ANALYSIS TOOLS WITH APPLICATIONS 493
27. Sobolev Inequalities 27.1. Morrey’s Inequality.
d 1 d Notation 27.1. Let S − be the sphere of radius one centered at zero inside R . d 1 d For a set Γ S − ,x R , and r (0, ), let ⊂ ∈ ∈ ∞ Γx,r x + sω : ω Γ such that 0 s r . ≡ { ∈ ≤ ≤ } So Γx,r = x + Γ0,r where Γ0,r is a cone based on Γ, seeFigure49below.
Γ
Γ
Figure 49. The cone Γ0,r.
d 1 Notation 27.2. If Γ S − is a measurable set let Γ = σ(Γ) be the surface “area” of Γ. ⊂ | |
Notation 27.3. If Ω Rd is a measurable set and f : Rd C is a measurable function let ⊂ → 1 fΩ := f(x)dx := f(x)dx. − m(Ω) Ω ZΩ Z By Theorem 8.35, r d 1 (27.1) f(y)dy = f(x + y)dy = dt t − f(x + tω) dσ(ω) Γx,r Γ0,r 0 Z Z Z ZΓ and letting f =1in this equation implies d (27.2) m(Γx,r)= Γ r /d. | | d 1 Lemma 27.4. Let Γ S − be a measurable set such that Γ > 0. For u 1 ⊂ | | ∈ C (Γx,r), 1 u(y) (27.3) u(y) u(x) dy |∇ d | 1 dy. − | − | ≤ Γ x y − ΓZx,r | |ΓZx,r | − | 494 BRUCE K. DRIVER†
d 1 Proof. Write y = x + sω with ω S − , then by the fundamental theorem of calculus, ∈ s u(x + sω) u(x)= u(x + tω) ωdt − ∇ · Z0 and therefore, s u(x + sω) u(x) dσ(ω) u(x + tω) dσ(ω)dt | − | ≤ 0 Γ |∇ | ZΓ Z Z s d 1 u(x + tω) = t − dt |∇ d | 1 dσ(ω) 0 Γ x + tω x − Z Z | − | u(y) u(y) = |∇ d | 1 dy |∇ d | 1 dy, y x − ≤ x y − ΓZx,s | − | ΓZx,r | − | wherein the second equality we have used Eq. (27.1). Multiplying this inequality d 1 by s − and integrating on s [0,r] gives ∈ d r u(y) m(Γx,r) u(y) u(y) u(x) dy |∇ d | 1 dy = |∇ d | 1 dy | − | ≤ d x y − Γ x y − ΓZx,r ΓZx,r | − | | | ΓZx,r | − | which proves Eq. (27.3).
Corollary 27.5. Suppose d
0,r (0, ) and S − 1 ≤∞ ∈ B | | ∈ ∞ u C (Γx,r). Then ∈ (27.4) u(x) C( Γ ,r,d,p) u 1,p | | ≤ | | k kW (Γx,r ) where 1/p 1 1/p 1 d− p 1 − 1 d/p C( Γ ,r,d,p):= max , − r − . | | Γ 1/p r p d · | | Ã µ − ¶ ! Proof. For y Γx,r, ∈ u(x) u(y) + u(y) u(x) | | ≤ | | | − | and hence using Eq. (27.3) and Hölder’s inequality, 1 u(y) u(x) u(y) dy + |∇ d | 1 dy | | ≤ − | | Γ x y − ΓZx,r | |ΓZx,r | − | 1 1 1 (27.5) u p 1 p + u p q L (Γx,r ) L (Γx,r ) L (Γx,r ) d 1 L (Γx,r ) ≤ m(Γx,r) k k k k Γ k∇ k k x k | | | − ·| − p where q = p 1 as before. Now − r 1 q d 1 d 1 q q = dt t − t − − dσ(ω) d 1 L (Γ0,r ) k − k 0 |·| Z ZΓ ¡ ¢ r p r d 1 d 1 1 p 1 − = Γ dt t − − − = Γ dt t− p 1 | | | | − Z0 Z0 and since ¡ ¢ d 1 p d 1 − = − − p 1 p 1 − − ANALYSIS TOOLS WITH APPLICATIONS 495 we find p 1 1/q − 1 p 1 p d p 1 p d p−1 1 p (27.6) q = − Γ r − = − Γ r − . k d 1 kL (Γ0,r) p d | | p d | | |·| − µ − ¶ µ − ¶ Combining Eqs. (27.5), Eq. (27.6) along with the identity,
1 1 1/q d 1/p (27.7) 1 q = m(Γ ) = Γ r /d − , L (Γx,r ) x,r m(Γx,r) k k m(Γx,r) | | shows ¡ ¢ 1 1/p d 1/p 1 p 1 − 1 d/p u(x) u p Γ r /d − + u Lp(Γ ) − Γ r − | | ≤ k kL (Γx,r ) | | Γ k∇ k x,r p d | | | | µ − ¶ ¡ ¢ 1/p 1 1/p 1 d− p 1 − 1 d/p = u p + u Lp(Γ ) − r − . Γ 1/p k kL (Γx,r ) r k∇ k x,r p d | | " µ − ¶ # 1/p 1 1/p 1 d− p 1 − 1 d/p max , − u 1,p r − . ≤ Γ 1/p r p d k kW (Γx,r ) · | | Ã µ − ¶ !
Corollary 27.6. For d N and p (d, ] there are constants α = αd and β = βd ∈ ∈ ∞ such that if u C1(Rd) then for all x, y Rd, ∈ ∈ p 1 −p 1/p p 1 (1 d ) (27.8) u(y) u(x) 2βα − u Lp(B(x,r) B(y,r)) x y − p | − | ≤ p d k∇ k ∩ ·| − | µ − ¶ where r := x y . | − | d 1 Proof. Let r := x y ,V := Bx(r) By(r) and Γ, Λ S − be chosen so that | − | ∩ ⊂ x + rΓ = ∂Bx(r) By(r) and y + rΛ = ∂By(r) Bx(r), i.e. ∩ ∩ 1 1 Γ = (∂Bx(r) By(r) x) and Λ = (∂By(r) Bx(r) y)= Γ. r ∩ − r ∩ − − Also let W = Γx,r Λy,r, see Figure 50 below. By a scaling, ∩ Γx,r Λy,r Γx,1 Λy,1 βd := | ∩ | = | ∩ | (0, 1) Γx,r Γx,1 ∈ | | | | is a constant only depending on d, i.e. we have Γx,r = Λy,r = β W . Integrating the inequality | | | | | | u(x) u(y) u(x) u(z) + u(z) u(y) | − | ≤ | − | | − | over z W gives ∈ u(x) u(y) u(x) u(z) dz + u(z) u(y) dz | − | ≤ − | − | − | − | ZW ZW β = u(x) u(z) dz + u(z) u(y) dz Γx,r | − | | − | | | WZ WZ β u(x) u(z) dz + u(z) u(y) dz . ≤ Γx,r | − | | − | | | ΓZ ΛZ x,r y,r 496 BRUCE K. DRIVER†
Λ Γ
Λ Λ Γ Γ
Figure 50. The geometry of two intersecting balls of radius r := x y . Here W = Γx,r Λy,r and V = B(x, r) B(y, r). | − | ∩ ∩
Hence by Lemma 27.4, Hölder’s inequality and translation and rotation invariance of Lebesgue measure,
β u(z) u(z) u(x) u(y) dz + dz |∇ d | 1 |∇ d |1 | − | ≤ Γ x z − z y − | | ΓZ | − | ΛZ | − | x,r y,r β 1 1 u p q + u p q ≤ Γ k∇ kL (Γx,r )k x d 1 kL (Γx,r ) k∇ kL (Λy,r)k y d 1 kL (Λy,r) | | µ | − ·| − | − ·| − ¶ (27.9) 2β 1 u p q ≤ Γ k∇ kL (V )k d 1 kL (Γ0,r ) | | |·| − p where q = p 1 is the conjugate exponent to p. Combining Eqs. (27.9) and (27.6) − 1 gives Eq. (27.8) with α := Γ − . | | Theorem 27.7 (Morrey’s Inequality). If d
1 d Proof. For p< and u Cc (R ), Corollaries 27.5 and 27.6 imply ∞ ∈ u(y) u(x) u d C u 1,p d and | − | C u p d BC(R ) W (R ) 1 d L (R ) k k ≤ k k x y − p ≤ k∇ k | − | ANALYSIS TOOLS WITH APPLICATIONS 497 which implies [u]1 d C u Lp(Rd) C u W 1,p(Rd)and hence − p ≤ k∇ k ≤ k k
(27.11) u 0,1 d C u W 1,p(Rd). k kC − p (Rd) ≤ k k
1,p d 1 d Now suppose u W (R ), choose (using Exercise 21.2) un Cc (R ) such that 1,p d∈ ∈ un u in W (R ). Then by Eq. (27.11), un um 0,1 d 0 as m, n → k − kC − p (Rd) → →∞ 0,1 d d 0,1 d d and therefore there exists u∗ C − p (R ) such that un u∗ in C − p (R ). ∈ → Clearly u∗ = u a.e. and Eq. (27.10) holds. 1, d If p = and u W ∞ R , then by Proposition 21.29 there is a version u∗ of u which∞ is Lipschitz∈ continuous. Now in both cases, p< and p = , the ¡ ¢ d ∞ ∞ sequence um := u ηm = u∗ ηm C∞ R and um u∗ uniformly on compact ∗ ∗ ∈ → subsets of d. Using Eq. (27.3) with u replaced by u along with a (by now) R ¡ ¢ m standard limiting argument shows that Eq. (27.3) still holds with u replaced by u∗. The proofs of Eqs. (27.4) and (27.8) only relied on Eq. (27.3) and hence go through without change. Similarly the argument in the first paragraph only relied on Eqs. (27.4) and (27.8) and hence Eq. (27.10) is also valid for p = . ∞ d Corollary 27.8 (Morrey’s Inequality). Suppose Ω o R such that Ω is compact C1-manifold with boundary and d
(27.12) u∗ 0,1 d C u W 1,p(Ω), k kC − p (Ω) ≤ k k where C = C(p, d, Ω).
Proof. Let U be a precompact open subset of Rd and E : W 1,p(Ω) W 1,p(Rd) be an extension operator as in Theorem 25.35. For u W 1,p (Ω) with→d
u∗ 0,1 d U ∗ 0,1 d C Eu W 1,p(Rd) C u W 1,p(Ω) . k kC − p (Ω) ≤ k kC − p (Rd) ≤ k k ≤ k k
d 1,d d 1,d d The following example shows that L∞(R ) W (R ), i.e. W (R ) contains unbounded elements. Therefore Theorem 27.76⊆ and Corollary 27.8 are not valid for p = d. It turns out that for p = d, W 1,d Rd embeds into BMO(Rd) —thespace of functions with “bounded mean oscillation.” ¡ ¢ 1 d Example 27.9. Let u(x)=ψ(x)loglog 1+ x where ψ Cc∞(R ) is chosen so | | ∈ d 1,d d that ψ(x)=1for x 1. Then u/L∞³(R ) while´ u W (R ). Let us check | | ≤ ∈ ∈ this claim. Using Theorem 8.35, one easily shows u Lp(Rd). A short computation shows, for x < 1, that ∈ | | 1 1 1 u(x)= ∇ 1 1+ 1 ∇ x log 1+ x x | | | | | | 1³ ´ 1 1 = xˆ 1+ 1 1 − x x log 1+ x µ | | ¶ | | | | ³ ´ 498 BRUCE K. DRIVER† where xˆ = x/ x and so again by Theorem 8.35, | | d d 1 1 u(x) dx 2 dx |∇ | ≥ x <1 x + x log 1+ 1 Zd Z| | | | | | x R | | d 1 ³ ´ d 1 2 d 1 σ(S − ) r − dr = . ≥ r log 1+ 1 ∞ Z0 Ã r ! 27.2. Rademacher’s Theorem. ¡ ¢ Theorem 27.10. Suppose that u W 1,p(Ω) for some d
lim u(y) u(x) pdy =0for x Ω E. r 0 − |∇ −∇ | ∈ \ ↓ B(Zx,r) Fix a point x Ω E and let v(y):=u(y) u(x) u(x) (y x) and notice that v(y)= u(y∈) \ u(x). Applying Eq. (27.13)− to−∇v then implies· − ∇ ∇ −∇ u(y) u(x) u(x) (y x) | − −∇ · − | (1 d ) C u( ) u(x) Lp(B(x,r) B(y,r)) r − p ≤ k∇ · −∇ k ∩ · 1/p p (1 d ) C u(y) u(x) dy r − p ≤ |∇ −∇ | · ÃZB(x,r) ! 1/p
d 1 1/p d/p p (1 d ) = Cσ S − r u(y) u(x) dy r − p − |∇ −∇ | · B(Zx,r) ¡ ¢ 1/p
d 1 1/p p = Cσ S − u(y) u(x) dy x y − |∇ −∇ | ·| − | B(Zx,r) ¡ ¢ which shows u is differentiable at x and u(x)=w- u(x). ∇ ∇ Theorem 27.11 (Rademacher’s Theorem). Let u be locally Lipschitz continuous d on Ω o R . Then u is differentiable almost everywhere and w-∂iu = ∂iu a.e. on Ω. ⊂
(w) d Proof. By Proposition 21.29 ∂i u exists weakly and is in ∂iu L∞(R ) for i =1, 2,...,d. The result now follows from Theorem 27.10. ∈ ANALYSIS TOOLS WITH APPLICATIONS 499
27.3. Gagliardo-Nirenberg-Sobolev Inequality. In this section our goal is to prove an inequality of the form: 1 d (27.14) u Lq C u Lp( d) for u Cc (R ). k k ≤ k∇ k R ∈ For λ>0, let uλ(x)=u(λx). Then
q q q dy uλ Lq = u(λx) dx = u(y) d k k d | | d | | λ ZR ZR d/q and hence uλ Lq = λ− u Lq . Moreover, uλ(x)=λ( u)(λx) and thus k k k k ∇ ∇ d/p uλ Lp = λ ( u)λ Lp = λλ− u Lp . k∇ k k ∇ k k∇ k 1 d If (27.14) is to hold for all u Cc (R ) then we must have ∈ d/q 1 d/p λ− u Lq = uλ Lq C uλ p d = Cλ − u Lp for all λ>0 k k k k ≤ k∇ kL (R ) k∇ k which is only possible if (27.15) 1 d/p + d/q =0, i.e. 1/p =1/d +1/q. − dp Notation 27.12. For p [1,d], let p∗ := d p with the convention that p∗ = if ∈ − ∞ p = d. That is p∗ = q where q solves Eq. (27.15). d Theorem 27.13. Let p =1so 1∗ = d 1 , then − 1 d d 1 d 2 (27.16) u 1∗ = u ∂iu(x) dx d− u 1 k k k k d 1 ≤ d | | ≤ k∇ k − i=1 R Y µZ ¶ for all u W 1,1(Rd). ∈ 1 d 1,1 d Proof. Since there exists un Cc (R ) such that un u in W (R ), asimple ∈ → 1 d limiting argument shows that it suffices to prove Eq. (27.16) for u Cc (R ). To help the reader understand the proof, let us give the proof for d 3 ∈first and with the 1/2 ≤ constant d− being replaced by 1. After that the general induction argument will be given. (The adventurous reader may skip directly to the paragraph containing Eq. (27.17.) (d =1,p∗ = ) By the fundamental theorem of calculus, ∞ x x u(x) = u0(y)dy u0(y) dy u0(x) dx. | | ≤ | | ≤ R | | ¯Z−∞ ¯ Z−∞ Z ¯ ¯ Therefore u L u¯0 1 , proving¯ the d =1case. k k ∞ ≤ k ¯kL ¯ (d =2,p∗ =2)Applyingthesameargumentasabovetoy1 u(y1,x2) and → y2 u(x1,y2),, → ∞ ∞ u(x1,x2) ∂1u(y1,x2) dy1 u(y1,x2) dy1 and | | ≤ | | ≤ |∇ | Z−∞ Z−∞ ∞ ∞ u(x1,x2) ∂2u(x1,y2) dy2 u(x1,y2) dy2 | | ≤ | | ≤ |∇ | Z−∞ Z−∞ and therefore
2 ∞ ∞ u(x1,x2) ∂1u(y1,x2) dy1 ∂2u(x1,y2) dy2. | | ≤ | | · | | Z−∞ Z−∞ 500 BRUCE K. DRIVER†
Integrating this equation relative to x1 and x2 gives
2 2 ∞ ∞ u L2 = u(x) dx ∂1u(x) dx ∂2u(x) dx k k R2 | | ≤ | | | | Z µZ−∞ ¶µZ−∞ ¶ 2 ∞ u(x) dx ≤ |∇ | µZ−∞ ¶ which proves the d =2case. 1 2 3 (d =3,p∗ =3/2) Let x =(y1,x2,x3),x =(x1,y2,x3), and x =(x1,x2,y3). Then as above, ∞ i u(x) ∂iu(x ) dyi for i =1, 2, 3 | | ≤ | | Z−∞ and hence 1 3 2 3 ∞ i u(x) 2 ∂iu(x ) dyi . | | ≤ | | i=1 Y µZ−∞ ¶ Integrating this equation on x1 gives, 1 1 2 3 2 3 ∞ 1 ∞ i u(x) 2 dx1 ∂1u(x ) dy1 ∂iu(x ) dyi dx1 R | | ≤ | | | | Z µZ−∞ ¶ Z i=2 µZ−∞ ¶ 1 Y 1 2 3 2 ∞ ∞ i ∂1u(x) dx1 ∂iu(x ) dx1dyi ≤ | | | | i=2 µZ−∞ ¶ Y µZ−∞ ¶ wherein the second equality we have used the Hölder’s inequality with p = q =2. Integrating this result on x2 and using Hölder’s inequality gives 1 1 1 2 2 2 3 ∞ 3 u(x) 2 dx1dx2 ∂2u(x) dx1dx2 dx2 ∂1u(x) dx1 ∂3u(x ) dx1dy3 R2 | | ≤ R2 | | R | | R2 | | Z µZ ¶ 1 Z µZ−∞ 1 ¶ µZ 1 ¶ 2 2 2 ∂2u(x) dx1dx2 ∂1u(x) dx1dx2 ∂3u(x) dx . ≤ 2 | | 2 | | 3 | | µZR ¶ µZR ¶ µZR ¶ One more integration of x3 and application of Hölder’s inequality, implies 1 3 3 2 2 3 u(x) 2 dx ∂iu(x) dx u(x) dx 3 | | ≤ 3 | | ≤ 3 |∇ | R i=1 R R Z Y µZ ¶ µZ ¶ proving the d =3case. d i For general d (p∗ = d 1 ), as above let x =(x1,...,xi 1,yi,xi+1 ...,xd). Then − − ∞ i u(x) ∂iu(x ) dyi | | ≤ | | µZ−∞ ¶ and 1 d d 1 d ∞ − d 1 i (27.17) u(x) − ∂iu(x ) dyi . | | ≤ | | i=1 Y µZ−∞ ¶ Integrating this equation relative to x1 and making use of Hölder’s inequality in the form d d
(27.18) fi fi d 1 ° ° ≤ k k − °i=2 °1 i=2 °Y ° Y ° ° ° ° ANALYSIS TOOLS WITH APPLICATIONS 501
(see Corollary 9.3) we find
1 1 d 1 d d 1 d − − d 1 i u(x) − dx1 ∂1u(x)dx1 dx1 ∂iu(x ) dyi | | ≤ | | ZR µZR ¶ ZR i=2 µZR ¶ 1 Y 1 d 1 d d 1 − i − ∂1u(x)dx1 ∂iu(x ) dx1dyi ≤ 2 | | µZR ¶ i=2 µZR ¶ 1 Y 1 1 d 1 d 1 d d 1 − − i − = ∂1u(x)dx1 ∂2u(x) dx1dx2 ∂iu(x ) dx1dyi . 2 | | 2 | | R R i=3 R µZ ¶ µZ ¶ Y µZ ¶ Integrating this equation on x2 and using Eq. (27.18) once again implies,
1 1 d 1 d 1 d − − d 1 u(x) − dx1dx2 ∂2u(x) dx1dx2 dx2 ∂1u(x)dx1 R2 | | ≤ R2 | | R R Z µZ ¶ Z 1 µZ ¶ d d 1 i − ∂iu(x ) dx1dyi × 2 | | i=3 µZR ¶ Y 1 1 d 1 d 1 − − ∂2u(x) dx1dx2 ∂1u(x) dx1dx2 ≤ R2 | | R2 | | µZ ¶ µZ 1 ¶ d d 1 i − ∂iu(x ) dx1dx2dyi . × 3 | | i=3 R Y µZ ¶ Continuing this way inductively, one shows
1 k d 1 d − d 1 u(x) − dx1dx2 ...dxk ∂iu(x) dx1dx2 ...dxk k | | ≤ k | | ZR i=1 µZR ¶ Y 1 d d 1 i − ∂iu(x ) dx1dx2 ...dxkdyk+1 × 3 | | i=k+1 R Y µZ ¶ andinparticularwhenk = d,
1 d d 1 d − d 1 (27.19) u(x) − dx ∂iu(x) dx1dx2 ...dxd d | | ≤ d | | ZR i=1 µZR ¶ Y 1 d d d 1 d 1 u(x) dx − = u(x) dx − . ≤ d |∇ | d |∇ | i=1 R R Y µZ ¶ µZ ¶ This estimate may now be improved on by using Young’s inequality (see Exercise d 1 d d 27.1) in the form ai d i=1 ai . Indeed by Eq. (27.19) and Young’s inequality, i=1 ≤
Q d P 1 d d 1 u d ∂iu(x) dx ∂iu(x) dx k k d 1 ≤ d | | ≤ d d | | − i=1 R i=1 R Y µZ ¶ X µZ ¶ 1 d 1 = ∂iu(x) dx √d u(x) dx d d | | ≤ d d |∇ | R i=1 R Z X Z 502 BRUCE K. DRIVER† wherein the last inequality we have used Hölder’s inequality for sums,
d d 1/2 d 1/2 2 ai 1 ai = √d a . | | ≤ | | | | i=1 Ãi=1 ! Ãi=1 ! X X X The next theorem generalizes Theorem 27.13 to an inequality of the form in Eq. (27.14). Theorem 27.14. If p [1,d) then, ∈ 1/2 p(d 1) 1,p d p (27.20) u Lp∗ d− − u L for all u W (R ). k k ≤ d p k∇ k ∈ − 1 d 1,p d Proof. As usual since Cc (R ) is dense in W R it suffices to prove Eq. 1 d 1 d s 1 d s (27.20) for u Cc (R ). For u Cc (R ) and s>1, u Cc (R ) and u = s 1 ∈ ∈ ¡| |¢ ∈ s ∇ | | s u − sgn(u) u. Applying Eq. (27.16) with u replaced by u andthenusing Holder’s| | inequality∇ gives | | s 1 s 1 s 1 u 1 d− 2 u = sd− 2 u − u 1 k| | k ∗ ≤ k∇ | | k1 k| | ∇ kL s s 1 (27.21) u Lp u − Lq ≤ √d k∇ k ·k| | k p where q = p 1 . We will now choose s so that s1∗ =(s 1)q, i.e. − − q 1 1 s = = 1 = q 1∗ 1 1∗ d 1 − q 1 d 1 1 p − − − − p (d 1) p (d ³1) ´d 1 = − = − = p∗ − . p (d 1) d (p 1) d p d − − − − For this choice of s, s1∗ = p∗ =(s 1)q and Eq. (27.21) becomes − 1/1∗ 1/q p∗ s p∗ (27.22) u dm u Lp u dm . d | | ≤ √d k∇ k · d | | ·ZR ¸ ·ZR ¸ Since 1 1 d 1 p 1 p(d 1) d(p 1) = − − = − − − 1∗ − q d − p dp d p 1 = − = , pd p∗ Eq. (27.22) implies Eq. (27.20).
Corollary 27.15. Suppose Ω Rd is bounded open set with C1-boundary, then ⊂ for all p [1,d) and 1 q p∗ there exists C = C(Ω,p,q) such that ∈ ≤ ≤ u q C u 1,p . k kL (Ω) ≤ k kW (Ω) Proof. Let U beaprecompactopensubsetofRd such that Ω¯ U and E : ⊂ W 1,p (Ω) W 1,p Rd be an extension operator as in Theorem 25.35. Then for → u C1(Ω) W 1,p(Ω), ∈ ∩ ¡ ¢ u p C Eu p d C (Eu) p d C u 1,p , k kL ∗ (Ω) ≤ k kL ∗ (R ) ≤ k∇ kL (R ) ≤ k kW (Ω) i.e.
(27.23) u p C u 1,p k kL ∗ (Ω) ≤ k kW (Ω) ANALYSIS TOOLS WITH APPLICATIONS 503
Since C1(Ω) is dense in W 1,p(Ω), Eq. (27.23) holds for all u W 1,p(Ω). Finally for ∈ all 1 q
Theorem 27.16. Let p [1, ] and u W 1,p Rd . Then ∈ ∞ ∈ 1,p 0,1 d (1) Morrey’s Inequality. If p>d,then W¡ ¢ C − p and → u∗ 0,1 d C u W 1,p(Rd). k kC − p (Rd) ≤ k k
(2) When p = d there is an L∞ — like space called BMO (which is not defined in these notes) such that W 1,p BMO. → (3) GNS Inequality. If 1 p