The first and second expansion of large solutions for quasilinear elliptic equations with weight functions

Yun-Feng Ma; Zhong Bo Fang

doi:10.1186/s13661-015-0498-y

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The first and second expansion of large solutions for quasilinear elliptic equations with weight functions

Yun-Feng Ma¹ and
Zhong Bo Fang²Email author

Boundary Value Problems20152015:234

https://doi.org/10.1186/s13661-015-0498-y

Received: 29 July 2015

Accepted: 26 November 2015

Published: 10 December 2015

Abstract

By the Karamata regular variation theory and comparison principle, we establish the boundary behavior of positive weak solutions for the problem

$$\Delta_{p}u=b(x)f(u), \quad x\in\Omega, \qquad u|_{\partial\Omega}= \infty, $$

where Ω is a bounded domain with smooth boundary in $R^{N}$, the weight $b(x)\in C^{\alpha}(\overline{\Omega})$, which may be vanishing on the boundary and rapidly varying near the boundary, and the nonlinearity f may be rapidly varying at infinity. For the case $f(s)=s^{m}\pm f_{1}(s)$ with sufficiently large s, where $m>p-1$ and $f_{1}$ is normalized regularly varying at infinity with index $m_{1}\in(0,p-1)$, we show the influence of the geometry of Ω on the boundary behavior of solutions. Finally, we prove the existence and uniqueness of the solution for the problem.

Keywords

quasilinear elliptic equation large solution blow-up rate first and second expansion

MSC

35B40 35H30 35J70 35J65

1 Introduction and main results

In this paper, we consider the first and second expansions of positive weak large solutions near the boundary for the quasilinear elliptic problem of the form

$$ \Delta_{p}u=b(x)f(u),\quad x\in\Omega, \qquad u|_{\partial\Omega }= \infty, $$

(1.1)

where $\Delta_{p}u=\operatorname{div}(|\nabla u|^{p-2}\nabla u)$ ($p>2$), $\Omega\subset R^{N}$ ($N\geq2$) is a bounded domain with $C^{4}$-smooth boundary, $b(x)$ satisfies (b₁) and (b₂), and f satisfies (f₁), (f₂), and (f₃), where

(b₁):: $b(x)\in C^{\alpha}(\overline{\Omega})$ for some $\alpha\in(0,1)$, and $b(x)$ is positive in Ω;

(b₂):: there exist $k\in\Lambda$ and $b_{0}\in R$ such that
$$\lim_{d(x)\rightarrow0}\frac{b(x)}{K^{p-2}(d(x))k^{p}(d(x))}=b_{0}, $$
where Λ denotes the set of all positive nondecreasing functions in $C^{1}(0,\delta_{0})$ ($\delta_{0}>0$) such that
$$\lim_{t\rightarrow 0+}\frac{d}{dt}\biggl(\frac{K(t)}{k(t)} \biggr):=C_{k}\in[0,\infty), \quad K(t)= \int^{t}_{0}k(s)\, ds; $$

(f₁):: $f\in C^{1}[0,\infty)$, $f(0)=0$, f is increasing in $(0,\infty)$;

(f₂):: $\int^{\infty}_{1}f^{-\frac{1}{p-1}}(v)\, dv<\infty$;

(f₃):: there exists $C_{f}>0$ such that $\lim_{s\rightarrow\infty}f'(s)\int^{\infty}_{s}\frac{dv}{f(v)}=C_{f}$.

Note that, some basic examples for $k\in\Lambda$ can be given as follows:

(1)

$k(t)=t^{\frac{\alpha}{2}}$, $\alpha>0$, $C_{k}=2(2+\alpha)^{-1}$;
(2)

$k(t)=e^{-t^{-\alpha}}$, $\alpha>0$, $C_{k}=0$;
(3)

$k(t)=\frac{1}{(-\ln t)^{\alpha}}$, $\alpha>0$, $C_{k}=1$;
(4)

$k(t)=e^{-e^{t^{-\alpha}}}$, $\alpha>0$, $C_{k}=0$;
(5)

$k(t)=(\ln(1+t))^{\alpha}$, $\alpha>0$, $C_{k}=(1+\alpha)^{-1}$.

p-Laplacian equations like (1.1) usually occur in the study of the generalized reaction-diffusion theory, non-Newtonian fluid theory, non-Newtonian filtration, and the turbulent flow of a gas in porous medium. In the non-Newtonian theory, the quantity p is a characteristic of the medium. Media with $p>2$ are called dilatant fluids, and those with $p<2$ are called pseudoplastics. If $p=2$, then they are Newtonian fluids. The p-Laplacian operator also appears in the study of torsional creep (elastic for $p=2 $ and plastic for $p<2$; see [1]), flow through porous media ($p=\frac{3}{2}$; see [2]), and glacial sliding ($p\in(1,\frac{3}{4}]$; see [3]).

We are concerned with the positive weak large solutions for problem (1.1). By a solution for problem (1.1) we understand a function $u\in W^{1,p}_{\mathrm{loc}}(\Omega)\cap L^{\infty}_{\mathrm{loc}}(\Omega)$ that satisfies $\Delta_{p}u=b(x)f(u)$ in the weak sense and $u(x)\rightarrow\infty$ as $d(x)=\operatorname{dist}(x,\partial\Omega)\rightarrow 0$. Sometimes, the solution is also called a large solution, an explosive solution, or a boundary blow-up solution.

The study of large solutions started from the work of Bieberbach [4] for the case $b(x)=1$, $f(u)=e^{u}$, $p=2$, and $N=2$, which plays an important role in the theories of Riemannian surfaces of negative constant curvatures and automorphic functions. More exactly, if a Riemannian metric of the form $|ds|^{2}=e^{2u(x)}|dx|^{2}$ has a constant Gaussian curvature $-b^{2}$, then $\Delta u=b^{2}e^{2u}$. Rademacher [5] extended the results in [4] to the three-dimensional space. Later, C Bandle et al. discussed the existence, uniqueness, and accurate estimate of boundary behavior of large solutions for problem (1.1) with $p=2$ and $b(x)$, $f(u)$ satisfying some proper conditions and obtained some better results dealing with a gradient term (see [4–40] and the references therein). Also, some results in [4–40] have been extended to $p>2$ (see [41–54]). Recently, boundary blow-up problems have been applied to Liouville theorems for logistic-like equations in $R^{N}$ in [13], the analysis of blow-up for a parabolic equation with a nonlinear boundary condition in [14], and the characterization of the long-time behavior of positive solutions for the parabolic equations in [15, 16].

However, Cirstea and Rădulescu [17] first introduced Karamata regular variation theory approaching to study the uniqueness and asymptotic behavior of boundary blow-up solutions, which enables us to obtain some qualitative behavior of the boundary blow-up solutions in a general framework. The asymptotic behavior of the boundary blow-up solutions near the boundary has been investigated by many researchers (see [17–39] and their references). It is well known that the first-order asymptotic expansion of the solution $u(x)$ in terms of $d(x)$ is independent of the geometry of the domain, whereas the second-order asymptotic expansion of the solution $u(x)$ depends linearly on the mean curvature of the boundary of Ω. There have been many results about the first expansion of large solution for problem (1.1) with $p=2$ and $b(x)$, $f(u)$ satisfying some proper conditions under different regularity boundary conditions (see [21–28]) and the second expansion (see[29–34] and references therein). Bandle and Marcus [29] first studied the influence of the geometry of Ω on the boundary behavior of the unique radially symmetric solution for problem (1.1) in a ball or an annulus when $f(u)$ is of power form. Their results were extended by Bandle, Anedda, Porru et al. to more general boundary smooth domains, weights, and nonlinearities (see [30–34]). Specially, Cirstea et al. [17, 35–40] used the Karamata regular variation theory, nonlinear transformations, the perturbed method, the upper and lower solution method, and localization method to establish the first and second expansion of large solutions for problem (1.1) with $p=2$, and Cirstea and Rădulescu [17] first introduced the set Λ. Recently, some results in [17, 35–40] have been extended to $p>2$. For instance, Huang et al. [46–48] studied the existence and the first and second expansions of weak solutions when $b(x)$ and $f(u)$ satisfy some suitable conditions, which are different from the conditions in our paper. For more results about the p-Laplacian equations, we refer to [49–53] and references therein.

Inspired by the above works, in this paper, we introduce the constants $C_{f}$ and $C_{k}$ to get the asymptotic expansion of solutions for problem (1.1). In particular, when $b(x)=K^{p-2}(d(x))k(d(x))$ near the boundary and $f(s)=s^{m}\pm f_{1}(s)$ for sufficiently large s, where $m>p-1$, and $f_{1}$ satisfies

(f₄):: there exists $m_{1}\in(0,p-1)$ such that
$$\lim_{s\rightarrow\infty}\frac{sf'_{1}(s)}{f_{1}(s)}=m_{1}, $$

we show the influence of the geometry of Ω on the boundary behavior of solutions for problem (1.1). Finally, we prove the existence and uniqueness of the solution for problem (1.1). More precisely, we obtain the following results.

Theorem 1

Let f satisfy (f₁)-(f₃), and b satisfy (b₁)-(b₂). Suppose that $1< C_{f}<\frac{p-1}{p-2}$ in (f₃) and

$$ 2C_{f}+C_{k}>2+\frac{p-2}{p-1}C_{f}C_{k}. $$

(1.2)

Then, for any solution u of problem (1.1), we have

$$ \lim_{d(x)\rightarrow0}\frac{u(x)}{\phi(\gamma K^{2}(d(x)))}=1, $$

(1.3)

where ϕ is uniquely defined by

$$ \int^{\infty}_{\phi(t)}f^{-\frac{1}{p-1}}(\mu)\, d\mu=t, \quad \forall t>0 $$

(1.4)

and

$$ \gamma=\frac{1}{2} \biggl(\frac{b_{0}}{p-1}\cdot \frac{(p-1)(C_{f}-1)-C_{f}}{(2-C_{k})(p-1)(C_{f}-1)-C_{f}C_{k}} \biggr)^{\frac{1}{p-1}}. $$

(1.5)

Remark 1

By (1.2) one can see that if $C_{f}>1$, then $C_{k}$ can be equal to zero and if $C_{k}>0$, then $C_{f}$ can be equal to 1.

Theorem 2

Let f satisfy (f₁), $f(s)=s^{m}\pm f_{1}(s)$ for sufficiently large s, $m>p-1$, $f_{1}$ satisfy (f₄), and $b(x)=K^{p-2}(d(x))k(d(x))$ near the boundary, where k satisfies

(k₁):: $k\in C[0,a]\cap C^{2}(0,a]$ for some $a>0$, $k(t)>0$, $k'(t)>0$, $\forall t\in(0,a]$, and $k(0)=0$;

(k₂):: $k\in\Lambda$ with $C_{k}>0$;

(k₃):: $\lim_{t\rightarrow0}\frac{d^{2}}{dt^{2}}(\frac {K(t)}{k(t)})=0$.

The following two results hold:

(1)

if $m+1-p>2m_{1}$, then, in a sufficiently small neighborhood of ∂Ω, for any solution u of problem (1.1), we have
$$ u(x)=C_{1}\bigl(K\bigl(d(x)\bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \biggl(1+C_{2}(N-1)H(\overline {x})\frac{K(d(x))}{k(d(x))}+o\bigl(d(x)\bigr) \biggr), $$

(1.6)
where
$$\begin{aligned}& C_{1}= \biggl( \biggl(\frac{2(p-1)}{m+1-p} \biggr)^{p} \biggl(p-1+\frac {(m+1-p)C_{k}}{2} \biggr) \biggr)^{\frac{1}{m+1-p}}, \\& C_{2}=\frac{m+1-p}{2(p-1)(m-1)+(m+1)(m+1-p)C_{k}}. \end{aligned}$$
(2)

if $m+1-p\leq2m_{1}$ and $k(t)=t^{\frac{\theta}{2}}$ with $\theta>0$ such that $\frac{\theta}{2+\theta}>\frac{2m_{1}-(m+p-1)}{m+1-p}$, then (1) still holds.

Remark 2

Some basic examples of k that satisfy (k₁)-(k₃) can be given as follows:

(1)

$k(t)=t^{\frac{\alpha}{2}}$, $\alpha>0$, where $C_{k}=\frac{2}{2+\alpha}$;
(2)

$k(t)=e^{t^{\alpha}}-1$, $\alpha>1$, where $C_{k}=\frac{1}{1+\alpha}$;
(3)

$k(t)=\ln(1+t^{\alpha})$, $\alpha>1$, where $C_{k}=\frac{1}{1+\alpha}$.

Remark 3

If $k(t)=(\ln(1+t))^{\alpha}$, $\alpha>0$, then $\lim_{t\rightarrow 0+}\frac{d^{2}}{dt^{2}}(\frac{K(t)}{k(t)})=\frac{\alpha}{2(1+\alpha )(2+\alpha)}$. In this case, $k(t)$ does not satisfy (k₃).

This paper is organized as follows. In Section 2, we present some notation and results in regular variation theory. Theorems 1 and 2 will be proved in Section 3. Finally, we prove the existence and uniqueness of the solution for problem (1.1) in Appendices A.1 and A.2.

2 Preliminary results

2.1 Properties of regularly varying function

Karamata regular variation theory was established by Karamata in 1930 and is a basic tool in stochastic process. In 1970, Haan improved the results, which have been applied in stochastic process, analytical function theory, integral functions, integral transform and asymptotic estimation of an integral sequence (see [55–57]).

In this section, we recall some basic definitions and qualities in regular variation theory.

Definition 1

A positive measurable function f defined on $[a,\infty)$ for some $a>0$ is called regularly varying at infinity with index ρ (written as $f\in \mathit{RV}_{\rho}$) if for each $\xi >0$ and some $\rho\in R$,

$$ \lim_{t\rightarrow\infty}\frac{f(\xi t)}{f(t)}=\xi^{\rho}. $$

(2.1)

In particular, when $\rho=0$, f is called slowly varying at infinity. Clearly, if $f\in \mathit{RV}_{\rho}$, then $L(s):=\frac{f(s)}{s^{\rho}}$ is slowly varying at infinity.

Definition 2

A positive measurable function f defined on $[a,\infty)$ for some $a>0$ is called rapidly varying at infinity if for each $\rho>1$,

$$ \lim_{s\rightarrow\infty}\frac{f(s)}{s^{\rho}}=\infty. $$

(2.2)

Some basic examples of slowly varying functions at infinity are listed as follows:

(1)

every measurable function on $[a,\infty)$ which has a positive limit at infinity;
(2)

$(\ln t)^{s}$ and $(\ln( \ln t))^{s}$, $s\in R$;
(3)

$e^{(\ln t)^{s}}$, $0< s<1$.

Some basic examples of rapidly varying functions at infinity are given as follows:

(1)

$e^{t}$ and $e^{e^{t}}$;
(2)

$e^{e^{(\ln t)^{s}}}$, $e^{e^{t^{s}}}$ and $e^{e^{t^{s}}}$, $s>0$;
(3)

$t^{\gamma}e^{(\ln t)^{q}}$ and $(\ln t)^{\gamma}e^{(\ln t)^{q}}$, $q>1$, $\gamma\in R$;
(4)

$(\ln t)^{\gamma}e^{t^{q}}$ and $t^{\gamma}e^{t^{\gamma}}$, $q>0$, $\gamma\in R$.

We see that a positive measurable function h defined on $(0,a)$ for some $a>0$ is regularly varying at zero with index σ (written as $g\in \mathit{RVZ}_{\sigma}$) if $t\rightarrow g(\frac{1}{t})$ belongs to $\mathit{RV}_{-\sigma}$. Similarly, g is called rapidly varying at zero if $t\rightarrow g(\frac{1}{t})$ is rapidly varying at infinity.

Proposition 1

(Uniform convergence theorem)

If $f\in \mathit{RV}_{\rho}$, then (2.1) holds uniformly for $\xi\in[c_{1},c_{2}]$ with $0< c_{1}< c_{2}$. Moreover, if $\rho<0$, then uniform convergence holds on intervals of the form $(a_{1},\infty)$ with $a_{1}>0$; if $\rho>0$, then uniform convergence holds on intervals $(0,a_{1}]$, provided that f is bounded on $(0,a_{1}]$ for all $a_{1}>0$.

Proposition 2

(Representation theorem)

A function L is slowly varying at infinity if and only if it can be written in the form

$$ L(s)=\varphi(s)\exp\biggl( \int^{s}_{a_{1}}\frac{y(t)}{t}\, dt\biggr),\quad s \geq a_{1} $$

(2.3)

for some $a_{1}\geq a$, where the functions φ and y are measurable and as $s\rightarrow\infty$, $y(s)\rightarrow0$ and $\varphi(s)\rightarrow c_{0}>0$.

We say that

$$ \hat {L}(s)=c_{0}\exp\biggl( \int^{s}_{a_{1}}\frac{y(t)}{t}\, dt\biggr),\quad s \geq a_{1}, $$

(2.4)

is normalized slowly varying at infinity and

$$ f(s)=c_{0}s^{\rho} \hat {L}(s), \quad s\geq a_{1}, $$

(2.5)

is normalized regularly varying at infinity with index ρ (written as $f\in \mathit{NRV}_{\rho}$).

Similarly, g is called normalized regularly varying at zero with index σ (written as $g\in \mathit{NRVZ}_{\sigma}$) if $t\rightarrow g(\frac{1}{t})$ belongs to $\mathit{NRV}_{-\sigma}$. A function $f\in \mathit{RV}_{\rho}$ belongs to $\mathit{NRV}_{\rho}$ if and only if

$$ f\in C^{1}[a_{1},\infty) \quad \mbox{for some } a_{1}>0 \quad \mbox{and}\quad \lim_{s\rightarrow\infty} \frac{sf'(s)}{f(s)}=\rho. $$

(2.6)

Proposition 3

If functions $L_{1}$, $L_{2}$ are slowly varying at infinity, then

(1)

$L^{\sigma}$ for every $\sigma\in R$, $c_{1}L+c_{2}L_{1}$ ($c_{1}\geq0$, $c_{2}\geq0$ with $c_{1}+c_{2}>0$), $L\circ L_{1}$ (if $L_{1}(t)\rightarrow+\infty$ as $t\rightarrow+\infty$) are also slowly varying at infinity;
(2)

for every $\theta>0$, $t^{\theta}L(t)\rightarrow+\infty$ and $t^{-\theta}L(t)\rightarrow0$ as $t\rightarrow\infty$;
(3)

for $\rho\in R$, $\frac{\ln(L(t))}{\ln t}\rightarrow0$ and $\frac{\ln(t^{\rho}L(t))}{\ln t}\rightarrow\rho$ as $t\rightarrow+\infty$.

Proposition 4

If $f_{1}\in \mathit{RV}_{\rho_{1}}$, $f_{2}\in \mathit{RV}_{\rho_{2}}$ with $\lim_{t\rightarrow\infty}f_{2}(t)=\infty$, then $f_{1}\circ f_{2}\in \mathit{RV}_{\rho_{1}\rho_{2}}$.

Proposition 5

(Asymptotic behavior)

If a function L is slowly varying at infinity, then for $a\geq0$ and $t\rightarrow\infty$, we have

(1)

$\int^{t}_{a}s^{\beta}L(s)\, ds\cong(\beta+1)^{-1}t^{1+\beta}L(t)$ for $\beta>-1$;
(2)

$\int^{\infty}_{t}s^{\beta}L(s)\, ds\cong(-\beta-1)^{-1}t^{1+\beta}L(t)$ for $\beta<-1$.

Proposition 6

(Asymptotic behavior)

If a function H is slowly varying at infinity, then for $a>0$ and $t\rightarrow0^{+}$, we have

(1)

$\int^{t}_{0}s^{\beta}H(s)\, ds\cong(\beta+1)^{-1}t^{1+\beta}H(t)$ for $\beta>-1$;
(2)

$\int^{\infty}_{t}s^{\beta}H(s)\, ds\cong(-\beta-1)^{-1}t^{1+\beta}H(t)$ for $\beta<-1$.

2.2 Auxiliary results

In this section, we give some auxiliary results, which will be used in Theorems 1 and 2.

Lemma 1

[38, 40]

(I)
If $k\in\Lambda$, then we have:
1. (1)
  
  $\lim_{t\rightarrow0+}\frac{K(t)}{k(t)}=0$;
2. (2)
  
  $C_{k}\in[0,1]$ and $\lim_{t\rightarrow0+}\frac{K(t)k'(t)}{k^{2}(t)}=1-C_{k}$.
(II)
(k₁)-(k₃) implies that
1. (3)
  
  $\lim_{t\rightarrow0+} (\frac{K(t)k'(t)}{k^{2}(t)}-(1-C_{k}) )\frac{k(t)}{K(t)}=0$.

Lemma 2

[40]

Let f satisfy (f₁), (f₂), and (f₃). Then

(1)

$C_{f}\in[1,\infty)$;
(2)

there exists $S_{0}>0$ such that $\frac{f(s)}{s^{q}}$ is increasing in $[S_{0},\infty)$, where $q\in(p-1,\frac{C_{f}}{C_{f}-1})$ for $1< C_{f}<\frac{p-1}{p-2}$ and $q\in(p-1,\infty)$ for $C_{f}=1$;
(3)

f satisfies the Keller-Osserman condition
$$ \int^{\infty}_{1}\frac{dt}{(p'F(t))^{\frac{1}{p}}}< \infty,\quad F(t)= \int ^{t}_{0}f(s)\, ds, $$

(2.7)
where $\frac{1}{p'}+\frac{1}{p}=1$;
(4)

(f₃) holds for $C_{f} > 1$ if and only if $f\in \mathit{NRV}_{\frac{C_{f}}{C_{f}-1}}$;
(5)

$C_{f}=1$, and f is rapidly varying at infinity.

Lemma 3

Let f satisfy (f₁)-(f₃), and ϕ be the solution for the problem

$$\int^{\infty}_{\phi(t)}f^{-\frac{1}{p-1}}(s)\, ds=t, \quad \forall t>0. $$

Then we have

(1)

$-\phi'(t)=f^{\frac{1}{p-1}}(\phi(t))$, $\phi(t)>0$, $t>0$, $\phi (0):=\lim_{t\rightarrow0+}\phi(t)=+\infty$, $\phi''(t)=\frac{1}{p-1}f^{\frac{2}{p-1}-1}(\phi(t))f'(\phi(t))$;
(2)

$\lim_{t\rightarrow0+}\frac{t\phi'(t)}{\phi(t)}=-\frac {(p-1)(C_{f}-1)}{C_{f}-(p-1)(C_{f}-1)}$, i.e., $\phi\in \mathit{NRVZ}_{-\frac{(p-1)(C_{f}-1)}{C_{f}-(p-1)(C_{f}-1)}}$;
(3)

$\lim_{t\rightarrow0+}\frac{t\phi''(t)}{\phi'(t)}=-\frac {C_{f}}{C_{f}-(p-1)(C_{f}-1)}$, i.e., $-\phi'\in \mathit{NRVZ}_{-\frac{C_{f}}{C_{f}-(p-1)(C_{f}-1)}}$;
(4)

$\lim_{t\rightarrow0+}\frac{\ln(\phi(t))}{-\ln t}=\frac{(p-1)(C_{f}-1)}{C_{f}-(p-1)(C_{f}-1)}$, $\lim_{t\rightarrow0+}\frac{\ln(\phi'(t))}{-\ln t}=\frac{(p-1)C_{f}}{C_{f}-(p-1)(C_{f}-1)}$.

Proof

(1) By the definition of ϕ and a direct calculation we can show (1).

(2) It follows from Proposition 5 that

$$\begin{aligned} \lim_{t\rightarrow0+}\frac{t\phi'(t)}{\phi(t)} = & -\lim_{t\rightarrow0+} \frac{t f^{\frac{1}{p-1}}(\phi(t))}{\phi(t)} \\ = & -\lim_{u\rightarrow\infty}\frac{(f(u))^{\frac{1}{p-1}}}{u} \int^{\infty }_{u}\frac{dv}{f^{\frac{1}{p-1}(v)}} \\ = & -\lim_{u\rightarrow\infty}u^{\frac{C_{f}}{(p-1)(C_{f}-1)}-1}\hat {L}^{\frac{1}{p-1}}(u) \int^{\infty}_{u}v^{-\frac{C_{f}}{(p-1)(C_{f}-1)}}\hat {L}^{-\frac {1}{p-1}}(v) \, dv \\ = & - \biggl(\frac{C_{f}}{(p-1)(C_{f}-1)}-1 \biggr)^{-1} \\ &{} \cdot\lim_{u\rightarrow\infty}u^{\frac{C_{f}}{(p-1)(C_{f}-1)}-1}\hat {L}^{\frac{1}{p-1}}(u) u^{-\frac{C_{f}}{(p-1)(C_{f}-1)}+1}\hat {L}^{-\frac{1}{p-1}}(u) \\ = & -\frac{(p-1)(C_{f}-1)}{C_{f}-(p-1)(C_{f}-1)}. \end{aligned}$$

(3) (f₃) implies that

$$\begin{aligned} \lim_{t\rightarrow0+}\frac{t\phi''(t)}{\phi'(t)} = & -\frac{1}{p-1}\lim _{t\rightarrow0+}tf^{\frac{1}{p-1}-1}\bigl(\phi(t)\bigr)f'\bigl( \phi(t)\bigr) \\ = & -\frac{1}{p-1}\cdot\lim_{u\rightarrow\infty}f^{\frac{1}{p-1}-1}(u)f'(u) \int^{\infty}_{u}\frac{dv}{f^{\frac{1}{p-1}}(v)} \\ = & -\frac{1}{p-1}\cdot\lim_{u\rightarrow\infty}\frac{u f'(u)}{f(u)} \frac{f^{\frac{1}{p-1}}(u)}{u} \int^{\infty}_{u}\frac{dv}{f^{\frac{1}{p-1}}(v)} \\ = & -\frac{1}{p-1}\cdot\frac{(p-1)(C_{f}-1)}{C_{f}-(p-1)(C_{f}-1)}\cdot\frac {C_{f}}{C_{f}-1} \\ = & -\frac{C_{f}}{C_{f}-(p-1)(C_{f}-1)}. \end{aligned}$$

The last result (4) follows from (2)-(3) and Proposition 3(3). □

Lemma 4

Under the hypotheses in Theorem 2, let $k\in\Lambda$ and

$$\Phi(t)=\bigl(K(t)\bigr)^{-\frac{2(p-1)}{m+1-p}}\bigl(1+h(t)\bigr) $$

with $\lim_{t\rightarrow0}h(t)=0$. The following two results hold:

(1)

if $m+1-p>2m_{1}$, then $k(t)(K(t))^{\frac{(m+p-1)(p-1)}{m+1-p}}f_{1}(\Phi(t))\rightarrow0$ as $t\rightarrow0$;
(2)

if $m+1-p\leq2m_{1}$ and $k(t)=t^{\frac{\theta}{2}}$ with $\theta>0$ such that $\frac{\theta}{2+\theta}>\frac{2m_{1}-(m+p-1)}{m+1-p}$, then (1) still holds.

Proof

We know that $f_{1}\in \mathit{NRV}_{m_{1}}$ by (f₄) with $m_{1}\in(0,m)$ and $f_{1}(s)=c_{0}s^{m_{1}}\hat {L}(s)$ for sufficiently large s, where L̂ is normalized slowly varying at infinity, and $c_{0}>0$.

Let

$$\Phi_{1}(t)=\bigl(K(t)\bigr)^{-\frac{2(p-1)}{m+1-p}}. $$

We see that $\hat {L}(\Phi_{1}(t))$ is also normalized slowly varying at zero, and by a similar argument as in Propositions 1 and 3(2), for every $\beta>0$ and $t\rightarrow0+$, we have

$$ \bigl(\Phi_{1}(t)\bigr)^{\beta} \hat {L}\bigl( \Phi_{1}(t)\bigr)\rightarrow0 \quad \mbox{and}\quad \hat {L}\bigl( \Phi(t)\bigr) \bigl(\hat {L}\bigl(\Phi _{1}(t)\bigr) \bigr)^{-1}\bigl(1+h(t)\bigr)^{m_{1}}\rightarrow 0. $$

(2.8)

(1) If $m+1-p>2m_{1}$, let $2\beta\in(0,m+p-1-2m_{1})$, then by (2.8) we have

$$\begin{aligned}& k(t) \bigl(K(t)\bigr)^{\frac{(m+p-1)(p-1)}{m+1-p}}f_{1}\bigl(\Phi(t)\bigr) \\& \quad = k(t) \bigl(K(t)\bigr)^{\frac{(m+p-1)(p-1)}{m+1-p}}c_{0}\bigl(\Phi (t) \bigr)^{m_{1}}\hat {L}\bigl(\Phi(t)\bigr) \\& \quad = c_{0}k(t) \bigl(K(t)\bigr)^{\frac{(m+p-1)(p-1)-2(p-1)m_{1}-2(p-1)\beta }{m+1-p}}\bigl( \Phi_{1}(t)\bigr)^{\beta} \hat {L}\bigl(\Phi_{1}(t) \bigr) \\& \qquad {}\cdot \hat {L}\bigl(\Phi(t)\bigr) \bigl(\hat {L}\bigl(\Phi _{1}(t)\bigr)\bigr)^{-1}\bigl(1+h(t)\bigr)^{m_{1}} \rightarrow0\quad \mbox{as } t\rightarrow0. \end{aligned}$$

(2) If $m+1-p\leq2m_{1}$ and $k(t)=t^{\frac{\theta}{2}}$ with $\theta>0 $ such that $\frac{\theta}{2+\theta}>\frac{2m_{1}-(m+p-1)}{m+1-p}$ and $\frac{2(p-1)m_{1}}{m+1-p}\in(0,\frac{\theta}{2+\theta}-\frac {2m_{1}-(m+p-1)}{m+1-p})$, then we get

$$\begin{aligned}& k(t) \bigl(K(t)\bigr)^{\frac{(m+p-1)(p-1)}{m+1-p}}f_{1}\bigl(\Phi(t)\bigr) \\& \quad = ct^{\sigma}\bigl(\Phi_{1}(t)\bigr)^{\beta} \hat {L}\bigl(\Phi_{1}(t)\bigr) \hat {L}\bigl(\Phi(t)\bigr) \bigl( \hat {L}\bigl(\Phi _{1}(t)\bigr)\bigr)^{-1}\bigl(1+h(t) \bigr)^{m_{1}}\rightarrow0 \quad \mbox{as } t\rightarrow0, \end{aligned}$$

where

$$\begin{aligned}& c=c_{0}\biggl(\frac{\theta+2}{2}\biggr)^{\frac{(p-1)(2m_{1}+2\beta-m+1-p)}{m+1-p}}, \\& \sigma=\frac{\theta(m+1-p)-(2+\theta)(p-1)(2m_{1}+2\beta-m+1-p)}{2(m+1-p)}>0. \end{aligned}$$

□

3 Proofs of main results

In this section, we mainly prove Theorem 1 and Theorem 2. For the proofs, we use the upper and lower solution method. One critical step is to set up the comparison principle. Thus, we first give the comparison principle in general form for quasilinear elliptic equations.

Lemma 5

[54]

Suppose that D is a bounded domain in $R^{N}$ and $a(x)$ and $\beta(x)$ are continuous functions on D with $\|a\|_{L^{\infty}(D)}<\infty$, $\beta(x)\geq0$, $\beta(x)\neq0$ for $x\in D$. Let $u_{1}, u_{2}\in C^{1}(D)$ be positive in D and satisfy in the sense of distributions

$$\begin{aligned}& -\Delta_{p}u_{1}-a(x)u_{1}^{p-1}+ \beta(x)g(u_{1})\geq0\geq-\Delta _{p}u_{2}-a(x)u_{2}^{p-1}+ \beta(x)g(u_{2}), \\ & \varlimsup_{d(x,\partial\Omega)\rightarrow 0}\bigl(u_{2}^{p-1}-u_{1}^{p-1} \bigr)\leq0, \end{aligned}$$

where $g\in C^{0}([0,\infty))$, and $\frac{g(s)}{s^{p-1}}$ is increasing for

$$s\in \Bigl(\inf_{D}\{u_{1},u_{2}\}, \sup_{D}\{u_{1},u_{2}\} \Bigr). $$

Then $u_{1}\geq u_{2}$ in D.

Next, fix $\epsilon>0$. For all $\delta>0$, we define $\Omega_{\delta}=\{x\in\Omega:0< d(x)<\delta\}$. Since Ω is smooth, there exists $\delta_{0}>0$ such that $d\in C^{2}(\Omega_{\delta_{0}})$ and

$$ \bigl\vert \nabla d(x)\bigr\vert =1,\qquad \Delta d(x)=-(N-1)H( \overline{x})d(x)+o(1),\quad \forall x\in \Omega_{\delta_{0}}. $$

(3.1)

Proof of Theorem 1

Let $\epsilon\in(0,\frac{b_{0}}{4})$ and $\gamma_{1}=\gamma-\frac{2\epsilon\gamma}{b_{0}}$, $\gamma_{2}=\gamma+\frac{2\epsilon\gamma}{b_{0}}$. We have

$$\frac{\gamma}{2}< \gamma_{1}< \gamma< \gamma_{2}< 2\gamma. $$

Set

$$\begin{aligned}& d_{1}(x)=d(x)-\rho, \qquad d_{2}(x)=d(x)+ \rho, \end{aligned}$$

(3.2)

$$\begin{aligned}& \overline{u}_{\epsilon}=\phi\bigl(\gamma_{1} K^{2} \bigl(d_{1}(x)\bigr)\bigr),\quad x\in D^{-}_{\rho} \quad \mbox{and}\quad \underline{u}_{\epsilon}=\phi\bigl( \gamma_{2} K^{2}\bigl(d_{2}(x)\bigr)\bigr),\quad x\in D^{+}_{\rho}. \end{aligned}$$

(3.3)

Then, for $x\in D^{-}_{\rho}$,

$$\begin{aligned} \begin{aligned} &\Delta_{p}\overline{u}_{\epsilon}-b(x)f(\overline{u}_{\epsilon}) \\ &\quad = (p-1) \bigl\vert 2\gamma_{1}\phi'\bigl(\gamma _{1}K^{2}\bigl(d_{1}(x)\bigr)\bigr)K \bigl(d_{1}(x)\bigr)k\bigl(d_{1}(x)\bigr)\bigr\vert ^{p-2} \\ &\qquad {}\cdot (\phi''\bigl(\gamma_{1}K ^{2}\bigl(d_{1}(x)\bigr)\bigr)4\gamma_{1}^{2}K ^{2}\bigl(d_{1}(x)\bigr)k^{2} \bigl(d_{1}(x)\bigr) \\ &\qquad {}+\phi'\bigl(\gamma_{1}K ^{2} \bigl(d_{1}(x)\bigr)\bigr)2\gamma_{1}k^{2} \bigl(d_{1}(x)\bigr)+\phi'\bigl(\gamma_{1}K ^{2}\bigl(d_{1}(x)\bigr)\bigr)2\gamma_{1}K \bigl(d_{1}(x)\bigr)k'\bigl(d_{1}(x)\bigr) \\ &\qquad {}+2\gamma_{1}\phi'\bigl(\gamma_{1}K ^{2}\bigl(d_{1}(x)\bigr)\bigr)K\bigl(d_{1}(x) \bigr)k\bigl(d_{1}(x)\bigr)\Delta d(x) ) \\ &\qquad {}-b_{0}K^{p-2}\bigl(d_{1}(x) \bigr)k^{p}\bigl(d_{1}(x)\bigr) f\bigl(\phi\bigl( \gamma_{1}K^{2}\bigl(d_{1}(x)\bigr)\bigr)\bigr) \\ &\quad = (p-1) (2\gamma_{1})^{p-2}f\bigl(\phi\bigl(\gamma _{1}K^{2}\bigl(d_{1}(x)\bigr)\bigr) \bigr)K^{p-2}\bigl(d_{1}(x)\bigr)k^{p} \bigl(d_{1}(x)\bigr) \\ &\qquad {}\cdot \biggl(4\gamma_{1} \biggl(\frac{\gamma_{1}K^{2}(d_{1}(x))\phi''(\gamma _{1}K^{2}(d_{1}(x)))}{-\phi'(\gamma_{1}K^{2}(d_{1}(x)))}- \frac{C_{f}}{C_{f}-(p-1)(C_{f}-1)} \biggr) \\ &\qquad {}-2\gamma_{1} \biggl(\frac {K(d_{1}(x))k'(d_{1}(x))}{k^{2}(d_{1}(x))}-(1-C_{k}) \biggr)-2\gamma _{1}\frac{K(d_{1}(x))}{k(d_{1}(x))}\Delta d(x) \\ &\qquad {}- \biggl(\frac{1}{(2\gamma_{1})^{p-2}(p-1)}\frac {b(x)}{K^{p-2}(d_{1}(x))k^{p}(d_{1}(x))}-\frac{b_{0}}{(2\gamma _{1})^{p-2}(p-1)} \biggr) \\ &\qquad {}-\frac{b_{0}}{(2\gamma_{1})^{p-2}(p-1)}+\frac{4\gamma _{1}C_{f}}{C_{f}-(p-1)(C_{f}-1)}-2\gamma_{1}(1-C_{k})-2 \gamma_{1} \biggr). \end{aligned} \end{aligned}$$

By (b₁), (b₂), and Lemmas 1-3 we see that there exists $\delta_{\epsilon}\in(0,\frac{\delta_{0}}{2})$ sufficiently small such that

(r₁):: $(b_{0}-\epsilon)K^{p-2}(d(x)-\rho)k^{p}(d(x)-\rho)\leq(b_{0}-\epsilon )K^{p-2}(d(x))k^{p}(d(x))< b(x)$, $x\in D^{-}_{\rho}=\Omega_{2\delta_{\epsilon}}/\overline{\Omega}_{\rho}$; $b(x)<(b_{0}+\epsilon)K^{p-2}(d(x))k^{p}(d(x))\leq(b_{0}+\epsilon )K^{p-2}(d(x)+\rho)k^{p}(d(x)+\rho) $, $x\in D^{+}_{\rho}=\Omega_{2\delta_{\epsilon}-{\rho}}$, where $\rho\in(0,\delta_{\epsilon})$,

(r₂):: $$\begin{aligned}& 4\gamma\biggl\vert \gamma_{1}\frac{K^{2}(t)\phi''(\gamma_{1}K^{2}(t))}{\phi '(\gamma_{1}K^{2}(t))} -\frac{C_{f}}{C_{f}-(p-1)(C_{f}-1)} \biggr\vert +2\gamma\biggl\vert \frac {K(t)k'(t)}{k^{2}(t)}-(1-C_{k})\biggr\vert \\& \quad {}+2\gamma\frac{K(t)}{k(t)}\bigl\vert \Delta d(x)\bigr\vert < \epsilon, \quad \forall(x,t)\in \Omega_{2\delta_{\epsilon}}\times(0,2\delta_{\epsilon}), \end{aligned}$$

and by the value of $\gamma_{1}$ in Theorem 1,

$$-\frac{b_{0}}{(2\gamma_{1})^{p-2}(p-1)}+\frac{4\gamma _{1}C_{f}}{C_{f}-(p-1)(C_{f}-1)}-2\gamma_{1}(1-C_{k})-2 \gamma_{1}=0. $$

Then

$$\Delta_{p}\overline{u}_{\epsilon}-b(x)f(\overline{u}_{\epsilon}) \leq0, $$

i.e., $\overline{u}_{\epsilon}$ is a supersolution of Eq. (1.1) in $D^{-}_{\rho}$.

Similarly, we can show that $\underline{u}_{\epsilon}$ is a subsolution of Eq. (1.1) in $D^{+}_{\rho}$.

Now let u be an arbitrary solution of problem (1.1) and $C_{1}(\delta_{\epsilon}):=\max_{d(x)\geq \delta_{\epsilon}}u(x)$. We see that

$$u\leq C_{1}(\delta_{\epsilon})+\overline{u}_{\epsilon} \quad \mbox{on } \partial D^{-}_{\rho}. $$

Since ϕ is decreasing and $\gamma_{1}>\gamma$, we have

$$\underline{u}_{\epsilon}\leq\phi\bigl(\gamma K(2\delta_{\epsilon }) \bigr):=C_{2}(\delta_{\epsilon}) \quad \mbox{whenever } d(x)=2 \delta _{\epsilon}-\rho $$

and

$$\underline{u}_{\epsilon}\leq u+C_{2}(\delta_{\epsilon}) \quad \mbox{on } \partial D^{+}_{\rho}. $$

It follows by (f₁) and Lemma 5 that

$$ u\leq C_{1}(\delta_{\epsilon})+\overline{u}_{\epsilon},\quad x\in D^{-}_{\rho} \quad \mbox{and} \quad \underline{u}_{\epsilon} \leq u+C_{2}(\delta_{\epsilon}), \quad x\in D^{+}_{\rho}. $$

(3.4)

Hence, letting $\rho\rightarrow0$, we have, for $x\in D^{-}_{\rho}\cap D^{+}_{\rho}$,

$$1-\frac{C_{2}(\delta_{\epsilon})}{\phi(\gamma_{2}K^{2}(d(x)))}\leq\frac {u(x)}{\phi(\gamma_{2}K^{2}(d(x)))} $$

and

$$\frac{u(x)}{\phi(\gamma_{1}K^{2}(d(x)))}\leq1+\frac{C_{1}(\delta _{\epsilon})}{\phi(\gamma_{1})K^{2}(d(x))}. $$

Consequently,

$$1\leq\liminf_{d(x)\rightarrow0}\frac{u(x)}{\phi(\gamma_{2}K^{2}(d(x)))} \quad \mbox{and} \quad \limsup_{d(x)\rightarrow0}\frac{u(x)}{\phi(\gamma _{1}K^{2}(d(x)))}\leq 1. $$

Thus, letting $\epsilon\rightarrow0$, we have

$$1\leq\liminf_{d(x)\rightarrow0}\frac{u(x)}{\phi(\gamma K^{2}(d(x)))} \quad \mbox{and} \quad \limsup_{d(x)\rightarrow0}\frac {u(x)}{\phi(\gamma K^{2}(d(x)))}\leq1, $$

that is,

$$\lim_{d(x)\rightarrow0}\frac{u(x)}{\phi(\gamma K^{2}(d(x)))}=1. $$

The proof is complete. □

Proof of Theorem 2

Let $\epsilon\in(0,1)$ and

$$\begin{aligned}& \overline{u}_{\epsilon}=C_{1}\bigl(K\bigl(d_{1}(x) \bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac {K(d_{1}(x))}{k(d_{1}(x))} \biggr),\quad x\in D^{-}_{\rho}, \\& \underline{u}_{\epsilon}=C_{1}\bigl(K\bigl(d_{1}(x) \bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})- \epsilon\bigr)\frac {K(d_{2}(x))}{k(d_{2}(x))} \biggr),\quad x\in D^{+}_{\rho}. \end{aligned}$$

Using Lemma 4 and a direct calculation we see that, for $x\in D^{-}_{\rho}$,

$$\begin{aligned}& K^{p-2}\bigl(d_{1}(x)\bigr)k^{p} \bigl(d_{1}(x)\bigr)f\bigl(\overline{u}_{\epsilon}(x)\bigr) \\& \quad = K^{p-2}\bigl(d_{1}(x)\bigr)k^{p} \bigl(d_{1}(x)\bigr) \bigl(\overline{u}^{m}_{\epsilon}(x) \pm c_{0}\overline{u}^{m_{1}}_{\epsilon}(x)\hat {L} \bigl(\overline {u}_{\epsilon}(x)\bigr)\bigr) \\& \quad = K^{p-2}\bigl(d_{1}(x)\bigr)k^{p} \bigl(d_{1}(x)\bigr) \\& \qquad {}\cdot \biggl[ C_{1}^{m}\bigl(K\bigl(d_{1}(x) \bigr)\bigr)^{-\frac{2m(p-1)}{m+1-p}} \biggl(1+mC_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac {K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\& \qquad {}\pm c_{0}C^{m_{1}}_{1}\bigl(K \bigl(d_{1}(x)\bigr)\bigr)^{-\frac{2m_{1}(p-1)}{m+1-p}}\hat {L}\bigl( \overline{u}_{\epsilon}(x)\bigr) \\& \qquad {}\cdot \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+\epsilon \bigr)\frac {K(d_{1}(x))}{k(d_{1}(x))} \biggr)^{m_{1}} \biggr] \\& \quad = K^{p-2}\bigl(d_{1}(x)\bigr)k^{p-1} \bigl(d_{1}(x)\bigr) \bigl(K\bigl(d_{1}(x)\bigr) \bigr)^{-\frac {2m(p-1)}{m+1-p}+1} \\& \qquad {}\cdot \biggl[C_{1}^{m}\frac {k(d_{1}(x))}{K(d_{1}(x))}+mC_{1}^{m}C_{2}(N-1) \bigl(H(\overline{x})+\epsilon\bigr) \\& \qquad {}\pm\bigl(K\bigl(d_{1}(x)\bigr)\bigr)^{-\frac{2(m_{1}+m)(p-1)}{m+1-p}-1}k(t) \hat {L}\bigl(\overline{u}_{\epsilon}(x)\bigr) \\& \qquad {}\cdot \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+\epsilon \bigr)\frac {K(d_{1}(x))}{k(d_{1}(x))} \biggr)^{m_{1}} \biggr] \end{aligned}$$

and

$$\begin{aligned}& |\nabla\overline{u}_{\epsilon}| = \bigl(K\bigl(d_{1}(x)\bigr) \bigr)^{-\frac{m+p-1}{m+1-p}}k\bigl(d_{1}(x)\bigr)\nabla d(x) \\& \hphantom{|\nabla\overline{u}_{\epsilon}|={}}{}\cdot \biggl(1+C_{2}(N-1) (H\overline{x}+\epsilon) \frac {K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\& \hphantom{|\nabla\overline{u}_{\epsilon}|={}}{}+{\biggl. C_{1}\bigl(K\bigl(d_{1}(x)\bigr) \bigr)^{-\frac{2(p-1)}{m+1-p}}C_{2}(N-1) \bigl(H(\overline {x}+\epsilon)\bigr) \frac{d}{dt} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}}\nabla d(x), \\& \Delta _{p}\overline{u}_{\epsilon} = (p-1)|\nabla \overline{u}_{\epsilon}|^{p-2} \times \biggl[\frac{2(p-1)(m+p-1)}{(m+1-p)^{2}} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot\bigl(K\bigl(d_{1}(x)\bigr)\bigr)^{-\frac{m+p-1}{m+1-p}-1}k^{2} \bigl(d_{1}(x)\bigr) \biggl(1+C_{2}(N-1) \bigl(H( \overline{x})+\epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}}{(m+1-p)} \bigl(K\bigl(d_{1}(x)\bigr) \bigr)^{-\frac{m+p-1}{m+1-p}}k'\bigl(d_{1}(x)\bigr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{} \cdot \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}}{(m+1-p)} \bigl(K\bigl(d_{1}(x)\bigr) \bigr)^{-\frac{m+p-1}{m+1-p}}k\bigl(d_{1}(x)\bigr)\Delta d(x) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{4(p-1)C_{1}}{(m+1-p)} \bigl(K\bigl(d_{1}(x)\bigr) \bigr)^{-\frac{m+p-1}{m+1-p}} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot {\biggl.k\bigl(d_{1}(x)\bigr)C_{2}(N-1) \bigl(H(\overline{x})+\epsilon\bigr)\frac{d}{dt} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+{\biggl.C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr) \bigl(K\bigl(d_{1}(x)\bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \frac{d^{2}}{dt^{2}} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr) \bigl(K\bigl(d_{1}(x)\bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \frac{d}{dt} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot {\biggl.\biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}} \Delta d(x) \biggr] \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon}}= (p-1) \biggl(\frac{2(p-1)C_{1}}{m+1-p} \biggr)^{p-2}\bigl(K \bigl(d_{1}(x)\bigr)\bigr)^{-\frac{(p-1)(p-2)+mp}{m+1-p}}k^{p} \bigl(d_{1}(x)\bigr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot \biggl[\frac{2(p-1)(m+p-1)C_{1}}{(m+1-p)^{2}} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+\frac{2(p-1)(m+p-1)C_{1}C_{2}}{(m+1-p)^{2}} (N-1) \bigl(H(\overline{x})+\epsilon\bigr) \frac{K(d_{1}(x))}{k(d_{1}(x))} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}}{(m+1-p)} \biggl(\frac{K(d_{1}(x))k'(d_{1}(x))}{k^{2}(d_{1}(x))}-(1-C_{k}) \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}}{(m+1-p)} \biggl(\frac{K(d_{1}(x))k'(d_{1}(x))}{k^{2}(d_{1}(x))}-(1-C_{k}) \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot C_{2}(N-1) \bigl(H(\overline{x})+\epsilon \bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}}{(m+1-p)} (1-C_{k}) \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+\epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}}{(m+1-p)} \frac{K(d_{1}(x))}{k(d_{1}(x))}\Delta d(x) \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+\epsilon\bigr) \frac{K(d_{1}(x))}{k(d_{1}(x))} \biggr) \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-{\biggl.\frac{4(p-1)C_{1}C_{2}}{(m+1-p)} \frac{K(d_{1}(x))}{k(d_{1}(x))} (N-1) \bigl(H( \overline{x})+\epsilon\bigr) \biggl(\frac{d}{dt} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}} \\ & \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-C_{k}+C_{k}\biggr) \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+{\biggl.C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K^{2}(d_{1}(x))}{k^{2}(d_{1}(x))} \frac{d^{2}}{dt^{2}} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}} \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+{\biggl.C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \frac{d}{dt} \biggl(\frac{K^{2}(t)}{k^{2}(t)} \biggr) \biggr|_{t=d_{1}(x)}}\Delta d(x) \biggr] \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon}}= (p-1) \biggl(\frac{2(p-1)C_{1}}{m+1-p} \biggr)^{p-2}\bigl(K \bigl(d_{1}(x)\bigr)\bigr)^{-\frac {(p-1)(m+p-1)}{m+1-p}}k^{p-1} \bigl(d_{1}(x)\bigr) \biggl[\frac{k(d_{1}(x))}{K(d_{1}(x))} \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot \biggl(\frac{2(p-1)(m+p-1)C_{1}}{(m+1-p)^{2}}-\frac {2(p-1)C_{1}}{(m+1-p)}(1-C_{k}) \biggr) \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr) \biggl(\frac{2(p-1)(m+p-1)}{(m+1-p)^{2}}-\frac{2(p-1)}{(m+1-p)}(1-C_{k}) \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{4(p-1)C_{k}}{(m+1-p)} \biggr) -\frac{2(p-1)C_{1}}{(m+1-p)} \Delta d(x)-\frac{2(p-1)C_{1}}{(m+1-p)} \biggl(\frac{K(d_{1}(x))k'(d_{1}(x))}{k^{2}(d_{1}(x))} \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-(1-C_{k}) \biggr) \frac{k(d_{1}(x))}{K(d_{1}(x))}- \frac{2(p-1)C_{1}C_{2}}{(m+1-p)} \biggl(\frac{K(d_{1}(x))k'(d_{1}(x))}{k^{2}(d_{1}(x))}-(1-C_{k}) \biggr) \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot(N-1) \bigl(H(\overline{x})+\epsilon\bigr) - \frac{4(p-1)C_{1}C_{2}}{(m+1-p)} (N-1) \bigl(H(\overline{x})+\epsilon\bigr) \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}\cdot {\biggl.\biggl(\frac{d}{dt} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}}-C_{k} \biggr) \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}-\frac{2(p-1)C_{1}C_{2}}{(m+1-p)} \Delta d(x) (N-1) \bigl(H( \overline{x})+\epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+{\biggl.C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \frac{d^{2}}{dt^{2}} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}} \\& \hphantom{\Delta _{p}\overline{u}_{\epsilon} ={}}{}+{\biggl.C_{1}C_{2}(N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K(d_{1}(x))}{k(d_{1}(x))} \frac{d}{dt} \biggl(\frac{K(t)}{k(t)} \biggr) \biggr|_{t=d_{1}(x)}}\Delta d(x) \biggr]. \end{aligned}$$

By the value of $C_{1}$, $C_{2}$ from Theorem 2 and (3.1) we know that

$$\begin{aligned}& \frac{2(p-1)(m +p-1)C_{1}}{(m+1-p)^{2}}-\frac{2(p-1)C_{1}(1-C_{k})}{(m+1-p)}= \frac{C_{1}^{m}}{p-1}\biggl( \frac{2(p-1)C_{1}}{m+1-p}\biggr)^{-(p-2)}, \\& \frac{2(p-1)(m +p-1)C_{1}C_{2}}{(m+1-p)^{2}}-\frac{2(p-1)C_{1}C_{2}(1-C_{k})}{(m+1-p)}- \frac{4(p-1)C_{1}C_{2}C_{k}}{(m+1-p)} \\& \quad {}+\frac{2(p-1)C_{1}}{(m+1-p)}=\frac{mC_{1}^{m}C_{2}}{p-1}\biggl(\frac {2(p-1)C_{1}}{m+1-p} \biggr)^{-(p-2)}, \end{aligned}$$

and by Lemmas 1 and 4 we get that there exists $\delta_{\epsilon}\in(0,\frac{\delta}{2})$ sufficiently small such that, for $(x,t)\in\Omega_{2\delta_{\epsilon}}\times(0,2\delta_{\epsilon})$,

$$\begin{aligned}& -\frac{2(p-1)C_{1}}{(m+1-p)} \biggl(\frac{K(t)k'(t)}{k^{2}(t)}-(1-C_{k}) \biggr) \frac{k(t)}{K(t)} \\& \qquad {} -\frac{2(p-1)C_{1}C_{2}}{(m+1-p)} \biggl(\frac{K(t)k'(t)}{k^{2}(t)}-(1-C_{k}) \biggr) \\& \qquad {}\cdot(N-1) \bigl(H(\overline{x})+\epsilon\bigr)-\frac{4(p-1)C_{1}C_{2}}{(m+1-p)}(N-1) \bigl(H(\overline{x})+\epsilon\bigr) \biggl(\frac{d}{dt} \biggl( \frac{K(t)}{k(t)} \biggr)-C_{k} \biggr) \\& \qquad {}-\frac{2(p-1)C_{1}C_{2}}{(m+1-p)} \Delta d(x) (N-1) \bigl(H(\overline{x})+ \epsilon\bigr)\frac{K(t)}{k(t)} \\& \qquad {}+C_{1}C_{2}(N-1) \bigl(H(\overline{x})+\epsilon \bigr)\frac{K(t)}{k(t)} \frac{d^{2}}{dt^{2}} \biggl(\frac{K(t)}{k(t)} \biggr) \\& \qquad {}+C_{1}C_{2}(N-1) \bigl(H(\overline{x})+\epsilon \bigr)\frac{K(t)}{k(t)} \frac{d}{dt} \biggl(\frac{K(t)}{k(t)} \biggr) \Delta d(x)\mp\frac{c_{0}C^{m}_{1}}{p-1}\biggl(\frac{2(p-1)C_{1}}{m+1-p}\biggr)^{-(p-2)} \\& \qquad {}\cdot \bigl(K(t)\bigr)^{-\frac{2(m_{1}+m)(p-1)}{m+1-p}-1}k(t)\hat {L}\bigl(\Phi(t)\bigr) \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+\epsilon\bigr) \frac{K(t)}{k(t)} \biggr)^{m_{1}} \\& \quad \leq\frac{C_{1}(N-1)}{m+1-p}\epsilon, \end{aligned}$$

where $\Phi(t)$ is given in Lemma 4 with $h(t)=\pm C_{2}(N-1)(H(\overline{x})+1)\frac{K(t)}{k(t)}$.

Thus, for $x\in D^{-}_{\rho}$, we have

$$\begin{aligned}& \Delta_{p}\overline{u}_{\epsilon }(x)-K^{p-2} \bigl(d_{1}(x)\bigr)k^{p}\bigl(d_{1}(x)\bigr)f\bigl( \overline{u}_{\epsilon}(x)\bigr) \\& \quad \leq (p-1) \biggl(\frac{2(p-1)C_{1}}{m+1-p} \biggr)^{p-2}\bigl(K \bigl(d_{1}(x)\bigr)\bigr)^{-\frac {(p-1)(m+p-1)}{m+1-p}} \\& \qquad {}\cdot k^{p-1}\bigl(d_{1}(x)\bigr) \biggl(- \frac{2C_{1}(N-1)}{m+1-p}\epsilon+\frac{C_{1}(N-1)}{m+1-p}\epsilon\biggr) \\& \quad \leq 0, \end{aligned}$$

i.e., $\overline{u}_{\epsilon}(x)$ is a supersolution of Eq. (1.1) in $D^{-}_{\rho}$.

Similarly, we can show that $\underline{u}_{\epsilon}$ is a subsolution of Eq. (1.1) in $D^{+}_{\rho}$.

By (3.4) and letting $\rho\rightarrow0$, we have that, for $x\in D^{-}_{\rho}\cap D^{+}_{\rho}$,

$$\begin{aligned}& C_{1}\bigl(K\bigl(d(x)\bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})+\epsilon\bigr) \frac{K(d(x))}{k(d(x))} \biggr)+C_{1}(\delta_{\epsilon})\geq u(x), \end{aligned}$$

(3.5)

$$\begin{aligned}& C_{1}\bigl(K\bigl(d(x)\bigr)\bigr)^{-\frac{2(p-1)}{m+1-p}} \biggl(1+C_{2}(N-1) \bigl(H(\overline{x})-\epsilon\bigr) \frac{K(d(x))}{k(d(x))} \biggr)-C_{2}(\delta_{\epsilon})\leq u(x). \end{aligned}$$

(3.6)

The proof is complete. □

Declarations

Acknowledgements

This work is supported by the Natural Science Foundation of Shandong Province of China (ZR2012AM018) and the Fundamental Research Funds for the Central Universities (No. 201362032). The authors would like to deeply thank all the reviewers for their insightful and constructive comments.

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Appendix

In this appendix, we prove the existence and uniqueness of the solution for problem (1.1).

A.1 The existence of solutions for problem (1.1)

In the first part, we give the existence of solutions for problem (1.1).

Theorem 3

Let f satisfy (f₁) and the Keller-Osserman condition (2.7), and b satisfy (b₁). Then problem (1.1) has at least one solution $u\in W^{1,p}_{\mathrm{loc}}(\overline{\Omega})$ satisfying

$$ u(x)\geq\psi\bigl(\overline{v}(x)\bigr), \quad \forall x\in\Omega. $$

(A.1)

Furthermore, if f satisfies $\int^{1}_{0}f^{-\frac{1}{p-1}}(s)\, ds=\infty$, then

$$ u>0, \quad \forall x\in\Omega, $$

(A.2)

where ψ is the solution of problem (1.4) and $\overline {v}\in W^{1,p}_{0}(\Omega)$ is the unique solution for problem

$$ -\Delta_{p}\overline{v}=b(x),\qquad \overline{v}(x)>0,\quad x\in \Omega,\qquad \overline {v}|_{\partial\Omega}=0. $$

(A.3)

Remark 4

By Lemma 2(3), we can see that f satisfies the Keller-Osserman condition under our hypotheses on f in Theorem 1.

Remark 5

By the similar argument in [46], we show that (f₁) and the Keller-Osserman condition imply (f₂). Indeed, if we can prove that there exist two positive numbers ρ and M such that

$$ \frac{f^{p'-1}(s)}{s}\geq\rho^{p'} \quad \mbox{for } s\geq M, $$

(A.4)

then it will be done since

$$F(s)= \int^{s}_{0}f(t)\, dt\leq sf(s)\leq \frac{f^{p'}(s)}{\rho^{p'}} \quad \mbox{for } s\geq M, $$

which, in turn, yields $[F(s)]^{-\frac{1}{p}}\geq\frac{\rho^{\frac{1}{p-1}}}{f^{\frac{1}{p-1}}(s)}$, so that the Keller-Osserman condition implies (A.4). Then, we will prove (A.4) by contradiction. Assume that there exists an increasing sequence ${s_{j}}$ of real numbers such that $\lim_{j\rightarrow\infty}s_{j}=\infty$ and $\frac{f(s_{j})}{s_{j}}<\frac{1}{j}$ for all j. Since f is increasing, we have $f(s)\leq f(s_{j})$ for all $s\in[0,s_{j} ]$, which, in turn, produces $F(s)\leq sf(s)\leq sf(s_{j})\rightarrow\infty$ for $s\in[0,s_{j}]$. Hence,

$$\begin{aligned} \int^{s_{j}}_{s_{1}}\bigl[F(s)\bigr]^{-\frac{1}{p}}\, ds &\geq \int ^{s_{j}}_{s_{1}}\bigl[F(s)\bigr]^{-\frac{1}{p}}\, ds \geq \biggl[\frac{j}{s_{j}} \biggr]^{\frac{1}{p'}} \int^{s_{j}}_{s_{1}}s^{-\frac{1}{p}}\, ds \\ &= \frac{p}{p-1}j^{\frac{1}{p'}} \biggl(1- \biggl(\frac{s_{1}}{s_{j}} \biggr) \biggr)\rightarrow\infty \end{aligned}$$

as $j\rightarrow\infty$, which contradicts the Keller-Osserman condition (2.7). Thus, (A.4) must be true, and then (f₂) holds.

Proof

Let

$$ v=\phi(u)= \int^{\infty}_{u}f^{-\frac{1}{p-1}}(v)\, dv, \quad u>0. $$

(A.5)

We see that problem (1.1) is equivalent to the following problem:

$$ -\Delta_{p}v+g(v)|\nabla v|^{p}=b(x), \quad v>0, x\in \Omega, \qquad \overline {v}|_{\partial\Omega}=0, $$

(A.6)

where $g(v)=f'(\psi(v))$, and ϕ is also the inverse function of ψ.

Now let $v\in W^{1,p}_{\mathrm{loc}}(\Omega)\cap L^{\infty}_{\mathrm{loc}}(\Omega)$ be any solution of problem (A.6). We claim that

$$ v(x)\leq \overline{v}(x), \quad \forall x\in\Omega. $$

(A.7)

Indeed, assume on the contrary that $\{x\in\Omega:v(x)>\overline{v}(x)\}\neq\emptyset$. Then, on its arbitrary connected component D, we have $-\Delta _{p}(v-\overline{v})(x)\leq0$, $x\in D$, since $g(v)\geq0$. It follows by $(v-\overline{v})|_{\partial\Omega}=0$ and the maximum principle that $v(x)\leq\overline{v}(x)$ for all $x\in D$. This is a contradiction. Thus, (A.7) holds, i.e., any weak solution u of problem (1.1) satisfies (A.1). Moreover, by the definition of ψ and the condition $\int^{1}_{0}\frac{ds}{f(s)}=\infty$ we see that $\psi(\overline{v}(x))>0$, $\forall x\in\Omega$, and (A.2) holds. Next, we consider the perturbed problem

$$ \Delta_{p}u=b(x)f(u), \quad x\in\Omega,\qquad u|_{\partial\Omega}=m\in N. $$

(A.8)

By (b₁) and (f₁) we see that $\overline{u}_{m}=m$ is a supersolution of problem (A.8). To construct a subsolution $\underline{u}_{1}$ of problem (A.8), we let $\overline{v}_{1}\in C^{2+\alpha}(\overline{\Omega})$ be the unique solution of the problem

$$ -\Delta_{p}\overline{v}_{1}=b(x), \qquad \overline{v}(x)>0, \quad x\in\Omega, \qquad \overline{v}_{1}|_{\partial\Omega}= \int^{\infty }_{1}f^{-\frac{1}{p-1}}(s)\, ds, $$

(A.9)

and $\overline{u}_{1}=\psi(\overline{v}_{1})$. Then we see that $\underline{u}_{1}|_{\partial\Omega}=1\leq m$ and

$$-\Delta _{p}\overline{v}_{1}=\frac{\Delta_{p}\underline {u}_{1}}{f(\underline{u}_{1})} - \frac{f'(\underline{u}_{1})}{f^{2}(\underline{u}_{1})}|\nabla\underline {u}_{1}|^{p}=b(x), \quad x\in\Omega, $$

which yields

$$\Delta_{p}\underline{u}_{1}\geq b(x)f(\underline{u}_{1}), \quad x\in\Omega, $$

i.e., $\underline{u}_{1}$ is a subsolution of problem (A.8). Moreover, $\underline{u}_{1}\leq1\leq m$, $x\in\Omega$, due to the maximum principle. Thus, problem (A.8) has one solution $u_{m}\in W^{1,p}_{0}$ in the order interval $[u_{1},m]$, and the maximum principle again yields that the map $m\rightarrow u_{m}$ is increasing. On the other hand, the classical Keller-Osserman condition guarantees that the problem

$$ \Delta_{p}u=b_{0}f(u), \quad x\in\Omega_{0}, \qquad u|_{\partial\Omega _{0}}=\infty, $$

(A.10)

has one solution $u_{\Omega_{0}}\in W^{1,p}_{\mathrm{loc}}(\Omega)$ for each $\Omega_{0}\subset\subset\Omega$, where $b_{0}=\min_{x\in\overline{\Omega}_{0}}b(x)$. By the maximum principle we have $u_{m}\leq u_{\Omega_{0}}(x)$, $x\in\Omega_{0}$, and $u(x):=\lim_{m\rightarrow\infty}u_{m}(x)$ exists for $x\in\Omega_{0}$. Thus, u is the desired solution for problem (1.1) by the standard bootstrap argument, the arbitrariness of $\Omega_{0}$, and (A.1). □

A.2 The uniqueness of the solution for problem (1.1)

In the second part, we prove the uniqueness of the solution for problem (1.1). The method is similar to the idea in [40, 58].

Theorem 4

Under the hypotheses in Theorem 1, problem (1.1) admits a unique solution.

Proof

Since $\frac{f(s)}{s^{q}}$ is increasing in $[S_{0},\infty)$ for some $q>p-1$ and $S_{0}$ large enough, by Lemma 2(2) we have

$$ \frac{f(s)}{s} \mbox{ is also increasing in } [S_{0}, \infty). $$

(A.11)

Let $u_{0}$ be the minimal solution for problem (1.3), and u be another solution for problem (1.1). We prove that $u = u_{0}$ in Ω. In fact, by the maximum principle we have

$$ u_{0}\leq u \quad \mbox{in } \Omega. $$

(A.12)

Moreover, by the asymptotic behavior (1.3) we deduce that

$$ \lim_{d(x)\rightarrow0}\frac{u_{0}(x)}{u(x)}=1. $$

(A.13)

For any $\epsilon>0$, setting $w=(1+\epsilon)u_{0}$, we have

$$ \lim_{d(x)\rightarrow0}\bigl(w(x)-u(x)\bigr) =\lim_{d(x)\rightarrow0} \biggl(\frac{(1+\epsilon)u_{0}(s)}{u(s)}-1 \biggr)=+\infty. $$

(A.14)

Now, for small $\epsilon> 0$, we define the open set

$$ D_{\epsilon}=\bigl\{ x\in\Omega:w(x)< u(x)\bigr\} . $$

(A.15)

We may assume that $D_{\epsilon}$ is nonempty for ϵ small enough; otherwise, there is nothing to prove. Indeed, notice that $D_{\epsilon}$ increases as $\epsilon\rightarrow0$. Moreover, we may also assume that $D_{\epsilon}\rightarrow\Omega$ as $\epsilon\rightarrow0$; if there exists $x_{0}\in\Omega$ and a sequence $\epsilon_{n}\rightarrow0$ such that $x_{0}\in D_{\epsilon_{n}}$ for all n, then we have $(1+\epsilon_{n})u_{0}(x_{0})\geq u(x_{0})$. Then the strong maximum principle yields $u\equiv u_{0}$ in Ω. Finally, we have $D_{\epsilon}\subset\Omega$ by (A.13).

Next, we choose $\eta>0$ such that $u_{0}\geq S_{0}$ in $\Omega_{\eta}$ and define $D_{\epsilon,\eta}=D_{\epsilon}\cap D_{\eta}$. Notice that $D_{\epsilon,\eta}$ is a nonempty open set for small ϵ. Moreover, by (A.11) we have

$$ \Delta _{p}w=(1+\epsilon)b(x)f(u_{0})\leq b(x)f(w),\quad x\in D_{\epsilon,\eta}. $$

(A.16)

It follows by (f₁) that

$$ \Delta _{p}(u-w)\geq b(x) \bigl(f(u)-f(w)\bigr)\geq0, \quad x\in D_{\epsilon,\eta }. $$

(A.17)

Thus, by the maximum principle we obtain

$$ u(x)-w(x)\leq\max_{\partial D_{\epsilon,\eta}}(u-w), \quad x\in D_{\epsilon,\eta}. $$

(A.18)

Since $\partial D_{\epsilon,\eta}=(\partial D_{\epsilon}\cap D_{\eta})\cup( D_{\epsilon}\cap\partial D_{\eta})$, $D_{\epsilon}\cap\partial\Omega=\emptyset$, and $(u-w)|_{\partial D_{\epsilon}}=0$, we see that the maximum of $u-w$ is achieved on $D_{\epsilon}\cap\partial D_{\eta}=( D_{\epsilon}\cap {x:d(x)=\eta})$. Hence,

$$ u(x)-w(x)\leq\max_{( D_{\epsilon}\cap {x:d(x)=\eta})}(u-w), \quad x\in D_{\epsilon,\eta}. $$

(A.19)

Letting $\epsilon\rightarrow0$ in (A.19), we obtain

$$ u-u_{0}\leq\max_{d(x)=\eta}(u-u_{0}):=\theta \quad \mbox{in } \Omega _{\eta}. $$

(A.20)

On the other hand, by (A.12) and (f₁) we have

$$ \Delta _{p}(u-u_{0})=b(x) \bigl(f(u)-f(u_{0}) \bigr)\geq0, \quad x\in\Omega^{\eta }={x\in\Omega\mbox{: }d(x)> \eta}. $$

(A.21)

The maximum principle implies that $u-u_{0}\leq\theta$ in $\Omega^{\eta}$, and hence $u-u_{0}\leq\theta$ in the whole Ω. Then the strong maximum principle gives $u-u_{0}\equiv\theta$. We obtain that $f(u)=f(u+\theta)$ in Ω, which can only hold if $\theta=0$. Thus, $u=u_{0}$, which shows the uniqueness. □

Authors’ Affiliations

(1)

Department of Fundamental Courses, Qingdao College, Qingdao Technological University

(2)

School of Mathematical Sciences, Ocean University of China

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The first and second expansion of large solutions for quasilinear elliptic equations with weight functions

Abstract

Keywords

MSC

1 Introduction and main results

Theorem 1

Remark 1

Theorem 2

Remark 2

Remark 3

2 Preliminary results

2.1 Properties of regularly varying function

Definition 1

Definition 2

Proposition 1

Proposition 2

Proposition 3

Proposition 4

Proposition 5

Proposition 6

2.2 Auxiliary results

Lemma 1

Lemma 2

Lemma 3

Proof

Lemma 4

Proof

3 Proofs of main results

Lemma 5

Proof of Theorem 1

Proof of Theorem 2

Declarations

Acknowledgements

Authors’ Affiliations

References

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