and Z
Ω
|φ−un−1|2 = Z
Ω\S
|un−un−1|2+ Z
S
|ku0k∞−un−1|2
= Z
Ω
|un−un−1|2+ Z
S
ku0k2∞−u2n−2un−1(ku0k∞−un)
= Z
Ω
|un−un−1|2+ Z
S
(ku0k∞−un) (ku0k∞+un−2un−1)
<
Z
Ω
|un−un−1|2,
since in setS, we haveku0k∞−un<0 andku0k∞+un−2un−1 >2(ku0k∞−un−1)≥0 which follows from (7.10). Hence,Fnh(φ)<Fnh(un). A contradiction!
We end this section with some estimates regarding the minimizer, which we shall utilize in the succeeding arguments.
Lemma 7.3. If un minimizes Fnh(n= 1, . . . , M) for h, λ >0, then (i.) k∇unkL2(Ω)≤ k∇u0kL2(Ω),
(ii.) kun−un−1kL2(Ω)≤√
hk∇u0kL2(Ω), (iii.) f(|{un>0}|)≤λ−1k∇u0k2L2(Ω). Proof. Denote
J(u) :=
Z
Ω
|∇u|2+λf(|{u >0}|).
Then,Fnh(un)≤ Fnh(un−1) =J(un−1) implies J(un)≤
Z
Ω
|un−un−1|2
h +J(un)≤ J(un−1),
which implies that J(un)≤ J(un−1)≤ · · · ≤ J(u0). Since |{u0 >0}|=α, then Fnh(un)≤ Fnh(un−1) =J(un−1)≤ J(u0) =k∇u0k2L2(Ω),
which yields the desired results.
Proof. Consider an arbitrary ball BR such thatBR⊂Ω. Define function φ=η2(un−k)+,
where η ∈ C0∞(Ω; [0,1]) such that η ≡ 1 in a smaller concentric ball Br and |∇η| ≤ c/(R−r) for some constant c >1. Fix k ∈ R and denote A+R := BR∩ {un > k}. By Theorem 7.2, we can assume thatk≤ ku0k∞. Since f is 1-Lipschitz continuous, then
f(|{un−φ >0}|)−f(|{un>0}|) ≤ ||{un−φ >0}| − |{un>0}||
≤
{un−φ >0} ∩A+R +
{un>0} ∩A+R
≤ 2 A+R
. Then,Fnh(un)≤ Fnh(un−φ) implies that
0≤ −2 Z
A+R
un−un−1
h φ+
Z
A+R
φ2 h −2
Z
A+R
∇un· ∇φ+ Z
A+R
|∇φ|2+ 2λ|A+R|. (7.11) Since un is bounded byku0k∞ almost everywhere, then
− Z
A+R
(un−un−1)φ = Z
A+R
(un−1−un)η2(un−k)
≤ Z
A+R
|un−1−k−(un−k)|(un−k)
≤ Z
A+R
|un−1−k||un−k|+ Z
A+R
(un−k)2
≤ Z
A+R
(|un−1|+|k|) (|un|+|k|) + Z
A+R
(un−k)2
≤ 4ku0k2∞|A+R|+ R2 (R−r)2
Z
A+R
(un−k)2, and
Z
A+R
φ2 = Z
A+R
η4(un−k)2 ≤ R2 (R−r)2
Z
A+R
(un−k)2. Using Young’s inequality, we have for some ε1 ∈(0,1),
−2 Z
A+R
∇un· ∇φ = −2 Z
A+R
∇un·
η2∇un+ 2(un−k)η∇η
≤ (−2 +ε1) Z
A+R
η2|∇un|2+ 4 ε1
Z
A+R
(un−k)2|∇η|2. Again, by Young’s inequality, we have for some ε2 ∈(0,1−ε1),
Z
A+R
|∇φ|2 = Z
A+R
η4|∇un|2+ 4 Z
A+R
η3(un−k)∇un·∇η+ 4 Z
A+R
η2(un−k)2|∇η|2
≤ (1 +ε2) Z
A+R
η4|∇un|2+ 4 1 +ε1
2
Z
A+R
η2(un−k)2|∇η|2
≤ (1 +ε2) Z
A+R
η2|∇un|2+ 4 1 +ε1
2
Z
A+R
(un−k)2|∇η|2.
Thus, (7.11) becomes (1−ε1−ε2)
Z
A+r
|∇un|2 ≤ (−1+ε1+ε2) Z
A+R\A+r
η2|∇un|2+ 4 1+ε1
1+ε1
2
Z
A+R
(un−k)2|∇η|2 + 3R2
h(R−r)2 Z
A+R
(un−k)2+ 2 max
4ku0k2∞ h , λ
|A+R|.
≤ C
(R−r)2 Z
A+R
(un−k)2+ 2 max
4ku0k2∞ h , λ
|A+R|, whereC(h, R) := max
4c(1+ε1
1+ε1
2),3R2h−1
. Hence, Z
A+r
|∇un|2 ≤ ρ
"
1
(R−r)2max
A+R
(un−k)2+ 1
#
|A+R|,
where ρ(1−ε1 −ε2) = max
4c(1 + ε1
1 + ε1
2),3R2h−1,8ku0k2∞h−1,2λ
. Analogously, takingφ=η2(un−k)− yields the above inequality forA−R:=BR∩ {un< k}. Moreover, by Theorem 7.2,un is bounded with ess supun≤ ku0k∞. It follows that un belongs to Di Giorgi classB2(Ω,ku0k∞, ρ,∞,0).
Fix x0 ∈ Ω and consider an open ball BR := B(x0, R) ⊂ Ω for some R ≤1. For any x, y∈BR, denote r =|x−y|< R. By Theorem H.7 [62, Chapter 2, Theorem 6.1], we can find constantsγ <1 and C(γ, N, R)>0 such that
|un(x)−un(y)| ≤ sup
Br
un−inf
Br
un≤C|x−y|γ. Then,un is H¨older continuous near x0.
Next, we show that the minimizer is a subsolution to an elliptic partial differential equation on domain Ω. In fact, on the region where it is strictly positive, the minimizer is a solution and locally aC2 function.
Theorem 7.5. If un minimizesFnh(n= 1, ..., M) for h, λ >0, then (in the weak sense) (i.) ∆un≥ un−un−1
h in Ω,
(ii.) ∆un= un−un−1
h in the open set {un>0}.
Proof. For ε >0 and nonnegative functions φ∈C0∞(Ω), considerψ:=un−εφ. Hence, if ψ(x) > 0 for some x ∈ Ω, then clearly we have un(x) > εφ(x) > 0. Thus, we get f(|{ψ >0}|)≤f(|{un>0}|), which implies that
0 ≤ Fnh(ψ)− Fnh(un)
≤ −2ε Z
Ω
un−un−1
h φ+∇un· ∇φ
+ε2 Z
Ω
|φ|2
h +|∇φ|2
. Dividing by 2εand takingε→0 yields
Z
Ω
un−un−1
h φ+∇un· ∇φ≤0, (7.12)
thereby, proving (i).
To prove (ii), it suffices to show the reverse inequality of (7.12). Consider ψ:=un+εφ whereφ∈C0∞({un>0}) with
|ε|< m
maxφ where m:= min
suppφun>0.
It follows that the penalization ofψ is equal to that ofun, and so, we get 0 ≤ Fnh(ψ)− Fnh(un)
≤ 2ε Z
{un>0}
un−un−1
h φ+∇un· ∇φ
+ε2 Z
{un>0}
|φ|2
h +|∇φ|2
. Dividing by 2ε and takingε→0 gives the desired result.
Corollary 7.6. IfunminimizesFnh(n= 1, ..., M)forh, λ >0, thenun∈Cloc2 ({un>0}).
Proof. Fix x0 ∈ {un > 0}. Consider function φ ∈ C0∞({un > 0}) such that φ ≡ 1 in Br :=B(x0, r)⊂ {un >0} for some r >0. Let w= ψ∗g where where ψ denotes the fundamental solution of Laplace equation and functiong is defined by
g := un−un−1
h φ.
By Theorem 7.4 and [49, Lemma 4.2], we see thatw∈C2(Ω) and ∆w=gin Ω. Hence, by Theorem 7.5, we get
∆(un−w) = un−un−1
h (1−φ) = 0 inBr,
which implies that un−w is harmonic (hence,C∞) in Br. Thus, un isC2 nearx0. The following remark will be utilized in the succeeding arguments.
Remark. Fix a ball Br⊂Ω. Define functional In,Br(u) :=
Z
Br
|u−un−1|2
h +|∇u|2
dx.
Then, there exists a unique minimizer v ∈ A := {v ∈ H1(Br) : v = un on ∂Br} such that
In,Br(v) = min
A In,Br(·).
Moreover, in the weak sense,
∆v= v−un−1
h inBr, (7.13)
which follows from the proof of Theorem 7.5 by simply dropping the penalty arguments.
Existence. A similar argument as in the proof of Theorem 7.1 shows that we can find a minimizing sequence {uk} ⊂ A that is uniformly bounded in H1(Br) and whose
subsequence converges weakly inH1(Br) to somev∈H1(Br) and In,Br(v)≤lim inf
k→∞ In,Br(uk).
Note that there exists a trace operator T :H1(Br) → L2(∂Br). SinceT is a compact operator, then we can find a subsequence (still denoted by uk) such that
T(uk)→T(v) strongly inL2(∂Br).
Noting that T(uk) = un on ∂Br, we see v = un on ∂Br in the sense of trace, and so, v∈A.
Uniqueness. Suppose there exist minimizersu, v∈A, that is,In,Br(u) =In,Br(v) =m.
Considerw:= 12(u+v). By the parallelogram law, we have kw−un−1k2L2(Br) =
12(u−un−1) +12(v−un−1)
2 L2(Br)
= 12ku−un−1k2L2(Br)+ 12kv−un−1k2L2(Br)−
u−v 2
2
L2(Br)
k∇wk2L2(Br) = 12k∇uk2L2(Br)+12k∇vk2L2(Br)−
∇u− ∇v 2
2
L2(Br)
Hence,
m≤ In,Br(w) = 12In,Br(u) +12In,Br(v)−1 4
Z
Br
|u−v|2
h −1
4 Z
Br
|∇(u−v)|2
≤ m− 1
4hku−vk2L2(Br),
which implies that ku−vkL2(Br)= 0, and so, u=v almost everywhere inBr.
Using the above remark, we now show that asλ→ ∞, the set of positive values of the minimizer un preserves the prescribed measure. Later, we shall establish that for large enough λ > 0, this prescribed measure can be attained without having to take λ to infinity.
Theorem 7.7. If un minimizesFnh(n= 1, . . . , M), then we have
α≤ |{un>0}| ≤α+λ−1k∇u0k2L2(Ω). (7.14) Proof. Assume that |{un >0}|< α. We will deduce a contradiction by constructing a suitable perturbationv of the minimizerun.
Since un≥0, then settingE :={un= 0}, we have|E|>|Ω| −α >0. Takex∈∂E\∂Ω such that
|B(x, r)∩E|>0, (7.15) for all r >0. Fix r, sufficiently small such thatBr:=B(x, r)⊂Ω and
0<|Br| ≤α− |{un>0}|. (7.16)
Let v ∈ H1(Ω) be the unique minimizer of In,Br in Br and equal to un outside Br. Then, we must have In,Br(v)≤ In,Br(un), that is,
Z
Br
|v−un−1|2
h +|∇v|2 ≤ Z
Br
|un−un−1|2
h +|∇un|2. (7.17)
Note thatf(|{un>0}|) = 0. Also, by (7.16), we have
|{v >0}| = |{un>0}\Br|+|{v >0} ∩Br|
≤ |{un>0}|+|Br| ≤α, which implies that f(|{v >0}|) = 0.
On the other hand, (7.17) givesFnh(v)≤ Fnh(un). Sinceun minimizes Fnh, then we get Fnh(v) = Fnh(un). Equivalently, In,Br(v) = In,Br(un), which follows from the previous remark thatv =un. By (7.15), we see thatv is a nonconstant function. Note that
∆v−v
h =−un−1
h ≤0 inBr.
By [49, Theorem 3.5], v cannot achieve a nonpositive minimum in Br, that is, v >0 in Br. However, since |B(x, r)∩E|>0, then v6=un. A contradiction!
Lastly, the second inequality of (7.14) follows from the first inequality and Lemma 7.3, as follows:
|{un>0}| −α=f(|{un>0}| −α)≤λ−1k∇u0k2L2(Ω), which gives the desired result.
Following the arguments in [77], we show that the minimizerunis locally Lipschitz con-tinuous. To start, we establish the following lemma that guarantees Lipschitz continuity at the free boundary.
Lemma 7.8. (cf. [77, Lemma 4.1]) If un minimizes Fnh(n= 1, . . . , M) for h, λ > 0, then there exists constants r0 >0 and C(r0)>0 such that ifx∈Ω satisfies
r(x) :=dist(x,{un= 0})<min
dist(x, ∂Ω) 2 , r0
, (7.18)
thenun(x)≤Cr√
λ. Here, constant C does not depend onN and λ.
Proof. Letx∈Ω such that (7.18) holds. Assume thatun(x)>0, that is,r :=r(x)>0.
(The case when un(x) = 0 is trivial.) We claim that for some M >0, we haveun(x)≤ M r. Suppose not. Then for any M >0, there existsx0∈Ω satisfying (7.18) such that
un(x0)> M r. (7.19)
By Theorem 7.2, we see that for any n, Z
Ω
|un|p ≤ |Ω|ku0kp∞<∞, ∀p≥1, and so, sup
n≥1
kun−1kLp(Ω) <+∞.
It follows from [49, Theorem 8.17 and 8.18] that un(x0) ≤ C1 inf
B(x0,34r)
un(x) +k(r),
!
(7.20) whereC1 =C1(r, h, q)>0 with the property limr↓0C1(r, h, q)>0,q > N, and
k(r) =r2(1−N/q)sup
n≥1
un−1
h
Lq/2(Ω)=o(r) as r↓0. (7.21) Lety∈∂B(x0, r)∩ {un= 0} and consider a functionv∈H1(B(y, r)) such that
In,B(y,r)(v) = min
A In,B(y,r)(·),
where A :={v ∈ H1(B(y, r)) :v =un on∂B(y, r)}. By the previous remark, we have for any φ∈C0∞(B(y, r)),
Z
B(y,r)
v−un−1
h φ+∇v· ∇φ= 0. (7.22)
By Theorem 7.5, we have (in the weak sense)
∆(un−v) ≥ un−v
h , inB(y, r), and so, [49, Theorem 8.1] gives
sup
B(y,r)
(un−v)≤ sup
∂B(y,r)
(un−v) = 0.
This implies that
0≤un≤v inB(y, r). (7.23)
Now, extend functionv by un outside the ball, and define
vb:=
(
v, on B(y, r) un, on Ω\B(y, r).
By the minimality ofun and takingφ=v−un in (7.22), we get Z
B(y,r)
|v−un|2
h +|∇(v−un)|2 = Fn(un)− Fn(v) +λ(f(|{bv >0}|)−f(|{un>0}|)) + 2
Z
B(y,r)
(v−un−1)(v−un)
h +∇v· ∇(v−un)
≤ λ(f(|{bv >0}|)−f(|{un>0}|)) (7.24) By (7.23), we see that{un>0} ∩B(y, r)⊆ {v >0} ∩B(y, r). It follows from Theorem 7.7 that
|{bv >0}| = |{v >0} ∩B(y, r)|+|{un>0}\B(y, r)|
≥ |{un>0} ∩B(y, r)|+|{un>0}\B(y, r)|
= |{un>0}| ≥α.
Thus, (7.24) becomes Z
B(y,r)
|∇(v−un)|2 ≤ λ(|{v >b 0}| − |{un>0}|)
= λ|{bv >0} ∩ {un= 0} ∩B(y, r)|. (7.25) By (7.21), there exists small ε1 1 such that forr < ε1, we have
k(r)≤r inf
B(x0,34r)
un(x).
Also, by (7.23), we get inf
B(x0,34r)
un(x)≤ inf
B(x0,34r)∩B(y,r)
un(x)≤ inf
B(x0,34r)∩B(y,r)
v(x).
Hence, (7.19) and (7.20) implies
M r < un(x0)≤C1(1 +r) inf
B(x0,34r)∩B(y,r)
v(x), that is,
v(x) ≥ M r 2C1
, inB(x0,34r)∩B(y, r).
Invoking this inequality in [49, Theorem 8.18] yields the following for 1≤p < N/(N−2), inf
B(y,12r)
v(x) +k(r) ≥ C2(r, h)r−N/pkvkLp(B(y,r))
≥ C2r−N/pkvkLp(B(x0,34r)∩B(y,r))
≥ C2r−N/p|B(x0,34r)∩B(y, r)|1/pM r 2C1
=: 2C3M r.
where lim
r↓0 C3(C2, C1−1) >0. Again, by (7.21), we can find sufficiently small ε2 1 so that forr < ε2, we have
k(r)≤r inf
B(y,12r)
v(x)< inf
B(y,12r)
v(x), which implies that
inf
B(y,12r)
v(x)≥C3M r. (7.26)
Now, define a function
w(x) = C3M r
exp
−µρ2(x) r2
−exp(−µ)
, whereρ(x) = dist(x, y) and
µ ≥ N +
r
N2+r02
h. (7.27)
Here, we take r0 = min(ε1, ε2)1. Then, we have
∆w−w−un−1
h ≥ ∆w− w
h
= C3M rexp
−µρ2 r2
4µ2ρ2
r4 −2µN r2 − 1
h
+C3M r
h exp(−µ)
≥ 0 inB(y, r)\B(y,12r). (7.28)
(Indeed, ifx∈B(y, r)\B(y,12r), then 12r ≤ρ(x)≤r. Also from (7.27), we get (µ−N)2 ≥ N2+r02
h. Then, we have
4µ2ρ2
r4 −2µN r2 − 1
h ≥ µ2
r2 −2µN r2 −1
h = (µ−N)2 r2 −N2
r2 − 1 h
≥ r2
h r20−r2
≥0.)
Meanwhile, we note that for any x ∈ ∂B(y, r), we have v(x) = un(x) ≥ 0, and so, w(x) = 0≤v(x). Also, (7.26) implies that if ρ(x) = 12r, then
w(x) = C3M r
exp −14µ
−exp(−µ) ≤C3M r
≤ inf
B(y,12r)
v(x)
≤ v(x) inB(y,12r).
Hence, we have
w(x) ≤ v(x) on∂(B(y, r)\B(y,12r)).
Note that from (7.28), we get
∆w− w
h ≥ −un−1
h = ∆v− v
h inB(y, r)\B(y,12r).
Then, the maximum principle [49, Theorem 8.1] gives sup
B(y,r)\B(y,12r)
(w−v) ≤ sup
∂(B(y,r)\B(y,12r))
(w−v)≤0, that is,
w(x) ≤ v(x) inB(y, r)\B(y,12r).
There exists constant C4>0 such thatw(x)≥C4(r−ρ) in B(y, r)\B(y,12r). (Indeed, if x ∈ B(y, r)\B(y,12r), then 12r ≤ ρ(x) < r, that is, r−ρ ≤ 12r. Moreover, since the exponential function is nonincreasing, then for someδ >0,
w(x) ≥ 12δC3M r≥εC3M(r−ρ).
Take C4 :=δC3M >0.) Combining this with (7.26) implies that
v(x)≥C5M(r−ρ) inB(y, r), (7.29)
for some constantC5>0.
Take two disjoint balls B(yi,18r) ⊂B(y,12r) for i= 1,2. For ξ ∈ ∂B(y, r), let zi(ξ) be the point on the line segmentξyisuch that the length of segment`i(ξ) :=ξzi(ξ) becomes the largest with zi(ξ)∈/ B(yi, δr) and u(zi(ξ)) = 0. In caseu(x)6= 0 for all x∈ξyi, we set zi(ξ) = ξ. For x ∈ B(y, r)\yi, let ξi(x) ∈ ∂B(y, r) be a point such that x ∈ yiξi. Then by (7.29), we have for someC6 >0
v(x)≥C5M(r−ρ)≥ψi(x) :=C6M rdist(yi, ξi)−dist(yi, x) dist(yi, ξi) . Hence,
Z zi
ξ
d d`i
ψid`i =:ψi(zi) ≤ v(zi) :=
Z zi
ξ
d d`i
(v−un)d`i, that is,
Z zi
ξ
C5M r
dist(yi, ξ)d`i ≤ Z zi
ξ
|∇(v−un)|d`i.
Integrating with respect to ξ ∈ ∂B(y, r), summing up with respect to i, noting that r/dist(yi, ξ) =O(1) asr ↓0, squaring both sides, and finally, invoking Schwarz’ inequal-ity yields
C62M2|V| ≤ Z
V
|∇(v−un)|2, (7.30)
where
V :=V1∪V2, Vi = [
ξ∈∂B(y,r)
`i(ξ).
Combining this with (7.25) gives
C62M2|V| ≤λ|{v >0} ∩ {un= 0} ∩B(y, r)| ≤λ|{un= 0} ∩B(y, r)|, (7.31) thereby, contradicting the arbitrariness of M.
Finally, we note that {un= 0} ∩B(y, r)⊂V. By (7.31), we get
C62M2|{un= 0} ∩B(y, r)| ≤C6M|V| ≤λ|{un= 0} ∩B(y, r)|.
Hence, invoking the above claim givesun(x)≤rC6−1√
λfor anyx∈Ω satisfying (7.18).
Using the above lemma, we can show that the minimizer un is locally Lipschitz in Ω.
Theorem 7.9. If un minimizes Fnh(n= 1, . . . , M) for h, λ >0, then un∈Cloc0,1(Ω). In particular, the (local) Lipschitz coefficients of un do not depend on n.
Proof. A similar argument as in the proof of [77, Proposition 4.1] whereQmax=√ λ.