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and Z

|φ−un−1|2 = Z

Ω\S

|un−un−1|2+ Z

S

|ku0k−un−1|2

= Z

|un−un−1|2+ Z

S

ku0k2−u2n−2un−1(ku0k−un)

= Z

|un−un−1|2+ Z

S

(ku0k−un) (ku0k+un−2un−1)

<

Z

|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

|∇u|2+λf(|{u >0}|).

Then,Fnh(un)≤ Fnh(un−1) =J(un−1) implies J(un)≤

Z

|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−un2(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+ε12) 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−1,8ku0k2h−1,2λ

. Analogously, takingφ=η2(un−k) yields the above inequality forAR:=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

un−un−1

h φ+∇un· ∇φ

2 Z

|φ|2

h +|∇φ|2

. Dividing by 2εand takingε→0 yields

Z

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

2 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

|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

2ρ2

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

2ρ2

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.