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Research article

Positive radial solutions for the problem with Minkowski-curvature operator on an exterior domain

  • Received: 20 March 2023 Revised: 07 June 2023 Accepted: 12 June 2023 Published: 27 June 2023
  • MSC : 35A01, 35B09, 35J93, 53A10

  • We are concerned with the problem with Minkowski-curvature operator on an exterior domain

    {div(u1|u|2)=λK(|x|)f(u)uγ   in Bc,un|Bc=0,  lim|x|u(x)=0,(P)

    where 0γ<1, Bc={xRN:|x|>R} is a exterior domain in RN, N>2, R>0, KC([R,),(0,)) is such that RrK(r)dr<, the function f:[0,)(0,) is a continuous function such that limsf(s)sγ+1=0 and λ>0 is a parameter. We show that problem (P) has at least one positive radial solution for all λ>0. The proof of our main result is based upon the method of sub and super solutions.

    Citation: Zhongzi Zhao, Meng Yan. Positive radial solutions for the problem with Minkowski-curvature operator on an exterior domain[J]. AIMS Mathematics, 2023, 8(9): 20654-20664. doi: 10.3934/math.20231052

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  • We are concerned with the problem with Minkowski-curvature operator on an exterior domain

    {div(u1|u|2)=λK(|x|)f(u)uγ   in Bc,un|Bc=0,  lim|x|u(x)=0,(P)

    where 0γ<1, Bc={xRN:|x|>R} is a exterior domain in RN, N>2, R>0, KC([R,),(0,)) is such that RrK(r)dr<, the function f:[0,)(0,) is a continuous function such that limsf(s)sγ+1=0 and λ>0 is a parameter. We show that problem (P) has at least one positive radial solution for all λ>0. The proof of our main result is based upon the method of sub and super solutions.



    In this paper, we are concerned with the problem with Minkowski-curvature operator on an exterior domain

    {div(u1|u|2)=λK(|x|)f(u)uγ   in Bc,un|Bc=0,  lim|x|u(x)=0, (1.1)

    where 0γ<1, Bc={xRN:|x|>R} is a exterior domain in RN, N>2, R>0, the function f:[0,)(0,) is a continuous function such that limsf(s)sγ+1=0 and λ>0 is a parameter. Assume that

    (K1) KC([R,),(0,)) is such that RrK(r)dr<.

    The prescribed mean curvature equation

    div(u1|u|2)=H(x,u)   in Ω (1.2)

    with some boundary value condition is related to problems on a flat Minkowski space with a Lorentzian metric in differential geometry and the theory of classical relativity, see R. Bartnik and L. Simon [1], C. Gerhardt [6] and A. E. Treibergs [15].

    If Ω is a strictly convex bounded domain in RN with C2 boundary Ω, there are some classic papers on the existence of solutions of Eq (1.2) with Dirichlet, Neuuman or periodic boundary conditions using the fixed point theory or topological methods (mostly bifurcation technique), see Bereanu, Jebelean and Mawhin [2,3], Bereanu, Jebelean and Torres [4], Ma, Gao and Lu [10], Obersnel, Omari and Rivetti [12] and the references therein.

    The presence in the existing literature of very few results about the (1.2) in a exterior domain is in sharp contrast with the wide number of works that are available in the bounded domains {setting}. The likely reasons are that the singular coefficient and singular weight will occur in the problems considered on the exterior of a ball and the concave-convex properties of solutions are uncertain owing to the influence of the mean curvature operator and coefficient function, see [16].

    Yang, Lee and Sim [16] concerned with the existence of nodal radial solutions of the following problem

    {div(u1|u|2)=λk(|x|)g(u)   in Bc,u|Bc=0,  lim|x|u(x)=0, (1.3)

    where g:RR a continuous and odd function satisfying g(s)s>0 for s0. As the main assumption on the nonlinearity they required g(0)=0, which guarantees that 0 is the trivial solution of the problem (1.3). Therefore, the bifurcation from the trivial solution can be considered in [16].

    Although Yang, Lee and Sim [16] obtained the existence result of the radial solutions of the problem with mean curvature operator on the exterior domain of a ball; it is worth noticing, however, that the application to problem (1.1) of the method described in [16] is not feasible as nonlinearity in (1.1) is singular at 0.

    Existence of positive radial solutions of the prescribed mean curvature problem (1.1) with singular nonlinearity on the exterior domain of a ball have not been introduced yet as far as the authors know.

    The novelty of this paper is twofold: we develop a method of sub-super solutions for a singular problem with mean curvature operator, and provide a existence result of the positive radial solutions for problem (1.1) which is a prescribed mean curvature problem with singular nonlinearity on the exterior domain of a ball.

    In order to study the radial solutions of (1.1), we transform problem (1.1) into the one-dimensional problem via consecutive transformations r=|x| and t=(rR)(N2) as follows

    {(p(t)φ(1p(t)u(t)))=λh(t)f(u(t))(u(t))γ,   t(0,1),u(0)=u(1)=0, (1.4)

    where φ(y)=y1y2 with y(1,1), p and h can be obtained as

    p(t)=RN2tN1N2,  h(t)=p2(t)K(Rt1N2). (1.5)

    Notice that p(t)>0,p(t)0, t[0,1] and

    hH={qC((0,1),(0,)):10sq(s)ds<}

    since K satisfies RrK(r)dr< (see [16]). We assume that

    (F1) f(s)>0 for all s0;

    (F2)limsf(s)sγ+1=0.

    Theorem 1.1. Let (F1), (F2) and (K1) hold. Then problem (1.1) has at least one positive radial solution for all λ>0.

    Example 1.1. Consider the problem (1.1) with

    K(r)=1r3

    and

    f(s)=sγ+2.

    Obviously, lims0f(s)sγ=, i.e. nonlinearity f(s)sγ is singular at 0. It is easy to check that K and f satisfies

    RrK(r)dr=1R<,  limsf(s)sγ+1=limssγ+2sγ+1=0

    and (F1). According to Theorem 1.1, the problem (1.1) has at least one positive radial solution for all λ>0.

    As a by-product of the proof of Theorem 1.1, we also proved the following theorem.

    Theorem 1.2. Assume that hH. Then for any fixed M>0, the problem

    {(p(t)φ(1p(t)u(t)))=Mh(t)(u(t))γ,   t(0,1),u(0)=u(1)=0 (1.6)

    have a unique positive solution wC([0,1],[0,))C1((0,1],R).

    Remark 1.1. For the existence of solutions of the problems with a elliptic operator on an unbounded domain, see Dai et al. [5], Iaia [7,8], Ko et al. [9] and Ma et al. [11] and the references therein.

    Motivated by [13], we consider the perturbation problem

    {(p(t)φ(1p(t)u(t)))=Mh(t)(u(t))γ,   t(0,1),u(0)=n,u(1)=0, (2.1n)

    where n0 is any constant, M>0 is a fixed constant, p,h are defined by (1.5).

    Lemma 2.1. For each fixed constant n0, problem (2.1)n has at most one positive solution.

    Proof. Assume on the contrary that the functions u1 and u2 are all the positive solutions of (2.1)n and u1u2 on [0,1]. Then there exists t0(0,1] such that u1(t0)u2(t0). Without loss of generality, we assume that u1(t0)>u2(t0). Then there exists an interval [a,b][0,1] such that b is the point of positive maximum of u1(t)u2(t) on [a,b] and

    u1(t)>u2(t)  for  t(a,b],  u1(b)=u2(b),  u1(a)=u2(a).

    Integrating both sides of the equation in (2.1)n over [t,b][a,b], we can obtain

    ui(t)=p(t)φ1(p(b)p(t)φ(1p(b)ui(b))+1p(t)btMh(r)(ui(r))γdr),  i=1,2.

    Integrating both sides of the above equalities from a to b, we have

    ui(b)ui(a)=bap(t)φ1(p(b)p(t)φ(1p(b)ui(b))+1p(t)btMh(r)(ui(r))γdr)dt,  i=1,2.

    By a simple calculation, we can obtain

    u1(b)=u1(a)+bap(t)φ1(p(b)p(t)φ(1p(b)u1(b))+1p(t)btMh(r)(u1(r))γdr)dt<u2(a)+bap(t)φ1(p(b)p(t)φ(1p(b)u2(b))+1p(t)btMh(r)(u2(r))γdr)dt=u2(b).

    This is a contradiction. The proof of Lemma 2.1 is complete.

    Let

    Dn:={vC[0,1]:v(r)n  on  [0,1]}.

    Now, we consider the following problem

    {(p(t)φ(1p(t)u(t)))=Mh(t)(v(t))γ,   t(0,1),u(0)=n,u(1)=0, (2.2n)

    where vDn.

    Lemma 2.2. For each fixed n>0 and each vDn, (2.2)n has a unique solution uC[0,1]C1(0,1] satisfying u(t)n on [0,1].

    Proof. Define A:DnDn by

    (Av)(t)=n+t0p(r)φ1(1p(r)1rMh(τ)(v(τ))γdτ)dr. (2.3n)

    Obviously, φ1(y)=y1+y2 and φ1(y)y for any yR+. Then for any vDn,

    0t0p(r)φ1(1p(r)1rMh(τ)(v(τ))γdτ)drt0p(r)φ1(1p(r)1rMh(τ)nγdτ)drMnγt0p(r)1p(r)1rh(τ)dτdrMnγ101rh(τ)dτdrMnγ10τh(τ)dτ<+

    and (Av)(t) is continuous on [0,1]. This suggests that AvDn and A is well defined.

    Let u=Av, then uC[0,1]C1(0,1], u(0)=n,u(1)=0 and

    u(t)=p(t)φ1(1p(t)1tMh(r)(v(r))γdr),  t(0,1).

    It is easy to verify

    (p(t)φ(1p(t)u(t)))=Mh(t)(v(t))γ,  t(0,1).

    Therefore, u(t) is a solution of problem (2.2)n. The proof of the uniqueness of solution of (2.2)n is similar to that of Lemma 2.1.

    From the definition of mapping A, we can easily get the following lemma.

    Lemma 2.3. Let A:DnDn be the mapping defined by (2.3)n. Then, for any v1,v2Dn with v1(t)v2(t) on [0,1],

    n(Av2)(t)(Av1)(t)(An)(t),  t[0,1].

    We can verify that A:DnDn is a compact continuous mapping. For any fixed n>0, the problem (2.1)n has at least one solution u(t,n)n,t[0,1], by Schauder fixed point theorem, see [13]. Furthermore, the uniqueness of the solution u(t,n) of (2.2)n is guaranteed by Lemma 2.1. Applying the method of similarity to the proof of Lemma 2.1, we can obtain the following result.

    Lemma 2.4. Let u(t,n) be the unique solution of (2.1)n. Then for n1>n2>0, we have

    0u(t,n1)u(t,n2)n1n2,   t[0,1].

    The proof of Theorem 1.2. Let {nj}j=1 be a decreasing sequence which converges to 0. We known that (2.1)nj has a unique solution u(t,nj). From Lemma 2.4, for each j<k,

    0u(t,j)u(t,k)njnk,  t[0,1]. (2.4)

    Then there exists uC[0,1] such that

    limju(t,j)=u(t)0  uniformly on  [0,1].

    Claim. For any t(0,1], u(t)>0.

    Let δ=max0t1u(t,1). From (2.4), we have

    u(t,j)δ,  t[0,1], j=1,2,.

    This suggests that for any j=1,2,

    u(t,j)=nj+t0p(r)φ1(1p(r)1rMh(τ)(u(τ,j))γdτ)dr>t0p(r)φ1(1p(r)1rMh(τ)δγdτ)dr=:ρ,  t(0,1].

    Passing to the limit, we have

    u(t)ρ>0,  t(0,1].

    From the Monotone convergence theorem (see [14]),

    u(t)=t0p(r)φ1(1p(r)1rMh(τ)(u(τ))γdτ)dr.

    It is easy to verify that u is a solution of (2.1)0, i.e., u is a solution of (1.6). The uniqueness of the solution u is guaranteed by Lemma 2.1.

    In this section, we will develop a method of sub-super solutions for (1.4) which is a singular problem with mean curvature operator. By a subsolution of (1.4) we mean a function αC[0,1]C1(0,1] such that

    {(p(t)φ(1p(t)α(t)))λh(t)f(u(t))(α(t))γ,   t(0,1),α(0)=α(1)=0, (3.1)

    and by a supersolution of (1.4) we mean a function βC[0,1]C1(0,1] such that

    {(p(t)φ(1p(t)β(t)))λh(t)f(u(t))(β(t))γ,   t(0,1),β(0)=β(1)=0. (3.2)

    Theorem 3.1. Suppose there exist a subsolution α and a supersolution β of (1.4) such that 0<αβ on (0,1), then (1.4) has at least one positive solution u satisfying αuβ on [0,1].

    Proof. Step 1. Construction of a modified problem. Take a sequence of subintervals of (0,1), say {Ij}j=1, such that

    I1⊂⊂I2⊂⊂⊂⊂Ij⊂⊂Ij+1⊂⊂

    and j=1Ij=(0,1). For any j=1,2,, we are consider the problem

    {(p(t)φ(1p(t)u))=λh(t)f(u)uγ,   tIj,u(t)=α(t),  tIj. (3.3j)

    Let αj=minˉIjα and βj=maxˉIjβ. Define ˉgj:Ij×(0,)R+ by

    ˉgj(t,s)={h(t)f(αj)/αγj,  sαj,h(t)f(s)/sγ,  αj<s<βj,h(t)f(βj)/βγj,  sβj.

    Then we consider the modified problem

    {(p(t)φ(1p(t)u))=λˉgj(t,u),   tIj,u(t)=α(t),  tIj. (3.4j)

    Obviously the restrictions of the functions α and β on Ij are the subsolution and supersolution of (3.4)j, respectively. In other words, for any tIj, αj and βj satisfy

    (p(t)φ(1p(t)αj))λh(t)f(αj)αγj=λˉgj(t,αj),

    and

    (p(t)φ(1p(t)βj))λh(t)f(βj)βγj=λˉgj(t,βj).

    Step 2. Every solution uj of (3.4)j satisfies αujβ on Ij. Let wj=(ujαj)C1(ˉIj) and Ij={tIj:uj(t)αj(t)}. By a calculation, we obtain

    Ijp(t)φ(1p(t)uj(t))(ujαj)dt=Ij(p(t)φ(1p(t)uj(t)))(ujαj)dt=λIjˉgj(t,uj)(ujαj)dt=λIjˉgj(t,uj)(ujαj)dt,

    and

    Ijp(t)φ(1p(t)αj(t))(ujαj)dt=Ij(p(t)φ(1p(t)αj(t)))(ujαj)dtλIjˉgj(t,αj)(ujαj)dt=λIjˉgj(t,αj)(ujαj)dt.

    Summing up we obtain

    Ijp(t)[φ(1p(t)uj(t))φ(1p(t)αj(t))](ujαj)dtλIj(ˉgj(t,uj)ˉgj(t,αj))(ujαj)dt=0.

    The strict monotonicity of the function yy/p1|y/p|2 yields (ujαj)=0 a.e. in Ij. Hence, (ujαj)=0 and ujαj on Ij. In a completely similar way we can obtain that ujβj on Ij.

    Step 3. Problem (3.3)j has at least one solution uj, with αujβ on Ij. Define an operator T:C1(ˉIj)C1(ˉIj) which sends any function vC1(ˉIj) onto the unique solution uC1(ˉIj), of the problem

    {(p(t)φ(1p(t)u))=λˉgj(t,v),   tIj,u(t)=α(t),  tIj. (3.5j)

    Similar to Section 2, the operator T is completely continuous. Clearly, uj is a solution of (3.5)j if and only if uj is a fixed point of T. Since for any tIj⊂⊂(0,1), there exist the constant ε2>ε1>0 and c=c(Ij,ε1,ε2)>0 such that ε1<minIjα<maxIjβ<ε2 and

    |ˉg(t,uj)|c   for all  (t,u)ˉIj×[ε1,ε2],

    and then

    deg(IT,[ε1,ε2],0)=1,

    where I is the identity operator. By Step 2 we know that uj satisfies αujβ on Ij and hence it is a solution of (3.4)j as well.

    Step 4. Complete the proof of result. We claim that, for fixed k, there exists Ck>0 such that for all j\geq k+1 . In fact, take J_k such that I_k\subset\subset J_k\subset\subset I_{k+1} . Define g_j(t) = h(t)\frac{f(u_j(t))}{(u_j(t))^\gamma} . Then

    -\big(p\varphi(u_j'/p)\big)' = \lambda g_j\ \ \ \text{on}\ \ J_k.

    Since \{u_j\}_{j\geq k+1} are uniformly bounded on \bar I_{k+1} , we know that there exists c_k > 0 such that

    \|g_j\|_{C(\bar J_k)} < c_k\ \ \ \text{for all}\ \ j\geq k+1.

    This suggests that there exists a constant C_k > 0 such that \|u_j\|_{C^2(\bar I_k)}\leq C_k for all j\geq k+1 .

    Since the embedding C^2(\bar I_k)\hookrightarrow C^1(\bar I_k) is compact, for each k , sequence \{u_j\}_{j = 1}^\infty has a subsequence, renamed \{u_j\}^\infty_{j = 1} , which converges to u in C^1(\bar I_k) . This implies that u\in C^1(\bar I_k) for every k . Consequently, u\in C^1(0, 1) . For any k , we have

    \int_{I_k}p(t)\Big(\varphi\Big(\frac{1}{p(t)}u_j'(t)\Big)\Big)\phi'(t)dt = \lambda\int_{I_k}h(t)\frac{f(u_j(t))}{(u_j(t))^\gamma}\phi(t)dt

    for all \phi\in C_0^\infty(I_k) and j\geq k+1 . By taking the limit of the sequence converging in C^1(\bar I_k) ,

    \int_{I_k}p(t)\Big(\varphi\Big(\frac{1}{p(t)}u'(t)\Big)\Big)\phi'(t)dt = \lambda\int_{I_k}h(t)\frac{f(u(t))}{(u(t))^\gamma}\phi(t)dt

    for all \phi\in C_0^\infty(I_k) . Also, since \alpha(t)\leq u_j(t)\leq\beta(t) for all j , we have \alpha(t)\leq u(t)\leq \beta(t) for all t\in(0, 1) . Thus, from \alpha(0) = \beta(0) = 0 and \alpha'(1) = \beta'(1) = 0 , we know that u\in C[0, 1]\cap C^1(0, 1] . This completes the proof of Theorem 3.1.

    Firstly, we construct a positive supersolution \beta of (1.4) . Let f^*(s) = \max\limits_{0\leq r\leq s}f(r) . Obviously, f^*(s) is nondecreasing and

    \frac{f^*(s)}{s^{\gamma+1}}\to 0\ \ \ \text{as}\ \ \ s\to\infty

    since \frac{f(s)}{s^{\gamma+1}}\to 0 as s\to\infty . Then there exists a constant M_\lambda\gg1 such that

    \frac{f^*(M_\lambda\|w\|_\infty)}{(M_\lambda\|w\|_\infty)^{\gamma+1}}\leq\frac{1}{\lambda\|w\|_\infty^{\gamma+1}},

    where w is the unique positive solution of (1.6) with M_\lambda . Then

    \begin{align*} -\Big(p(t)\varphi\big(\frac{1}{p(t)}w'(t)\big)\Big)'& = \frac{M_\lambda h(t)}{w^\gamma}\geq \lambda h(t)\frac{f^*(M_\lambda\|w\|_\infty)}{w^\gamma}\geq \lambda h(t)\frac{f^*(\|w\|_\infty)}{w^\gamma}\\ &\geq \lambda h(t)\frac{f^*(w)}{w^\gamma}\geq \lambda h(t)\frac{f(w)}{w^\gamma}. \end{align*}

    This suggests that w is a positive supersolution of (1.4).

    Next we construct a positive subsolution \alpha of (1.4). For any fixed constant m > 0 , the problem

    \left\{\begin{array}{ll} -\Big(p(t)\varphi\big(\frac{1}{p(t)}u'\big)\Big)' = m h(t),\ \ \ &t\in (0,1),\\[2ex] u(0) = 0, u'(1) = 0 \end{array} \right. (4.1_m)

    has a solution v_m . We can verify that v_m\to0 as m\to 0 . Since \frac{f(s)}{s^\gamma}\to\infty as s\to0 , for any fixed \lambda > 0 , there exists a sufficiently small m_\lambda \ll 1 such that

    m_\lambda \leq\lambda \frac{f(v)}{v^\gamma},

    where v is the solution of (4.1)_{m_\lambda} . Then

    \begin{align*} -\Big(p(t)\varphi\big(\frac{1}{p(t)}v'(t)\big)\Big)'& = m_\lambda h(t)\leq \lambda h(t)\frac{f(v)}{v^\gamma}. \end{align*}

    This suggests that v is a positive subsolution of (1.4) such that v\leq w for sufficiently small m_\lambda .

    From Theorem 3.1, (1.4) has a positive solution for all \lambda > 0 . This completes the proof of Theorem 1.1.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work was supported by National Natural Science Foundation of China (No.12061064) and Shaanxi Fundamental Science Research Project for Mathematics and Physics (Grant No. 22JSY018).

    All authors declare no conflicts of interest in this paper.



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