The Harnack inequality for second-order elliptic equations with divergence-free drifts
|
|
- Egbert Fitzgerald
- 6 years ago
- Views:
Transcription
1 The Harnack inequality for second-order elliptic equations with divergence-free drifts Mihaela Ignatova Igor Kukavica Lenya Ryzhik Monday 9 th July, 2012 Abstract We consider an elliptic equation with a divergence-free drift b. We prove that an inequality of Harnack type holds under the assumption b L n/2+δ L 2 where δ > 0. As an application we provide a one sided Liouville s theorem provided that b L n/2+δ R n L 2 R n. 1 Introduction In this paper, we consider elliptic equations of the form u + b u + au = in a domain Ω R n. Here ax is a given function and bx is a prescribed divergence free vector field, that is, div b = 0. The qualitative properties of solutions to elliptic and parabolic equations in divergence form with low regularity of the coefficients have been studied extensively, starting with the classical papers of De Giorgi [DG], Nash [N], and Moser [M]. We are mostly interested in the improved regularity for divergence free drifts b, which arise in fluid dynamics models c.f. [BKNR, CV1, FV, K, SSSZ, KNSS, Z]. As can be easily seen from a simple scaling argument, the natural Lebesgue spaces for the coefficients in the equation for the local regularity theory to hold are a L n/2, b L n, and, indeed, regularity properties of solutions in this case have been known since the work of Stampaccia [S]. It is well known that a strong divergence free flow may induce better regularity and decay of solutions of elliptic and parabolic problems by means of improved mixing see, for instance [CKRZ] and references therein. It is also known that a divergence free-drift of relatively low regularity can still lead to regular solutions [CV1, CV2]. The question we study in this paper is whether the divergence free condition on b allows to relax the regularity assumptions on b given by Stampaccia. Department of Mathematics, University of California, Riverside, Riverside, CA 92521, ignatova@math.ucr.edu Department of Mathematics, University of Southern California, Los Angeles, CA 90089, kukavica@usc.edu Department of Mathematics, Stanford University, Stanford CA 94305, ryzhik@math.stanford.edu 1
2 Let us recall some recent results in this direction. In a recent paper [NU], Nazarov and Ural tseva significantly relaxed the classical regularity assumptions for divergence-free b by establishing the Harnack inequality and the Liouville theorem for weak solutions to 1.1 if b belongs to a Morrey space Mq n/q 1 with n/2 < q n, which lies between L n and BMO 1. In [FV], Friedlander and Vicol proved the Hölder continuity of weak solutions to drift-diffusion equations with a drift in BMO 1. In [SSSZ], Seregin et al. established the Liouville theorem and the Harnack inequality for elliptic and parabolic equations with divergence free drifts b lying in the scale invariant space BMO 1. All these spaces share the same scaling properties as L n and are thus the natural candidates for good regularity theory. In the present paper, we establish the Harnack inequality and the one-sided Liouville theorem for Lipschitz generalized solutions to 1.1 when ax and bx lie in the space L q Ω with n/2 < q n, and b is divergence free. Our results also hold for weak solutions provided that the drift b satisfies certain additional assumptions c.f. equation 27 in [NU]. More precisely, we establish a Harnack-type inequality sup uy C inf uy, 1.2 y B R x y B R x for all R > 0 see Theorem 2.1, and use this estimate to establish the one-sided Liouville theorem when a = 0 in Theorem 2.3. The constant C in 1.2 depends on the L q -norms of a and b, where q > n/2, but not on the solution u. Note that the L n/2 -norm is not scale invariant: if we set b l x = 1/lbx/l then b l L n/2 = l n/2 b L n/2. Because of that, one can not expect the constant C to be independent of R, and, indeed, the constant given explicitly in Theorem 2.1 blows up as R 0. The paper is organized as follows. In Section 2, we state our main results, Theorems 2.1 and 2.3. The proof is based on two auxiliary results, Lemmas 2.4 and 2.5. We first show see Lemma 2.4 that weak solutions of 1.1 are locally bounded by employing the classical Moser iteration technique. Then, in Lemma 2.5, we derive a weak Harnack inequality, the proof of which is inspired by the proof of Han and Lin [HL, Theorem 4.15] for elliptic equations without lower-order coefficients. Our main results, Theorems 2.1 and 2.3, are direct consequences of Lemma 2.4 and 2.5. Acknowledgment. I.K. was supported in part by the NSF grant DMS , L.R. was supported in part by the NSF grant DMS , and both M.I and L.R. were supported in part by NSF FRG grant DMS The main results Our first result is the Harnack inequality. Theorem 2.1. Harnack inequality Let u be a nonnegative Lipschitz solution to the elliptic equation 1.1. Assume that a L q Ω, b L q Ω for n/2 < q, q n and q 2, and that div b = 0 in the sense of distributions. Then for any B R Ω we have sup B R u C inf B R u
3 Here C is a constant depending on n, q, q, R, and M 1 = 1 + a L q + b 2 L 2 + b L q. Remark 2.2. From the proof we can deduce that C = Cn, q, q R 1 + R 1 a L q 1/1 n/2q + R 1 b L q 1/1 n/2 q CnR 1 M 1, 2.2 where M 1 is as in the statement of Theorem 2.1. Theorem 2.1 has the following consequence when Ω = R n. Theorem 2.3. One-sided Liouville s theorem Let ax 0 and bx as in Theorem 2.1. Then any nonnegative Lipschitz solution u to the elliptic equation 1.1 in R n is equal to a constant. We note that [NU] provides a two-sided Liouville s theorem under the same assumptions, that is, the only solutions of 1.1 that are bounded both from above and from below are constants. However, the one-sided Liouville s theorem in [NU] requires b to belong to a Morrey space which is in the same scaling class as L n. Proof of Theorem 2.3. Without loss of generality, we may assume that u is a nonnegative Lipschitz solution to 1.1 with inf R n u = 0. Then for every ɛ > 0, we have inf BR u ɛ for any sufficiently large ball B R. By Theorem 2.1, sup BR u C inf BR u Cɛ for all sufficiently large R > 0. Observe that the constant C given explicitly by 2.2 depends on R but remains bounded as R. Therefore, the assertion is established. Theorem 2.1 is an immediate consequence of the following two lemmas that compare sup BθR u and inf BθR u to u L p R with some small p > 0 and 0 < θ < τ < 1. Lemma 2.4. Assume that u is a nonnegative Lipschitz subsolution to the equation u + b u + au = with a L q Ω, b L q Ω for n/2 < q, q n and div b 0 in the sense of distributions. Then for any B R Ω, p > 0, and 0 < θ < τ < 1 sup u C R n/p + R 1/2 n/q a 1/2 n/q n/p L B q Ω + R 1/2 n/ q b 1/2 n/ q n/p L q Ω u L p R, θr where C = Cn, p, q, θ, τ is a positive constant. Lemma 2.5. Assume that u is a nonnegative Lipschitz supersolution to 1.1 satisfying the assumptions of Theorem 2.1. Then for any B R Ω and 0 < θ < τ < 1 there exists a small positive number p 0 = p 0 n, q, q, θ, τ, R, M 1 such that 1/p0 inf u C 2.5 B θr R u p 0 where C = Cn, q, q, θ, τ, R, M 1 is a positive constant and M 1 = 1 + a L q + b 2 L 2 + b L q. The rest of the paper contains the proofs of Lemmas 2.4 and 2.5. Both lemmas are proved using the Moser iteration, with the general strategy based on the proof of the Harnack inequality in [HL]
4 3 The proof of Lemma 2.4 Let u be a nonnegative Lipschitz subsolution of 2.3 in Ω, that is, j u j ϕ + b j j uϕ + auϕ Ω Ω for any Lipschitz function ϕ 0 in Ω such that ϕ = 0 in Ω c. For simplicity of presentation, we assume a = 0. The proof consists of a priori estimates which can be made rigorous as in [G, HL]. First, we obtain an a priori bound on the L p 1 -norm of u on a smaller ball B r1, in terms of an L p 2 -norm of u on a larger ball B R2 with r 1 < r 2 but p 1 > p 2. Then an iterative procedure is used to bring the gap between r 1 and r 2 to zero and simultaneously send p 1 to infinity. Let β 0 and ηx be a Lipschitz cut-off in the ball R such that 0 ηx 1. We use β/2 + 1u β+1 η 2γ as a test function in 3.1 to obtain β β β j u j u β+1 η 2γ u β+1 j u j η 2γ b j u β+1 j uη 2γ 0. Let w = u β/2+1 so that j w = β/2 + 1u β/2 j u. By 3.2, we get β + 1 j w 2 η 2γ 2γ w j wη 2γ 1 j η β/2 + 1 For the first term in the right side we have 2γ w j wη 2γ 1 j η = γ Ω 3.2 b j w j wη 2γ. 3.3 w 2 η 2γ 1 η + 2γ 1η 2γ 2 j η 2, 3.4 while for the second b j w j wη 2γ = 1 2 j b j w 2 η 2γ + γ b j w 2 η 2γ 1 j η γ b j w 2 η 2γ 1 j η, 3.5 as div b 0. Next, set γ 0 = n/ q. Then, as q > n/2, we have γ 0 0, 2 and, in addition 1 q + γ γ 0 2 = for n 3. Note that if n = 2 then γ 0 can be also chosen so that 3.6 is satisfied. Assume also that γ is sufficiently large so that γγ 0 2γ 1. Then, by Hölder s inequality we have, using 3.6 b j w 2 η 2γ 1 j η b j wη γ γ 0 w 2 γ 0 j η b L q wη γ γ 0 L 2 w η 1/2 γ 0 2 γ 0 L 2, 3.7 as 0 η 1. By Young s and the Gagliardo-Nirenberg inequalities, this leads to b j w 2 η 2γ 1 j η 1 2 wηγ 2 L 2 + C b 1/1 n/2 q L q w η 1/2 n/ q 2 L
5 By 3.3, 3.4, and 3.8, we obtain u β/2+1 η γ 2 C u β+2 η 2γ 1 η C u β+2 η 2γ 2 η 2 + C b 1/1 n/2 q u β/2+1 η 1/2 n/ q 2 L q L. 2 By Sobolev embedding used in the left side of 3.9, we get 1/2 u β/2+1 η γ L 2χ C u β+2 η η 2γ 1 + C u β+2 η 2γ 2 η 2 1/ C b 1/2 n/ q L q u β/2+1 η 1/2 n/ q L 2 where χ = n/n 2 if n 3 and χ > 2 is arbitrary if n = 2. Now, let η C0 Ω be such that η 1 in B θr, η 0 in BτR c, η C/[Rτ θ] and η C/[R2 τ θ 2 ]. Then, we have u β/2+1 L 2χ B θr C 1/2 u β+2 + Rτ θ R C b 1/2 n/ q 1/2 n/ q Rτ θ L q R u β/2+1 L 2 R The main point of 3.11 is that, since χ > 1, we have a bound on a higher norm of u on a smaller ball in terms of the lower norm of u on a larger ball. We now apply the estimate 3.11 iteratively on pairs of balls B ri+1 B ri, and also let β i +. More precisely, we choose β i = 2χ i 1 and r i = θr + τ θr2 i for i = 0, 1, 2,..., so that r i r i+1 = τ θr2 i+1. We obtain u L 2χ i+1 B ri+1 C1/χi 2 i/χi Rτ θ 1/χi u L 2χ i B ri C2 i/2 n/ q Rτ θ 1/2 n/ q b 1/2 n/ q L q B ri 1/χ i u L 2χ i B ri. By iteration, letting i +, we conclude that the estimate 2.4 holds for p 2. Now, let p 0, 2. We have just shown that sup u C Rτ θ n/2 + Rτ θ 1/2 n/ q b 1/2 n/ q n/2 B L q B ri u L 2 R 3.13 θr C Rτ θ n/2 + Rτ θ 1/2 n/ q b 1/2 n/ q n/2 L q B ri u 1 p/2 L R u p/2 L p R which implies sup u 1 B θr 2 u L R + C sup u C B θr Rτ θ n/p + Rτ θ 1/2 n/ q b 1/2 n/ q L q B ri A standard iteration argument c.f. [HL, Lemma 4.3] then implies Rτ θ n/p + Rτ θ 1/2 n/ q b 1/2 n/ q L q B ri and the proof of Lemma 2.4 is complete. n/p u L p R. n/p u L p R
6 4 Proof of Lemma 2.5 We assume without loss of generality that R = 1. The proof is similar in spirit to that of Lemma 2.4: we obtain an a priori bound and use it iteratively. Assume that u is a nonnegative Lipschitz supersolution to 1.1, and consider v = 1/u. The function v satisfies or equivalently v + b v av 0 in Ω 4.1 j v j ϕ + b j j vϕ avϕ for any function ϕ C0 Ω such that ϕ 0 in Ω. By Lemma 2.4, it follows that for any 0 < θ < τ < 1 and p > 0, we have with C = Cn, p, q, q, τ, θ, M 1. Therefore, we have inf u 1 1/p B θ C sup B θ v C v L p 4.3 u p We claim that there exists p 0 > 0 such that u p 0 u p u p 1/p. 4.4 u p 0 C 4.5 with a constant C = Cn, q, q, τ, M 1, which would finish the proof of Lemma 2.5. Reduction to an exponential bound In order to prove 4.5 for some sufficiently small p 0 > 0, denote log u Bτ = 1 log u, and set We shall show that there exists p 0 > 0 such that w = log u log u Bτ. 4.6 e p 0 w C 4.7 where C = Cτ, which in turn implies 4.5. Indeed, if we assume that 4.7 holds, then and e p 0log u log u Bτ C 4.8 e p 0log u log u Bτ C. 4.9 Therefore, we have e p 0log u Bτ e p 0 log u C and e p 0log u Bτ e p 0 log u C. Multiplying these two inequalities then leads to
7 An L 2 -bound for w We now prove 4.7. First, we establish bounds on the L 2 -norm of w. The function w satisfies w 2 w + b w + a in Fix τ 0, 1, and let η C0 1Ω with 0 η 1 be a cutoff such that η 1 on +τ/2, η 0 on B1 c, and η C/1 τ. Multiplying 4.10 by η2 and integrating over, we obtain w 2 η 2 2 j wη j η + b j j wη 2 + aη η w L 2 η L 2 + b L 2 η w L 2 η L + a L q η 2 L q where 1/q + 1/q = 1. Absorbing the factors η w L 2 on the right using the term on the left, we get w 2 C τ M τ/2 where M 0 = 1 + a L q + b 2 L 2, and the constant C τ may depend on τ 0, 1. Also, since w = 0, and 1 + τ/2 τ, we have by the Poincaré inequality w 2 C +τ/2 w 2 C τ M 0. +τ/ Bounds on the higher norms of w Next, we need to estimate w β for all β 1. As in the proof of Lemma 2.4 the idea is to bound first the higher norms of w on smaller balls in terms of the lower norms of w on larger balls and then use the iteration process. We multiply 4.10 by w 2β η 2γ and integrate over in order to obtain w 2β w 2 η 2γ 2β w 2β 2 w w 2 η 2γ + 2γ w 2β j wη 2γ 1 j η γ 2β + 1 b j w 2β wη 2γ 1 j η + a w 2β η 2γ. Here we utilized div b = 0 and j w = w j w/ w. For the first term in the right side of 4.14 we use 2β w 2β w 2β + 8β 2β, 4.15 while for the second 2γ w 2β j wη 2γ 1 j η 1 w 2β w 2 η 2γ + Cγ 2 w 2β η 2γ 2 η
8 This leads to w 2β w 2 η 2γ C8β 2β w 2 η 2γ + Cγ 2 w 2β η 2γ 2 η Cγ b w 2β+1 η 2γ 1 η + C a w 2β η 2γ. β + 1 Let τ r R 1 + τ/2. We now choose a cutoff η C0 1 Ω with 0 η 1 such that η 1 on B r, η 0 on BR c, and η C/R r. By 4.11, for the first term in the right side of 4.17 we have 8β 2β w 2 η 2γ 8β 2β w 2 C τ 8β 2β M τ/2 On the other hand, for the left side of 4.17, we use w β+1 η γ 2 2γ 2 w 2β+2 η 2γ 2 η 2 + 2β w 2β w 2 η 2γ Hence, we obtain w β+1 η γ 2 Cγ 2 w B 2β+2 η 2γ 2 η 2 + Cβ β 2β M Cγ 2 β w 2β η 2γ 2 η 2 B 1 + Cγβ + 1 b w 2β+1 η 2γ 1 η + Cβ a w 2β η 2γ. For the third term in the right side we utilize β w 2β β + 12β+2 β w 2β β+1/β β + 1/β 8β 2β + w 2β which gives Cγ 2 β w 2β η 2γ 2 η 2 C8β 2β γ 2 η 2γ 2 η 2 + Cγ 2 w 2β+2 η 2γ 2 η 2 C8β2β γ 2 M 0 R r 2 + Cγ 2 w 2β+2 η 2γ 2 η 2, 4.22 as M 0 1. The last two terms in 4.20 are estimated as follows. First, we have a w 2β η 2γ = a w β+1 η γ 2β/β+1 η 2γ/β+1 a L q w β+1 η γ 2β/β+1 L B /β where 1/q + 1/q = 1. Now, we use the Gagliardo-Nirenberg inequality w β+1 η γ L 2βq /β+1 C w β+1 η γ 1 α L 2 w β+1 η γ α L
9 with α = n/2 n/2βq /β +1 if 2βq /β +1 2, and α = 0 otherwise. By Young s inequality, we obtain a w 2β η 2γ C a L q w β+1 η γ 21 αβ/β+1 L 2 w β+1 η γ 2αβ/β+1 L β+1/αβ 1 2β + 1 2αβ/β+1 w β+1 η γ 2αβ/β+1 L 2 + C 2β + 1 2αβ/β+1 a L q w β+1 η γ 21 αβ/β+1 β+1/β1 α+1 L. 2 As α 0, 1, this implies a w 2β η 2γ 1 2β w β+1 η γ 2 L + Cβ + 1 2α 1 a α 2 1 L w β+1 η γ α q L 2 Here we denoted α 1 = β + 1/β1 α + 1 and α 2 = 2β1 α/β1 α + 1. Observe that α 1 1 and α 1 is smaller than a constant independent of β, while 0 < α 2 < 2 with α 2 2 as β. For the last remaining term in 4.20, we have Cγβ + 1 b w 2β+1 η 2γ 1 η = Cγβ + 1 b w β+1 η γ 2β+1/β+1 η γ/β+1 1 η Let us choose γ = β + 1. Then, the above expression becomes Cγβ + 1 b w β+1 η γ 2β+1/β+1 η Cβ b L q w β+1 η γ 2β+1/β+1 η L 2β+1 q /β+1 L where 1/ q + 1/ q = 1. Once again we apply the Gagliardo-Nirenberg inequality 4.28 w β+1 η γ L 2β+1 q /β+1 C w β+1 η γ 1 ᾱ L 2 w β+1 η γ ᾱl with ᾱ = n/2 n/2β + 1 q /β + 1 if 2β + 1 q /β and ᾱ = 0 otherwise. Thus, by Young s inequality, we have Cγβ + 1 b w β+1 η γ 2β+1/β+1 η 4.30 Cβ b L q w β+1 η γ 1 ᾱ2β+1/β+1 L w β+1 η γ 2 L + Cβ + 12ᾱ 1 2 R b ᾱ1 w β+1 η γ L q ᾱ2. rᾱ1 L 2 w β+1 η γ ᾱ2β+1/β+1 η L 2 L Here we denoted ᾱ 1 = 2β +2/2β1 ᾱ+2 ᾱ and ᾱ 2 = 22β +11 ᾱ/2β1 ᾱ+2 ᾱ. Note that, as in 4.24, we have ᾱ 1 1 and ᾱ 1 is less than a constant independent of β, while 0 < ᾱ 2 < 2, and ᾱ 2 2 when β. 9
10 Putting together 4.20, 4.21, 4.24, and 4.30, we obtain w β+1 η γ 2 L 2 B r Cβ + 12 R r 2 w β+1 2 L 2 B R + Cβ β 2β M 0 R r Cβ + 1 2α 1+2 a α 1 L q B R w β+1 α 2 L 2 B R + Cβ + 12ᾱ 1 R rᾱ1 Using Sobolev embedding, we may rewrite 4.31 in the form w β+1 2 L 2χ B r b ᾱ1 L q B R w β+1 ᾱ2 L 2 B R. Cβ + 12κ w β+1 2 R rᾱ1+2 L 2 B R + 8β2β M a α 1 L q B R w β+1 α 2 L 2 B R + b ᾱ1 L q B R w β+1 ᾱ2 L 2 B R where κ = max{α 1 + 1, ᾱ 1 } and χ = n/n 2 if n 3 and χ > 2 if n = 2. Estimate 4.32 is analogous to 3.11: a higher norm of w on a smaller ball is bounded in terms of a lower norm of w on a larger ball. The iteration process Next, we consider the iteration process. Let β i = χ i 1 and r i = τ +1+τ/2 i+1 for i = 0, 1, 2,.... From 4.32, we get w χi 2 L 2χ B ri+1 Cχ2κi 2 ᾱ 1+2i+2 w χi 2 L 2 B ri + 8χi 2χi M a α 1 L q B ri w χi α 2 L 2 B ri + b ᾱ1 L q w χi ᾱ2 B ri L 2 B ri for all i = 0, 1, 2,.... Taking 1/2χ i power on both sides of 4.33 gives w L 2χ i+1 B ri+1 C1/2χi χ κi/χi 2 ᾱ 1+2i+2/2χ i w L 2χ i B ri + 8χi M 1/2χi a α 1/2χ i L q B ri w α 2/2 + i L 2χi B ri b ᾱ1/2χ L q B ri w ᾱ2/2. L 2χi B ri This leads to the inequality w L 2χ i+1 B ri+1 CM 1 eα/2χi 2χ κi/χi w L 2χ i B ri + 8χi + w α 2/2 + L 2χi B ri w ᾱ2/2 L 2χi B ri CM 1 eα/2χi 2χ κi/χi w L 2χ i B ri + 8χi, 4.35 for all i = 0, 1, 2,..., with α = max{α 1, ᾱ 1 } and M 1 = 1 + a L q + b 2 L + b L q. For 2 the second inequality in 4.35 we also used α 2, ᾱ 2 2, so that w α 2/2 L 1 + w 2 p L p and w ᾱ2/2 L 1 + w 2 p L p. Note that if a sequence Y i satisfies Y i+1 C i Y i + χ i with C i 1 and i=1 C i K, then by induction we have Y i C KY 0 + i χ i 1 CY 0 + χ i, 4.36 j=0 10
11 for all i = 0, 1, 2,.... Thus, iterating 4.35, we obtain w L 2χ i+1 B ri+1 Cn CM1 CM1 + χ i+1 CM Cn 1 χ i for all i = 0, 1, 2,..., as i j=1 j/χj C and i j=1 χj χ i+1 for χ > 1. Finally, for any β 1 there exists i = 0, 1, 2,... such that Thus, in particular, we have w β+1 2χ i β + 1 2χ i /β+1 Cn C w L2χi+1 B ri+1 CM 1 β Therefore, for all β 1, we obtain Bτ p 0 w β+1 β + 1! p β+1 0 CM Cn β e 2 β by taking p 0 = 1 CM Cn 1 e 4.41 sufficiently small. By 4.13, we also have w C w 2 CM which gives 4.40 for β = 0 as well. It follows from 4.40 that 4.7 holds, and therefore the proof of the lemma is complete. References [BKNR] [CV1] H. Berestycki, A. Kiselev, A. Novikov, and L. Ryzhik, The explosion problem in a flow, J. Anal. Math , L.A. Caffarelli and A.F. Vasseur, The De Giorgi method for regularity of solutions of elliptic equations and its applications to fluid dynamics, Discrete Contin. Dyn. Syst. Ser. S , no. 3, [CV2] L.A. Caffarelli and A.F. Vasseur, Drift diffusion equations with fractional diffusion and the quasi-geostrophic equation, Ann. of Math. 171, 2010, [CKRZ] P. Constantin, A. Kiselev, L. Ryzhik and A. Zlatos, Diffusion and mixing in a fluid flow, Ann. Math., 68, 2008,
12 [DG] [FV] [G] [HL] [K] [KNSS] [M] E. De Giorgi, Sulla differenziabilità e l analiticità delle estremali degli integrali multipli regolari, Mem. Accad. Sci. Torino. Cl. Sci. Fis. Mat. Nat , S. Friedlander and V. Vicol, Global well-posedness for an advection-diffusion equation arising in magneto-geostrophic dynamics, Ann. Inst. H. Poincaré Anal. Non Linéaire , no. 2, M. Giaquinta, Introduction to regularity theory for nonlinear elliptic systems, Lectures in Mathematics ETH Zürich, Birkhäuser Verlag, Basel, Q. Han and F. Lin, Elliptic partial differential equations, second ed., Courant Lecture Notes in Mathematics, vol. 1, Courant Institute of Mathematical Sciences, New York, I. Kukavica, On the dissipative scale for the Navier-Stokes equation, Indiana Univ. Math. J , no. 3, G. Koch, N. Nadirashvili, G.A. Seregin, and V. Šverák, Liouville theorems for the Navier-Stokes equations and applications, Acta Math , no. 1, J. Moser, A Harnack inequality for parabolic differential equations, Comm. Pure Appl. Math , [N] J. Nash, Continuity of solutions of parabolic and elliptic equations, Amer. J. Math , [NU] [S] [SSSZ] A.I. Nazarov and N.N. Ural tseva, The Harnack inequality and related properties of solutions of elliptic and parabolic equations with divergence-free lower-order coefficients, Algebra i Analiz , no. 1, G. Stampacchia, Le problème de Dirichlet pour les équations elliptiques du second ordre à coefficients discontinus, Ann. Inst. Fourier Grenoble , no. fasc. 1, G. Seregin, L. Silvestre, V. Šverák, and A. Zlatoš, On divergence-free drifts, J. Differential Equations , no. 1, [Z] Q.S. Zhang, A strong regularity result for parabolic equations, Comm. Math. Phys , no. 2,
c 2014 International Press u+b u+au=0 (1.1)
COMMUN. MATH. SCI. Vol. 2, No. 4, pp. 68 694 c 204 International Press THE HARNACK INEQUALITY FOR SECOND-ORDER ELLIPTIC EQUATIONS WITH DIVERGENCE-FREE DRIFTS MIHAELA IGNATOVA, IGOR KUKAVICA, AND LENYA
More informationarxiv: v1 [math.ap] 27 May 2010
A NOTE ON THE PROOF OF HÖLDER CONTINUITY TO WEAK SOLUTIONS OF ELLIPTIC EQUATIONS JUHANA SILJANDER arxiv:1005.5080v1 [math.ap] 27 May 2010 Abstract. By borrowing ideas from the parabolic theory, we use
More informationANNALES DE L I. H. P., SECTION C
ANNALES DE L I. H. P., SECTION C E. DI BENEDETTO NEIL S. TRUDINGER Harnack inequalities for quasi-minima of variational integrals Annales de l I. H. P., section C, tome 1, n o 4 (1984), p. 295-308
More informationOn the local existence for an active scalar equation in critical regularity setting
On the local existence for an active scalar equation in critical regularity setting Walter Rusin Department of Mathematics, Oklahoma State University, Stillwater, OK 7478 Fei Wang Department of Mathematics,
More informationOn the uniqueness of heat flow of harmonic maps and hydrodynamic flow of nematic liquid crystals
On the uniqueness of heat flow of harmonic maps and hydrodynamic flow of nematic liquid crystals Fanghua Lin Changyou Wang Dedicated to Professor Roger Temam on the occasion of his 7th birthday Abstract
More informationContinuity of Solutions of Linear, Degenerate Elliptic Equations
Continuity of Solutions of Linear, Degenerate Elliptic Equations Jani Onninen Xiao Zhong Abstract We consider the simplest form of a second order, linear, degenerate, divergence structure equation in the
More informationSufficient conditions on Liouville type theorems for the 3D steady Navier-Stokes equations
arxiv:1805.07v1 [math.ap] 6 May 018 Sufficient conditions on Liouville type theorems for the D steady Navier-Stokes euations G. Seregin, W. Wang May 8, 018 Abstract Our aim is to prove Liouville type theorems
More informationThe De Giorgi-Nash-Moser Estimates
The De Giorgi-Nash-Moser Estimates We are going to discuss the the equation Lu D i (a ij (x)d j u) = 0 in B 4 R n. (1) The a ij, with i, j {1,..., n}, are functions on the ball B 4. Here and in the following
More informationThe enigma of the equations of fluid motion: A survey of existence and regularity results
The enigma of the equations of fluid motion: A survey of existence and regularity results RTG summer school: Analysis, PDEs and Mathematical Physics The University of Texas at Austin Lecture 1 1 The review
More informationOn the ill-posedness of active scalar equations with odd singular kernels
April 26, 206 22:49 WSPC Proceedings - 9in x 6in Volum final page 209 209 On the ill-posedness of active scalar equations with odd singular kernels Igor Kukavica Vlad Vicol Fei Wang Department of Mathematics,
More informationREGULARITY AND COMPARISON PRINCIPLES FOR p-laplace EQUATIONS WITH VANISHING SOURCE TERM. Contents
REGULARITY AND COMPARISON PRINCIPLES FOR p-laplace EQUATIONS WITH VANISHING SOURCE TERM BERARDINO SCIUNZI Abstract. We prove some sharp estimates on the summability properties of the second derivatives
More informationHARNACK S INEQUALITY FOR GENERAL SOLUTIONS WITH NONSTANDARD GROWTH
Annales Academiæ Scientiarum Fennicæ Mathematica Volumen 37, 2012, 571 577 HARNACK S INEQUALITY FOR GENERAL SOLUTIONS WITH NONSTANDARD GROWTH Olli Toivanen University of Eastern Finland, Department of
More informationAn Introduction to Second Order Partial Differential Equations Downloaded from Bibliography
Bibliography [1] R.A. Adams, Sobolev Spaces, Academic Press, New York, 1965. [2] F. Black and M. Scholes, The pricing of options and corporate liabilities, Journal of Political Economy, 81 (3) 1973, 637-654.
More informationHölder estimates for solutions of integro differential equations like the fractional laplace
Hölder estimates for solutions of integro differential equations like the fractional laplace Luis Silvestre September 4, 2005 bstract We provide a purely analytical proof of Hölder continuity for harmonic
More informationESTIMATES FOR ELLIPTIC HOMOGENIZATION PROBLEMS IN NONSMOOTH DOMAINS. Zhongwei Shen
W,p ESTIMATES FOR ELLIPTIC HOMOGENIZATION PROBLEMS IN NONSMOOTH DOMAINS Zhongwei Shen Abstract. Let L = div`a` x, > be a family of second order elliptic operators with real, symmetric coefficients on a
More informationPartial regularity for suitable weak solutions to Navier-Stokes equations
Partial regularity for suitable weak solutions to Navier-Stokes equations Yanqing Wang Capital Normal University Joint work with: Quansen Jiu, Gang Wu Contents 1 What is the partial regularity? 2 Review
More informationRegularity of Weak Solution to Parabolic Fractional p-laplacian
Regularity of Weak Solution to Parabolic Fractional p-laplacian Lan Tang at BCAM Seminar July 18th, 2012 Table of contents 1 1. Introduction 1.1. Background 1.2. Some Classical Results for Local Case 2
More informationNote on the Chen-Lin Result with the Li-Zhang Method
J. Math. Sci. Univ. Tokyo 18 (2011), 429 439. Note on the Chen-Lin Result with the Li-Zhang Method By Samy Skander Bahoura Abstract. We give a new proof of the Chen-Lin result with the method of moving
More informationBoundedness, Harnack inequality and Hölder continuity for weak solutions
Boundedness, Harnack inequality and Hölder continuity for weak solutions Intoduction to PDE We describe results for weak solutions of elliptic equations with bounded coefficients in divergence-form. The
More informationApplying Moser s Iteration to the 3D Axially Symmetric Navier Stokes Equations (ASNSE)
Applying Moser s Iteration to the 3D Axially Symmetric Navier Stokes Equations (ASNSE) Advisor: Qi Zhang Department of Mathematics University of California, Riverside November 4, 2012 / Graduate Student
More informationON THE LOSS OF CONTINUITY FOR SUPER-CRITICAL DRIFT-DIFFUSION EQUATIONS
ON THE LOSS OF CONTINUITY FOR SUPER-CRITICAL DRIFT-DIFFUSION EQUATIONS LUIS SILVESTRE, VLAD VICOL, AND ANDREJ ZLATOŠ ABSTRACT. We show that there exist solutions of drift-diffusion equations in two dimensions
More informationSome lecture notes for Math 6050E: PDEs, Fall 2016
Some lecture notes for Math 65E: PDEs, Fall 216 Tianling Jin December 1, 216 1 Variational methods We discuss an example of the use of variational methods in obtaining existence of solutions. Theorem 1.1.
More informationOn Smoothness of Suitable Weak Solutions to the Navier-Stokes Equations
On Smoothness of Suitable Weak Solutions to the Navier-Stokes Equations G. Seregin, V. Šverák Dedicated to Vsevolod Alexeevich Solonnikov Abstract We prove two sufficient conditions for local regularity
More informationREGULARITY CRITERIA FOR WEAK SOLUTIONS TO 3D INCOMPRESSIBLE MHD EQUATIONS WITH HALL TERM
Electronic Journal of Differential Equations, Vol. 2018 (2018), No. 10, pp. 1 12. ISSN: 1072-6691. UL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu EGULAITY CITEIA FO WEAK SOLUTIONS TO D INCOMPESSIBLE
More informationMULTIPLE SOLUTIONS FOR CRITICAL ELLIPTIC PROBLEMS WITH FRACTIONAL LAPLACIAN
Electronic Journal of Differential Equations, Vol. 016 (016), No. 97, pp. 1 11. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu MULTIPLE SOLUTIONS
More informationON THE REGULARITY OF WEAK SOLUTIONS OF THE 3D NAVIER-STOKES EQUATIONS IN B 1
ON THE REGULARITY OF WEAK SOLUTIONS OF THE 3D NAVIER-STOKES EQUATIONS IN B 1, A. CHESKIDOV AND R. SHVYDKOY ABSTRACT. We show that if a Leray-Hopf solution u to the 3D Navier- Stokes equation belongs to
More informationDETERMINATION OF THE BLOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION
DETERMINATION OF THE LOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION y FRANK MERLE and HATEM ZAAG Abstract. In this paper, we find the optimal blow-up rate for the semilinear wave equation with a power nonlinearity.
More informationON THE REGULARITY OF SAMPLE PATHS OF SUB-ELLIPTIC DIFFUSIONS ON MANIFOLDS
Bendikov, A. and Saloff-Coste, L. Osaka J. Math. 4 (5), 677 7 ON THE REGULARITY OF SAMPLE PATHS OF SUB-ELLIPTIC DIFFUSIONS ON MANIFOLDS ALEXANDER BENDIKOV and LAURENT SALOFF-COSTE (Received March 4, 4)
More informationA regularity criterion for the 3D NSE in a local version of the space of functions of bounded mean oscillations
Ann. I. H. Poincaré AN 27 (2010) 773 778 www.elsevier.com/locate/anihpc A regularity criterion for the 3D NSE in a local version of the space of functions of bounded mean oscillations Zoran Grujić a,,
More informationA Product Property of Sobolev Spaces with Application to Elliptic Estimates
Rend. Sem. Mat. Univ. Padova Manoscritto in corso di stampa pervenuto il 23 luglio 2012 accettato l 1 ottobre 2012 A Product Property of Sobolev Spaces with Application to Elliptic Estimates by Henry C.
More informationDescription of my current research
Description of my current research Luis Silvestre September 7, 2010 My research concerns partial differential equations. I am mostly interested in regularity for elliptic and parabolic PDEs, with an emphasis
More informationOn the Boundary Partial Regularity for the incompressible Navier-Stokes Equations
On the for the incompressible Navier-Stokes Equations Jitao Liu Federal University Rio de Janeiro Joint work with Wendong Wang and Zhouping Xin Rio, Brazil, May 30 2014 Outline Introduction 1 Introduction
More informationLiquid crystal flows in two dimensions
Liquid crystal flows in two dimensions Fanghua Lin Junyu Lin Changyou Wang Abstract The paper is concerned with a simplified hydrodynamic equation, proposed by Ericksen and Leslie, modeling the flow of
More informationEXISTENCE AND REGULARITY RESULTS FOR SOME NONLINEAR PARABOLIC EQUATIONS
EXISTECE AD REGULARITY RESULTS FOR SOME OLIEAR PARABOLIC EUATIOS Lucio BOCCARDO 1 Andrea DALL AGLIO 2 Thierry GALLOUËT3 Luigi ORSIA 1 Abstract We prove summability results for the solutions of nonlinear
More informationON PARABOLIC HARNACK INEQUALITY
ON PARABOLIC HARNACK INEQUALITY JIAXIN HU Abstract. We show that the parabolic Harnack inequality is equivalent to the near-diagonal lower bound of the Dirichlet heat kernel on any ball in a metric measure-energy
More informationCRITERIA FOR THE 3D NAVIER-STOKES SYSTEM
LOCAL ENERGY BOUNDS AND ɛ-regularity CRITERIA FOR THE 3D NAVIER-STOKES SYSTEM CRISTI GUEVARA AND NGUYEN CONG PHUC Abstract. The system of three dimensional Navier-Stokes equations is considered. We obtain
More informationA RELATIONSHIP BETWEEN THE DIRICHLET AND REGULARITY PROBLEMS FOR ELLIPTIC EQUATIONS. Zhongwei Shen
A RELATIONSHIP BETWEEN THE DIRICHLET AND REGULARITY PROBLEMS FOR ELLIPTIC EQUATIONS Zhongwei Shen Abstract. Let L = diva be a real, symmetric second order elliptic operator with bounded measurable coefficients.
More informationhal , version 1-22 Nov 2009
Author manuscript, published in "Kinet. Relat. Models 1, 3 8) 355-368" PROPAGATION OF GEVREY REGULARITY FOR SOLUTIONS OF LANDAU EQUATIONS HUA CHEN, WEI-XI LI AND CHAO-JIANG XU Abstract. By using the energy-type
More informationPERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS
Annales Academiæ Scientiarum Fennicæ Mathematica Volumen 28, 2003, 207 222 PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS Fumi-Yuki Maeda and Takayori Ono Hiroshima Institute of Technology, Miyake,
More informationGlobal regularity of a modified Navier-Stokes equation
Global regularity of a modified Navier-Stokes equation Tobias Grafke, Rainer Grauer and Thomas C. Sideris Institut für Theoretische Physik I, Ruhr-Universität Bochum, Germany Department of Mathematics,
More informationBlow up of solutions for a 1D transport equation with nonlocal velocity and supercritical dissipation
Blow up of solutions for a 1D transport equation with nonlocal velocity and supercritical dissipation Dong Li a,1 a School of Mathematics, Institute for Advanced Study, Einstein Drive, Princeton, NJ 854,
More informationSome aspects of vanishing properties of solutions to nonlinear elliptic equations
RIMS Kôkyûroku, 2014, pp. 1 9 Some aspects of vanishing properties of solutions to nonlinear elliptic equations By Seppo Granlund and Niko Marola Abstract We discuss some aspects of vanishing properties
More informationWeights, inequalities and a local HÖlder norm for solutions to ( / t-l)(u)=divf on bounded domains
Weights, inequalities and a local HÖlder norm for solutions to ( / t-l)(u)=divf on bounded domains CAROLINE SWEEZY Department of Mathematical Sciences New Mexico State University Las Cruces, New Mexico
More informationnp n p n, where P (E) denotes the
Mathematical Research Letters 1, 263 268 (1994) AN ISOPERIMETRIC INEQUALITY AND THE GEOMETRIC SOBOLEV EMBEDDING FOR VECTOR FIELDS Luca Capogna, Donatella Danielli, and Nicola Garofalo 1. Introduction The
More informationREGULARITY AND EXISTENCE OF GLOBAL SOLUTIONS TO THE ERICKSEN-LESLIE SYSTEM IN R 2
REGULARITY AND EXISTENCE OF GLOBAL SOLUTIONS TO THE ERICKSEN-LESLIE SYSTEM IN R JINRUI HUANG, FANGHUA LIN, AND CHANGYOU WANG Abstract. In this paper, we first establish the regularity theorem for suitable
More informationJUHA KINNUNEN. Harmonic Analysis
JUHA KINNUNEN Harmonic Analysis Department of Mathematics and Systems Analysis, Aalto University 27 Contents Calderón-Zygmund decomposition. Dyadic subcubes of a cube.........................2 Dyadic cubes
More informationGlobal well-posedness for the critical 2D dissipative quasi-geostrophic equation
Invent. math. 167, 445 453 (7) DOI: 1.17/s-6--3 Global well-posedness for the critical D dissipative quasi-geostrophic equation A. Kiselev 1, F. Nazarov, A. Volberg 1 Department of Mathematics, University
More informationON SOME ELLIPTIC PROBLEMS IN UNBOUNDED DOMAINS
Chin. Ann. Math.??B(?), 200?, 1 20 DOI: 10.1007/s11401-007-0001-x ON SOME ELLIPTIC PROBLEMS IN UNBOUNDED DOMAINS Michel CHIPOT Abstract We present a method allowing to obtain existence of a solution for
More informationRegularity estimates for fully non linear elliptic equations which are asymptotically convex
Regularity estimates for fully non linear elliptic equations which are asymptotically convex Luis Silvestre and Eduardo V. Teixeira Abstract In this paper we deliver improved C 1,α regularity estimates
More informationOn partial regularity for the Navier-Stokes equations
On partial regularity for the Navier-Stokes equations Igor Kukavica July, 2008 Department of Mathematics University of Southern California Los Angeles, CA 90089 e-mail: kukavica@usc.edu Abstract We consider
More informationNonlinear Analysis. A regularity criterion for the 3D magneto-micropolar fluid equations in Triebel Lizorkin spaces
Nonlinear Analysis 74 (11) 5 Contents lists available at ScienceDirect Nonlinear Analysis journal homepage: www.elsevier.com/locate/na A regularity criterion for the 3D magneto-micropolar fluid equations
More informationThe 3D Euler and 2D surface quasi-geostrophic equations
The 3D Euler and 2D surface quasi-geostrophic equations organized by Peter Constantin, Diego Cordoba, and Jiahong Wu Workshop Summary This workshop focused on the fundamental problem of whether classical
More informationANISOTROPIC EQUATIONS: UNIQUENESS AND EXISTENCE RESULTS
ANISOTROPIC EQUATIONS: UNIQUENESS AND EXISTENCE RESULTS STANISLAV ANTONTSEV, MICHEL CHIPOT Abstract. We study uniqueness of weak solutions for elliptic equations of the following type ) xi (a i (x, u)
More informationON THE STRONG SOLUTIONS OF THE INHOMOGENEOUS INCOMPRESSIBLE NAVIER-STOKES EQUATIONS IN A THIN DOMAIN
ON THE STRONG SOLUTIONS OF THE INHOMOGENEOUS INCOMPRESSIBLE NAVIER-STOKES EQUATIONS IN A THIN DOMAIN XIAN LIAO Abstract. In this work we will show the global existence of the strong solutions of the inhomogeneous
More informationGlobal unbounded solutions of the Fujita equation in the intermediate range
Global unbounded solutions of the Fujita equation in the intermediate range Peter Poláčik School of Mathematics, University of Minnesota, Minneapolis, MN 55455, USA Eiji Yanagida Department of Mathematics,
More informationOn non negative solutions of some quasilinear elliptic inequalities
On non negative solutions of some quasilinear elliptic inequalities Lorenzo D Ambrosio and Enzo Mitidieri September 28 2006 Abstract Let f : R R be a continuous function. We prove that under some additional
More informationNon-radial solutions to a bi-harmonic equation with negative exponent
Non-radial solutions to a bi-harmonic equation with negative exponent Ali Hyder Department of Mathematics, University of British Columbia, Vancouver BC V6TZ2, Canada ali.hyder@math.ubc.ca Juncheng Wei
More informationA NOTE ON THE LADYŽENSKAJA-BABUŠKA-BREZZI CONDITION
A NOTE ON THE LADYŽENSKAJA-BABUŠKA-BREZZI CONDITION JOHNNY GUZMÁN, ABNER J. SALGADO, AND FRANCISCO-JAVIER SAYAS Abstract. The analysis of finite-element-like Galerkin discretization techniques for the
More informationSobolev Spaces. Chapter Hölder spaces
Chapter 2 Sobolev Spaces Sobolev spaces turn out often to be the proper setting in which to apply ideas of functional analysis to get information concerning partial differential equations. Here, we collect
More informationTRAVELING WAVES IN 2D REACTIVE BOUSSINESQ SYSTEMS WITH NO-SLIP BOUNDARY CONDITIONS
TRAVELING WAVES IN 2D REACTIVE BOUSSINESQ SYSTEMS WITH NO-SLIP BOUNDARY CONDITIONS PETER CONSTANTIN, MARTA LEWICKA AND LENYA RYZHIK Abstract. We consider systems of reactive Boussinesq equations in two
More informationNonlinear Diffusion and Free Boundaries
Nonlinear Diffusion and Free Boundaries Juan Luis Vázquez Departamento de Matemáticas Universidad Autónoma de Madrid Madrid, Spain V EN AMA USP-São Carlos, November 2011 Juan Luis Vázquez (Univ. Autónoma
More informationA generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem
A generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem Dave McCormick joint work with James Robinson and José Rodrigo Mathematics and Statistics Centre for Doctoral Training University
More informationAnisotropic partial regularity criteria for the Navier-Stokes equations
Anisotropic partial regularity criteria for the Navier-Stokes equations Walter Rusin Department of Mathematics Mathflows 205 Porquerolles September 7, 205 The question of regularity of the weak solutions
More informationREGULARITY OF GENERALIZED NAVEIR-STOKES EQUATIONS IN TERMS OF DIRECTION OF THE VELOCITY
Electronic Journal of Differential Equations, Vol. 00(00), No. 05, pp. 5. ISSN: 07-669. UR: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu REGUARITY OF GENERAIZED NAVEIR-STOKES
More informationDIRECTION OF VORTICITY AND A REFINED BLOW-UP CRITERION FOR THE NAVIER-STOKES EQUATIONS WITH FRACTIONAL LAPLACIAN
DIRECTION OF VORTICITY AND A REFINED BLOW-UP CRITERION FOR THE NAVIER-STOKES EQUATIONS WITH FRACTIONAL LAPLACIAN KENGO NAKAI Abstract. We give a refined blow-up criterion for solutions of the D Navier-
More informationDissipative quasi-geostrophic equations with L p data
Electronic Journal of Differential Equations, Vol. (), No. 56, pp. 3. ISSN: 7-669. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) Dissipative quasi-geostrophic
More informationarxiv: v2 [math.ap] 6 Sep 2007
ON THE REGULARITY OF WEAK SOLUTIONS OF THE 3D NAVIER-STOKES EQUATIONS IN B 1, arxiv:0708.3067v2 [math.ap] 6 Sep 2007 A. CHESKIDOV AND R. SHVYDKOY ABSTRACT. We show that if a Leray-Hopf solution u to the
More informationASYMPTOTIC BEHAVIOR OF SOLUTIONS FOR PARABOLIC OPERATORS OF LERAY-LIONS TYPE AND MEASURE DATA
ASYMPTOTIC BEHAVIOR OF SOLUTIONS FOR PARABOLIC OPERATORS OF LERAY-LIONS TYPE AND MEASURE DATA FRANCESCO PETITTA Abstract. Let R N a bounded open set, N 2, and let p > 1; we study the asymptotic behavior
More informationarxiv: v1 [math.ap] 16 May 2007
arxiv:0705.446v1 [math.ap] 16 May 007 Regularity criterion for 3D Navier-Stokes equations in terms of the direction of the velocity Alexis Vasseur October 3, 018 Abstract In this short note, we give a
More informationDecay in Time of Incompressible Flows
J. math. fluid mech. 5 (23) 231 244 1422-6928/3/3231-14 c 23 Birkhäuser Verlag, Basel DOI 1.17/s21-3-79-1 Journal of Mathematical Fluid Mechanics Decay in Time of Incompressible Flows Heinz-Otto Kreiss,
More informationBLOWUP THEORY FOR THE CRITICAL NONLINEAR SCHRÖDINGER EQUATIONS REVISITED
BLOWUP THEORY FOR THE CRITICAL NONLINEAR SCHRÖDINGER EQUATIONS REVISITED TAOUFIK HMIDI AND SAHBI KERAANI Abstract. In this note we prove a refined version of compactness lemma adapted to the blowup analysis
More information2 A Model, Harmonic Map, Problem
ELLIPTIC SYSTEMS JOHN E. HUTCHINSON Department of Mathematics School of Mathematical Sciences, A.N.U. 1 Introduction Elliptic equations model the behaviour of scalar quantities u, such as temperature or
More informationGRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS
LE MATEMATICHE Vol. LI (1996) Fasc. II, pp. 335347 GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS CARLO SBORDONE Dedicated to Professor Francesco Guglielmino on his 7th birthday W
More informationAn estimate on the parabolic fractal dimension of the singular set for solutions of the
Home Search ollections Journals About ontact us My IOPscience An estimate on the parabolic fractal dimension of the singular set for solutions of the Navier Stokes system This article has been downloaded
More informationINSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES. Note on the fast decay property of steady Navier-Stokes flows in the whole space
INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES Note on the fast decay property of stea Navier-Stokes flows in the whole space Tomoyuki Nakatsuka Preprint No. 15-017 PRAHA 017 Note on the fast
More informationarxiv: v2 [math.ap] 14 May 2016
THE MINKOWSKI DIMENSION OF INTERIOR SINGULAR POINTS IN THE INCOMPRESSIBLE NAVIER STOKES EQUATIONS YOUNGWOO KOH & MINSUK YANG arxiv:16.17v2 [math.ap] 14 May 216 ABSTRACT. We study the possible interior
More informationA comparison theorem for nonsmooth nonlinear operators
A comparison theorem for nonsmooth nonlinear operators Vladimir Kozlov and Alexander Nazarov arxiv:1901.08631v1 [math.ap] 24 Jan 2019 Abstract We prove a comparison theorem for super- and sub-solutions
More informationJournal of Differential Equations
J. Differential Equations 48 (1) 6 74 Contents lists available at ScienceDirect Journal of Differential Equations www.elsevier.com/locate/jde Two regularity criteria for the D MHD equations Chongsheng
More informationTakens embedding theorem for infinite-dimensional dynamical systems
Takens embedding theorem for infinite-dimensional dynamical systems James C. Robinson Mathematics Institute, University of Warwick, Coventry, CV4 7AL, U.K. E-mail: jcr@maths.warwick.ac.uk Abstract. Takens
More informationis a weak solution with the a ij,b i,c2 C 1 ( )
Thus @u @x i PDE 69 is a weak solution with the RHS @f @x i L. Thus u W 3, loc (). Iterating further, and using a generalized Sobolev imbedding gives that u is smooth. Theorem 3.33 (Local smoothness).
More informationLORENTZ ESTIMATES FOR ASYMPTOTICALLY REGULAR FULLY NONLINEAR ELLIPTIC EQUATIONS
Electronic Journal of Differential Equations, Vol. 27 27), No. 2, pp. 3. ISSN: 72-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu LORENTZ ESTIMATES FOR ASYMPTOTICALLY REGULAR FULLY NONLINEAR
More informationMIXED BOUNDARY-VALUE PROBLEMS FOR QUANTUM HYDRODYNAMIC MODELS WITH SEMICONDUCTORS IN THERMAL EQUILIBRIUM
Electronic Journal of Differential Equations, Vol. 2005(2005), No. 123, pp. 1 8. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) MIXED
More informationHARDY INEQUALITIES WITH BOUNDARY TERMS. x 2 dx u 2 dx. (1.2) u 2 = u 2 dx.
Electronic Journal of Differential Equations, Vol. 003(003), No. 3, pp. 1 8. ISSN: 107-6691. UL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) HADY INEQUALITIES
More informationHarmonic maps on domains with piecewise Lipschitz continuous metrics
Harmonic maps on domains with piecewise Lipschitz continuous metrics Haigang Li, Changyou Wang Abstract For a bounded domain Ω equipped with a piecewise Lipschitz continuous Riemannian metric g, we consider
More informationVISCOSITY SOLUTIONS. We follow Han and Lin, Elliptic Partial Differential Equations, 5.
VISCOSITY SOLUTIONS PETER HINTZ We follow Han and Lin, Elliptic Partial Differential Equations, 5. 1. Motivation Throughout, we will assume that Ω R n is a bounded and connected domain and that a ij C(Ω)
More informationhal , version 6-26 Dec 2012
ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS ABDEHAFID YOUNSI Abstract. In this paper, we give a new regularity criterion on the uniqueness results of weak solutions for the 3D Navier-Stokes equations
More informationIncompressible Navier-Stokes Equations in R 3
Incompressible Navier-Stokes Equations in R 3 Zhen Lei ( ) School of Mathematical Sciences Fudan University Incompressible Navier-Stokes Equations in R 3 p. 1/5 Contents Fundamental Work by Jean Leray
More informationALEKSANDROV-TYPE ESTIMATES FOR A PARABOLIC MONGE-AMPÈRE EQUATION
Electronic Journal of Differential Equations, Vol. 2005(2005), No. 11, pp. 1 8. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) ALEKSANDROV-TYPE
More informationPartial Differential Equations, 2nd Edition, L.C.Evans Chapter 5 Sobolev Spaces
Partial Differential Equations, nd Edition, L.C.Evans Chapter 5 Sobolev Spaces Shih-Hsin Chen, Yung-Hsiang Huang 7.8.3 Abstract In these exercises always denote an open set of with smooth boundary. As
More informationThe Maximum Principles and Symmetry results for Viscosity Solutions of Fully Nonlinear Equations
The Maximum Principles and Symmetry results for Viscosity Solutions of Fully Nonlinear Equations Guozhen Lu and Jiuyi Zhu Abstract. This paper is concerned about maximum principles and radial symmetry
More informationHeat kernels of some Schrödinger operators
Heat kernels of some Schrödinger operators Alexander Grigor yan Tsinghua University 28 September 2016 Consider an elliptic Schrödinger operator H = Δ + Φ, where Δ = n 2 i=1 is the Laplace operator in R
More informationREGULARITY RESULTS FOR THE EQUATION u 11 u 22 = Introduction
REGULARITY RESULTS FOR THE EQUATION u 11 u 22 = 1 CONNOR MOONEY AND OVIDIU SAVIN Abstract. We study the equation u 11 u 22 = 1 in R 2. Our results include an interior C 2 estimate, classical solvability
More informationA LOWER BOUND ON BLOWUP RATES FOR THE 3D INCOMPRESSIBLE EULER EQUATION AND A SINGLE EXPONENTIAL BEALE-KATO-MAJDA ESTIMATE. 1.
A LOWER BOUND ON BLOWUP RATES FOR THE 3D INCOMPRESSIBLE EULER EQUATION AND A SINGLE EXPONENTIAL BEALE-KATO-MAJDA ESTIMATE THOMAS CHEN AND NATAŠA PAVLOVIĆ Abstract. We prove a Beale-Kato-Majda criterion
More informationA HARNACK INEQUALITY FOR NONLINEAR EQUATIONS
A HARNACK INEQUALITY FOR NONLINEAR EQUATIONS BY JAMES SERRIN Communicated by Lawrence Markus, March 18, 1963 Recently Moser has obtained a Harnack inequality for linear divergence structure equations with
More informationA GENERAL CLASS OF FREE BOUNDARY PROBLEMS FOR FULLY NONLINEAR ELLIPTIC EQUATIONS
A GENERAL CLASS OF FREE BOUNDARY PROBLEMS FOR FULLY NONLINEAR ELLIPTIC EQUATIONS ALESSIO FIGALLI AND HENRIK SHAHGHOLIAN Abstract. In this paper we study the fully nonlinear free boundary problem { F (D
More informationHARNACK INEQUALITY FOR NONDIVERGENT ELLIPTIC OPERATORS ON RIEMANNIAN MANIFOLDS. Seick Kim
HARNACK INEQUALITY FOR NONDIVERGENT ELLIPTIC OPERATORS ON RIEMANNIAN MANIFOLDS Seick Kim We consider second-order linear elliptic operators of nondivergence type which are intrinsically defined on Riemannian
More informationarxiv: v1 [math.ap] 18 Jan 2019
Boundary Pointwise C 1,α C 2,α Regularity for Fully Nonlinear Elliptic Equations arxiv:1901.06060v1 [math.ap] 18 Jan 2019 Yuanyuan Lian a, Kai Zhang a, a Department of Applied Mathematics, Northwestern
More informationFachrichtung 6.1 Mathematik
Universität des Saarlandes U N I V E R S I T A S S A R A V I E N I S S Fachrichtung 6.1 Mathematik Preprint Nr. A note on splitting-type variational problems with subquadratic growth Dominic reit Saarbrücken
More informationANALYTIC SMOOTHING EFFECT FOR NONLI TitleSCHRÖDINGER EQUATION IN TWO SPACE DIMENSIONS. Citation Osaka Journal of Mathematics.
ANALYTIC SMOOTHING EFFECT FOR NONLI TitleSCHRÖDINGER EQUATION IN TWO SPACE DIMENSIONS Author(s) Hoshino, Gaku; Ozawa, Tohru Citation Osaka Journal of Mathematics. 51(3) Issue 014-07 Date Text Version publisher
More informationEverywhere differentiability of infinity harmonic functions
Everywhere differentiability of infinity harmonic functions Lawrence C. Evans and Charles K. Smart Department of Mathematics University of California, Berkeley Abstract We show that an infinity harmonic
More information