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Boundary regularity for elliptic systems with supquadratic growth
Journal of Inequalities and Applications volume 2012, Article number: 220 (2012)
Abstract
We consider boundary regularity for weak solutions of quasilinear elliptic systems with the supquadratic growth condition and obtain a general criterion for a weak solution to be regular in the neighborhood of a given boundary point. By an element covering argument combined with existing interior partial regularity results, we establish the boundary regularity result.
1 Introduction
In this paper, we consider the partial regularity for weak solutions of elliptic systems
where Ω is a bounded domain in with a boundary of class , , u and take values in , . Each maps into R, and each maps into R. In theory partial regularity to (1.1) needs a priori existence of weak solutions. In order to define weak solutions to (1.1), one needs to impose certain structural and regularity conditions on and the inhomogeneity as follows. For ,
(H1) There exists such that
(H2) is uniformly strongly elliptic, that is, for some , we have
(H3) There exists a monotone nondecreasing concave function with , continuous at 0, such that for all , ,
(H4) The inhomogeneity satisfies the following growth condition:
for all , , and where for some .
(H5) There exists s with and a function such that
Note that we trivially have . Further, by the Sobolev embedding theorem, we have for any . If , we will take on Ω.
If the domain in this case is a half unit ball, then the boundary condition is as follows:
(H5)′ There exists s with and a function such that
Here we write , and further , . Similarly, we denote upper half balls as follows: for , we write for and set , . For , we further write for and set , .
Definition 1.1 By a weak solution of (1.1), we mean for all test-functions , a function satisfying
It is easily seen that by closure (1.2) holds for every φ in .
Under such assumptions on the structural conditions, full regularity of (1.1) at the boundary cannot, in general, be expected [1] even if the boundary data is smooth. Then our goal is to establish a partial boundary regularity for weak solutions of systems (1.1).
There are some previous partial regularity results for quasilinear systems. For example, Arkhipova has studied regularity up to the boundary for nonlinear and quasilinear systems [2–4]. For systems in a diagonal form, boundary regularity was first established by Wiegner [5], and the proof was generalized and extended by Hildebrandt-Widman [6]. In the case of minima of functionals of the form , Jost-Meier [7] established full regularity in a neighborhood of the boundary.
The result which is most closely related to that given here was shown by Grotowski [8]. Grotowski obtained boundary partial regularity results for more general systems: , . In this paper, we extend the results in [9]. However the results in the current paper do not follow from those in [8]; in the current situation, we need only to impose weaker structure conditions and, at the same time, we can obtain stronger conclusions.
The technique of A-harmonic approximation is a natural extension of the technique of harmonic approximation. This technique has its origins in Simon’s [10] proof of the regularity theorem of Allard [11]. The technique of A-harmonic approximation then refers to the direct analog of the above situation. The interior version of this technique has previously been applied by Duzaar and Grotowski in [12].
In this context, as the argument for combining the boundary and the interior estimates is relatively standard, we omit it and obtain the following results.
Theorem 1.1 Consider a bounded domain Ω in , with a boundary of class . Let u be a bounded weak solution of (1.1) satisfying the boundary condition (H5), where the structure conditions (H1)-(H3) hold for , and (H4) holds for . Consider a fixed . Then there exist positive and (depending only on n, N, λ, L, b, M, , and γ) with the property that
for some for a given implies .
Note in particular that the boundary condition (H5) means that makes sense; in fact, we have .
Combining this result with the analogous interior [13] and a standard covering argument allows us to obtain the following bound on the size of the singular set.
Corollary 1.1 Under the assumptions of Theorem 1.1, the singular set of the weak solution u has -dimensional Hausdorff measure zero in .
If the domain of the main step in proving Theorem 1.1 is a half ball, the result is then:
Theorem 1.2 Consider a bounded weak solution of (1.1) on the upper half unit ball which satisfies the boundary condition (H5)′, where the structure conditions (H1)-(H3) hold for , and (H4) holds for . Then there exist positive and (depending only on n, N, λ, L, b, M, , M, and γ) with the property that
for some for a given implies that holds.
Note that analogously to above, the boundary condition (H5)′ ensures that exists, and we have indeed .
2 The A-harmonic approximation technique
In this section, we present the A-harmonic approximation lemma [9] and some standard results due to Campanato [14, 15].
Lemma 2.1 Consider fixed positive λ and L, and with . Then for any given , there exists with the following property: for any satisfying
and
for any (for some , ) satisfying
and
and
for all , there exists an A-harmonic function
with
Next, we recall a slight modification of a characterization of Hölder continuous functions originally due to Campanato [14].
Lemma 2.2 Consider , and . Suppose that there are positive constants κ and α, with , such that for some , the following inequalities hold:
for all and ; and
for all and .
Then there exists a Hölder continuous representative of the -class of ν on , and for this representative ,
holds for all , for a constant depending only on n and α.
We close this section by a standard estimate for the solutions to homogeneous second-order elliptic systems with constant coefficients due originally to Campanato [15].
Lemma 2.3 Consider fixed positive λ and L, and with . Then there exists depending only on n, N, λ and L (without loss of generality, we take ) such that for satisfying (2.1) and (2.2), any A-harmonic function h on with satisfies
3 Caccioppoli inequality
In this section, we prove the Caccioppoli inequality. First of all, we recall two useful inequalities. The Sobolev embedding theorem yields the existence of a constant depending only on s, n and N such that
holds for , . Obviously, the inequality remains true if we replace by , which we will henceforth abbreviate simply as .
Now, we note that the Poincare inequality in this setting for , yields
for a constant which depends only on n.
Finally, we fix an exponent as follows: if , σ can be chosen arbitrarily (but henceforth fixed); otherwise, we take σ fixed in .
Then we prove an appropriate inequality for Caccioppoli.
Theorem 3.1 (Caccioppoli inequality)
Let u be a weak solution of systems (1.1) under (H1)-(H5). Then there exists , , depending only on L, M, s and , such that for all , with , there holds
where , depending only on λ and L, m and depending on these quantities and, in addition, on , and s.
Proof We consider a cut-off function satisfying , on and . Then the function is in , and thus can be taken as a test-function in (1.2). By (H2) and (H4), we have
Using (H5) and Young’s inequality, we have
Recalling the definition of and by (3.1) and (3.2), we have
Using (H2), we can get with ε positive but arbitrary (to be fixed later)
We can find a constant yields
Choosing ε small enough, we can get the desired result immediately. □
4 The proof of the main theorem
In this section, we proceed with the proof of the partial regularity result, and hence consider u to be a weak solution of (1.1). We consider and , , for , and with . First of all, we have
Lemma 4.1
here and hereafter, for , , we define
Proof Consider and , for , and with . Using (1.2), we have
Henceforth, we restrict ρ sufficiently small and keeping the definition of in mind,
where we define that for , ,
Applying (H3), Theorem 3.1 and Jensen’s inequality, we can calculate from (4.2)
Take (4.3) and (4.4) into (4.2), for arbitrary , we thus have
Multiplying through by , this yields
for defined by . □
Lemma 4.2 Consider u satisfying the conditions of Theorem 1.1 and σ fixed, then we can find δ and together with positive constants such that the smallness conditions
together imply the growth condition
Proof We now set , using in turn (H1), Young’s inequality and Hölder’s inequality. We have from (4.5)
for .
We now define by and set , for . From (4.5), we then have
and from (4.6), we observe from the definition of (recalling also the definition of γ)
Further, we note
For , we take to be the corresponding δ from A-harmonic approximation. Suppose that we could ensure that the smallness condition
holds. Then in view of (4.7), (4.8) and (4.9), we would be able to apply Lemma 2.1 to conclude the existence of a function which is -harmonic, with such that
For arbitrary (to be fixed later), we have from the Campanato theorem, noting (4.11) and recalling also that ,
Using (4.12) and (4.13) we observe
and hence, on multiplying this through by , we obtain the estimate
For the time being, we restrict to the case that g does not vanish identically. Recalling that , using in turn Poincare’s, Sobolev’s and then Hölder’s inequalities, noting also that , thus from (4.14), we can get
for , and provided and , we have
At the same time, from (4.15), we can see that for (), we have , where
Therefore, we can find such that .
Using Sobolev’s, Caccioppoli’s and Young’s inequalities with (4.15), we have
provided and where .
We then fix , note that this also fixed δ. Since , from the definition of I, we can get , and .
Combining these estimates with (4.16) and (4.17), we can get
Choosing sufficiently small that there holds , we can see from (4.18)
We now choose such that and define by . Suppose that we have
for some , where .
For any , we use the Sobolev inequality to calculate
and
And then we can calculate
Then we have
which means that the condition (4.20) is sufficient to guarantee the smallness condition (4.10) for , for all . We can thus conclude that (4.18) holds in this situation. From (4.18), we thus have
meaning that we can apply (4.18) on as well, yielding
and inductively,
The next step is to go from a discrete to a continuous version of the decay estimate. Given , we can find such that . We calculate in a similar manner to above. Firstly, we use the Sobolev inequality, to see
which allows us to deduce
and similarly, we can get
and
and hence, finally,
for . Combining this with (4.22) and (4.21), we have
and more particularly
for given by . Recalling that this estimate is valid for all and ρ with , assuming only the condition (4.20) on . This yields - after replacing R by 6R - the boundary estimate (2.7) requiring to apply Lemma 2.2.
The analogous interior estimate to (4.22) is standard, and we obtain the desired interior estimate (2.8) by a standard argument. Hence, we can apply Lemma 2.2 and conclude the desired Hölder continuity. □
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Acknowledgements
This work was supported by the National Natural Science Foundation of China (Nos: 11201415, 11271305); the Natural Science Foundation of Zhejiang Province (Y6110078); the Natural Science Foundation of Fujian Province (2012J01027) and Training Programme Foundation for Excellent Youth Researching Talents of Fujian’s Universities (JA12205).
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SC participated in design of the study and drafted the manuscript. ZT participated in conceived of the study and the amendment of the paper. All authors read and approved the final manuscript.
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Chen, S., Tan, Z. Boundary regularity for elliptic systems with supquadratic growth. J Inequal Appl 2012, 220 (2012). https://doi.org/10.1186/1029-242X-2012-220
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DOI: https://doi.org/10.1186/1029-242X-2012-220