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Higher integrability for weak solutions to a degenerate parabolic system with singular coefficients
Boundary Value Problems volume 2019, Article number: 166 (2019)
Abstract
In this paper, we study the degenerate parabolic system
where \(X=\{X_{1},\ldots,X_{m} \}\) is a system of smooth real vector fields satisfying Hörmander’s condition and the coefficients \(a_{ij}^{\alpha \beta }\) are measurable functions and their skew-symmetric part can be unbounded. After proving the \(L^{2}\) estimates for the weak solutions, the higher integrability is proved by establishing a reverse Hölder inequality for weak solutions.
1 Introduction
Let \(\{X_{1},\dots,X_{q}\}\) be a system of smooth real vector fields in a neighborhood Ω̃ of some bounded domain \(\varOmega \subset \mathbb{R}^{n}\) \((n\geq q)\), satisfying Hörmander’s rank condition up to the order s and free up to the order s. The main purpose of this paper is to study higher integrability for weak solutions to nondiagonal quasilinear degenerate parabolic system
where \(i,j=1,2,\ldots,N\); \(\alpha,\beta =1,2,\ldots,q\); \(z=(x,t) \in Q_{T}=\varOmega \times (0,T)\); \(X_{\alpha }^{\ast }=-X_{\alpha }+c _{\alpha }\) \((c_{\alpha }=\sum_{k = 1}^{n} b_{\alpha k}(x)\frac{ \partial }{\partial x_{k}}\in C^{\infty })\) is the transposed vector field of \(X_{\alpha }\). The assumptions on functions \(g_{i}\), \(f_{i}^{\alpha }\) and the coefficients will be specified later.
A function \(u \in W_{2}^{1,1}(Q_{T}, \mathbb{R}^{N})\) is called a weak solution to (1.1) if
for all \(\psi \in C_{0}^{\infty }({Q_{T}},\mathbb{R}^{N})\).
In the Euclidean space, regularity to elliptic and parabolic equations and systems has been studied by many authors (see [1,2,3,4,5,6,7,8] and the references therein). Giaquinta in [5] proved the reverse Hölder estimates for weak solutions to diagonal elliptic systems with Hölder continuous coefficients and obtained the higher integrability of weak solutions. Giaquinta and Struwe in [2] treated partial regularity for weak solutions to diagonal quasilinear parabolic systems with the natural growth conditions and got Hölder continuity. Wiegner in [9] derived Hölder continuity of weak solutions to nondiagonal elliptic systems with VMO coefficients and natural growth conditions. Recently, Földes and Phan [10] got the higher integrability for gradients of weak solutions to a linear elliptic equation having the skew-symmetric part of coefficients unbounded.
Based on Hömander’s fundamental work [11], there has been tremendous work on degenerate PDEs arising from non-commuting vector fields; see, for example, [12,13,14,15,16,17,18,19,20,21]. Di Fazio and Fanciullo in [14] obtained gradient estimates for weak solutions to linear diagonal elliptic systems with bounded VMO coefficients. Dong and Niu [17] got the higher \(L^{p}\) estimates for the gradient of weak solutions to nondiagonal quasilinear degenerate elliptic systems. In [16, 18], Dong and her collaborators studied Morrey and Hölder regularity for weak solutions to diagonal and nondiagonal parabolic systems with bounded VMO coefficients.
However, as far as we know, there is no relevant research about quasilinear degenerate parabolic systems with skew-symmetric coefficients. In this paper, we try to generalize the results in [10] to quasilinear degenerate parabolic systems constructed by Hörmander’s vector fields. The aim of this paper is to get the higher integrability for weak solutions to (1.1). In order to state our results, we make the following hypotheses:
(H1) The coefficients \(a_{ij}^{\alpha \beta }(z) = A_{ij}^{\alpha \beta }(z) + B_{ij}^{\alpha \beta }(z)\), where \(A_{ij}^{\alpha \beta }\) are symmetric (\(A_{ij}^{\alpha \beta } = A_{ji}^{\alpha \beta }\)), bounded, and satisfy the uniform ellipticity condition that for some \(\varLambda >0\),
\(B_{ij}^{\alpha \beta }(z)\) are skew-symmetric (\(B_{ij}^{\alpha \beta } = - B_{ji}^{\alpha \beta }\)) and belong to BMO space (therefore they can be unbounded).
(H2) For any \((z,u,\xi )\in Q_{T} \times \mathbb{R}^{N}\times \mathbb{R}^{qN}\),
where \(1\leq \gamma _{0}<1/q_{0}\), \(q_{0}=\frac{Q+2}{Q + 4}\), L is a positive constant satisfying \(L<\varLambda \), and
Here Q is the homogeneous dimension relative to Ω, and in the sequel we set \(\tilde{g}=(g^{i})\), \(\tilde{\tilde{g}}=(g_{i}^{\alpha })\), \(\tilde{q}=2q_{0}\).
Now we state our main result.
Theorem 1.1
Suppose that (H1) and (H2) hold. Let \(u \in W_{2}^{1,1}( {Q_{T}},\mathbb{R}^{N})\) be a weak solutions to (1.1), then there exists a constant \(\varepsilon _{0}>\) such that for any \(p \in [2,2 +\tilde{q}{\varepsilon _{0}})\), we have \(Xu \in L_{ \mathrm{loc}}^{p} (Q_{T},\mathbb{R}^{N})\), and for every \(Q_{T}' \subset \subset Q_{T}\), there exists a constant \(C>0\) such that
The main difficulty in the proof is establishing the reverse Hölder inequality for gradients of weak solutions. We first establish the \(L^{2}\) estimates of weak solutions by constructing suitable test functions. Then the reverse Hölder inequality of gradients is obtained by the \(L^{2}\) estimates and the Gehring lemma on a metric measure space.
The paper is organized as follows. In Sect. 2, we introduce some concepts and results related to Hörmander’s vector fields that will be used in our proof. Section 3 is devoted to establishing the reverse Hölder inequality for gradients of weak solutions to (1.1) and giving the proof of Theorem 1.1.
2 Preliminaries
Let
be a family of vector fields in a neighborhood Ω̃ of some bounded domain \(\varOmega \subset \mathbb{R}^{n}\). For a multiindex \(\alpha =(i_{1},\ldots, i_{k})\), denote by \(X_{\beta }=[X_{i_{1}},[X _{i_{2}},\ldots,[X_{i_{k-1}},X_{i_{k}}]]\ldots ]\) the commutator of vector fields \(X_{1},\dots,X_{q}\) with length \(k=|\beta |\). We say that the vector fields \(X_{1},\ldots,X_{q}\) satisfy Hörmander’s condition up to the order s (see [11]) provided there exists \(s>0\) such that \(\{X_{\beta }\}_{|\beta |\leq s}\) span the tangent space at each point in \(\mathbb{R}^{n}\).
We denote by \(Xu=(X_{1} u,\dots,X_{q}u)\) the gradient of u with respect to the system \(X=\{X_{1},\ldots,X_{q}\}\) and hence
An absolutely continuous curve \(\gamma:[a,b]\to \tilde{\varOmega }\) is said to be admissible for the family X, if there exist functions \(c_{\alpha }(t)\), \(a\leq t\leq b\), satisfying
The Carnot–Carathéodory distance induced by X is defined by
Then \(d_{X}\) is a local metric on Ω̃. The metric ball is denoted by
If one does not need to consider the center of the ball, then we also write \(B_{R}\) instead of \(B(x,R)\).
It is well known that the doubling property for metric balls holds true (see [22, 23]): there exist positive constants \(R_{d}>0\) and \(C_{d}\geq 1\) such that for any \(x\in \varOmega \) and \(0<2R\le R_{d}\),
Here, \(|B(x,R)|\) denotes the Lebesgue measure of \(B(x,R)\). The number \(Q=\log _{2} C_{d} \) is called the homogeneous dimension relative to Ω. Clearly, \(Q\geq n\). From the doubling property, we can see that
where \(C=C_{d}^{-2}\). In particular, if the vector fields \(X_{1}, \dots,X_{q}\) are free up to the order s, there exist two positive constants \(C_{1}\) and \(C_{2}\) such that ([24])
For \({z_{0}}=(x_{0},t_{0})\in {Q_{T}}\subset \mathbb{R}^{n + 1}\), the parabolic cylinder with vertex at \(z_{0}\) is defined by
Let \(I_{R} (t_{0}) = ({t_{0}-\frac{R^{2}}{2}},{t_{0}+\frac{R ^{2}}{2}} ]\), and the parabolic boundary of \(Q_{R}({z_{0}})\) be denoted by
For any \((x,t),(y,s) \in {Q_{T}}\), the parabolic distance in \(Q_{T}\) is defined by
and the parabolic ball is defined by
To simplify the notations, in the sequel, \(Q_{R} (z_{0})\), \(B_{R} (x _{0})\), and \(I_{R} (t_{0})\) are written as \(Q_{R}\), \(B_{R}\), and \(I_{R}\), respectively. Furthermore, if E is a Lebesgue measurable set with Lebesgue measure \(|E|\), we set to be the integral average of u on E.
We define the parabolic Sobolev space by
with the norm
For any \(f\in L_{\mathrm{loc}}^{1}({Q_{T}})\), if
we say that \(f\in {\mathrm{BMO}}(Q_{T})\) (i.e., f has bounded mean oscillation).
Lemma 2.1
(Sobolev inequality, see [12, 23])
For every compact set \(K\subset \varOmega \), there exist constants \(C>0\) and \(\bar{R}>0\) such that for any metric ball \(B=B(x_{0},R)\) with \(x_{0}\in K\) and \(0< R\leq \bar{R}\), it holds that for any \(f\in C^{ \infty }(\overline{B_{R}})\),
where is the integral average of f on \(B_{R}\), and \(1\leq \kappa \leq Q/(Q-p)\), if \(1\leq p< Q\); \(1\leq \kappa <\infty \), if \(p\geq Q\). Moreover,
whenever \(f \in C_{0}^{\infty }(\overline{B_{R}})\).
Lemma 2.2
(Iterative lemma, see [25])
Let \(\varphi (t) \) be a bounded nonnegative function on \([{T_{0}},T _{1}]\), where \(T_{1} > {T_{0}} \ge 0\). Suppose that for any t and s, \(T_{0} \leq t < s \le {T_{1}}\), \(\varphi (t) \) satisfies
where \(\theta,A,B\), and α are nonnegative constants with \(\theta < 1\). Then for any \({T_{0}} \leq \rho < R \leq {T_{1}}\), one has
where c depends only on α and θ.
The following Gehring lemma on the metric measure space \((Y,d,\mu )\) (d is a metric and μ is a doubling measure) can be found in [13, 26].
Lemma 2.3
Let \(q\in [q_{0},2Q]\), where \(q_{0}>1\) is fixed. Assume that functions \(f,g\) are nonnegative and \(g\in L_{\mathrm{loc}}^{q}(Y,\mu )\), \(f\in L_{\mathrm{loc}}^{r_{0}}(Y,\mu )\), for some \(r_{0}>q\). If there exist constants \(b>1\) and θ such that for every ball \(B\subset \sigma B\subset Y\) the following inequality holds:
then there exist nonnegative constants \(\theta _{0}=\theta _{0}(q_{0},Q,C _{d},\sigma )\) and \(\varepsilon _{0}=\varepsilon _{0}(b,q_{0},Q,C_{d}, \sigma )\) such that if \(0<\theta <\theta _{0}\) then \(g\in L_{ \mathrm{loc}}^{p}(Y,\mu )\) for \(p\in [q,q+\varepsilon _{0})\) and moreover
for some positive constant \(C=C(q_{0},Q,C_{d},\sigma )\).
3 Higher integrability
We first introduce two cutoff functions \(\xi (x)\) and \(\eta (t)\) (see to [4]) such that for any \(0 < \rho < R, {B_{ \rho }} \subset {B_{R}} \subset \varOmega \),
Setting , we denote the average of \(u(x,t)\) on \({B_{R}}\) by
Lemma 3.1
Let \(u \in W_{2}^{1,1}({\varOmega _{T}},{\mathbb{R}^{N}}) \) be a weak solution to (1.1). Then for any \({Q_{R}} \subset \subset {\varOmega _{T}}\), we have
Proof
Multiplying both sides of (1.1) by the test function \(u-\bar{u}(t)\) and integrating on \({Q_{R}}\), we get
So we have
By (H1), the above can be written as
Due to the skew-symmetry of \(B_{ij}^{\alpha \beta }\),
By (H2), Hölder’s, Sobolev’s, and Young’s inequalities, we have
and
Inserting (3.4), (3.5), and (3.6) into (3.3), and by (H1), we get
where \(\theta = \varepsilon {R^{\frac{4}{Q}}}\sup_{I_{R}} { ( {\int _{{B_{R}}} {{{ \vert {Xu} \vert }^{2}}} \,dx} )^{ \frac{2}{Q}}} + c{R^{\frac{{Q + 2 - Q{\gamma _{0}}}}{2}}}\sup_{I_{R}} { ( {\int _{{B_{R}}} {{{ \vert {Xu} \vert }^{2}}} \,dx} ) ^{\frac{{{\gamma _{0}} - 1}}{2}}} + \varepsilon + L\). Because \(L < \varLambda \), by choosing \(\varepsilon,R\) small enough we can get that \(\theta < \varLambda \). So using Lemma 2.2, we complete the proof. □
Lemma 3.2
Let \(u \in W_{2}^{1,1}({\varOmega _{T}},{\mathbb{R}^{N}})\) be a weak solution of (1.1). Then for any \(0 < \rho < R\), \(Q_{R} \subset \subset \varOmega _{T}\), we have
Proof
Let \({B_{\rho }} \subset {B_{R}} \subset \varOmega \). Multiplying both sides of (1.1) by the test function \(( {u - \bar{u}(t)} )\times {\xi ^{2}}(x)\eta (t)\) and integrating on \({Q'_{R}} = {B_{R}}( {x_{0}}) \times ({t_{0}} - \frac{{{R^{2}}}}{2},s]\) (\(s \le {t_{0}} + \frac{ {{R^{2}}}}{2}\)), we get
By (H1), one has
and
By the above, (3.8) can be written as
Due to the skew-symmetry of \(B_{ij}^{\alpha \beta }\),
By (H1), (3.10) and Young’s inequality, we have
By Hölder’s and Sobolev’s inequalities, we have
Putting (3.12) into (3.11), we get
Using properties of \(\xi (x),\eta (t)\) and (3.5),
By (H2), Hölder’s and Young’s inequalities,
Inserting (3.13), (3.14), and (3.15) into (3.9), and by (H1), (3.3), (3.4), and Young’s inequality, we get
where \({\theta _{1}} = \varepsilon {R^{\frac{4}{Q}}}\sup_{I_{R}} { ( {\int _{{B_{R}}} {{{ \vert {Xu} \vert }^{2}}} \,dx} )^{ \frac{2}{Q}}} + c{R^{\frac{{Q + 2 - Q{\gamma _{0}}}}{2}}}\sup_{I_{R}} { ( {\int _{{B_{R}}} {{{ \vert {Xu} \vert }^{2}}} \,dx} ) ^{\frac{{{\gamma _{0}} - 1}}{2}}} + 4\varepsilon + L\). Employing properties of \(\xi (x),\eta (t)\), (H1), and since \(\frac{1}{R^{2}-\rho ^{2}}\leq \frac{C}{(R-\rho )^{2}}\), we have
Because \(L < \varLambda \), by choosing \(\varepsilon,R\) small enough we can get that \({\theta _{1}} < \varLambda \), so Lemma 2.2 yields
By (3.1),
Then
The proof is completed. □
Lemma 3.3
Let \(u \in W_{2}^{1,1}({\varOmega _{T}},{\mathbb{R}^{N}})\) be a weak solution of (1.1). Then there exists a positive constant \(\varepsilon _{0}\) such that for any \(p \in [ {2,2 + \tilde{q} {\varepsilon _{0}}} )\), we have \(u \in L_{\mathrm{loc}}^{\frac{ {p\gamma }}{2}}({Q_{T}}),Xu \in L_{\mathrm{loc}}^{p}({Q_{T}})\), and for any \({Q_{2R}} \subset \subset {Q_{T}}\),
Proof
By (3.7) and Sobolev’s inequality,
By Hölder’s and Sobolev’s inequalities, it follows
where \(\gamma =\frac{2(Q+2)}{Q}\). By (3.16) and (3.17),
By Young’s inequality,
Inserting the estimates of \(I_{1}\) and \(I_{2}\) into (3.18), we get
Let \(\hat{g} = { \vert {Xu} \vert ^{\tilde{q}}}\) (\(\hat{q} = \frac{2}{ {\tilde{q}}} = \frac{{Q + 4}}{{Q + 2}} > 1\)), \(\hat{f} = { ( {{{ \vert {\tilde{g}} \vert }^{\tilde{q}}} + {{ \vert {\tilde{\tilde{g}}} \vert }^{2}}} )^{\frac{{\tilde{q}}}{2}}}\), then the above can be written as
By Lemma 2.3, we know that there exists a positive constant \(\varepsilon _{0}\) such that for any \(\hat{p} \in [\hat{q},\hat{q} + {\varepsilon _{0}})\),
Letting \(p = \hat{p}\tilde{q} \in [ {2,2 + \tilde{q}{\varepsilon _{0}}} )\), we finish the proof. □
Proof of Theorem 1.1
By (3.1), Lemma 3.3, and Hölder’s inequality, we have
The proof is completed. □
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This work is supported by the National Natural Science Foundation of China (11701162); National Science Foundation of Shandong Province of China (ZR2019MA067); Research Fund for the Doctoral Program of Hubei University of Economics (XJ16BS28); Guangxi Natural Science Foundation (2017GXNSFBA198130).
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Dong, Y., Du, G. & Zhang, K. Higher integrability for weak solutions to a degenerate parabolic system with singular coefficients. Bound Value Probl 2019, 166 (2019). https://doi.org/10.1186/s13661-019-1285-y
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DOI: https://doi.org/10.1186/s13661-019-1285-y