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A new version of Carleson measure associated with Hermite operator
Journal of Inequalities and Applications volume 2018, Article number: 177 (2018)
Abstract
Let \(L=-\Delta+|x|^{2}\) be a Hermite operator, where Δ is the Laplacian on \(\mathbb {R}^{d}\). In this paper we define a new version of Carleson measure associated with Hermite operator, which is adapted to the operator L. Then, we will use it to characterize the dual spaces and predual spaces of the Hardy spaces \(H_{L}^{p}(\mathbb {R}^{d})\) associated with L.
1 Introduction
In recent years, the study of function spaces associated with Hermite operators has inspired great interest. Dziubański [7] introduced the Hardy space \(H_{L}^{p}(\mathbb {R}^{d})\), \(0< p\leq1\), by using the heat maximal function and established its atomic characterization. Dziubański et al. [8] and Yang et al. [20] introduced and studied some BMO spaces and Morrey–Campanato spaces associated with operators. Deng et al. [5] introduced the space \(\mathit{VMO}_{L}(\mathbb {R}^{d})\) and proved that \((\mathit{VMO}_{L}(\mathbb {R}^{d}))^{*}=H_{L}^{1}(\mathbb {R}^{d})\). Moreover, recently, Jiang et al. in [14] defined the predual spaces of Banach completions of Orlicz–Hardy spaces associated with operators. Bui et al. [3] considered the Besov and Triebel–Lizorkin spaces associated with Hermite operators.
One of the main purposes of studying the function spaces is to give the equivalent characterizations of them, for example, square functions characterizations for Hardy spaces [10], Carleson measure characterizations for BMO spaces [8] or Morry–Campanato spaces [6]. The aim of this paper is to give characterizations of the dual spaces and predual spaces of the Hardy spaces \(H_{L}^{p}(\mathbb {R}^{d})\) by a new version of Carleson measure. Now, let us review some known facts about the function spaces for L.
Let L be the basic Schrödinger operator in \(\mathbb {R}^{d}\), \(d\geq 1\), the harmonic oscillator \(L=-\Delta+|x|^{2}\). Let \(\{T_{t}^{L}\}_{t>0}\) be a semigroup of linear operators generated by −L and \(K_{t}^{L}(x,y)\) be their kernels. The Feynman–Kac formula implies that
Dziubański [7] defined Hardy space \(H_{L}^{p}(\mathbb{R}^{d})\), \(0< p\leq1\) as
where
The norm of Hardy space \(H_{L}^{p}(\mathbb{R}^{d})\) is defined by \(\|f\|_{H_{L}^{p}}=\|Mf\|_{L^{p}}\).
Remark 1
For simplicity, we just consider the case of \(\frac{d}{d+1}< p\leq1\) in this paper. But all of our results hold for \(0< p\leq1\).
Let \(\rho(x)=\frac{1}{1+|x|}\) be the auxiliary function defined in [17]. This auxiliary function plays an important role in the estimates of the operators and in the description of the spaces associated with L. Then, for \(\frac{d}{d+1}< p\leq1\) and \(1\leq q\leq\infty\), a function a is an \(H_{L}^{p, q}\)-atom for the Hardy space \(H_{L}^{p}(\mathbb {R}^{d})\) associated with a ball \(B(x_{0},r)\) if
The atomic quasi-norm in \(H_{L}^{p}(\mathbb {R}^{d})\) is defined by
where the infimum is taken over all decompositions \(f=\sum c_{j}a_{j}\) and \(a_{j}\) are \(H_{L}^{p, q}\)-atoms.
The atomic decomposition for \(H_{L}^{p}(\mathbb{R}^{d})\) is as follows (see [7]).
Proposition 1
Let \(\frac{d}{d+1}< p\leq1\), we have that the norms \(\|f\|_{H_{L}^{p}}\) and \(\|f\|_{L\textit{-}\mathrm{atom},q}\) are equivalent, that is, there exists a constant \(C>0\) such that
where \(1\leq q\leq\infty\).
We define Campanato space associated with L as (cf. [1] or [20]).
Definition 1
Let \(0\leq\alpha<1\), a locally integrable function g on \(\mathbb {R}^{d}\) belongs to \(\Lambda_{\alpha}^{L}\) if and only if \(\|g\|_{\Lambda_{\alpha}^{L}}<\infty\), where
and
The duality of \(H_{L}^{p}(\mathbb {R}^{d})\) and \(\Lambda_{d(1/p-1)}^{L}\) can be found in [12] or [20].
In order to give the Carleson measure characterization of \(\Lambda _{d(1/p-1)}^{L}\), we need some notations of the tent spaces (cf. [4]).
Let \(0< p<\infty\) and \(1\leq q\leq\infty\). Then the tent space \(T^{p}_{q}\) is defined as the space of functions f on \(\mathbb {R}^{d+1}_{+}\) so that
and
where \(\Gamma(x)\) is the standard cone whose vertex is \(x\in\mathbb {R}^{d}\), i.e.,
Assume that \(B(x_{0},r)\) is a ball in \(\mathbb {R}^{d}\), its tent B̂ is defined by \(\widehat{B}=\{(x,t):|x-x_{0}|\leq r-t\}\). A function \(a(x,t)\) that is supported in a tent B̂, B is a ball in \(\mathbb {R}^{d}\), is said to be an atom in the tent space \(T^{p}_{2}\) if it satisfies
The atomic decomposition of \(T^{p}_{2}\) is stated as follows.
Proposition 2
When \(0< p\leq1\), then every \(f\in T^{p}_{2}\) can be written as \(f=\sum\lambda_{k}a_{k}\), where \(a_{k}\) are atoms and \(\sum|\lambda_{k}|^{p}\leq C\|f\|_{T^{p}_{2}}^{p}\).
Let
where
Assume \(0< p\leq1\), we say a function \(f\in T_{2}^{p,\infty}\) belongs to the space \(T_{2, 0}^{p,\infty}\) if f satisfies \(\eta_{1}(f)=\eta_{1}2(f)=\eta_{3}(f)=0\), where
Let \(\widetilde{T_{2}^{p}}=\{F(x,t)=\sum_{i}\lambda_{i}a_{i}(x,t): a_{i}(x,t) \text{are } T_{2}^{p} \text{ atoms and } \sum_{i}|\lambda_{i}|^{p}<\infty\}\) and \(\|F\|_{\widetilde{T_{2}^{p}}}=\inf\{ (\sum_{i}|\lambda_{i}|^{p} )^{1/p}: F(x,t)=\sum_{i}\lambda_{i}a_{i}(x,t)\}\). Then \(\widetilde{T_{2}^{p}}\) is a Banach space. In fact, it is the completeness of \(T_{2}^{p}\). Especially, \(\widetilde{T_{2}^{1}}=T_{2}^{1}\).
In [19], the author proved the following result.
Proposition 3
Let \(0< p\leq1\). Then
Let \(\{P_{t}^{L}\}_{t>0}\) be the semigroup of linear operators generated by \(-\sqrt{L}\) and \(D_{t}^{L}f(x)=t|\nabla P_{t}^{L}f |(x)\), where \(\nabla=(\partial_{t},\partial_{x_{1}},\ldots,\partial _{x_{d}})\). The Carleson measure characterization of the Campanato space \(\Lambda_{d(1/p-1)}^{L}\) as (cf. [6]).
Proposition 4
Let \(\frac{d}{d+1}< p\leq1\). Then, for any \(f\in L_{\mathrm{loc}}^{2}(\mathbb{R}^{d})\), we have:
-
(a)
If \(f \in\Lambda_{d(1/p-1)}^{L}\), then \(D^{L}_{t}f\in T_{2}^{p,\infty}\); moreover, we have
$$ \bigl\Vert D^{L}_{t}f \bigr\Vert _{T_{2}^{p,\infty}} \leq C \Vert f \Vert _{\Lambda_{d(1/p-1)}^{L}}. $$ -
(b)
Conversely, if \(f\in L^{1}((1+|x|)^{-(d+1)}\,dx)\) and \(D^{L}_{t}f\in T_{2}^{p,\infty}\), then \(f \in\Lambda_{d(1/p-1)}^{L}\) and
$$ \Vert f \Vert _{\Lambda_{d(1/p-1)}^{L}} \leq C \bigl\Vert D^{L}_{t}f \bigr\Vert _{T_{2}^{p,\infty}}. $$
The predual space of the classical Hardy space has been studied in [19] and [16].
Definition 2
Let \(\alpha>0\), we will say a function f of \(\Lambda_{\alpha}^{L}\) is in \(\lambda_{\alpha}^{L}\) if it satisfies \(\gamma_{1}(f)=\gamma_{2}(f)=\gamma_{3}(f)=0\), where
The dual space of \(\lambda_{d(1/p-1)}^{L}\) is \(B_{L}^{p}(\mathbb{R}^{d})\), which is the completeness of \(H_{L}^{p}(\mathbb{R}^{d})\) (cf. [14]).
We can give a Carleson measure characterization of \(\lambda_{d(1/p-1)}^{L}\) as follows (see [14]).
Proposition 5
Let \(\frac{d}{d+1}< p\leq1\). Then, for any \(f\in L_{\mathrm{loc}}^{2}(\mathbb{R}^{d})\), we have:
-
(a)
If \(f \in\lambda_{d(1/p-1)}^{L}\), then \(D^{L}_{t}f\in T_{2}^{p,\infty}\); moreover, we have
$$ \bigl\Vert D^{L}_{t}f \bigr\Vert _{T_{2}^{p,\infty}} \leq C \Vert f \Vert _{\lambda_{d(1/p-1)}^{L}}. $$ -
(b)
Conversely, if \(f\in L^{1}((1+|x|)^{-(d+1)}\,dx)\) and \(D^{L}_{t}f\in T_{2}^{p,\infty}\), then \(f \in\lambda_{d(1/p-1)}^{L}\) and
$$ \Vert f \Vert _{\lambda_{d(1/p-1)}^{L}} \leq C \bigl\Vert D^{L}_{t}f \bigr\Vert _{T_{2}^{p,\infty}}. $$
Let \(A_{j}=\partial_{x_{j}}+x_{j}\) and \(A_{-j}=\partial_{x_{j}}-x_{j}\) for \(j=1,2,\ldots, d\). Then
Therefore, in the harmonic analysis associated with L, the operators \(A_{j}\) play the role of the classical partial derivatives \(\partial _{x_{j}}\) in the Euclidean harmonic analysis (see [2, 11, 18]). Now, it is natural to consider the derivatives \(A_{i}\) other than \(\partial_{x_{j}}\). In [13], the author defined the Lusin area integral operator by \(A_{j}\) and characterized the Hardy space \(H_{L}^{1}(\mathbb {R}^{d})\). As a continuous study of the function spaces associated with L, in this paper we will define the Carleson measure by \(A_{j}\) and characterize the dual spaces and predual spaces of \(H_{L}^{p}(\mathbb {R}^{d})\). Moreover, let \(Q_{t}^{L}f(x)=t|\tilde{\nabla} P_{t}^{L}f |(x)\), where \(\tilde {\nabla}=(\partial_{t},A_{-1},\ldots,A_{-d}, A_{1},\ldots,A_{d})\). Then the main results of this paper can be stated as follows.
Theorem 1
Let \(\frac{d}{d+1}< p\leq1\). Then, for every \(f\in L_{\mathrm{loc}}^{2}(\mathbb{R}^{d})\), we have:
-
(a)
If \(f \in\Lambda_{d(1/p-1)}^{L}\), then \(Q^{L}_{t}f\in T_{2}^{p,\infty}\); moreover, we have
$$ \bigl\Vert Q^{L}_{t}f \bigr\Vert _{T_{2}^{p,\infty}} \leq C \Vert f \Vert _{\Lambda_{d(1/p-1)}^{L}}. $$ -
(b)
Conversely, if \(f\in L^{1}((1+|x|)^{-(d+1)}\,dx)\) and \(Q^{L}_{t}f\in T_{2}^{p,\infty}\), then \(f \in\Lambda_{d(1/p-1)}^{L}\) and
$$ \Vert f \Vert _{\Lambda_{d(1/p-1)}^{L}} \leq C \bigl\Vert Q^{L}_{t}f \bigr\Vert _{T_{2}^{p,\infty}}. $$
Remark 2
In [8], the authors characterize the case \(p=0\), i.e., \(\mathit{BMO}_{L}\), by the heat semigroup with the classical derivatives. In [15], the authors characterize the space \(\mathit{BMO}_{L}\) by the Poisson semigroup with the classical derivatives. In this paper, we will use the new derivatives \(A_{j}\) of the Poisson semigroup to characterize the space \(\Lambda_{d(1/p-1)}^{L}\) for \(\frac{d}{d+1}< p\leq1\).
Theorem 2
Let \(\frac{d}{d+1}< p\leq1\). Then, for any \(f\in L_{\mathrm{loc}}^{2}(\mathbb{R}^{d})\), we have:
-
(a)
If \(f \in\lambda_{d(1/p-1)}^{L}\), then \(Q^{L}_{t}f\in T_{2, 0}^{p,\infty}\); moreover, we have
$$ \bigl\Vert Q^{L}_{t}f \bigr\Vert _{T_{2, 0}^{p,\infty}} \leq C \Vert f \Vert _{\lambda_{d(1/p-1)}^{L}}. $$ -
(b)
Conversely, if \(f\in L^{1}((1+|x|)^{-(d+1)}\,dx)\) and \(Q^{L}_{t}f\in T_{2, 0}^{p,\infty}\), then \(f \in\lambda_{d(1/p-1)}^{L}\) and
$$ \Vert f \Vert _{\lambda_{d(1/p-1)}^{L}} \leq C \bigl\Vert Q^{L}_{t}f \bigr\Vert _{T_{2, 0}^{p,\infty}}. $$
The paper is organized as follows. In Sect. 2, we give some estimates of the kernels. In Sect. 3, we give the proof of Theorem 1. The proofs of Theorem 2 will be given in Sect. 4.
Throughout the article, we will use A and C to denote the positive constants, which are independent of the main parameters and may be different at each occurrence. By \(B_{1} \sim B_{2}\), we mean that there exists a constant \(C>1\) such that \(\frac{1}{C} \leq \frac{B_{1}}{B_{2}}\leq C\).
2 Estimates of the kernels
In this section, we give some estimates of the kernels, which we will use in the sequel.
The proofs of these estimates can be found in [9].
Lemma 1
-
(a)
For every \(N\in\mathbb{N}\), there is a constant \(C_{N}>0\) such that
$$ 0\leq K_{t}^{L}(x,y)\leq C_{N}t^{-\frac{d}{2}}e^{-(5t)^{-1}|x-y|^{2}} \biggl(1+\frac{\sqrt{t}}{\rho(x)}+\frac{\sqrt{t}}{\rho(y)} \biggr)^{-N}. $$(2) -
(b)
There exists \(C>0\) such that, for every \(N>0\), there is a constant \(C_{N}>0\) so that, for all \(|h|\leq \sqrt{t}\),
$$ \bigl\vert K_{t}^{L}(x+h,y)-K_{t}^{L}(x,y) \bigr\vert \leq C_{N}\frac{|h|}{\sqrt{t}}t^{-\frac{d}{2}} e^{-At^{-1}|x-y|^{2}} \biggl(1+\frac{\sqrt{t}}{\rho(x)}+\frac{\sqrt {t}}{\rho(y)} \biggr)^{-N}. $$(3)
By subordination formula, we can give the following estimates about the Poisson kernel.
Lemma 2
-
(a)
For every N, there is a constant \(C_{N}>0\), \(A>0\) such that
$$ 0\leq P_{t}^{L}(x,y)\leq C_{N} \frac{t}{(t^{2}+A|x-y|^{2})^{(d+1)/2}} \biggl(1+\frac{t}{\rho(x)}+\frac{t}{\rho(y)} \biggr)^{-N}. $$(4) -
(b)
Let \(|h|<\frac{|x-y|}{2}\). Then, for any \(N>0\), there exist constants \(C>0\), \(C_{N}>0\) such that
$$ \bigl\vert P_{t}^{L}(x+h,y)-P_{t}^{L}(x,y) \bigr\vert \leq C_{N}\frac{|h|}{\sqrt{t}}\frac{t}{(t^{2}+A|x-y|^{2})^{(d+1)/2}} \biggl(1+ \frac{t}{\rho(x)}+\frac{t}{\rho(y)} \biggr)^{-N}. $$(5)
Duong et al. [6] proved the following estimates about the kernel \(D_{t}^{L}(x,y)\).
Lemma 3
There exist constants C such that, for every N, there is a constant \(C_{N}>0\), so that
Let \(t=\frac{1}{2}\ln\frac{1+s}{1-s}\), \(s\in(0,1)\). Then
The following estimations are very important for the proofs of the main result in this paper.
Lemma 4
There is \(C>0\) for \(N\in\mathbb {N}\) and \(|x-x'|\leq\frac{|x-y|}{2}\), any \(j=-1,\ldots,-d,1,\ldots,d\), we can find \(C_{N}>0\) such that
Proof
By
and \(t=\frac{1}{2}\ln\frac{1+s}{1-s}\sim s\), \(s\rightarrow0^{+}\), for \(s\in(0,\frac{1}{2}]\), we have
If \(x\cdot y\leq0\), then \(|x|\leq|x-y|\). So
If \(x\cdot y\geq0\), then \(|x|\leq|x+y|\). So
Therefore,
Since
we get \((\frac{1-s^{2}}{4\pi s} )^{d/2}\leq t^{-d}\) for \(s\in[\frac{1}{2}, 1)\).
When \(s\in[\frac{1}{2},1)\), we get \(t=\frac{1}{2}\ln\frac {1+s}{1-s}> s\). Therefore
Then
By (6), we get
and
Therefore, when \(s\in(0,\frac{1}{2}]\), we have
When \(s\in[\frac{1}{2},1)\), we have
Then
Similar to the proof of (10), for any \(N>0\), we can prove
and
Since \(\rho(x)=\frac{1}{1+|x|}\), we get \(\frac{\sqrt{t}}{\rho(x)}=\sqrt {t}(1+|x|)\). Then, for \(N>0\),
Since x and y are symmetric, we also have
Then (a) follows from (10)–(12).
(b) Note that
For \(J_{2}\), let
where \(\alpha(s,z,y)=s|z+y|^{2}+\frac{1}{s}|z-y|^{2}\).
Then
Therefore
Let \(\theta=\lambda x+(1-\lambda)x'\), \(0<\lambda<1\). Then
When \(|x-x'|\leq\frac{|x-y|}{2}\), we can get \(|\theta-y|\sim|x-y|\). Therefore, there exists \(A>0\) such that
For \(J_{1}\),
Let
Then
Therefore, similar to the proofs of (13) and (14), we can prove
and
Inequalities (13) and (15) show
Then, similar to the proof of (a), we have
(c) Noting that
The proof of part I can be found in Lemma 3.9 of [6]. For part II, since \(|x_{j}|\leq1+|x|=\frac{1}{\rho(x)}\) and Lemma 1, we get
Therefore, part (c) holds and this completes the proof of Proposition 4. □
Lemma 4 and the subordination formula give the following.
Lemma 5
There is \(C>0\) for \(N\in\mathbb {N}\) and \(|x-x'|\leq\frac{|x-y|}{2}\), we can find \(C_{N}>0\) such that
3 Carleson measure characterization of \(\Lambda_{\alpha}^{L}\)
Let \(s_{L}\) denote the Littlewood–Paley g-function associated with L, i.e.,
and \(A_{L}\) denote the Lusin area integral associated with L, i.e.,
Then we can prove the following.
Lemma 6
The operators \(s_{L}\) and \(A_{L}\) are isometries on \(L^{2}(\mathbb{R}^{d})\) up to constant factors. Exactly,
The proof of Lemma 6 is standard, we omit it.
Let \(F(x,t)=Q_{t}^{L}f(x)\) and \(G(x,t)=Q_{t}^{L}g(x)\). Then we have the following lemma.
Lemma 7
If \(g\in L^{1} ((1+|x|)^{-(d+1)}\,dx )\) and f is an \(H_{L}^{p, \infty}\)-atom, then
Lemma 8
There exists \(C>0\) such that, for any \(H_{L}^{p, \infty}\)-atom \(a(x)\), we have \(\|A_{L}a\|_{L^{p}}\leq C\).
The proofs of Lemmas 7 and 8 can be found in [8].
Now we can give the proof of Theorem 1.
Proof of Theorem 1
Let \(f \in \Lambda_{d(1/p-1)}^{L}\), then \(f\in L^{1} ((1+|x|)^{-(d+1)}\,dx )\). By Lemma 5(a), we know
is absolutely convergent. To prove the assertion (a), we need to prove that, for any ball \(B=B(x_{0},r)\),
Set \(B_{k}=B(x_{0},2^{k}r)\) and
By Lemma 6, we have
Note that
Therefore
For \(x \in B(x_{0},r)\), by Lemma 5(a) and (18),
In the last step of the above, we use the facts \(\frac{d}{d+1}< p\leq1\) to get \(d(1/p-1)-1<0\).
Thus we have
It remains to estimate the constant term. Assume first that \(r< \rho(x_{0})\). Taking \(k_{0}\) such that \(2^{k_{0}}r< \rho(x_{0}) \leq 2^{k_{0}+1}r\), we have
Note that \(\rho(x) \sim\rho(x_{0})>r\) for any \(x \in B(x_{0},r)\), by using Lemma 5(c), we get
In the last step of the above, we use the fact \(d(1/p-1)<1\). For \(r \geq\rho(x_{0})\), we have \(| f(B_{1}) | \leq C |B_{1}|^{1/p-1} \| f \|_{\Lambda_{d(1/p-1)}^{L}}\).
Note that \(\rho(x) \leq Cr\) for any \(x \in B(x_{0},r)\), again by Lemma 5(c), we get
Then (17) follows from (18)–(21). This proves part (a).
Let \(f\in L^{1} ((1+|x|)^{-(d+1)}\,dx )\) and \(Q_{t}^{L}f(x)\in T_{2}^{p,\infty}\). We want to prove that \(f\in \Lambda_{d(1/p-1)}^{L}\). By \(\Lambda_{d(1/p-1)}^{L}\) is the dual space of \(H_{L}^{p}(\mathbb {R}^{d})\), it is sufficient to prove that
defined on finite linear combinations of \(H_{L}^{p,\infty}\)-atoms satisfies the estimate
By Lemma 7, Lemma 8, and Proposition 3, we get
This gives the proof of part (b) and then Theorem 1 is proved. □
4 The predual space of Hardy space \(H_{L}^{p}(\mathbb{R}^{d})\)
In this section, we give a Carleson measure characterization of the space \(\lambda_{d(1/p-1)}^{L}(\mathbb{R}^{d})\).
Proof of Theorem 2
Let \(f\in\lambda_{d(1/p-1)}^{L}\), then \(f\in \Lambda_{d(1/p-1)}^{L}\). By Theorem 1, we know \(f\in L^{1} ((1+|x|)^{-(d+1)}\,dx )\). To prove \(Q_{t}^{L} f\in T_{2, 0}^{p,\infty}\), we first prove that there exists a constant \(C>0\) such that, for any ball \(B=B(x_{0}, r)\), we have
where
We first assume (22) holds, then we show that \(Q_{t}^{k} f\in T_{2, 0}^{p,\infty}\). In fact, as \(f\in\lambda_{d(1/p-1)}^{L}\), we have \(f\in \Lambda_{d(1/p-1)}^{L}\) and there exists a constant \(C>0\) such that
Then, for any \(k\in\mathbb{N}\), we have
By (22), we have
We can take \(k_{0}\) large enough such that \(2^{-k_{0}/2}\|f\|_{\Lambda_{d(1/p-1)}^{L}}^{2}\) is small. This proves that \(\|Q_{t}^{L} f\|_{T_{2}^{p,\infty}}<\infty\) and \(\eta_{1}(f)=\eta_{2}(f)=\eta_{3}(f)=0\) follows from (23). Therefore \(Q_{t}^{L} f\in T_{2,0}^{p,\infty}\).
Now we give the proof of (22). Set \(B_{k}=B(x_{0}, 2^{k}r)\) and
By Lemma 6, we have
By
and Lemma 5(a), for \(x \in B(x_{0},r)\),
Therefore
It remains to estimate the constant term. Assume first that \(r< \rho(x_{0})\). Taking \(k_{0}\) such that \(2^{k_{0}}r< \rho(x_{0}) \leq 2^{k_{0}+1}r\), we have
Note that \(\rho(x) \sim\rho(x_{0})>r\) for any \(x \in B(x_{0},r)\), by Lemma 5(c), we get
For \(r \geq\rho(x_{0})\), we have
Note that \(\rho(x) \leq Cr\) for any \(x \in B(x_{0},r)\), again by Lemma 5(c),
Then (22) follows from (24)–(27).
For the reverse, by Theorem 1, we get \(f\in \Lambda_{d(1/p-1)}^{L}\) from \(Q_{t}^{L}f\in T_{2,0}^{p,\infty}\). For any ball \(B=B(x_{0},r)\),
Let \(G(x)= (g(x)-g(B) )\chi_{B}\). Then, by Lemma 7, we obtain
By Hölder’s inequality and Lemma 6, we have
Now, we estimate \(E_{k}\). By Hölder’s inequality again, we have that
where
and
When \(r<\rho(x_{0})\), then \(\int_{B}g(x)-g(B)\,dx=0\). Therefore, by Lemma 5(b),
Therefore
It follows that
When \(r\geq\rho(x_{0})\), we have \(\rho(y)\leq C r\) for \(y\in B(x_{0}, r)\). Then, by Lemma 5(a),
Then we can get
where
Then we can get \(\gamma_{1}(f)=\gamma_{2}(f)=\gamma_{3}(f)=0\) as the proof of the first part of this theorem. Therefore \(f\in\lambda_{\alpha}^{L}\) and the proof of Theorem 2 is completed. □
5 Conclusions
This paper defines a new version of Carleson measure associated with Hermite operator, which is adapted to the operator L. Then, we characterize the dual spaces and predual spaces of the Hardy spaces \(H_{L}^{p}(\mathbb {R}^{d})\) associated with L. The main results of this paper are the central problems in harmonic analysis, which can be used in PED or geometry widely.
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The research of the 1st author has been fully supported by the National Natural Science Foundation (Grant No. 11471018 and No. 11671031) of China.
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Huang, J., Wang, Y. & Li, W. A new version of Carleson measure associated with Hermite operator. J Inequal Appl 2018, 177 (2018). https://doi.org/10.1186/s13660-018-1771-2
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DOI: https://doi.org/10.1186/s13660-018-1771-2