Archive for Rational Mechanics and Analysis

, Volume 234, Issue 3, pp 1413–1444

# A New Boundary Harnack Principle (Equations with Right Hand Side)

Open Access
Article

## Abstract

We introduce a new boundary Harnack principle in Lipschitz domains for equations with a right hand side. Our approach, which uses comparisons and blow-ups, will adapt to more general domains as well as other types of operators. We prove the principle for divergence form elliptic equations with lower order terms including zero order terms. The inclusion of a zero order term appears to be new even in the absence of a right hand side.

## 1 Introduction

### 1.1 Background

The well-known boundary Harnack principle states that two non-negative harmonic functions are comparable close to part of the boundary of a given domain, where they both vanish. More exactly, if u and v are harmonic functions in $$D \cap B_1$$ and vanish on $$\partial D \cap B_1$$, with D a Lipschitz domain, then
\begin{aligned} \frac{1}{C} v(x) \le u(x) \le C v(x) , \end{aligned}
where C depends on space dimension and $$u(x^0)/v(x^0)$$ for a fixed $$x^0$$ in the domain.1
We are interested in extending this result to the case of equations with right hand side. Of course such a general result is doomed to fail, unless some further restrictions are imposed. This can be seen through a simple 2-dimensional example with
\begin{aligned} u(x)=x_1x_2(x_1^2 - x_2^2) , \qquad v(x) = x_2(x_1 - x_2) \end{aligned}
in the cone $$\{ x_1>x_2 > 0 \}$$ with aperture $$\pi /4$$, and $$\Delta u = 0$$, $$\Delta v = -2$$. Consequently, there cannot exist $$C >0$$ such that $$Cu \ge v$$.2 Another simple (and discouraging) example is
\begin{aligned} u(x) = x_1^2, \qquad v(x) = x_1 \end{aligned}
in the set $$\{x_1 > 0\}$$. Again, there cannot exist a constant C such that close to the boundary $$Cu \ge v$$.
Two observations can be made from the above examples:
1. (1)

In the first example the domain has a sharp corner at the boundary.

2. (2)

In the second example $$\Delta x_1^2 =2$$ is both positive and too large.

To put things in perspective, let $$D= \{ x_1>0 \} \cap \{x_1 > x_2\}$$ and consider the following function:
\begin{aligned} w(x) = x_1 (x_1 - x_2) \quad \hbox {in } D_r=D \cap B_r(0). \end{aligned}
Now let u be the positive homogeneous harmonic function vanishing on the boundary of the cone D, and set $$v= u -w$$. Since $$w>0$$ in D (by the definition) we have $$u (x) > v (x)$$. Next, due to the fact that $$w \approx r^2$$ and $$u \approx r^a$$ ($$a<2$$) (for r small), we will have $$v >0$$. We also have
\begin{aligned} \Delta u =0, \qquad \Delta v = -1 \qquad \hbox {in } D, \end{aligned}
with zero boundary values. In particular, we have a boundary Harnack principle $$u (x) > v (x)$$ where a harmonic function dominates a superharmonic one.

The difference between this example and the first example above is that the cone is wider. The question that naturally arises is: can such behaviour be structured through a general statement, and if so what are the conditions for such a boundary Harnack principle?

Let us also give a simple example where a subsolution controls a solution in the domain $$D = \{x: x_1 >0\}$$. We let $$u=x_1$$ and $$v=(\varepsilon /2)x_1^2 + x_1$$. Although v is subharmonic, it will control the harmonic solution u. In this example $$\Delta v$$ is small and $$v(e_1)$$ is large. These are the two conditions that will in general guarantee a subsolution may control a solution.

A further observation is that when the domain D is uniformly $$C^{1,Dini}$$ then a boundary Harnack principle holds between a positive harmonic and a super-harmonic functions (with bounded right-hand side), vanishing on the boundary $$(\partial D) \cap B_1$$. This is an easy consequence of Hopf’s boundary point lemma and $$C^1$$-regularity of solutions. Indeed, let u be a non-negative harmonic function in D and v satisfy $$\Delta v = -1$$ in D, both with zero Dirichlet data on $$(\partial D) \cap B_1$$. Then by Hopf’s boundary principle (applied to u) and feat that v is uniformly $$C^1$$, we have
\begin{aligned}&\partial _\nu u \ge C_0 > 0 \quad \hbox {on } \partial D \cap B_1, \qquad \hbox {universal } C_0,\\&\partial _\nu v \le C_1 \quad \qquad \hbox {on } \partial D, \qquad \hbox {universal } C_1, \end{aligned}
where $$\nu$$ is the interior normal direction, on $$\partial D$$. Hence for k large, the function $$w_k := k u - v$$ satisfies
\begin{aligned} \partial _\nu w_k= k \partial _\nu u - \partial _\nu v \ge k C_0 - C_1 > 0 \qquad \hbox {on } \partial D \cap B_1. \end{aligned}
Hence $$w_k > 0$$ in D in a small neighbourhood of the $$\partial D \cap B_1$$ and inside D; this is exactly the boundary Harnack we asked for.

### 1.2 Main Result

Our main result is the following:

### Theorem 1.1

Let D be a Lipschitz domain with small Lipschitz constant $$c \le c(n)$$ and the origin $$0 \in \partial D$$. There exists $$\varepsilon$$ such that if u satisfies
\begin{aligned} -C_0\le & {} \Delta u \le \varepsilon \ \text { in } D_L \cap B_2, \\ u= & {} 0 \ \text { on } \partial D_L \cap B_2 , \\ u\ge & {} 0 \ \text { in } D_L \cap B_2, \\ u(e_n/2) = 1, \end{aligned}
and v satisfies
\begin{aligned} |\Delta v|\le & {} C_0 \ \text { in } D_L \cap B_2 ,\\ v= & {} 0 \ \text { on } \partial D_L \cap B_2,\\ \sup _{B_1\cap D_L} |v|= & {} 1 , \end{aligned}
then for a universal positive constants $$C , \beta >$$, depending on $$n,C_0$$, one has
\begin{aligned} \left\| \frac{v}{u} \right\| _{C^{0,\beta }(B_{1/4})} \le C . \end{aligned}

### Remark 1.2

We prove Theorem 1.1 for the Laplace operator, however the result will also be true for divergence form operators as given in Theorem 4.7. The methods in Lemmas 3.12– 3.14 will also apply to divergence form operators to show that the quotient is not only bounded as stated in Theorem 4.7 but also Hölder continuous up to the boundary.

For instructional reasons and for the benefit of the non-expert reader, we first state and prove the theorem inside a cone; see Theorem 2.1. The proof in this case presents the main ideas for the general case. Next, we do the same for a Lipschitz domain; see Theorem 3.10. We then apply the ideas to divergence operators, see Theorem 4.7. Our result holds even when including zero-order terms. This result appears to be new even when considering the standard boundary Harnack principle without right hand side, that is for solutions rather than supersolutions.

In proving our boundary Harnack principle, we will often utilize the boundary Harnack principle (without right hand side) for two nonnegative solutions. To avoid confusion we will henceforth refer to this as the “standard boundary Harnack principle”.

### 1.3 Related Results

As previously mentioned the boundary Harnack principle has been proven in very general domains as well as for various operators. Recently, De Silva and Savin in  generalized the result in a new direction by showing that improving the regularity of the boundary improves the regularity of the boundary Harnack inequality. Their result applies to elliptic operators in divergence form with appropriate smoothness assumptions on the coefficients. Roughly speaking, if uv vanish on $$\partial D$$ with $$\mathcal {L}u=0$$ and $$\mathcal {L}v=f$$ in D, and if $$u>0$$ in D and $$\partial D \in C^{k,\beta }$$, then
\begin{aligned} \left\| \frac{v}{u} \right\| _{C^{k,\beta }} \le C \left( \Vert v \Vert _{L^{\infty }} + \Vert f \Vert _{C^{k-1,\beta }} \right) . \end{aligned}
(1.1)
The result in  illustrates the principle that improving the regularity of the boundary gives a boundary Harnack principle for solutions with a right hand side. Our result shows that Lipschitz regularity is a sufficient condition to obtain an estimate of the form (1.1) when $$k=0$$, and the allowed behavior for f is determined by the Lipschitz constant.

Another related result is found in , where it is shown that a superharmonic function is comparable to the first eigenfunction for a domain in $$\mathbb {R}^2$$ with finitely many corners and with an interior cone condition.

### 1.4 Applications

We present two applications of our boundary Harnack principle: to the Hele-Shaw flow and to the obstacle problem.

#### 1.4.1 Hele-Shaw Flow

The Hele-Shaw flow may be formulated as follows: for $$t >0$$ we define $$u^t(x)$$ as the solution of
\begin{aligned} \Delta u^t (x) = \chi _{\Omega ^t} - \chi _{\Omega ^0 } - t\delta _z \qquad \hbox {in } {\mathbb {R}}^n, \end{aligned}
where $$\Omega ^0$$ is the initial domain (filled with liquid) and $$\Omega ^t = \{u^t > 0\}$$, and $$z \in \Omega ^0$$ is the liquid-injection point. The Dirac mass at the point z means we inject more fluid at that point. This formulation is obtained after a Baiocchi-transformation, which is easily found in the classical literature for free boundary problems.
Now suppose we do the Hele-Shaw experiment on a “table” having corners of various angles. More exactly, suppose we consider
\begin{aligned} \Delta u^t (x) = \chi _{\Omega ^t} - \chi _{\Omega ^0 } - t\delta _z \quad \hbox {in } D, \qquad u^t (x) = 0 \quad \hbox {on } \partial D, \end{aligned}
where $$D \supset \Omega ^0$$ is a given domain. The zero boundary data on $$\partial D$$ means that the liquid, when reaching the edge of the table, will fall to the ground. The question is whether the liquid will reach all points of the boundary of D in finite time $$t_0< \infty$$.

By a barrier argument (see ) one can show that in two dimensions corners with angle smaller than or equal to $$\pi /2$$ will not get wet; an analogous result for higher dimensions is a consequence of Theorem 2.5 and  2.6 in this paper. Now the question is what can happen when the angle of the corner is larger than $$\pi /2$$; will the liquid reach such a corner? The answer to this question is yes; see .

We now consider D with Lipschitz boundary with Lipschitz constant $$L< 1$$. As a consequence of Theorem 3.10 we now show that every point of the boundary will get wet. We need to show for large values of t that $$u^t > 0$$ in $$D \cap B_r (z^1)$$, for any $$z^1 \in \partial D$$. We write $$u^t (x) = h^t (x) - k(x)$$ where $$h^t$$ is the harmonic function in $$B_r(z^1) \cap D$$ with boundary values $$h^t= u^t$$, and k (t-independent) satisfies
\begin{aligned} \Delta k = -1 \quad \hbox { in } B_r(z^1) \cap D, \end{aligned}
with zero boundary values on $$\partial ( B_r(z^1) \cap D)$$. It suffices then to show that for large values of t we have
\begin{aligned} h^t \ge k \qquad \hbox { in } B_r(z^1) \cap D. \end{aligned}
By Theorem 3.10, for fixed t there exists some large constant $$C_t$$ such that $$C_t h^t \ge k$$. By the standard boundary Harnack principle
\begin{aligned} \sup _{B_{r/2}(z^1)\cap D} \frac{h^t}{h^s} \le C \frac{h^t(z^2)}{h^s(z^2)}, \end{aligned}
for a fixed $$z^2 \in B_r(z^1)\cap D$$. Since $$\lim _{s \rightarrow \infty } h^s(z^2) = \infty$$, we choose s large enough so that $$h^t(z^2)/h^s(z^2) < C^{-1}/C_t$$. Then
\begin{aligned} \sup _{B_{r/2}(z^1) \cap D}\frac{h^t}{h^s} \le C\frac{h^t(z^2)}{h^s(z^2)} \le \frac{C C^{-1}}{C_t}, \end{aligned}
so that $$h^s \ge C_t h^t \ge k$$ to conclude that $$u^t>0$$ in $$B_{r/2}(z^1) \cap D$$, for t large enough.
A related question to the Hele-Shaw flow reaching corners, is whether for $$D \subset {\mathbb {R}}^n$$, with $$0 \in \partial D$$, and $$\partial B_1 \cap D \not =\emptyset$$, a solution to
\begin{aligned} \Delta v_m = 1 \quad \hbox { in } D \cap B_1, \qquad v_m=0 \hbox { on } \partial D \cap B_1 \qquad v_m=m \hbox { on } \partial B_1 \cap D, \end{aligned}
will be non-negative in $$D \cap B_1$$ for m large enough. The answer to this question is already given in the discussion for Hele-Shaw experiment above.

#### 1.4.2 Obstacle Problem

A further application can be made to the regularity theory of the free boundary for the obstacle problem, that is formulated as a solution to
\begin{aligned} \Delta v = h\chi _{\{v > 0\}}, \qquad v \ge 0 \qquad \hbox {in } B_1, \end{aligned}
with $$h \ge c_0 >0$$ Lipschitz, and a prescribed Dirichlet data on $$\partial B_1$$. In proving regularity of the free boundary for the obstacle problem one can show that if a free boundary point $$z \in \partial \{v > 0\} \cap B_{1/2}$$ is not a cusp point, then for some $$r>0$$ and direction e, $$v_e > 0$$ in the set $$\{ v> 0\} \cap B_r(z)$$, and that the free boundary is Lipschitz in $$B_r(z)$$.

One can actually show that the Lipschitz norm can be taken as small as one wishes by taking the neighbourhood of z smaller. The proof for (non-uniform) Lipschitz regularity is actually much simpler than proving uniform regularity. We refer to  for background and details as well as other related original references.

The boundary Harnack principle in this paper allows us to deduce $$C^{1,\alpha }$$-regularity of the free boundary for the obstacle problem, in an elementary way.3 Indeed, we consider the function $$H(x) = v_{e_1} - C v$$, which satisfies4
\begin{aligned} H> 0 , \qquad v_{e_1}> 0 , \qquad \Delta H = h_{e_1} - C h \le 0 \qquad \hbox {in } \{v >0\} \cap B_r(z). \end{aligned}
We will now apply Theorem 1.1 to the functions $$H=v_{e_1}-Cv$$ and $$v_e$$ (which satisfies $$\Delta v_e = h_e$$) for any direction e orthogonal to $$e_1$$. Both H and $$v_e$$ vanish on the free boundary $$\partial \{v>0\}$$. By taking a neighborhood of $$z \in \partial \{v > 0\} \cap B_{1/2}$$ small enough, the Lipschitz norm of $$\partial \{v > 0\} \cap B_{1/2}$$ can be made arbitrarily small. Since $$\Delta H \le 0$$ and $$|\Delta H|$$ is bounded (due to Lipschitz regularity of h), we may apply Theorem 1.1 to conclude that
\begin{aligned} \frac{ v_e }{ v_{e_1} - Cv } \end{aligned}
(1.2)
is $$C^\alpha$$ inside $$\{v >0\}$$ (close to the free boundary point z).
Next fix a level surface $$v=l$$, and denote the free boundary as a Lipschitz graph $$x_1=G(x')$$.5 Consider $$v(G(x') , x') = l$$, which after differentiation in the e-direction gives
\begin{aligned} -G_e = \frac{ v_e }{ v_{e_1} } , \end{aligned}
inserting this into (1.2) gives us
\begin{aligned} \frac{ v_e }{ v_{e_1} - Cv } = \frac{ \frac{ v_e}{ v_{e_1} } }{ 1 - \frac{ Cv}{ v_{e_1} }} = \frac{-G_e }{ 1 - \frac{ Cl}{ v_{e_1} } } , \end{aligned}
is $$C^\alpha$$, independent of l. Since $$v_{e_1} \approx \sqrt{l}$$ we have that
\begin{aligned} \frac{ v_e }{ v_{e_1} - Cv } = \frac{-G_e }{ 1 - \frac{ Cl}{ v_{e_1} } } \rightarrow -G_e, \end{aligned}
as $$l \rightarrow 0$$.6 Hence $$G_e$$ is $$C^\alpha$$.

### 1.5 Future Directions

It seems plausible that the results presented in this paper can be generalized to other operators, as well as more complicated domains. Here we have chosen to treat the problem in Lipschitz domains only. In the final section we consider second order elliptic equations of divergence form. The coefficients are variable and assumed to be only bounded and measurable.

Key elements of our approach are the standard boundary Harnack principle, barrier arguments, as well as scaling and blow-up invariance. Since our approach is indirect and uses scalings, the core idea is to look at nonnegative solutions on global domains. The technical difficulties that seem to arise for generaliztions of our result concern the invariance of the domains in scaling.

The methods presented here should also work to prove a boundary Harnack principle for the positivity set of a solution to the thin obstacle problem as long as it is assumed a priori that the free boundary is Lipschitz. Then we may argue in a similar way as above for the thin obstacle problem, with equations having Lipschitz right hand side; see  in combination with our result.

## 2 Boundary Harnack in Cones

We let $$\mathcal {C}$$ be any open cone in $${\mathbb {R}}^n$$, with vertex at the origin such that $$\mathcal {C}\cap \mathbb {S}^{n-1}$$ is connected. If u is any harmonic function on $${\mathcal {C}}$$ with $$u=0$$ on $$\partial {\mathcal {C}}$$, then in spherical coordinates
\begin{aligned} u(r,\theta ) = \sum _{k=1}^{\infty } r^{\alpha _k} f_k(\theta ), \end{aligned}
(2.1)
where $$f_k$$ are the eigenfunctions to the Laplace-Beltrami on $${\mathcal {C}}\cap \partial B_1$$. If u is harmonic on $${\mathcal {C}}$$ and nonnegative, then u is unique up to multiplicative constant to $$r^{\alpha _1}f_1(\theta )$$.

### Theorem 2.1

Let $${\mathcal {C}}$$ be a connected open cone in $${\mathbb {R}}^n$$ with $$\partial {\mathcal {C}}\cap \mathbb {S}^{n-1}$$ an $$(n-2)$$-dimensional $$C^{1,\alpha }$$ submanifold.7 Let $$r^{\alpha _1}f_1(\theta )\ge 0$$ be harmonic in $${\mathcal {C}}$$ with zero Dirichlet boundary data. Let u solve
\begin{aligned} \begin{aligned} \Delta u&=0 \text { in } {\mathcal {C}}\cap B_1 , \\ u&\ge 0 \text { in } {\mathcal {C}}\cap B_1 , \\ u&=0 \text { on } \partial {\mathcal {C}}\cap B_1, \end{aligned} \end{aligned}
and let v satisfy
\begin{aligned} \begin{aligned} 0 \ge \Delta&v(x)\ge -C_0|x|^{\gamma }&\,&\text { in } {\mathcal {C}}\cap B_1 , \\ v&=0&\,&\text { on } \partial {\mathcal {C}}\cap B_1 , \\ |v|&\le C_0&\,&\text { in } {\mathcal {C}}\cap B_1, \end{aligned} \end{aligned}
(2.2)
with $$2-\alpha _1+\gamma >0$$. If $$x^0 \in {\mathcal {C}}\cap B_1$$, then there exists a constant C depending only on $${\mathcal {C}},2-\alpha _1 + \gamma$$, dimension n, and dist$$(x^0, \partial ({\mathcal {C}}\cap B_1))$$ such that if $$u(x^0)=v(x^0)=1$$, then
\begin{aligned} C^{-1} v(x) \le u(x) \le C v(x) \ \text { for any } x \in {\mathcal {C}}\cap B_{1/2}. \end{aligned}

Theorem 2.1 is a boundary Harnack principle, but with a right hand side. Clearly, a harmonic solution will control a subsolution. The significance of Theorem 2.1 is that a harmonic solution can control a supersolution, and that the allowed behavior for the right hand side depends on the opening of the cone or more explicitly on $$\alpha _1$$. When the opening of the cone is large (so that $$\alpha _1$$ is small), then negative values for $$\gamma$$ are allowed, and the right hand side can have singular behavior near the boundary. When the opening of the cone is small (so that $$\alpha _1$$ is large), then $$\gamma$$ must be positive and large, so that the right hand side must decay as it approaches the boundary.

In order to prove Theorem 2.1, we will need the following convergence result:

### Lemma 2.2

Let $${\mathcal {C}}$$ be an open cone with $$\partial {\mathcal {C}}\cap \mathbb {S}^{n-1}$$ an $$(n-2)$$-dimensional $$C^{1,\alpha }$$ submanifold. Fix $$0< \varepsilon < R$$ and let $$\gamma >\alpha _1 - 2$$. For any sequence $$v_k$$ satisfying
\begin{aligned} \begin{aligned} |\Delta v_k|&\le C_0 |x|^{\gamma }&\text { in } {\mathcal {C}}\cap B_R , \\ |v_k|&\le C_0&\text { in } {\mathcal {C}}\cap B_R , \\ v_k&=0&\text { on } \partial {\mathcal {C}}\cap B_R , \\ \end{aligned} \end{aligned}
there exists a subsequence $$v_k \rightarrow v$$ uniformly on $${\mathcal {C}}\cap B_{R-\varepsilon }$$ with v inheriting the above properties.

### Proof

Since $${\mathcal {C}}\cap \partial B_R$$ is a $$C^{1,\alpha }$$ Lipschitz submanifold, $${\mathcal {C}}$$ is compactly contained in a slightly larger cone $${\mathcal {C}}' \supset {\mathcal {C}}$$, and the unique nonnegative harmonic solution with zero Dirichlet data on $$\partial {\mathcal {C}}'$$ is given as $$r^{\alpha _1-\delta } f_{\delta }$$. We note that $$f_{\delta }(\theta )$$ is uniformly bounded away from 0 on $${\mathcal {C}}$$. We let $$h=M_1 r^{\alpha _1-2\delta }f_{\delta }$$ with $$M_1$$ chosen later. Then
\begin{aligned} \Delta h = M_1[(\alpha _1-2\delta )(\alpha _1-2\delta +n-2) -(\alpha _1+\delta )(\alpha _1+\delta +n-2)] r^{\alpha _1-2 -2\delta }f_{\delta }. \end{aligned}
Since $$\alpha _1-2-2\delta < \gamma$$, we may choose $$M_1$$ large enough such that
\begin{aligned} \Delta h \le -C_0 |x|^{\alpha _1-2-2\delta } \le -C_0 |x|^{\gamma }. \end{aligned}
Using h as a barrier, the convergence result will follow by standard techniques. $$\square$$

An alternate proof of the above lemma, for a more general domain and more general operator, is given in the proof of Lemma 4.5.

We now give a proof of the main theorem in this Section.

### Proof of Theorem 2.1

Fix $$x^0 \in \mathcal {C}\cap B_{1/2}$$, and consider the nonnegative homogeneous solution $$u=r^{\alpha _1}f_1(\theta )$$. By the standard boundary Harnack principle, any solution u as given in the statement of Theorem 2.1 will be comparable, and consequently bounded from below up to a multiplicative constant, by $$r^{\alpha _1}f(\theta )$$. Thus, we consider $$u=r^{\alpha _1}f(\theta )$$. Furthermore, any function v as given in the statement of Theorem 2.1 will be bounded from above by a constant multiple of the superharmonic function defined by
\begin{aligned} \begin{aligned} \Delta v&=-|x|^{\gamma }&\text { in } {\mathcal {C}}\cap B_1 , \\ v&\ge 0&\text { in } {\mathcal {C}}\cap B_1 , \\ v&=0&\text { on } \partial {\mathcal {C}}\cap B_1 , \\ v&=1&\text { on } {\mathcal {C}}\cap \partial B_1 . \end{aligned} \end{aligned}
Thus, it suffices to prove the theorem for v as defined above and with $$u=r^{\alpha _1}f(\theta )$$.
In the following we use r as a scaling parameter which should not be confused when r is used as the polar axis for homogeneous functions. We first show that there exists some constant C such that $$v(rx^0)\le Cu(rx^0)$$ for all $$0<r\le 1/2$$. Suppose, by way of contradiction, that no such C exists, so that if $$v(t x^0)= t^{\alpha _1} h(t)$$, then $$\limsup _{t \rightarrow 0} h(t)=\infty$$. We note that h is continuous away from the origin since v is continuous. For $$0<r<1$$, we consider the rescaled functions
\begin{aligned} w_r(x) := \frac{v(rx)-\frac{v(rx^0)}{u(rx^0)}u(rx)}{\sup _{B_1 \cap \mathcal {C}} |v(rx)-\frac{v(rx^0)}{u(rx^0)}u(rx)|}, \end{aligned}
defined on $$B_{1/r}$$. We point out that $$w_r(x^0)=0$$ and $$\sup _{B_1 \cap \mathcal {C}} |w_r|=1$$. We also define
\begin{aligned} a_k := \sup _{B_1 \cap \mathcal {C}} \left| v(2^{-k}x)-\frac{v(2^{-k}x^0)}{u(2^{-k}x^0)}u(2^{-k}x)\right| 2^{k\alpha _1}. \end{aligned}
By letting $$x=tx^0$$, we have
\begin{aligned} v(rx)-\frac{v(rx^0)}{u(rx^0)}u(rx) = [h(rt)-h(r)](rt)^{\alpha _1}. \end{aligned}
If $$r_k = 2^{-k}$$, and if $$1/2\le t \le 1$$, we have
\begin{aligned} \text {osc}_{[r_k/2,r_k]} h \le a_k. \end{aligned}
Since $$\limsup _{t \rightarrow 0} h(t) = +\infty$$, it follows that
\begin{aligned} \sum a_k = + \infty . \end{aligned}
(2.3)
By the definition of $$w_r$$, we have
\begin{aligned} \sup _{B_{2^j}} |w_{r_k}(x)| = \frac{\sup _{B_{2^j}} |v(r_k x) - \frac{v( r_k x^0)}{u( r_k x^0)}u(r_k x)|}{a_k r_k^{\alpha _1}} . \end{aligned}
We use the triangle inequality to obtain
\begin{aligned} \begin{aligned} |v(r_k x) - \frac{v(r_k x^0)}{u(r_k x^0)}u(r_k x)|&\le | v(r_k x) - \frac{v(2^j r_k x^0)}{u(2^j r_k x^0)}u(r_k x)| \\&\quad + \sum _{i=0}^{j-1} \left| \frac{v(2^{j-i} r_k x^0)}{u(2^{j-i} r_k x^0)}u(r_k x) - \frac{v(2^{j-i-1} r_k x^0)}{u(2^{j-i-1} r_k x^0)}u(r_k x) \right| . \end{aligned} \end{aligned}
(2.4)
To bound the first term in the above inequality, we have, by definition, that
\begin{aligned} \sup _{B_{2^j}} | v(r_k x) - \frac{v(2^j r_k x^0)}{u(2^j r_k x^0)}u(r_k x)| = a_{k-j} (2^j r_k)^{\alpha _1}. \end{aligned}
(2.5)
To bound the second term in the inequality, we note first that
\begin{aligned} \begin{aligned}&\left| \frac{v(2^{j-i} r_k x^0)}{u(2^{j-i} r_k x^0)}u(2^{j-i-1}r_k x^0) - \frac{v(2^{j-i-1} r_k x^0)}{u(2^{j-i-1} r_k x^0)}u(2^{j-i-1}r_k x^0) \right| \\&\quad = \left| \frac{v(2^{j-i} r_k x^0)}{u(2^{j-i} r_k x^0)}u(r_k 2^{j-i-1}x^0) - v(2^{j-i-1} r_k x^0) \right| \\&\quad \le a_{k-(j-i)} (2^{j-i}r_k)^{\alpha _1}. \end{aligned} \end{aligned}
Also, we note that there exists C depending on $$x^0$$ such that if $$|x|=1$$, then $$u(rx)\le C u(rx^0)$$. If we utilize the homogeneity of u, we conclude that
\begin{aligned} \sup _{B_{2^j}} u(r_kx) \le Cu(2^j r_k x^0). \end{aligned}
We use this and the homogeneity of u to obtain
\begin{aligned} \begin{aligned}&\sup _{B_{2^j}} \left| \frac{v(2^{j-i} r_k x^0)}{u(2^{j-i} r_k x^0)}u(r_k x) - \frac{v(2^{j-i-1} r_k x^0)}{u(2^{j-i-1} r_k x^0)}u(r_k x) \right| \\&\quad = \sup _{B_{2^j}} \frac{u(r_k x)}{u(2^{j-i-1} r_k x^0)} \\&\qquad \times \left| \frac{v(2^{j-i} r_k x^0)}{u(2^{j-i} r_k x^0)}u(2^{j-i-1}r_k x^0) - v(2^{j-i-1} r_k x^0) \right| \\&\quad \le \frac{Cu(2^j r_k x^0)}{u(2^{j-i-1} r_k x^0)} a_{k-(j-i)} (2^{j-i} r_k)^{\alpha _1} \\&\quad = C a_{k-(j-i)} (2^{j+1} r_k)^{\alpha _1} . \end{aligned} \end{aligned}
(2.6)
From (2.3) we may apply Lemma A.1 to the sequence $$\{a_k\}$$ to conclude that there exists a subsequence $$k_l$$ such that for any $$j \in \mathbb {N}$$,
\begin{aligned} \limsup _{k_l \rightarrow \infty } \frac{\sum _{i=1}^j a_{k_l -i}}{a_{k_l}} \le j. \end{aligned}
By choosing $$r_{k_l}$$ and combining the above inequality with (2.4), (2.5) and (2.6), we conclude that
\begin{aligned} \sup _{B_{2^j}} |w_{r_{k_l}}(x)| \le C j 2^{j\alpha _1} \end{aligned}
(2.7)
for $$j \le k_l$$.
We will now bound the Laplacian of $$w_{r_k}$$. From the choice of $$a_{k_l}$$ in Lemma A.1 and the fact that $$\sum a_k = + \infty$$ it follows that eventually $$a_{k_l}\ge k_l^{-2}$$, so that if $$r_{k_l} = 2^{-k_l}$$, then
\begin{aligned} a_{k_l} \ge [\ln (1/r_k)]^{-2}. \end{aligned}
We now use the assumption $$2-\alpha _1 + \gamma >0$$. Since $$\Delta u=0$$ and $$\Delta v=-|x|^\gamma$$ we have that for a sequence $$r_{k_l} \rightarrow 0$$, it holds that
\begin{aligned} |\Delta w_k| \le \frac{r_k^{2+\gamma }|x|^{\gamma }}{\sup _{B_1 \cap \mathcal {C}} |v(rx)-\frac{v(rx^0)}{u(rx^0)}u(rx)|} \le C r_k^{2-\alpha _1+\gamma }[\ln (1/r_k)]^2 |x|^{\gamma }\quad \rightarrow \ 0 , \end{aligned}
(2.8)
as long as $$2-\alpha _1 + \gamma >0$$.
By Lemma 2.2 there exists a subsequence $$w_k \rightarrow w$$ uniformly in $$B_R \cap \mathcal {C}$$ for any $$R>0$$. Furthermore, w will satisfy
\begin{aligned} \begin{aligned}&(\mathrm{i})&\Delta w =0&\qquad \text { from } (2.8) ,\\&(\mathrm{ii})&\sup _{B_1 \cap {\mathcal {C}}} |w| =1&\ ,\\&(\mathrm{iii})&w(x^0) =0 , \\&(\mathrm{iv})&w(x) \le C|x|^{\alpha _1} \ln (|x|+1)&\qquad \text { for } |x| \ge 1 \text { from } (2.7). \end{aligned} \end{aligned}
By property $$(\mathrm{ii})$$ we have that w is not identically zero. By property $$(\mathrm{iii})$$ we have that w changes sign, so that by (2.1) we have $$\sup _{B_R} |w| \ge c R^{\alpha _2}$$ for $$R \ge 1$$. Since $$|x|^{\alpha _1} \ln (|x| +1) < |x|^{\alpha _2}$$, for large x, this contradicts property (iv).
Thus, we have shown that for any $$x^0 \in {\mathcal {C}}$$ there exists a constant C depending on $$x^0$$ such that
\begin{aligned} v(rx^0) \le C u(rx^0) \text { for any } 0<r\le 1/2. \end{aligned}
For any other point $$x^1 \in {\mathcal {C}}\cap B_{1/2}$$, we rescale by $$v(x|x^1|/2)$$, and note that $$|\Delta v(x|x^1|/2)| \le |x^1/2|^2 |x|^{\gamma }$$, so that $$|\Delta v(x|x^1|/2)| \le C_1$$ in $${\mathcal {C}}\cap (B_{3/4} \setminus B_{1/4})$$. We now restrict ourselves to the situation in which $$x^1/|x^1|$$ is uniformly bounded away from $$\partial {\mathcal {C}}$$. Since $$v(x^0 |x^1|/2)\le C_2 |x^1|^{\alpha _1}$$, we use the (interior) Harnack inequality on $${\mathcal {C}}\cap (B_{3/4} \setminus B_{1/4})$$ to conclude that
\begin{aligned} v(x^1) \le C_3(C_2 |x^1|^{\alpha _1} + C_1 |x^1|^{2+\gamma }) \le C_4 |x^1|^{\alpha _1}, \end{aligned}
where in the second inequality we have used $$2-\alpha _1 + \gamma >0$$, and $$|x^1| < 1$$.
The constant $$C_3$$ does not remain bounded as $$x^1$$ approaches $$\partial {\mathcal {C}}$$. Furthermore, we also have that $$f_1(x^1/ |x^1|)$$ goes to zero as $$x^1/|x^1|$$ approaches $$\partial {\mathcal {C}}\cap S^{n-1}$$. If $$x^1$$ is close to $$\partial {\mathcal {C}}$$, we employ the boundary Harnack principle (1.1) with right hand side as given in  which is applicable as long as $$\partial {\mathcal {C}}\cap (B_{3/4}\setminus B_{1/4}) \in C^{1,\beta }$$. We may then conclude that
\begin{aligned} v(x^1) \le C_5 u(x^1)(\Vert v \Vert _{L^{\infty }} + |x_1|^{2+\gamma }) \le C_6 u(x^1) = C_6 |x^1|^{\alpha _1}f_1(x^1/|x^1|), \end{aligned}
and this concludes the result. $$\quad \square$$

As a corollary we are able to bound a supersolution by a subsolution as long as the right hand side is small enough and the subharmonic solution has a large enough height.

### Corollary 2.3

Let $$\mathcal {C}$$ and $$\gamma$$ have the same assumptions as in Theorem 2.1. Let $$u,v \ge 0$$ with $$u=v=0$$ on $$\partial \mathcal {C} \cap B_1$$ and $$u(x^0)=v(x^0)=1$$. There exists $$\varepsilon >0$$ with the same dependence as C in Theorem 2.1 such that if
\begin{aligned} -C_0 |x|^{\gamma } \le \Delta u, \Delta v \le \varepsilon |x|^{\gamma }, \end{aligned}
then
\begin{aligned} \frac{v(x)}{u(x)} \le 4C \text { for any } x \in \mathcal {C} \cap B_{1/2}, \end{aligned}
where C is the constant appearing in Theorem 2.1.

### Proof

Let $$x^0 \in \mathcal {C} \cap B_{3/4}$$ and w solve $$\Delta w = \varepsilon |x|^{\gamma }$$ in $$\mathcal {C}\cap B_{3/4}$$, with $$w=0$$ on $$\partial (\mathcal {C}\cap B_{3/4})$$. We first observe that
\begin{aligned} -(C_0+\varepsilon )|x|^{\gamma } \le \Delta (u-w), \Delta (v-w) \le 0. \end{aligned}
For $$\varepsilon$$ small we have $$c_1 \varepsilon \le |w(x^0)| \le c_2 \varepsilon$$, with $$c_1,c_2$$ depending on M and the dist$$(x^0,\partial ({\mathcal {C}}\cap B_1))$$. We also let $$\tilde{u}$$ be the harmonic replacement of u in $$B_{3/4} \cap \mathcal {C}$$. Then $$\tilde{u}(x^0)$$ is bounded below by a constant with the same dependence as C in Theorem 2.1. Then applying Theorem 2.1 to $$\tilde{u}$$ and w we obtain that
\begin{aligned} \frac{-w(x)}{\tilde{u} (x)} \le C \frac{-w(x^0)}{\tilde{u} (x^0)} \le Cc_2\varepsilon \ \text { in } \mathcal {C} \cap B_{1/2}. \end{aligned}
(2.9)
Applying Theorem 2.1 to $$v-w$$ and $$\tilde{u}$$ we obtain
\begin{aligned} (v-w)(x) \le C \tilde{u} (x). \end{aligned}
(2.10)
Since $$\tilde{u}$$ is the harmonic replacement of u and $$\Delta (u-w) \le 0$$ with $$\tilde{u} = u-w$$ on $$\partial (\mathcal {C}\cap B_{3/4})$$, we have $$\tilde{u} \le u-w$$, and hence by (2.10) $$(v-w)(x) \le C(u-w)(x)$$ in $$\mathcal {C} \cap B_{1/2}$$. Now by (2.9) we have
\begin{aligned} -w(x) \le C c_2 \varepsilon \tilde{u} (x) \le C c_2 \varepsilon (u-w)(x). \end{aligned}
From these inequalities we conclude that
\begin{aligned} (v-w)(x) \le C(u-w)(x) \le Cu(x) - Cw(x) \le Cu(x) -C^2 c_2 \varepsilon (u-w)(x). \end{aligned}
We choose $$\varepsilon < (2C^2c_2)^{-1}$$ so that
\begin{aligned} v(x) \le (v-w/2)(x) \le Cu(x) \quad \text { in } \mathcal {C} \cap B_{1/2}. \end{aligned}
$$\square$$

We also state here another result which will be needed later in the proof of Lemma 3.14:

### Corollary 2.4

Let $$\mathcal {C}$$ and $$\gamma$$ have the same assumptions as in Theorem 2.1. Let u solve
\begin{aligned} \begin{aligned} \Delta u&=0 \text { in } \mathcal {C} \cap B_1 \\ u&=0 \text { on } \partial \mathcal {C} \cap B_1 \\ u&\ge 0, \end{aligned} \end{aligned}
and let v solve (for some $$\eta >0$$)
\begin{aligned} \begin{aligned} 0 \le \Delta v&\le \eta \text { in } \mathcal {C} \cap B_1 \\ v&=u \text { on } \partial (\mathcal {C} \cap B_1) . \end{aligned} \end{aligned}
There exists $$\eta _0 >0$$ with the same dependence as C in Theorem 2.1 such that if $$\eta \le \eta _0$$ then $$v>0$$ in $$B_r \cap \mathcal {C}$$ for r small enough.

### Proof

We let $$x^0$$ be as in Theorem 2.1. We note that $$u(x^0) - v(x^0)$$ is comparable to $$\eta$$, so we apply Theorem 2.1 to $$(u-v)/(u(x^0) - v(x^0))$$ and $$u/u(x^0)$$ to obtain that
\begin{aligned} \sup _{B_{1/2}} \frac{u-v}{u} \le C \frac{u(x^0)-v(x^0)}{u(x^0)} \le C_1 \eta . \end{aligned}
Then for $$C_1 \eta < 1/2$$ we have that $$0\le u \le 2w$$ on $$B_{1/2}$$ and this concludes the proof. $$\quad \square$$

We now show that the assumption that $$2-\alpha _1 + \gamma >0$$ is essential. We first consider the easier case when $$2-\alpha _1+\gamma <0$$, and show that Theorem 2.1 cannot possibly hold. For clarity of exposition we restrict the analysis to the case when $$\gamma =0$$, so that the right hand side is constant.

### Theorem 2.5

Let u and v be as in the statement of Theorem 2.1, and assume $$\Delta v = - 1$$ with $$2-\alpha _1 <0$$. Then, for any $$C>0$$, there exists $$\rho >0$$ such that
\begin{aligned} Cu < v \text { in } {\mathcal {C}}\cap B_{\rho }. \end{aligned}

### Proof

We note that by the standard boundary Harnack inequality, it is enough to consider $$u=r^{\alpha _1}f_1(\theta )$$. We normalize $$f_1$$ so that $$\sup f_1 =1$$. Fix $$C>0$$, and let $$z \in B_r \cap {\mathcal {C}}$$. Define $$h(x):=|x-z|^2/(2n)$$. We note that h is constant on $$\partial B_r(z)$$. If there exists $$y \in \partial B_r(z)$$ with $$h(y)\le Cu(y)-v(y)$$, then
\begin{aligned} \frac{r^2}{2n} = h(y) \le Cu(y)-v(y) \le Cr^{\alpha _1}. \end{aligned}
For small enough r, the above inequality cannot hold since $$2<\alpha _1$$. Then for small enough r, we have $$h \ge Cu-v$$ on $$\partial B_r(z)$$, and hence also on $$\partial (B_r(z)\cap {\mathcal {C}})$$. By the comparison principle $$h \ge Cu-v$$ in $$B_r(z)\cap {\mathcal {C}}$$, and so $$0=h(0)\ge Cu(z) - v(z)$$, so that $$Cu(z)-v(z)\le 0$$. Since C was arbitrary, for any $$\delta >0$$, we may choose $$r_0$$ such that if $$r<r_0$$ and $$x \in B_r \cap {\mathcal {C}}$$, then $$(C+\delta )u(x)-v(x)\le 0$$. Since $$u>0$$ in $$B_r \cap {\mathcal {C}}$$ it follows that $$Cu(x)-v(x) <0$$ for any $$x \in B_r \cap {\mathcal {C}}$$. $$\quad \square$$

We can show that Theorem 2.1 is sharp by considering the critical case when $$2-\alpha _1 =0$$. For when dimension $$n=2$$ this result was shown in .

### Theorem 2.6

Let $${\mathcal {C}}$$ be a cone in $${\mathbb {R}}^n$$ with $$\alpha _1=2$$. Then the boundary Harnack principle with right hand side does not hold.

### Proof

Let v be as in the statement of the Theorem, and let $$u=r^{\alpha _1}f_1(\theta )$$. Suppose that there exists $$C>0$$ such that
\begin{aligned} C^{-1}u(x)\le v(x)\le Cu(x) \text { for all } x \in {\mathcal {C}}\cap B_{1/2}. \end{aligned}
(2.11)
We now use a Weiss-type monotonicity formula for superharmonic functions as in . The function
\begin{aligned} W(r,v) := \frac{1}{r^{n+2}} \int _{B_r \cap {\mathcal {C}}} (|\nabla v|^2 -2v) \ - \frac{2}{r^{n+3}} \int _{\partial B_r \cap {\mathcal {C}}} v^2, \end{aligned}
is monotonically increasing in r and is constant if and only if v is homogeneous. We now consider the rescaled functions $$v_r(x):=v(rx)/r^2$$. From (2.11) and the fact that u is homogeneous of degree 2 we have that, for any fixed $$x \in {\mathcal {C}}\cap B_{1}$$, there exists $$C_x$$ such that
\begin{aligned} C_x^{-1} r^2 \le v_r(x) \le C_x r^2 \text { for any } 0<r<1. \end{aligned}
(2.12)
From Lemma 2.2 we obtain that for a sequence $$r_k \rightarrow 0$$, $$v_{r_k} \rightarrow v_0$$ uniformly in $${\mathcal {C}}\cap B_{R}$$ for any $$R>0$$. Furthermore, we will show that $$v_0$$ satisfies that
\begin{aligned} \begin{aligned} (\mathrm{i})&\quad v_0 \text { is homogeneous of degree } 2 , \\ (\mathrm{ii})&\quad v_0 \ge 0 ,\\ (\mathrm{iii})&\quad v_0 =0 \text { on } \partial {\mathcal {C}},\\ (\mathrm{iv})&\quad \Delta v_0 = -1 \text { in } {\mathcal {C}},\\ (\mathrm{v})&\quad v \text { is not identically zero.} \end{aligned} \end{aligned}
Property (i) follows from the Weiss-type monotonicity formula by checking that $$W(\rho r,v)=W(\rho , v_r)$$; since W(rv) is monotone in r, it follows that
\begin{aligned} W(\rho , v_0) = \lim _{r_k \rightarrow 0} W(\rho , v_{r_k}) = \lim _{r_k \rightarrow 0} W(\rho r_k ,v) = W(0+,v) \text { for any } \rho >0 \end{aligned}
and since $$W(\rho , v_0)$$ is constant, then $$v_0$$ is homogeneous of degree 2, see . Properties (ii)-(iv) follow easily from the definition of $$v_{r}$$ and the uniform convergence. Finally, property (v) follows from (2.12). Then $$v_0= r^2 g$$ where the spherical piece g satisfies $$2ng + \Delta _{\theta } g =-1$$. We now utilize the Fredholm Alternative for existence for weak solutions, see Chapter 6 in . Since $$f_1$$ (in (2.1)) is a nontrivial solution, the solution g exists if and only if
\begin{aligned} 0= \langle -1 , h \rangle = \int _{{\mathcal {C}}\cap \partial B_1} -h \end{aligned}
for all h such that $$2n h + \Delta _{\theta } h =0$$ (since the operator $$2n + \Delta _{\theta }$$ is self-adjoint). We recall that $$2nf_{1} + \Delta _{\theta } f_{1}=0$$. Then a necessary condition for g to exist is that
\begin{aligned} 0=\langle -1, f_1 \rangle = \int _{{\mathcal {C}}\cap \partial B_1} f_1. \end{aligned}
Since $$f_1>0$$ in $${\mathcal {C}}\cap \partial B_1$$, the above equality cannot be true. Consequently, a solution g cannot exist, and we have a contradiction. $$\quad \square$$

## 3 Boundary Harnack in Lipschitz Domains

In this section we consider Lipschitz domains $$D_{L,R}$$ where
\begin{aligned} D_{L,R} := \{(x',x_n) \in B_R : x_n>g(x')\}, \end{aligned}
and g is Lipschitz with constant L, that is $$|g(x')-g(y')|\le L |x'-y'|$$. We will assume $$g(0)=0$$, and will write $$D_{L}$$ when $$R=1$$ and $$D_{L,\infty }$$ if $$R=\infty$$. Also, we define $$u \in \mathcal {S}(D_{L,R})$$ if
\begin{aligned} \begin{aligned} \Delta u(x)&=0 \text { in } D_{L,R} ,\\ u(x)&=0 \text { on } D_{L,R}^c\cap B_R, \end{aligned} \end{aligned}
and for $$\gamma \in \mathbb {R}$$ we define $$u \in \mathcal {S}(D_{L,R},d^{\gamma })$$ if
\begin{aligned} \begin{aligned} |\Delta u(x)|&\le (\text {dist}(x,\partial D_{L,R} \cap B_R))^{\gamma }&\,&\text { in } D_{L,R} , \\ u(x)&=0&\,&\text { on } D_{L,R}^c\cap B_R. \end{aligned} \end{aligned}
It will be necessary to use the solutions on right circular cones as barriers. Consequently, we define
\begin{aligned} {\mathcal {C}}_L := \{(x',x_n): x_n > L |x'|\}. \end{aligned}
If $$u \in \mathcal {S}({\mathcal {C}}_{L,\infty })$$ and $$u\ge 0$$, then as noted in Section 2, we have $$u=r^{\alpha _1}f_1(\theta )$$ (and unique up to multiplicative constant), and we will denote $$r^{\alpha _1}f_1$$ by $$u_L$$. We note that the definition of $${\mathcal {C}}_{(-L)}$$ still makes sense when $$-L<0$$; although, the cone $${\mathcal {C}}_{(-L)}$$ is not convex. In this situation we write $${\mathcal {C}}_{(-L)}$$ and similarly $$u_{(-L)}$$ for the nonnegative solution with zero boundary data on $${\mathcal {C}}_{(-L)}$$.
In order to prove a boundary Harnack principle with a right hand side for Lipschitz domains we will adapt the proof from Section 2 in the following manner:
• We will employ compactness methods and thus need a convergence result provided by Lemma 3.2.

• We will need to bound the behavior of a nonnegative harmonic function at the boundary from above and below which is given in Lemma 3.3.

• We will need a Liouville type result which is given in Lemma 3.6.

• We will then adapt the proof of Theorem 2.1 (again using compactness techniques) to obtain the proof of Theorem 3.10.

### Lemma 3.1

Let $$L \le M$$ and $$u \in \mathcal {S}(D_L)$$ with $$u \ge 0$$. Let $$x \in \partial D_L \cap B_{1/2}$$ and let $$y \in D_L$$ with dist$$(y,\partial D_L)>\delta$$. Then there exists a constant $$C=C(n,M,\delta )$$ such that
\begin{aligned} \begin{aligned}&\sup _{B_r(x)} u \le C u(y)&\text { for all } r\le 1/4 , \\&\sup _{B_{1/4}} u \ge C^{-1} u(y). \end{aligned} \end{aligned}

We give later a proof of a more general version of this lemma; see Lemma 4.4 in Section 4.

### Lemma 3.2

Let $$D_{L_k,R_k}$$ be a sequence of domains with $$L_k \le M$$, $$R_k \ge 1$$, and $$0 \in \partial D_{L_k}$$. Let $$u_k \in \mathcal {S}(D_{L_k,R_k}, d^{\gamma })$$, and let $$\alpha$$ be the degree of homogeneity for $$u_M$$, and assume $$2-\alpha +\gamma >0$$. We further assume either
\begin{aligned} \begin{aligned}&(1) \quad u_k \ge 0 \ \text { and } \sup _{B_{1/2}} u_k \le 1 , \quad or \\&(2)\ \sup _{B_r} u_k \le C r^{\beta } \ \text { for } r\le 1 \text { and some constants } C, \beta >0. \end{aligned} \end{aligned}
Then there exists a subsequence with a limiting domain $$D_{L_0,R_0}$$ and a limiting function $$u_0 \in \mathcal {S}(D_{L_0,R_0},d^{\gamma })$$ such that
\begin{aligned} \sup _{B_r} |u_k - u_0| \rightarrow 0 \qquad \hbox {as } k \rightarrow \infty \end{aligned}
for all $$r<R_0$$.

We give later a proof of the more general Lemma 3.2 in Section 4 that implies Lemma 3.2.

### Lemma 3.3

Let $$u\in \mathcal {S}(D_L)$$ with $$u\ge 0$$. Let $$L<M$$ and let $$\alpha _1$$ be the degree of homogeneity for $$u_{M}$$ and $$\beta$$ the degree of homogeneity for $$u_{(-M)}$$. There exist constants $$c_1,c_2$$ depending only on nM,  and $$M-L$$ such that for any $$x \in \partial D_L \cap B_{1/2}$$,
\begin{aligned} \begin{aligned}&(1)\sup _{B_{r}(x)} u \ge c_1 u(e_n/2) r^{\alpha _1} , \\&(2)\sup _{B_{r}(x)} u \le c_2 u(e_n/2) r^{\beta } \end{aligned} \end{aligned}
for any $$r \le 1/4$$.

### Proof

Let $$x \in \partial D_{L} \cap B_{1/2}$$. From Lemma 3.1 we have $$u(y) \ge C_1 u(e_n/2)$$ for any $$y \in \partial B_{1/4}(x) \cap ({\mathcal {C}}_M+x)$$. We now consider the translated function $$u_{M}(y-x)$$ which is unique up to multiplicative constant and homogeneous of degree $$\alpha _1$$. By multiplying $$u_{M}(y-x)$$ by a positive constant, we may assume that $$\sup _{B_{1/4}(x)} u_{M}(y-x)=C_1 u(e_n/2)$$. Then $$u_M(y-x)\le u(y)$$ on $$\partial B_{1/4}(x) \cap ({\mathcal {C}}_{M}+x)$$. Since $$u_M(y-x)=0$$ on $$\partial ({\mathcal {C}}_M +x)$$, we may invoke the comparison principle to conclude that $$u_M(y-x)\le u(y)$$ on $$B_{1/4}(x) \cap ({\mathcal {C}}_{M}+x)$$. Then
\begin{aligned} \sup _{B_r(x)} u(y) \ge \sup _{B_r(x)} u_{M}(y-x) = C_1 u(e_n/2) r^{\alpha _1}, \end{aligned}
which proves (1). In a similar manner we obtain property (2) by bounding u from above by $$u_{(-M)}$$. $$\quad \square$$

### Corollary 3.4

(To Lemma 3.3) Let $$u\in \mathcal {S}(D_L)$$ with $$L<M$$, and let $$\beta$$ be the degree of homogeneity for $$u_{(-M)}$$. There exists a constant C depending only on dimension nM,  and $$M-L$$ such that for any $$x \in \partial D_L \cap B_{1/2}$$,
\begin{aligned} \sup _{B_{r}(x)} |u| \le C (\sup _{B_{1}} |u|) r^{\beta } \end{aligned}
for any $$r \le 1/4$$.

### Proof

We consider the solution
\begin{aligned} \begin{aligned} \Delta v&=0&\text { in } D_L , \\ v&= 0&\text { on } D_L^c \cap B_1 , \\ v&= \sup _{B_{1}} u&\text { on } \partial B_{1} \cap D_L. \end{aligned} \end{aligned}
From Lemma 3.3 we have that
\begin{aligned} v \le C v(0,1/2) r^{\beta } \le C (\sup _{B_1} v) r^{\beta }. \end{aligned}
From the comparison principle we have that $$u \le v$$ on $$B_1$$. By considering $$-v$$ we obtain a similar bound from below to conclude the proof. $$\quad \square$$

### Remark 3.5

A rescaling and translation to the origin of Corollary 3.4 shows that if $$L<M$$ and $$\beta$$ is the degree of homogeneity for $$u_{(-M)}$$, then if $$u \in \mathcal {S}(D_L,R)$$ with $$R>2$$, then
\begin{aligned} (\sup _{B_1}|u|)R^{\beta } \le c_2 \sup _{B_R} |u|. \end{aligned}

### Lemma 3.6

Let $$u,v \in \mathcal {S}(D_{L,\infty })$$ with $$u,v \ge 0$$, then $$u = cv$$ for some constant $$c\ge 0$$.

### Proof

Consider $$w=u+v$$. Then $$w \ge u$$. Let $$c \ge 1$$ be the largest constant such that $$cu \le w$$. Then there exists a sequence $$\{x_k \} \in D_{L,\infty }$$ such that
\begin{aligned} \lim _{k \rightarrow \infty } \frac{c u(x_k)}{w(x_k)} = 1. \end{aligned}
(3.1)
We now invoke the standard boundary Harnack principle for Lipschitz domains on the nonnegative harmonic functions $$w-cu$$ and w. There exists $$C_1>0$$ such that
\begin{aligned} \sup _{B_{r_k}} \frac{w-cu}{w} \le C_1 \inf _{B_{r_k}} \frac{w-cu}{w} \le C_1 \left( 1-\frac{cu(x_k)}{w(x_k)}\right) , \end{aligned}
(3.2)
with $$r_k := \max \{2|x_k|, k\}$$. From (3.1) the right hand side of (3.2) goes to zero. Then $$w\equiv cu$$, and the result follows. $$\quad \square$$

### Lemma 3.7

Let $$u,v \in \mathcal {S}(D_{L,\infty })$$ with $$u\ge 0$$. If there exist constants $$C,R>0$$ such that
\begin{aligned} \sup _{B_r} |v| \le C\sup _{B_r} u \quad \text { for } r\ge R, \end{aligned}
then $$v = cu$$ for some $$c \in {\mathbb {R}}$$.

### Remark 3.8

The significance of Lemma 3.7 is that we do not require $$v \ge 0$$.

### Proof

Let $$v_r$$ satisfy
\begin{aligned} \begin{aligned} \Delta v_r&= 0 \quad \text { in } B_r \cap D_{L,\infty } \\ v_r&= v^+ \ \text { on } \partial (B_r \cap D_{L,\infty }). \end{aligned} \end{aligned}
By Lemma 3.3 we have that
\begin{aligned} \sup _{B_{2r}} |v| \le C\sup _{B_{r}} |v| \text { for } r \ge 1, \end{aligned}
and some constant C independent of r. Then
\begin{aligned} v_r(r/2,0,\ldots ,0) \le C \sup _{B_r} |v| \le C \sup _{B_{r/2}} |v| \le C \sup _{B_{r/2}} u \le C u(r/2,0,\ldots ,0), \end{aligned}
with the last inequality following form Lemma 3.1. By the standard boundary Harnack principle,
\begin{aligned} \sup _{B_{r/2}} \frac{v^+}{u} \le \sup _{B_{r/2}} \frac{v_r}{u} \le C \frac{v(r/2,0,\ldots ,0)}{u(r/2,0,\ldots ,0)}\le C_1. \end{aligned}
Since the constants are independent of $$r \ge 1$$, we conclude that $$v^+ \le C_1 u$$ in $$D_{L,\infty }$$. The same argument holds for $$v^-$$ so that $$|v| \le C_1 u$$ in $$D_{L,\infty }$$.

Let $$w=C_1u-v\ge 0$$. Then from Lemma 3.6 we have that $$w=cu$$ for some constant c, so that $$v=(C_1-c)u$$. $$\quad \square$$

We will need an improvement over the previous lemma.

### Lemma 3.9

Let $$u,v \in \mathcal {S}(D_{L,\infty })$$ with $$u\ge 0$$. If there exist constants $$C,R>0$$ such that
\begin{aligned} \sup _{B_r} |v| \le C(\ln (r+1))\sup _{B_r} u \quad \text { for } r\ge 1, \end{aligned}
then $$v = cu$$ for some $$c \in {\mathbb {R}}$$.

In Section 4 we give a proof of a more general result in Theorem 4.2.

### Theorem 3.10

Let $$0 \in \partial D_{L,2}$$ with $$L<M$$, and fix $$x^0 \in D_L$$. Assume further that $$B_1 \cap \{x_n > 1/4\} \subseteq D_{L,2}$$. Let $$\alpha _1$$ be the degree of homogeneity for $$u_M$$, and assume that $$2-\alpha _1+\gamma >0$$. Let $$u,v \ge 0$$ with $$u(x^0)=v(x^0)=1$$. If
\begin{aligned} -C_0 (\text {dist}(x,\partial D_{L,R} \cap B_R))^{\gamma } \le \Delta u, \Delta v \le \varepsilon (\text {dist}(x,\partial D_{L,R} \cap B_R))^{\gamma }, \end{aligned}
(3.3)
then there exists constants $$C,\varepsilon >0$$ (depending only on dimension n, $$C_0$$, Lipschitz constant M, $$M-L$$, and $$\text {dist}(x^0,\partial D_{L,2})$$) such that
\begin{aligned} C^{-1} v(x) \le u(x) \le Cv(x) \end{aligned}
(3.4)
for all $$x \in B_{1/2}$$.

### Proof

For simplicity we assume $$\Delta u=0$$ and $$\Delta v \le 0$$ in $$D_{L,2}$$ and show that $$v \le Cu$$ in $$B_{1/2}$$. Once this has been shown, the situation when u and v satisfy (3.3) is proven exactly as in Corollary 2.3. We also initially prove the theorem for a fixed $$x^0 \in {\mathcal {C}}_M \cap \partial B_{1/2}$$.

Suppose by way of contradiction that the theorem is not true. Then there exists $$u_k, v_k$$ satisfying $$\Delta u_k=0$$ and
\begin{aligned} \Delta v_k \ge -(\text {dist}(x,\partial D_{L,R} \cap B_R))^{\gamma }, \end{aligned}
with $$v_k(x^0)=u_k(x^0)=1$$ and points $$x_k \in D_{L_k,2}\cap B_{1/2}$$ such that
\begin{aligned} ku_k(x_k) < v_k(x_k). \end{aligned}
(3.5)
Harnack chains work on Lipschitz domains; therefore, from the interior Harnack inequality, by multiplying $$v_k$$ and $$u_k$$ by constants (uniformly bounded above and below), we may assume that
\begin{aligned} v_k(x_k',e_n)=u_k(x_k',e_n)=1. \end{aligned}
(3.6)
Because of the interior Harnack inequality, and by the fact that $$\varepsilon _k \rightarrow 0$$, in order for (3.5) to occur, it is necessary that dist$$(x_k, \partial D_{L_k}) \rightarrow 0$$. We let $$y_k = (x_k', e_n)$$, and similar to the proof of Theorem 2.1 we define
\begin{aligned} w_{r,k}(x) := \frac{v_k(rx)-\frac{v_k(r y_k)}{u_k(r y_k)}u_k(rx)}{ \sup _{B_1 \cap D_{L_k}} |v_k(rx)-\frac{v_k(ry_k)}{u_k(ry_k)}u_k(rx)|}, \end{aligned}
and
\begin{aligned} a_{k,m} := \sup _{B_1 \cap D_{L_k}} |v_k(2^{-m}x)-\frac{v_k(2^{-m}y_k)}{u_k(2^{-m}y_k)}u_k(2^{-m}x)| \left( \sup _{B_{2^{-m}}} u_k \right) ^{-1}. \end{aligned}
For fixed m, it follows by the standard boundary Harnack Principle that
\begin{aligned} b_m := \sup _k a_{k,m} < \infty . \end{aligned}
Just as in the proof of Theorem 2.1, by the assumption (3.5) we necessarily obtain that
\begin{aligned} \sum b_m = \infty . \end{aligned}
From Lemma A.1 there exists a subsequence $$b_{m_l}$$ such that for any fixed j we have
\begin{aligned} \limsup _{m_l \rightarrow \infty } \frac{\sum _{i=1}^j b_{m_l -i}}{b_{m_l}} \le j. \end{aligned}
For any $$N>0$$ with $$N \in \mathbb {N}$$, there exists $$\tilde{N} \in \mathbb {N}$$, such that if $$m_l\ge \tilde{N}$$, then there is a $$k=k(m_l)$$ such that $$a_{k,m_l}$$ satisfies
\begin{aligned} \frac{\sum _{i=1}^j a_{k,m_l -i}}{a_{m_l}} \le C j \text { for } j\le N. \end{aligned}
(3.7)
If we let $$r_k = 2^{-m_l}$$, then for those chosen k we have that
\begin{aligned} \sup _{B_{2^j}} |w_{r_k,k}(x)| = \frac{\sup _{B_{2^j}} |v_k(r_k x) - \frac{v_k( r_k y_k)}{u_k( r_k y_k)}u_k(r_k x)|}{ \sup _{B_1 \cap D_{L_k}} |v_k(rx)-\frac{v_k(ry_k)}{u_k(ry_k)}u_k(rx)|}, \end{aligned}
and
\begin{aligned} \begin{aligned}&\left| \frac{v_k(2^{j-i} r_k y_k)}{u_k(2^{j-i} r_k y_k)}u_k(2^{j-i-1}r_k y_k) - \frac{v_k(2^{j-i-1} r_k y_k)}{u_k(2^{j-i-1} r_k y_k)}u_k(2^{j-i-1}r_k y_k) \right| \\&\quad = \left| \frac{v_k(2^{j-i} r_k y_k)}{u_k(2^{j-i} r_k y_k)}u_k(r_k 2^{j-i-1}y_k) - v_k(2^{j-i-1} r_k y_k) \right| \\&\quad \le a_{k,m_l-(j-i)} \sup _{B_{2^{j-i} r_k}} u_k. \end{aligned} \end{aligned}
Also we have that
\begin{aligned}&\sup _{B_{2^j}} \left| \frac{v_k(2^{j-i} r_k y_k)}{u_k(2^{j-i} r_k y_k)}u_k(r_k x) - \frac{v_k(2^{j-i-1} r_k y_k)}{u_k(2^{j-i-1} r_k y_k)}u_k(r_k x) \right| \nonumber \\&\quad = \sup _{B_{2^j}} \frac{u_k(r_k x)}{u_k(2^{j-i-1} r_k y_k)}\nonumber \\&\qquad \times \left| \frac{v_k(2^{j-i} r_k y_k)}{u_k(2^{j-i} r_k y_k)}u_k(2^{j-i-1}r_k y_k) - \frac{v_k(2^{j-i-1} r_k y_k)}{u_k(2^{j-i-1} r_k y_k)}u_k(2^{j-i-1}r_k y_k) \right| \nonumber \\&\quad \le \sup _{B_{2^j}}\frac{u_k(2^j r_k x)}{u_k(2^{j-i-1} r_k y_k)} a_{m_l-(j-i)} \sup _{B_{2^{j-i} r_k}} u_k \nonumber \\&\quad \le C a_{m_l-(j-i)} \frac{u_k(2^j r_k y_k)}{u_k(2^{j-i-1} r_k y_k)} u_k(2^{j-i}r_k y_k)\nonumber \\&\quad \le C a_{m_l-(j-i)} u_k(2^j r_k y_k), \end{aligned}
(3.8)
with the last inequality following from the bounds in Lemma 3.3. Then, combining estimates (3.7) and (3.8), we obtain
\begin{aligned} \sup _{B_{2^j}} |w_{r_k,k}(x)| \le C j \frac{\sup _{B_{2^j}} u_k(r_k x)}{\sup _{B_1} u_k(r_k x)}. \end{aligned}
(3.9)
We now use Lemma 3.2 as $$r_k \rightarrow 0$$ to obtain limiting functions and domains. By choosing a subsequence we first consider the limit function
\begin{aligned} u = \lim _{r_k \rightarrow 0} \frac{u_k(r_k x)}{\sup _{B_{r_k}} u_k}. \end{aligned}
We also obtain a limiting global Lipschitz domain D on which u is the unique (up to multiplicative constant) nonnegative harmonic function that vanishes on the boundary. A further subsequence guarantees $$y_k \rightarrow y_0 \in D$$. As in the proof of Theorem 2.1, as $$r_k \rightarrow 0$$ we have that $$|\Delta w_{r_k,k}| \rightarrow 0$$. Then by picking a further subsequence, as $$r_k \rightarrow 0$$ we obtain a limiting global Lipschitz domain function w with the following properties:
\begin{aligned} \begin{aligned}&(\mathrm{i}) \quad \Delta w =0 \text { in } D \text { and } w=0 \text { on } D^c ,\\&(\mathrm{ii}) \quad \sup _{B_1} |w| =1,&\ \\&(\mathrm{iii}) \quad w(y^0) =0 , \\&(\mathrm{iv}) \quad w(x) \le C u(x) \ln (|x|+1) \ \text { for } |x| \ge 1\quad \text { from } (3.9). \end{aligned} \end{aligned}
From property $$(\mathrm{iv})$$ Lemma 3.9 guarantees $$w(x)=cu(x)$$, but then both properties $$(\mathrm{ii})$$ and $$(\mathrm{iii})$$ cannot hold since $$u(y^0)>0$$.

An interior Harnack inequality with a Harnack chain will also give the result for $$x^0 \in B_{1/2}\cap D_L$$ and the constant C depending on dist$$(x^0,\partial D_L)$$. $$\quad \square$$

### Remark 3.11

If one does not assume that $$B_1 \cap \{x_n > 1/4\} \subseteq D_L$$, then one may modify the proof at the expense that (3.4) holds for $$x \in B_r$$ with $$r \le \min \{(2L)^{-1},1/2\}$$.

To show that the quotient is not only bounded but also Hölder continuous up to the boundary, we start with the following Lemma:

### Lemma 3.12

Let D be a Lipschitz domain with small Lipschitz constant $$c \le c(n)$$ and the origin $$0 \in \partial D$$. There exists $$\varepsilon ,\beta >0$$ such that if
\begin{aligned}&|\Delta u|, |\Delta v| \le \varepsilon \quad \text { in } D \cap B_1 , \\&u=v=0 \quad \text { on } \partial D \cap B_1 , \\&u , v \ge 0 , \end{aligned}
and $$u(x^0)=v(x^0)=1$$ for some $$x^0 \in D \cap B_1$$, thus
\begin{aligned} \left\| \frac{v}{u} \right\| _{C^{0,\beta }(B_{1/2}\cap D_L)}\le C, \end{aligned}
(3.10)
where the constants $$C,\varepsilon , \beta$$ depend on n and dist$$(x^0,\partial (D \cap B_{1/2}))$$.

### Proof

We let $$C>2$$ be the largest of C from Theorem 3.10 and $$1/c_1$$ from Lemma 3.3. From Lemma 3.3 we have that
\begin{aligned} \sup _{B_r} u, v \ge \frac{r^{\alpha _1}}{C} \text { in } B_{1/2}. \end{aligned}
As the Lipschitz constant M of the domain becomes smaller, the growth exponent $$\alpha _1 \ge 1$$ becomes closer to 1. By choosing M small enough, we may assume $$\alpha _1$$ is close to 1. Then
\begin{aligned} \frac{2^{-2k}}{(1-(2C)^{-1})^k(C-C^{-1}) \sup _{B_{2^{-k}}} u} \le \frac{C 2^{-2k}}{(1-(2C)^{-1})^k(C-C^{-1}) 2^{-\alpha _1 k}} \le 2. \end{aligned}
(3.11)
We also choose $$\varepsilon$$ small enough so that $$\varepsilon 2C < \tilde{\varepsilon }$$ where $$\tilde{\varepsilon }$$ is the $$\varepsilon$$ given in Theorem 3.10. We now follow the proof of Lemma 11.8 in . We will show that there exists two sequences $$a_k,b_k$$ with $$C^{-1} \le a_k \le b_k \le C$$ such that on $$D \cap B_{2^{-k}}$$
\begin{aligned} a_k u \le v \le b_k u \quad \text { and } \quad (b_k-a_k)= \left( 1- \frac{1}{2C} \right) (b_{k-1} - a_{k-1}) . \end{aligned}
We let $$a_1 = C^{-1}$$ and $$b_1=C$$, and this base case is true by Theorem 3.10. We suppose that $$a_{k}$$ and $$b_{k}$$ have been chosen inductively. We define $$\overline{u}:=u(2^{-k}x)$$ and $$\overline{v}:=v(2^{-k} x)$$ and also define the positive functions
\begin{aligned} \begin{aligned} w_1(x)&:= \frac{\overline{v} - a_k \overline{u}}{b_k - a_k} , \\ w_2(x)&:= \frac{b_k\overline{u} - \overline{v}}{b_k - a_k}. \end{aligned} \end{aligned}
Now either $$w_1(e_n/2)>\overline{u}(e_n/2)/2$$ or $$w_2(e_n/2)>\overline{u}(e_n/2)/2$$ since $$w_1 + w_2 = \overline{u}$$. We suppose that $$w_1(e_n/2)>\overline{u}(e_n/2)/2$$. The key difference in this proof with a right hand side is to note that, by (3.11), and by choosing $$\varepsilon$$ small, we have that
\begin{aligned} \left| \frac{\Delta w_1}{\overline{u}(e_n/2)} \right| \le \varepsilon \quad \text { in } B_1, \end{aligned}
so that we also have that
\begin{aligned} \left| \frac{\Delta w_1}{w_1(e_n/2)} \right| \le 2\varepsilon \quad \text { in } B_1 . \end{aligned}
We now apply Theorem 3.10 to $$w_1/w_1(e_n/2)$$ and $$\overline{u}/\overline{u}(e_n/2)$$ to conclude that
\begin{aligned} \frac{\frac{w_1}{w_1(e_n/2)}}{\frac{\overline{u}}{\overline{u}(e_n/2)}} \ge \frac{1}{C} \text { on } B_{1/2} \cap D. \end{aligned}
Thus we also have that
\begin{aligned} \frac{1}{C} \le \frac{\frac{2w_1}{\overline{u}(e_n/2)}}{\frac{\overline{u}}{\overline{u}(e_n/2)}} = \frac{2w_1}{\overline{u}} \text { on } B_{1/2} \cap D. \end{aligned}
Renormalizing back to $$B_{2^{-(k+1)}}$$, we have that
\begin{aligned} \frac{v-a_k u}{(b_k-a_k)u} \ge \frac{1}{2C}, \end{aligned}
that is, in $$B_{2^{-(k+1)}}$$,
\begin{aligned} \left[ a_k + \frac{1}{2C} (b_k - a_k) \right] u \le v \le b_k u, \end{aligned}
so $$b_{k+1} = b_k$$ and $$\displaystyle a_{k+1} + \frac{1}{2C}(b_k-a_k)$$.

This proves the Hölder estimate of u / v up to the boundary along rays in the $$e_n$$ direction. The quotient u / v is Hölder continuous in the interior from the usual interior estimates for u and v. This concludes the proof. $$\quad \square$$

### Lemma 3.13

Let D and uv have the same assumptions as in Lemma 3.12, except we now allow that
\begin{aligned} -C_0 \le \Delta u, \Delta v \le \varepsilon \text { in } D \cap B_1. \end{aligned}
Then
\begin{aligned} \left\| \frac{v}{u} \right\| _{C^{0,\beta }(B_{1/2}\cap D_L)}\le C, \end{aligned}
where $$C,\varepsilon ,\beta$$ have the same dependence as in Lemma 3.12.

### Proof

The main point to consider is that now $$-M \le \Delta u, \Delta v \le \varepsilon$$. Since $$u,v\ge 0$$, by Theorem 3.10 both u and v are comparable to harmonic functions and so are bounded away from zero in the interior. From interior Hölder estimates the quotient u / v is Hölder continuous in the interior. If y is close to the boundary, then by rewriting it as $$y= y' + y_ne_n$$, we rescale and translate as follows:
\begin{aligned} \overline{u}:=\frac{u(y' + y_n x)}{\sup _{B_{y_n}(y',0)} u}, \qquad \overline{v}:=\frac{v(y' + y_n x)}{\sup _{B_{y_n}(y',0)} m}. \end{aligned}
From Lemma 3.3 we have that
\begin{aligned} \sup _{B_{y_n}(y',0)} u \ge c y_n^{\alpha _1}. \end{aligned}
Since $$\alpha _1 <2$$, we have, for $$y_n$$ small enough, that $$|\Delta \overline{u}|, |\Delta \overline{v}| \le \varepsilon$$. By applying Lemma 3.12 we have that $$\overline{u}/\overline{v}$$ is Hölder continuous up to the boundary. Rescaling backward we obtain that u / v is Hölder continuous up to the boundary. $$\quad \square$$

For the application in Section 1.4.2 we actually need to consider the quotient v / u where v is not required to have a sign and $$|\Delta v| \le M$$. This is given in Theorem 1.1. We will need a decay rate for v near points $$x \in \partial D \cap \partial \{v>0\} \cap \partial \{v<0\}$$.

### Lemma 3.14

Let $$\varepsilon$$ be as in Theorem 1.1 and $$D_L$$ as in Theorem 1.1. Let u satisfy
\begin{aligned} \begin{aligned} -C_0&\le \Delta u \le \varepsilon \text { in } D_L ,\\ u&=0 \text { on } \partial D_L , \\ u&\ge 0 \text { in } D_L ,\\ u(e_n/2)&= 1. \end{aligned} \end{aligned}
Let v satisfy
\begin{aligned} \begin{aligned} |\Delta v|&\le C_0 \text { in } D_L , \\ v&=0 \text { on } \partial D_L , \\ |v|&\le 1 \text { in } D_L, \end{aligned} \end{aligned}
with $$0 \in \partial D \cap \partial \{v>0\} \cap \partial \{v<0\}$$. Then there exists $$C, \delta _0 >0$$ depending on $$n,C_0$$ such that
\begin{aligned} \sup _{B_r} |v| \le C \sup _{B_r} r^{\delta _0} u \text { for all } r \le 1/4. \end{aligned}

### Proof

Suppose by way of contradiction that the Lemma is not true. Then there exists sequences $$u_k,v_k$$ satisfying the assumptions of the Lemma and points $$x_k \in D_{L_k} \cap B_{1/4}$$ and $$\delta _k \rightarrow 0$$ such that
\begin{aligned} |v_k(x_k)| \ge k |x_k|^{\delta _k} u_k(x_k). \end{aligned}
(3.12)
By Theorem 3.10 we may bound the quotient $$v_k^{\pm }/u$$ uniformly on $$B_{1/4}$$, so it necessarily follows that $$|x_k| \rightarrow 0$$. We let $$r_k := |x_k|$$. Furthermore, we may choose $$x_k$$ such that
\begin{aligned} |v_k(x)| \le 2k |x|^{\delta _k} u_k(x) \text { in } B_{1/2} \setminus B_{r_k}, \end{aligned}
(3.13)
otherwise we simply choose new points in $$B_{1/4} \setminus B_{r_k}$$ satisfying (3.12). We rescale by letting
\begin{aligned} \overline{u}_k(x) := \frac{u_k(r_kx)}{\sup _{B_{r_k}} u} \qquad \overline{v}_k(x) := \frac{v_k(r_kx)}{\sup _{B_{r_k}} |v|}. \end{aligned}
Then $$\overline{u}_k \rightarrow u_0$$ uniformly on compact sets with $$\displaystyle \sup _{B_1 } u_0 =1$$. By (3.12) and (3.13) we have that
\begin{aligned} \begin{aligned} \overline{v}_k(x)&= \frac{v_k(r_kx)}{\sup _{B_{r_k}} |v|} \le \frac{2kr_k^{\delta _k} |x|^{\delta _k} u_k(x)}{\sup _{B_{r_k}} |v|} \\&\le \frac{2kr_k^{\delta _k} |x|^{\delta _k} u_k(x)}{k r_k^{\delta _k} \sup _{B_{r_k}} u} = 2 |x|^{\delta _k} \overline{u}_k. \end{aligned} \end{aligned}
Then $$\overline{v}_k \rightarrow v_0$$ uniformly on compact sets. Since $$D_{L_k}$$ have small Lipschitz constant we also have that in the limit $$\Delta u_0 = \Delta v_0 =0$$ in the limiting Lipschitz domain $$D_0$$. From Lemma 3.7 or Lemma 3.9 we have that $$u_0 = v_0$$. Hence $$(\overline{v}_k)^- \rightarrow 0$$ uniformly. We choose k large enough so that $$|\Delta \overline{u}_k|, |\Delta \overline{u}_k|\le \eta$$. We let $$w_k^1$$ satisfy
\begin{aligned} \begin{aligned} \Delta w_k^1&=- \eta \text { in } B_1 \cap \{\overline{u}_k>0\} , \\ w_k^1&= \overline{v}_k^- \text { on } \partial (B_1 \cap \{\overline{u}_k >0\}), \end{aligned} \end{aligned}
$$w_k^2$$ satisfy
\begin{aligned} \begin{aligned} \Delta w_k^2&= 0 \text { in } B_1 \cap \{\overline{u}_k>0\} ,\\ w_k^2&= \overline{v}_k^- \text { on } \partial (B_1 \cap \{\overline{u}_k >0\}) , \end{aligned} \end{aligned}
and $$w_k^3$$ satisfy
\begin{aligned} \begin{aligned} \Delta w_k^3&= \eta \text { in } B_1 \cap \{\overline{u}_k>0\} , \\ w_k^3&= \overline{v}_k^+ \text { on } \partial (B_1 \cap \{\overline{u}_k >0\}). \end{aligned} \end{aligned}
For $$\eta$$ chosen small enough, we have that $$w_k^3 >0$$ in $$\{\overline{u}_k >0\}$$. This is a consequence of the analogue of Corollary 2.4 for Theorem 3.10. Now $$w_k^1(e_n/2)$$ is comparable to $$\eta$$ with a constant depending only on n and the Lipschitz constant of the domain. We have chosen $$w_k^1,w_k^2$$ so that by normalizing by a constant we may apply Theorem 3.10 and conclude that
\begin{aligned} \frac{w_k^1}{w_k^3} \le C w_k^1(e_n/2) \qquad \text {and} \qquad \frac{w_k^2}{w_k^3} \le C w_k^2(e_n/2) \qquad \hbox {in } B_{1/4}. \end{aligned}
Then, for k large enough, we have that $$w_k^3 - w_k^1 - w_k^2 >0$$ in $$B_{1/4}$$, but we also have that $$v_k \ge w_k^3 - w_k^1 - w_k^2$$. Hence $$0 \notin \partial \{v_k<0\}$$, and this is a contradiction.

Now we give the proof of Theorem 1.1.

### Proof of Theorem 1.1

From Lemma 3.14 we have a Hölder growth rate whenever $$x^0 \in \partial D \cap \partial \{v>0\} \cap \partial \{v<0\}$$. We now assume that $$x^0 \in \partial D$$ but $$x^0 \notin \partial \{v<0\}$$, and without loss of generality we set $$x^0=0$$. Then $$v>0$$ in $$D \cap B_r$$ for r small. Suppose that there exists infinitely many $$r_k \rightarrow 0$$ such that
\begin{aligned} \frac{v(r_k e_n)}{u(r_k e_n)} > r_k^{1/2}. \end{aligned}
By Theorem 3.10 the function u is comparable to a harmonic function, and so we may apply Lemma 3.3 to u. Furthermore, since the Lipschitz constant for D is small, the constant $$\alpha _1$$ in Lemma 3.3 is close to 1; therefore, we may conclude that
\begin{aligned} \sup _{B_r} u \ge c r^{3/4}, \end{aligned}
in a neighborhood of the origin. When rescaling by $$v_r = u(rx)$$ we have $$\Delta v_r = r^2 \Delta v(rx)$$, so that
\begin{aligned} \frac{\Delta v_{r_k}(x)}{v_{r_k}(e_n)} = \frac{r_k^2 \Delta v(r_k x)}{v_{r_k}(e_n)} \le \frac{r_k^{3/2} \Delta v(r_k x)}{u(r_k e_n)} \le \frac{C_0}{c} r_k^{3/4}. \end{aligned}
Therefore, for $$r_k$$ small enough we may apply Theorem 1.1 to $$\displaystyle v_{r_k}/ v_{r_k} (r_k e_n)$$ and $$u_{r_k}/ u(r_k e_n)$$ and rescaling back we obtain that v / u has a Hölder growth rate in the $$e_n$$ direction away from the origin. When $$0 \notin \partial \{v>0\}$$, we simply apply the previous argument to $$-v$$. Now combined with Lemma 3.14 and interior estimates we have a Hölder continuity estimate at every point including those at the boundary. In order to make the estimate uniform across any domain $$D_L$$ with $$L \le M$$, we apply a compactness argument. $$\quad \square$$

## 4 Second-Order Elliptic Operators

The techniques employed in Section 3 can be applied to other elliptic operators, and in this section we extend the results of Section 3 to second order linear elliptic operators in divergence form on Lipschitz domains. Specifically, we consider operators of the form
\begin{aligned} \mathcal {L} u = (a^{ij}u_i)_j + b^i u_i + cu . \end{aligned}
We assume the following ellipticity conditions:
\begin{aligned} \Lambda ^{-1} |\xi |^2 \le \langle a^{ij}(x) \xi , \xi \rangle \le \Lambda |\xi |^2, \end{aligned}
for some $$\Lambda >0$$ and for all nonzero $$\xi \in {\mathbb {R}}^n$$. Furthermore, $$a^{ij}(x)$$ is a real $$n \times n$$ matrix. For the lower order terms we assume $$|c(x)|, \sum |b^i(x)| \le \Lambda -1$$ and that $$c(x) \le 0$$.
We will continue with the notation of Section 3, however, for now, we write $$u \in \mathcal {S_{\mathcal {L}}}(D_{L,R})$$ if
\begin{aligned} \begin{aligned} \mathcal {L} u(x)&=0 \text { in } D_{L,R} \cap B_R ,\\ u(x)&=0 \text { on } D_{L,R}^c\cap B_R, \end{aligned} \end{aligned}
and that $$u \in \mathcal {S_{\mathcal {L}}}(D_{L,R},d^{\gamma })$$ if
\begin{aligned} \begin{aligned} |\mathcal {L} u(x)|&\le (\text {dist}(x,\partial D_{L,R} \cap B_R))^{\gamma } \ \text { in } D_{L,R} , \\ u(x)&=0 \ \text { on } D_{L,R}^c\cap B_R. \end{aligned} \end{aligned}
To apply the Hölder continuity estimates for elliptic operators we will require that
\begin{aligned} \gamma >-2/n ; \end{aligned}
see Theorem 8.27 in . Since the boundary is Lipschitz, this will ensure the correct integrability assumptions for the right hand side. We will assume these bounds throughout the section whenever referencing $$\mathcal {S_{\mathcal {L}}}(D_{L,R},d^{\gamma })$$.

From the forthcoming Lemma 4.1, it will follow that if $$u \ge 0$$ and $$u \in \mathcal {S_{\mathcal {L}}}({\mathcal {C}}_L,\infty )$$, then u is unique up to multiplicative constant and we again denote u by $$u_L$$; however, $$u_L$$ will not necessarily be homogeneous. We recall that $${\mathcal {C}}_L$$ is defined although not convex when $$L<0$$. To emphasize when $$-L<0$$, we again write $${\mathcal {C}}_{(-L)}$$ and $$u_{(-L)}$$ when $$u \in \mathcal {S_{\mathcal {L}}}({\mathcal {C}}_{(-L)})$$. We will follow the same outline as in Section 3.

In Section 3 we utilized the standard boundary Harnack principle. Since the standard boundary Harnack principle is unavailable when considering the zero-order term c(x), we prove the next two Lemmas under the situation $$b^i, c \equiv 0$$.

### Lemma 4.1

Let $$u,v \in \mathcal {S}_{\mathcal {L}(D_{L,\infty })}$$ with $$u \ge 0$$. Assume also that $$b^i, c \equiv 0$$. If there exists $$C>0$$ such that
\begin{aligned} \sup _{B_R} |v| \le C \sup _{B_R} u \text { for } R \ge 1, \end{aligned}
then there exists $$c \in \mathbb {R}$$ such that $$v \equiv cu$$.

### Proof

When $$b^i, c \equiv 0$$, there is a standard Boundary Harnack principle for divergence form equations ; therefore, the proof of Lemma 3.6 holds in this situation, and so the proof of Lemma 3.7 also holds as well. $$\quad \square$$

### Theorem 4.2

Assume $$\mathcal {L}$$ has no lower order terms; that is, $$\mathcal {L}w = \partial _j(a^{ij} u_i)$$. Let $$v,u \in \mathcal {S}_{\mathcal {L}}(D_{L,\infty })$$ with $$u \ge 0$$, and assume $$b^i, c \equiv 0$$. If there exists $$C>0$$ such that
\begin{aligned} |v(x)| \le C\ln (|x|+1) u(x) \text { for } |x| \ge 1, \end{aligned}
then $$v(x)=cu(x)$$ for some $$c \in \mathbb {R}$$.

### Remark 4.3

The proof given below for Theorem 4.2 depends on the function g being slowly varying at $$\infty$$. Thus, the same proof will actually show a stronger result: If for every $$\varepsilon >0$$ there exists $$C_{\varepsilon }$$ such that
\begin{aligned} |v(x)|\le C_{\varepsilon } |x|^{\varepsilon }u(x) \text { for } |x| \ge 1, \end{aligned}
then $$v=cu$$ for some $$c \in \mathbb {R}$$.

### Proof

Suppose by way of contradiction that v is not a constant multiple of u. Then by Lemma 4.1 we have
\begin{aligned} \limsup _{R \rightarrow \infty } \left( \sup _{B_R} \frac{|v(x)|}{u(x)} \right) = \infty . \end{aligned}
If $$h(R)=\sup _{B_R} |v|/u$$, let g be the concave envelope of h. By assumption $$g(R) \le C \ln (R+1)$$ for $$R \ge 1$$. The function g satisfies,
\begin{aligned} \lim _{R \rightarrow \infty } \frac{g(CR)}{g(R)}=1 \text { for any } C>0. \end{aligned}
(4.1)
There also exist infinitely many $$R_k$$ such that $$h(R_k) = g(R_k)$$. We define
\begin{aligned} u_k(x):=\frac{u(R_k x)}{\sup _{B_{R_k}} u} \ \text { and } \ v_k(x)=\frac{v(R_k x)}{\sup _{B_{R_k}} |v|}. \end{aligned}
From (4.1) we have that for any fixed $$\rho >1$$, that
\begin{aligned} \lim _{R_k \rightarrow \infty } \frac{\sup _{B_{\rho }} |v|}{ \sup _{B_{\rho }} u} \le 1. \end{aligned}
(4.2)
By uniform continuity estimates up to the boundary for divergence form equations, by picking a subsequence we have that
\begin{aligned} \lim _{R_k \rightarrow \infty } u_k(x) = w_1, \end{aligned}
and that $$u_k$$ converges uniformly to $$w_1$$ on compact sets. From (4.2) we also have that
\begin{aligned} \lim _{R_k \rightarrow \infty } v_k(x)= w_2, \end{aligned}
with uniform convergence on compact sets and with $$|w_2| \le C w_1$$. There also exists a limiting operator $$\mathcal {L}_0$$ and limiting Lipschitz domain $$\tilde{D}$$ such that $$w_1, w_2 \in \mathcal {S}_{\mathcal {L}_0}(\tilde{D}_{L, \infty })$$. Then from Lemma 4.1 we conclude that $$w_2 = c w_1$$ for some $$c \in \mathbb {R}$$. Without loss of generality we assume $$c=1$$.
Then for any $$\varepsilon >0$$, there exists $$N_{\varepsilon } \in \mathbb {N}$$ such that if $$k \ge N_{\varepsilon }$$, then
\begin{aligned} \sup _{B_2} |v_k - u_k| < \varepsilon . \end{aligned}
By the standard boundary Harnack principle
\begin{aligned} \sup _{B_1} \frac{|v_k - u_k|}{u_k} \le C \frac{\Vert v_k - u_k \Vert _{L^{\infty }(B_2)}}{u_k(e_n/2)} \le C \varepsilon . \end{aligned}
We fix $$x^1 \in D_{L,\infty }$$. We also have
\begin{aligned} \lim _{R_k \rightarrow \infty } \frac{|v_k(R_k^{-1}x^1)|}{|u_k(R_k^{-1} x^1)|} \le \frac{v(x^1)}{u(x^1)}\frac{1}{g(R_k)} \rightarrow 0. \end{aligned}
Then for large enough k we have $$|v_k(R_k^{-1} x^1)|\le u_k(R_k^{-1} x^1)/2$$. Finally, we conclude then that
\begin{aligned} \frac{u(x^1)/2}{u(x^1)} \le \sup _{B_1} \frac{|v_k - u_k|}{u_k} \le C \varepsilon . \end{aligned}
The C in the above estimate only depends on the ellipticity constants of $$a^{ij}$$ and the Lipschitz constant for the domain. Consequently, we may choose $$\varepsilon$$ small enough so that $$2C \varepsilon <1$$, which implies $$u(x^1)=0$$ which is a contradiction since $$u>0$$ in $$D_{L,\infty }$$. $$\quad \square$$

For the remainder of the section we no longer assume that the lower order terms are zero.

### Lemma 4.4

Let $$L \le M$$ and $$u \in \mathcal {S_{\mathcal {L}}}(D_L, d^{\gamma })$$ with $$u \ge 0$$ and $$\mathcal {L} u \le 0$$. Assume also $$0 \in \partial D_L$$. Let $$x \in \partial D_L \cap B_{1/2}$$ and let $$y \in D_L \cap B_r(x)$$ with $$r \le 1/4$$. Then there exists a constant C depending only on dimension n, M, and $$\text {dist}(y, \partial D_L)$$ such that
\begin{aligned} \begin{aligned}&\sup _{B_r(x)} u \le C u(y)&\text { for all } r\le 1/4, \\&\sup _{B_{1/4}} u \ge C^{-1} u(y). \end{aligned} \end{aligned}

### Proof

Since $$u \ge 0$$ and $$\mathcal {L} u \le 0$$ and $$u \in \mathcal {S_{\mathcal {L}}}(D_{L,R},d^{\gamma })$$, this is an application of the interior weak Harnack inequality as well as uniform Hölder continuity up to the boundary, see . $$\quad \square$$

We now state the analogue of Lemma 3.2.

### Lemma 4.5

Let $$D_{L_k,R_k}$$ be a sequence of domains with $$L_k \le M$$, $$R_k \ge 1$$, and $$0 \in \partial D_{L_k}$$. Let $$u_k \in \mathcal {S_{\mathcal {L}}}(D_{L_k,R_k}, d^{\gamma })$$, and assume $$\gamma >-2/n$$. Further, assume either that
\begin{aligned} \begin{aligned}&(1) \qquad u_k \ge 0 \text { and } \sup _{B_{1/2}} u_k \le 1, \text { or } \\&(2)\qquad \sup _{B_r} |u_k| \le C r^{\beta } \text { for } r\le 1 \text { and some constants } C, \beta >0. \end{aligned} \end{aligned}
Then there exists a subsequence with a limiting domain $$D_{L_0,R_0}$$ and a limiting function $$u_0 \in \mathcal {S}(D_{L_0,R_0},d^{\gamma })$$ such that
\begin{aligned} \sup _{B_r} |u_k - u_0| \rightarrow 0 \end{aligned}
for all $$r<R_0$$.

### Proof

This is an application of uniform Hölder continuity up to the boundary, see . $$\quad \square$$

### Lemma 4.6

Let $$u\in \mathcal {S}_{\mathcal {L}}(D_L)$$ with $$u\ge 0$$ and $$\mathcal {L} u \le 0$$. Let $$L<M$$. There exist constants $$c_1,c_2, \beta ,\alpha$$ depending only on $$n,M,\Lambda$$ and $$M-L$$ such that for any $$x \in \partial D_L \cap B_{1/2}$$,
\begin{aligned} \begin{aligned}&(1) \qquad \sup _{B_{r}(x)} u \ge c_1 u(e_n/2) r^{\alpha } , \\&(2) \qquad \sup _{B_{r}(x)} u \le c_2 u(e_n/2) r^{\beta }, \end{aligned} \end{aligned}
for any $$r \le 1/4$$.

### Proof

Property (2) is just uniform Hölder continuity up to the boundary. Assume by way of contradiction that (1) is not true. Then there exists a sequence satisfying
\begin{aligned} \begin{aligned} (1)&\qquad u_k \in \mathcal {S}_{\mathcal {L}_k}(D_{L_k}, d^{\gamma }) \\ (2)&\qquad u_k \ge 0 \\ (3)&\qquad \mathcal {L}_k u_k \le 0 \\ (4)&\qquad u_k(e_n/4) \le \frac{u_k(e_n/2)}{k} \quad \text { from Lemma }~4.4. \end{aligned} \end{aligned}
We rescale and let
\begin{aligned} w_k = \frac{u_k(r_k x)}{ \sup _{B_{r_k}} u_k}. \end{aligned}
From Lemma 4.5 we have that $$w_k \rightarrow w_0$$ uniformly and there is a limiting Lipschitz domain $$D_{L_0}$$ and limiting elliptic operator $$\mathcal {L}_0$$ such that $$u \in \mathcal {S}_{\mathcal {L}_0}(D_{L_0})$$. Now $$w_0 \ge 0$$, and from the definition of $$w_k$$ we conclude that $$w_0$$ is not identically zero. However, $$w_0(e_n/4)=0$$, which contradicts the strong maximum principle. $$\quad \square$$

With the previous result, the proof of Theorem 4.7 proceeds exactly as in the case of Theorem 3.10.

### Theorem 4.7

Let $$0 \in \partial D_L$$ with $$L<M$$, and fix $$x^0 \in D_L$$. Assume further that $$B_1 \cap \{x_n > 1/4\} \subseteq D_L$$. Let $$\gamma >-2/n$$ and let $$\alpha$$ be as in Lemma 4.6. Assume $$u,v \ge 0$$ and $$u(x^0)=v(x^0)=1$$, and also assume that $$2-\alpha +\gamma >0$$ with $$\alpha$$ as given in Lemma 4.6. Then there exists a uniform constants $$C,\varepsilon >0$$ (depending only on dimension n, Lipschitz constant M, $$M-L$$, and dist$$(x^0,\partial D_L)$$) such that if
\begin{aligned} -(\text {dist}(x,\partial (D \cap B_1)))^{\gamma } \le \mathcal {L} u , \mathcal {L} v \le \varepsilon (\text {dist}(x,\partial (D \cap B_1)))^{\gamma } \end{aligned}
then
\begin{aligned} C^{-1} v(x) \le u(x) \le Cv(x) , \end{aligned}
(4.3)
for all $$x \in B_{1/2}$$.

### Proof

The proof proceeds exactly as the proof of Theorem 3.10. We only highlight how the lower order terms vanish in the blow-up regime. The rescaled functions
\begin{aligned} w_{r,k}(x) := \frac{v_k(rx)-\frac{v_k(r y_k)}{u_k(r y_k)}u_k(rx)}{ \sup _{B_1 \cap \mathcal {C}} |v_k(rx)-\frac{v_k(ry_k)}{u_k(ry_k)}u_k(rx)|}, \end{aligned}
satisfy
\begin{aligned} \mathcal {L}_r w_{r,k} = \frac{r^2\mathcal {L} v_k(rx)}{ \sup _{B_1 \cap \mathcal {C}} |v_k(rx)-\frac{v_k(ry_k)}{u_k(ry_k)}u_k(rx)|}, \end{aligned}
(4.4)
where for a function f we have
\begin{aligned} \mathcal {L}_r f = (a^{ij}(rx)f_i)_j + rb^{i}(rx)f_i + r^2c(rx)f. \end{aligned}
Thus, in the blow-up regime the lower order terms disappear. As in the proof of Theorems 2.1 and  3.10 we may bound the denominator in (4.4) from below by $$r_k^{\alpha } [\ln (1/r_k)]^2$$ for the constructed sequence of $$r_k \rightarrow 0$$. Using that the numerator is bounded from above by $$r_k^{2-\gamma }$$, we have that in the blow-up regime the right hand side and lower order terms vanish. We then apply Lemma 4.1 and Theorem 4.2 as in the proof of Theorem 3.10. $$\quad \square$$

## Footnotes

1. 1.

The boundary Harnack Principle holds in very general domains, such as NTA domains, and uniform domains. It also holds for solutions to a large class of elliptic equations.

2. 2.

One can actually prove the failure of boundary Harnack between harmonic and super-harmonic functions, in the first quadrant. This is illustrated in Example 1.2 in , in terms of free boundary problems.

3. 3.

This was done for constant h in  using the standard boundary Harnak principle for Lipschitz domains.

4. 4.

Actually this conclusion is part of proving the Lipschitz regularity of the free boundary; see 

5. 5.

The level surface is smooth since $$v_{e_1} > 0$$ there.

6. 6.

See for example .

7. 7.

The assumption that $$\partial {\mathcal {C}}\cap \mathbb {S}^{n-1}$$ is an $$(n-2)$$-dimensional manifold of class $$C^{1,\alpha }$$ is not necessary. As we will see in Section 3, $$\partial {\mathcal {C}}\cap \mathbb {S}^{n-1}$$ may be a Lipshitz manifold provided the Lipschitz constant is small enough depending on $$\gamma$$, that appears in (2.2).

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