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A weighted gradient estimate for solutions of Lp Christoffel-Minkowski problem

  • We extend the weighted gradient estimate for solutions of nonlinear PDE associated to the prescribed k-th Lp-area measure problem to the case 0<p<1. The estimate yields non-collapsing estimate for symmetric convex bodied with prescribed Lp-area measures.

    Citation: Pengfei Guan. A weighted gradient estimate for solutions of Lp Christoffel-Minkowski problem[J]. Mathematics in Engineering, 2023, 5(3): 1-14. doi: 10.3934/mine.2023067

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  • We extend the weighted gradient estimate for solutions of nonlinear PDE associated to the prescribed k-th Lp-area measure problem to the case 0<p<1. The estimate yields non-collapsing estimate for symmetric convex bodied with prescribed Lp-area measures.



    Dedicated to Professor Neil Trudinger on the occasion of his 80th birthday.

    The classical Christoffel-Minkowski problem is a problem of prescribing k-th area measure on Sn. Given a Borel measure μ=fdσSn on Sn, one seeks a convex body KRn+1 such that its k-th area measure Sk(K,x)=μ. It is a fundamental problem in convex geometry. The problem plays important rule in the development of nonlinear geometric partial differential equations.

    The Christoffel-Minkowski problem corresponds to solving the following fully nonlinear elliptic equation

    σk(W(x))=f(x),W(x)>0, xSn, (1.1)

    where u is the support function of K defined on Sn and

    W(x)=(uij(x)+uδij(x)),xSn.

    The Christoffel problem and the Minkowski problem correspond to the cases k=1 and k=n respectively [1,2,4,7,15,16,17]. The notion of area measures in the Brunn-Minkowski theory is based on Minkowski summation. Lutwak [12] developed corresponding Lp Brunn-Minkowski-Firey theory based on Firey's p-sum [5]. Lp-Minkowski problem has attracted much attention, we refer [3,6,12,13,14] and references therein.

    The focus of this paper is on the intermediate Lp-Christoffel-Minkowski problem. The problem is deduced to solve the following PDE on Sn,

    σk(W(x))=up1f(x),W(x)>0, xSn. (1.2)

    p=1 is the classical Christoffel-Minkowski problem [7,17]. The case pk+1 was considered by Hu-Ma-Shen [9] and the case 1<p<k+1 was considered by Guan-Xia [8]. Very little is known for Eq (1.2) in the case 0<p<1.

    In general, admissible solutions to σk(W)=f is not convex (i.e., W>0) if k<n. The existence of geometric solutions of (1.2) relies on two ingredients:

    1) A priori upper and lower bounds of solutions,

    2) Convexity of solutions (i.e., W>0).

    When p1<k<n, in general there is no direct non-collapsing estimate for convex body satisfying Eq (1.2) when k<n. For pk+1, maximum principle implies the upper and lower bounds of solutions [9]. When p<k+1, the lower bound of solutions are not true in general as discussed in examples in [8]. In [8], the upper and lower bounds for even solutions of (1.2) were obtained for 1<p<k+1. The estimate relies on a weighted gradient estimate for |u|2(umu)γ where mu=minxSnu. The purpose of this paper is to extend such estimate for the case 0<p<1.

    Similar to the classical intermediate Christoffel-Minkowski problem, one needs to impose appropriate appropriate conditions on the prescribed function f in Eq (1.1) to ensure the convexity of solutions to (1.2). The key is the Constant Rank Theorem established by Guan-Ma in [7]. When p>1, a corresponding condition was deduced in [9] from the Constant Rank Theorem in [7]. When 0<p<1, it is an open problem to find a clean condition on f to guarantee the convexity of solutions to (1.2).

    In this section, we modify the arguments in [8] to establish a weighted gradient estimate for solutions of the intermediate Christoffel-Minkowski problem (1.2) for 0<p1. Specifically, we extend Proposition 3.1 in [8] to the case 0<p<1. Recall Garding's cone

    Γk={λ=(λ1,,λn)Rn | σj(λ)>0, j=1,,k.}

    A symmetric matrix W is called in Γk if its eigenvalue vector λWΓk. A positive function uC2(Sn) is called an admissible solution to (1.2) if W(x)Γk, xSn.

    In the rest of the paper, we denote

    (λ | 1)=(0,λ2,,λn), λ=(λ1,λ2,,λn)Rn.

    Proposition 2.1. Let 0<p1 and let u be a positive admissible solution to (1.2). Denote mu=minu and Mu=maxu. Set

    γ=2pk+4. (2.1)

    Then there exist some positive constants A depending only on n,k,p and logfC1, such that

    |u|2|umu|γAM2γu. (2.2)

    The weighted gradient estimate for |u|2uγ was used in [6], later in [8,10,11]. It's useful tool to obtain lower bound of solution u.

    Proof. After proper rescale, we may assume minxSnf(x)=1. Maximum principle yields that there is Cn,k,p>0, such that

    MuCn,k,p.

    Set

    Φ=|u|2(umu)γ,

    where 0<γ<1 as in (2.1). As pointed out in [8] that Φ is well-defined and it makes sense to define Φ=0 at the minimum point of u.

    Let x0 be a maximum point of Φ. Then u(x0)>mu if u is not a constant. We may pick an orthonormal frame on Sn such that u1(x0)=|u|(x0) and ui(x0)=0 for i=2,,n. At x0,

    2ululi|u|2=γuiumu for each i.

    Thus u1i=0 for i=2,,n and

    u11=γ2u21umu=γ2Φ1(umu)1γ. (2.3)

    Re-rotating the remaining n1 coordinates, we may assume

    (uij)  is diagonal, so are (Wij(x0)) and (Fij)(x0)=(σkWij)(x0).

    We may assume ΦM2γu is sufficiently large at x0. In the rest of proof, constant C may change line by line, but under control.

    W11u11(1+C(M2γuΦ)). (2.4)

    At x0, it follows from (2.3) and (1.2),

    0Fii(logΦ)ii=Fii2u2ii+2ululii|u|2γFiiuiiumu+γ(1γ)Fiiu2i(umu)2=2Fiiu2iiu21+2Fiiu1(Wii1uiδ1i)u21γFiiuiiumu+γ(1γ)Fiiu2i(umu)2=2Fiiu2iiu21+2(p1)up2f+2up1f1u12F11γFiiuiiumu+γ(1γ)Fiiu2i(umu)22Fiiu2iiu21+2(p1)up2f+γ(1γ)F11u21(umu)2+2up1f1u12F11γFiiWiiumu2Fiiu2iiu21+2(1γ)F11u11umu+2up1f1u12F11(kγ2(p1))σk(W)umu2(1γ)F11u11umu+2up1f1u1+2F11(u211u211)(kγ2(p1))σk(W)umu. (2.5)

    It follows the definition of Φ,

    2up1f1u1Cup1fΦ12(umu)γ2Cσk(W)umuM1γ2uΦ12. (2.6)

    Note that M2γuΦ sufficiently small by the assumption.

    By (2.3) and (2.4),

    u211u211=γ2u11umu1=γ2W11umu(1CM2γuΦ). (2.7)
    W11γ4Φ(umu)1γγ4ΦM2γuM2γu(umu)1γ. (2.8)

    Put (2.6) and (2.7) to (2.5),

    0(2γCM2γuΦ)F11W11umu(kγ2(p1)+CM1γ2uΦ12)σk(W)umu (2.9)

    We divide in to two cases.

    Case Ⅰ.

    σk(W|1)γσk1(W|1)W11.

    We have,

    σk(W)=σk1(W|1)W11+σk(W|1)(1+γ)σk1(W|1)W11=(1+γ)F11W11.

    Put this into (2.9), we obtain

    02γ(1+γ)(kγ2(p1)+CM1γ2uΦ12).

    By the choice of γ in (2.1),

    CM1γ2uΦ12pk+4.

    (2.2) is verified in this case.

    Case Ⅱ.

    σk(W|1)>γσk1(W|1)W11.

    If k2, by the Newton-MacLaurin inequality,

    σkk1k1(W|1)Cn,kσk(W|1).

    In turn,

    σkk1k1(W|1)Cn,kσk(W|1)>Cn,kγσk1(W|1)W11.

    Hence, σ1k1k1(W|1)Cn,kγW11. We now have,

    up1f=σk(W)=σk(W|1)+σk1(W|1)W11(1+γ)σk1(W|1)W11(Cn,kγ)k1Wk11.

    Note that the above inequality is trivial for k=1 in this case. We obtain

    W11(Cn,kγ)k1kup1kf1k. (2.10)

    Then (2.2) follows from (2.10), (2.3) and (2.4).

    When u is a convex solution of (1.2), estimate (2.2) in Proposition 2.1 can be refined. We will use this type of refined estimates to establish existence of convex even solutions for Eq (1.2) when 0<1p is close to 0.

    Proposition 2.2. Let 0<p1 and let u be a positive convex solution to (1.2).

    a. If k=1, then

    Mγ2u|u(x)|2(u(x)mu)γ(2nγ)γpeγπplogfC0, 0<γ<1.  xSn. (2.11)

    b. If 2k<n, then there exists An,k,p depending only on n,k,p, such that

    Mγ2u|u|2|umu|γAn,k,peγπk1+plogfC0, (2.12)

    where

    γ=pk+1. (2.13)

    Proof. For 0<γ<1, let Φ=|u|2(umu)γ as in the proof of Proposition 2.1. We may assume

    minxSnf(x)=1.

    By Eq (1.2),

    Mk+1pu(nk)!k!n!. (2.14)

    Set

    q=2γp, β=1p(1γ), (2.15)

    and

    Aγ=maxxSnΦ(x)M2γu=Φ(x0)M2γu. (2.16)

    We want to estimate Aγ.

    Suppose x0 is a maximum point of Φ. Let η>0 is a positive number to be determined. If,

    (u(x0)muMu)1γ(γη)β,

    then

    (u(x0)mu)γMγu(γη)2q.

    Since u is convex, |u(x)|2M2u, xSn. We have

    Aγ=Φ(x0)M2γuMγu(umu)γ(ηγ)2q. (2.17)

    We now assume that at x0,

    (umuMu)1γ(γη)β. (2.18)

    As in the proof of Proposition 2.1, one may pick an orthonormal frame on Sn near x0, such that |u(x0)|=u1(x0), (Wij(x0)) is diagonal,

    u11=γ2u21umu=γ2AγM2γu(umu)1γ, (2.19)

    and

    W11>u11=γ2AγM2γu(umu)1γ. (2.20)

    We first consider the simple case k=1.

    Case k=1. Since p1, up1(umu)p1. By (2.20), at maximum point x0 of Φ,

    (umu)p1fup1f=σ1(W)W11u11=γ2AγM2γu(umu)1γ.

    It follows

    Aγ2nγ(umuMu)pγMp2uf2nγ(γη)(pγ)(2q)γf2nγ(γη)(pγ)(2q)γeπlogfC0, (2.21)

    here we used minxSnf(x)=1 and (2.14) for k=1. Use (2.15) to equalize quantities on the right hand sides of (2.17) and (2.21), we pick

    η=2neπlogfC0.

    Thus,

    Aγγγp(2neπlogfC0)γp, 0<γ<1.

    (2.11) is proved. We may let γ1,

    |u(x)|2u(x)mu(2neπlogfC0)1pMu, xSn. (2.22)

    We note that in this case, bound on f can be replaced by ratio of Mfmf in above estimate.

    Case 2k<n. At x0,

    W11=u11(1+2γA1γu(umu)1γM2γu). (2.23)

    By (2.5),

    02(1γ)F11u11umu+2up1f1u1+2F11(u211u211)(kγ2(p1))σk(W)umu. (2.24)

    Since f1flogfC0, (2.6) can be refined as

    2up1f1u12up1flogfC0Φ12(umu)γ2=2logfC0A12γ(umuMu)1γ2σk(W)umu. (2.25)

    By (2.19), (2.23) and (2.20),

    u211u211=γ2u11umu1γ2W11umu(18γ2A1γu(umu)1γM2γu). (2.26)

    Put (2.25) and (2.26) to (2.24), as p1,

    0(2γ)F11W11umu{kγ2(p1)+(4γA1γu(umu)1γM2γu+2logfC0A12γ(umuMu)1γ2)}σk(W)umu. (2.27)

    Choose

    η=(22k1(nk)k1nkkeπlogfC0)pk1+p, (2.28)

    and

    γ=pk+1, δ=12γ1pp. (2.29)

    We divide in to two subcases.

    Subcase Ⅰ. Assume that

    σk(W|1)>δσk1(W|1)W11.

    If k2, by the Newton-MacLaurin inequality,

    σkk1k1(W|1)Cn,kσk(W|1),

    where

    Cn,k=knk((n1)!(nk)!(k1)!)1k1. (2.30)

    In turn,

    σkk1k1(W|1)Cn,kσk(W|1)>Cn,kδσk1(W|1)W11.

    Hence,

    σ1k1k1(W|1)Cn,kδW11.

    By Eq (1.2),

    up1f=σk(W)σk1(W|1)W11(Cn,kδ)k1Wk11. (2.31)

    Note that (2.31) is trivial for k=1 in this subcase. Thus it is true k1. As p1, up1k(umu)p1k, we deduce from (2.20) and (2.31) that,

    Aγ2γ(Cn,kδ)1kkM1+p1ku(umuMu)1γ+p1kf1k.

    By (2.18), (2.14), (2.28), (2.29) and (2.30), and the fact that minf=1,

    Aγ2γ(Cn,kδ)1kkM1+p1ku(γη)2qγ(1γ+p1k)eπklogfC02(Cn,k2)1kk(n!(nk)!k!)1k(1η)2qγ(1+p1k)eπklogfC0(γη)q2=(γη)q2. (2.32)

    Subcase Ⅱ. Assume that

    σk(W|1)δσk1(W|1)W11.

    We have,

    σk(W)=σk1(W|1)W11+σk(W|1)(1+δ)σk1(W|1)W11=(1+δ)F11W11.

    Put this into (2.27), we obtain

    02γ(1+δ){kγ2(p1)+(4γA1γu(umu)1γM2γu+2logfC0A12γ(umuMu)1γ2)}.

    From (2.13) and (2.29),

    2γ(1+δ)(kγ2(p1))γ(1+δ).

    Hence

    0γ(4γA1γu(umu)1γM2γu+2logfC0A12γ(umuMu)1γ2).

    Again by (2.13) and (2.29),

    4γA1γu(umu)1γM2γu+2logfC0A12γ(umuMu)1γ2γ.

    It follows from (2.18) that,

    4γA1γ(γη)1γp+2logfC0A12γ(γη)1γ2pγ.

    We obtain

    Aγ8(η1pγ1p2+logf2C0η2pγ2p2)(ηγ)γp=8(η1pγ1p2+logf2C0η2pγ2p2)(ηγ)2q. (2.33)

    By (2.13) and (2.28), direct computation yields

    η1pγ1p2+logf2C0η2pγ2p24ek+2π2e2k4.

    We obtain that

    Aγ(4ek+2π2e2k4)(ηγ)γp, (2.34)

    where γ,η as in (2.13) and (2.28).

    Remark 2.1. Constant An,k,p in Proposition 2.2 can be computed explicitly. We observe that if u is even, (2.22) and (2.12) in Proposition 2.2 can be improved respectively as

    Mγ2u|u(x)|2(u(x)mu)γ(2nγ)γpeγπ2plogfC0, 0<γ<1,  xSn. (2.35)

    and

    Mγ2u|u|2|umu|γAn,k,peγπ2(k1+p)logfC0. (2.36)

    This is due to the fact that one may choose maximum and minimum points of f such that the distance is at most π2 in this case.

    Remark 2.2. It is of interest to obtain some form of weighted gradient estimate for Eq (1.2) in the case p=0.

    In general, there is no positive lower bound for convex solutions of (1.2) when p<k+1 [8]. We may obtain lower bound for even convex solutions of (1.2) in the case of 0<p<1.

    For convex body ΩRn+1, denote ρ(Ω) and ρ+(Ω) to be the inner radius and outer radius of Ω respectively.

    Lemma 3.1. If u is a positive convex function on Sn satisfying condition

    |u(x)|2(u(x)mu)γAM2γu, xSn, (3.1)

    for some γ>0, A>0. Let Ωu be the convex body with support function u, and suppose there is an ellipsoid E centred at the origin such that

    EΩuβE. (3.2)

    Then the following non-collapsing estimate holds,

    ρ+(Ωu)ρ(Ωu)β2γ+1A1γ24γ(2γ). (3.3)

    Proof. Write E

    x21a21++x2n+1a2n+11

    with longest axis a1, and the shortest axis an+1. We have

    a1Muβa1,an+1muβan+1.

    Recall that

    uE(x)=a21x21+a22x22++a2n+1x2n+1,xSn

    By (3.2), support functions of Ω and E are equivalent.

    uE(x)u(x)(n+1)uE(x), xSn.

    Restrict the support function uE,u to the slice S:={xSn|x=(x1,0,,0,xn+1)}. Set

    v(s):=uE(s,0,,0,1s2)=a21s2+a2n+1(1s2)=a2n+1+(a21a2n+1)s2.

    We have

    taγ21a2γ2n+1v(t(an+1a1)2γ2), t[0,1].

    On the other hand, set q(s)=(u(s,0,,0,1s2)mu)2γ2. By the weighted gradient estimate (3.1),

    |ddsq(s)|A12M1γ2uA12β1γ2a1γ21.

    This implies, 0<t1,

    q(t(an+1a1)2γ2)tA12β1γ2(an+1a1)2γ2a1γ21+q(0)=tβ1γ2A12a2γ2n+1+q(0).

    As q(0)β2γ2a2γ2n+1,

    q(t(an+1a1)2γ2)(tβ1γ2A12+β2γ2)a2γ2n+1.

    Thus,

    u((an+1a1)2γ2,0,,0,1(an+1a1)2γ)β1γ2(tA12+1)22γan+1.

    Since u(x)uE(x), we obtain

    taγ21a2γ2n+1β(tA12+1)22γan+1.

    This yields

    a1an+1(βt(tA12+1)22γ)2γ.

    Choose t=A12,

    a1an+1β2γA1γ24γ(2γ). (3.4)

    Corollary 3.1. If u is a positive, even, convex solution to (1.2) for 0<p<k+1. Then

    Mumu(An,k,peγπ2(k1+p)logfC0)1γ(n+1)1γ+1224γ(2γ), (3.5)

    where γ and An,k,p as in Proposition 2.2. As a consequence,

    |u(x)|2u2(x)(An,k,peγπ2(k1+p)logfC0)2γγ+1(n+1)4γ22γ24γ. (3.6)

    In the case k=1,

    |u(x)|2u2(x)8(n+1)32(2n)2peπplogfC0. (3.7)

    Moreover, there exist positive constant C1, C2 depending only on n,k,p,logfC1, such that

    C1u(x)C2>0, xSn;uC1(Sn)C.

    Proof. Since Ωu is even, we may pick β=n+1 in (3.2). We let A=An,k,peγπ2(k1+p)logfC0 as in (2.36). (3.5) follows Lemma 3.1. By (3.5),

    |u(x)|2u2(x)=|u(x)|2uγ(x)M2+γu(Muu)2γ|u(x)|2(umu)γM2+γu(Mumu)2γ(An,k,peγπ2(k1+p)logfC0)2γγ+1(n+1)4γ22γ24γ.

    Inequality (3.7) follows from (2.35). By Eq (1.2), mu is bounded from above and Mu is bounded from below. Therefore, u is bounded from below and above by (3.5).

    Lemma 3.1 yields a direct estimate of inner radius of the classical Christoffel-Minkowski problem: convex solutions to Eq (1.1). When k=n, such estimate was proved in [2], it also follows from John's lemma. For k<n, we are not aware any such estimate in the literature.

    Lemma 3.2. Suppose u is convex solution to (1.1). Let Ω be the convex body determined by u as the support function, let ρ(Ω) be the inner radius of Ω. Then there exist positive constants C1, C2 depending only on n,k and logfC1, such that

    C2ρ+(Ω)ρ(Ω)C1.

    Proof. As we may shift the origin to the center of the ellipsoid E in (3.2) with β=n+1. Lemma follows Lemma 3.1, since mu is bounded from above and Mu is bounded from below by (1.1).

    With the upper and lower bounds of u for solutions of (1.2), the maximum principle (e.g., [8]) yields C2 estimate. Higher regularity a priori estimates follows the standard elliptic theory.

    Proposition 3.1. Let u be a positive, even convex solution to (1.2). For any lZ+ and 0<α<1, there exists some positive constant C, depending on n,k,p,l,α and logfCl, such that

    uCl+1,α(Sn)C. (3.8)

    For Lp Christoffel-Minkowski problem, we want to find solution u of (1.2) which is convex, i.e., W>0. The sufficient condition introduced in [7] for convexity of solution u to equation (1.1) is

    ((f1k)ij(x)+f1k(x)δij)0, xSn. (4.1)

    Corresponding condition for (1.2) for p>1 is

    ((˜f1k)ij(x)+˜f1k(x)δij)0, xSn, (4.2)

    where ˜f=up1f. Write ˜h=log˜f=(p1)logu+logf, (4.2) is equivalent to

    1k(˜h)2+k˜h(x)0, xSn, (4.3)

    where derivatives are along any geodesic passing through x. Denote ϕ=logf, (4.3) is equivalent to

    1k(ϕ)2+kϕ+(p1){uu+(1+p1k)(uu)2+2kuuϕ}0. (4.4)

    In the case p1, it was observed in [9] that (4.2) would be valid if f satisfies

    ((f1k+p1)ij(x)+f1k+p1(x)δij)>0, xSn. (4.5)

    This relies on the fact that the coefficient p1+(p1)2k in front of term (uu)2 in (4.4) is nonnegative when p1. In the case 0<p<1, p1+(p1)2k<0. If

    k1+pϕ+(p1)(uu)20, (4.6)

    then (4.4) holds, as W is assumed semi-positive definite.

    The main problem is to control (p1)(uu)2 in (4.6) when p<1. When 01p is small, one may impose a condition that f is a positive C2 even function on Sn satisfying

    k1+pϕ+(p1)(An,k,peγπ2(k1+p)ϕC0)2γγ+1(n+1)4γ22γ24γ0. (4.7)

    By Corollary 3.1, Condition (4.7) implies Condition (4.6). The Constant Rank Theorem in [7] implies that there is a convex even solution uC3,α(Sn), 0<α<1 of (1.2).

    In the case k=1, one may use (3.7) to deduce a simpler condition for convex even solutions to Lp Christoffel problem:

    pϕ+8(p1)(n+1)32(2n)2peπplogfC00, (4.8)

    Conditions (4.7) and (4.8) are not satisfactory. It only makes some sense when 1p is small. It is an open problem to find a clean pointwise condition on f for existence of convexity solutions to equation (1.2), 0<p<1.

    Research is supported in part by an NSERC Discovery grant.

    The author declares no conflict of interest.



    [1] C. Berg, Corps convexes et potentiels spheriques, 1969.
    [2] S. Y. Cheng, S. T. Yau, On the Regularity for the Solution of the n-dimensional Minkowski Problem, Commun. Pure Appl. Math., 24 (1976), 495–516. https://doi.org/10.1002/cpa.3160290504 doi: 10.1002/cpa.3160290504
    [3] K. S. Chou, X. J. Wang, The Lp-Minkowski problem and the Minkowski problem in centroaffine geometry, Adv. Math., 205 (2006), 33–83. https://doi.org/10.1016/j.aim.2005.07.004 doi: 10.1016/j.aim.2005.07.004
    [4] W. J. Firey, The determination of convex bodies from their mean radius of curvature functions, Mathematik, 14 (1967), 1–13. https://doi.org/10.1112/s0025579300007956 doi: 10.1112/s0025579300007956
    [5] W. J. Firey, p-Means of convex bodies, Math. Scand., 10 (1962), 17–24. https://doi.org/10.7146/math.scand.a-10510 doi: 10.7146/math.scand.a-10510
    [6] P. Guan, C. S. Lin, On equation det(uij+δiju)=upf on Sn, NCTS in Tsing-Hua University, 2000, preprint No 2000-7.
    [7] P. Guan, X. Ma, The Christoffel-Minkowski problem. I. Convexity of solutions of a Hessian equation, Invent. Math., 151 (2003), 553–577. https://doi.org/10.1007/s00222-002-0259-2 doi: 10.1007/s00222-002-0259-2
    [8] P. Guan, C. Xia, Lp Christoffel-Minkowski problem: the case 1pk+1, Calc. Var., 57 (2018), 69. https://doi.org/10.1007/s00526-018-1341-y doi: 10.1007/s00526-018-1341-y
    [9] C. Hu, X. Ma, C. Shen, On the Christoffel-Minkowski problem of Firey's p-sum, Calc. Var., 21 (2004), 137–155. https://doi.org/10.1007/s00526-003-0250-9 doi: 10.1007/s00526-003-0250-9
    [10] Y. Huang, Q. Lu, On the regularity of the Lp Minkowski problem, Adv. Appl. Math., 50 (2013), 268–280. https://doi.org/10.1016/j.aam.2012.08.005 doi: 10.1016/j.aam.2012.08.005
    [11] Q. Lu, The Minkowski problem for p-sums, Master thesis, McMaster University, 2004.
    [12] E. Lutwak, The Brunn-Minkowski-Firey theory. I. Mixed volumes and the Minkowski problem, J. Differential Geom., 38 (1993), 131–150. https://doi.org/10.4310/jdg/1214454097 doi: 10.4310/jdg/1214454097
    [13] E. Lutwak, V. Oliker, On the regularity of solutions to a generalization of the Minkowski problem, J. Differential Geom., 41 (1995), 227–246. https://doi.org/10.4310/jdg/1214456011 doi: 10.4310/jdg/1214456011
    [14] E. Lutwak, D. Yang, G. Zhang, On the Lp-Minkowski problem, Trans. Amer. Math. Soc., 356 (2004), 4359–4370. https://doi.org/10.1090/S0002-9947-03-03403-2 doi: 10.1090/S0002-9947-03-03403-2
    [15] L. Nirenberg, The Weyl and Minkowski problems in differential geometry in the large, Commun. Pure Appl. Math., 6 (1953), 337–394. https://doi.org/10.1002/cpa.3160060303 doi: 10.1002/cpa.3160060303
    [16] A. V. Pogorelov, Regularity of a convex surface with given Gaussian curvature, Mat. Sb., 31 (1952), 88–103.
    [17] A. V. Pogorelov, The Minkowski multidimensional problem, New York: Wiley, 1978.
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