrightarrow{h}_{l}\Vert _{L^2}^2\rightarrow 0\) as \(s_1,s_2\rightarrow \infty \).
Fix \(Q\in {\mathcal {B}}\). Let k be such that \(\delta ^k=\ell (Q)\). From (8.15) and Lemma 7.6 we obtain
On the other hand we conclude from (8.16) that for \({\mathbf {x}},{\mathbf {y}}\in \tilde{Q}\) we have the following estimate on the finite sum:
From (8.28) and (8.29) we obtain that the series \(\sum _{j\ge 0} \overrightarrow{E}_j({\mathbf {x}})\) converges in \(L^1_\mathrm{loc}\) to \(\overrightarrow{E}^0({\mathbf {x}})\) and
Since \(\sum _{j=0}^l \overrightarrow{h}_j+\overrightarrow{E}_j=\overrightarrow{g}_l-\overrightarrow{g}_{-1}\), we conclude (8.6) from (8.7), (8.27), (8.28), and (8.4).
Having (8.3)–(8.16) already proved we are in a position to complete the proof of Theorem 5.3.
It follows from (8.24) and Lemma 7.6 that
Thus if \(d({\mathbf {x}},{\mathbf {z}}_B)>2C_{10}\), then thanks to (7.26), (8.1), and (8.2) we have
By (8.27), \(\sum _{l\ge 0} \overrightarrow{h}_l({\mathbf {x}}) =\sum _{l(Q)\le 1} \lambda _Q \overrightarrow{b}_Q\) converges in \(L^2({\mathbf {X}})\) and
We decompose
Now using (8.31) combined with (8.8) we get
and, consequently,
Finally, from (8.32) and (8.36) we deduce
Let
Lemma 4.2 together with (8.35) and duality argument give \(\Vert F\Vert _{BMO({\mathbf {X}})}\le \!C \Vert f\Vert _{{ BMO}({\mathbf {X}})}^2\). Moreover, \(|F({\mathbf {x}})| \le C \Vert f\Vert ^2_{BMO({\mathbf {X}})}\) for \(d({\mathbf {x}},{\mathbf {z}}_B)>4C_{10}\). Putting
we obtain the required decomposition. \(\square \)
Rights and permissions
Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
About this article
Cite this article
Dziubański, J., Jotsaroop, K. On Hardy and BMO Spaces for Grushin Operator. J Fourier Anal Appl 22, 954–995 (2016). https://doi.org/10.1007/s00041-015-9447-5
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s00041-015-9447-5
Keywords
- Grushin operator
- Heat kernel
- Hardy space
- Maximal operator
- Atomic decomposition
- Riesz transforms
- BMO space