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        A BOUNDARY SCHWARZ LEMMA FOR PLURIHARMONIC MAPPINGS FROM THE UNIT POLYDISK TO THE UNIT BALL?

        2018-07-23 08:42:28LingLI李靈HongyiLI李紅裔DiZHAO趙迪

        Ling LI(李靈)Hongyi LI(李紅裔)Di ZHAO(趙迪)

        LMIB,School of Mathematics and Systems Science,Beihang University,Beijing 100191,China

        E-mail:normalee 2013@163.com;hylbuaa@163.com;zdhyl2010@163.com

        Abstract In this article,we present a Schwarz lemma at the boundary for pluriharmonic mappings from the unit polydisk to the unit ball,which generalizes classical Schwarz lemma for bounded harmonic functions to higher dimensions.It is proved that if the pluriharmonic mapping f∈P(Dn,BN)is C1+αat z0∈Er??Dnwith f(0)=0 and f(z0)=w0∈?BN for any n,N ≥ 1,then there exist a nonnegative vector λf=(λ1,0,···,λr,0,···,0)T ∈ R2n satisfyingfor 1≤ i≤ r such that whereand are real versions of z0and w0,respectively.

        Key words Boundary Schwarz lemma;pluriharmonic mapping;unit polydisk;unit ball

        1 Introduction

        As one of the most famous results in complex analysis,the Schwarz lemma[1–10]has drawn much attention in recent years,especially in several complex analyses.Some commonly known results,such as Schwarz lemmas for holomorphic mappings corresponding to the unit ball and polydisk[1,2,13,14],the boundary Schwarz lemma for holomorphic mappings between unit balls[3],and the Schwarz-Pick type estimates of pluriharmonic mappings in the unit polydisk[4],play important roles in the field of Schwarz lemma research.For example,as an indirect extension of results in[1],authors in[5]presented a Schwarz-Pick lemma for the modulus of holomorphic mappings between p-balls.With the popularity of Schwarz lemma,furthermore,some extended results associated with boundary Schwarz lemma have also been presented based on different mappings and domains,such as pluriharmonic mappings between unit balls[6],and Schwarz lemma at the boundary of strongly pseudoconvex domain in Cn[7].Theories on strongly pseudoconvex are also hot topics discussed like Schwarz lemma.Specially in[11,12],discussions about peak function are really similar to the results of boundary Schwarz lemma.However,so far as we know,there is no discussions about boundary Schwarz lemma presented for the pluriharmonic mappings from the polydisk to the unit ball,and that is the most direct reason for us to write this article.

        And Cα(V)represents the set of all functions f on a bounded domain V ∈Cnfor which

        Classical Schwarz lemma[1]states that for every holomorphic mapping of D into itself satisfying the condition f(0)=0,it holds that

        which implies

        holds for every holomorphic mapping g of D into itself.In[2],the result of boundary Schwarz lemma for holomorphic mappings on D is described as follows.

        Theorem 1.1([8]) Let f be the self-holomorphic mapping of D.If f is holomorphic at z=1 with f(0)=0 and f(1)=1,then f′(1)≥ 1.

        Specially,Liu et al[2]presented the result of Schwarz lemma for holomorphic mappings from the unit polydisk Dnto the unit ball BNat the boundary,which is described in the following theorem.

        For the harmonic mappings of D into itself,there are also some interesting results closely related to Schwarz lemma.

        Theorem 1.3([6]) If f is a harmonic mapping of D into itself,and f(0)=0,then

        Theorem 1.4([6]) If f is a harmonic mapping of D into itself,then

        Apparently,Theorem 1.4 is a generalized version of Theorem 1.3,where the condition f(0)=0 is removed.

        In[4],Chen et al presented the Schwarz-Pick type estimates of arbitrary order partial derivatives for bounded pluriharmonic mappings defined in the unit polydisk.

        Theorem 1.5([4])Let f∈P(Dn,D),then

        where α =(α1,···,αn)is a multi-index with αj>0,j ∈ {1,···,n}.

        Theorem 1.6([4]) Let f∈P(Dn,BN)for n,N≥1,then

        Specially,if we add the condition that f(0)=0,then

        When n=N=1,(1.8)is equivalent to(1.4).

        Inspired by[2,4,6],but mainly by[2],we consider the boundary Schwarz lemma for pluriharmonic mappings from the unit polydisk to the unit ball in this work.

        As Dnand BNare equivalent to the unit polydisk D2n?R2nand the unit ball B2N?R2N,respectively,we consider the real version of this problem.For z=(z1,···,zn)T∈ Cnwith zj=xj+iyjfor 1 ≤ j ≤ n,denote z′=(x1,y1,···,xn,yn)T∈ R2nas the real version of z.

        Referring to[3],where Liu et al presented the boundary Schwarz lemma for holomorphic mappings between unit balls of different dimensions,and by Theorem 1.6,we get the following boundary Schwarz lemma for pluriharmonic mappings in P(Dn,BN).

        Theorem 1.7Let f∈P(Dn,BN)with f(0)=0 for n,N≥1.For a given z0∈?Dn,assume z0∈Erwith the first r components at the boundary of D for some 1≤r≤n.If f is C1+αat z0and f(z0)=w0∈ ?BN,then there exist a nonnegative vector λf=(λ1,0,···,λr,0,···,0)satisfyingfor 1≤ i≤ r such that

        2 Proof of Theorem 1.7

        The following lemma plays a significant role in the proof of our main result.

        ProofAccording to the description of Theorem 3.1 in[6],it holds that for a nonnegative function f defined on the unit ball B2nin R2n,if f is continuous on the ball and harmonic on its interior,then for any point z′=(x1,y1,···,xn,yn)Twith|z′|=r0<1,we have

        from which we have

        when applying the maximum modulus principle.

        In the following,we will prove Theorem 1.7 by the following five steps.

        which gives that

        Letting xi→1?and referring to[2],we can derive

        for 1≤i≤r(r≤n).

        By the special case of Theorem 1.6,when f(0)=0,

        Considering that

        and it is not difficult to derive

        and

        when referring to[6].Thus,(2.2)is equivalent to

        which means that

        Letting t→0+,we have

        that is,

        that is,

        As(2.4)is valid for any k∈R,it holds that

        which gives

        and

        Same as Step 2,it is not difficult to obtain

        that is,

        which is equivalent to

        As(2.6)and(2.7)is valid for k∈R,

        holds for k≤0 and 1≤j≤r.Thus,we can derive

        because k≤0 is arbitrary.

        from which it is obvious that

        that is,

        As the above equality is valid forwe have

        According to(2.1)and(2.5),it is obvious that

        Similarly,according to(2.9)and(2.10),we have

        Step 5Letbe any given point atwith the first r pairs of components at the boundary of D2?R2,that is,is not necessary,then,there exists a special kind of real-valued diagonal unitary matrix Uz0′such thatwhen referring to[2].Assume that f′is the real version of f,andwhereis not necessaryat?B2N.Then,there exists a Uw0′such that.Denote

        and

        where Uw0and Uz0represent complex unitary matrices corresponding to Uw0′and Uz0′,respectively,such that andThen,we can draw the conclusion that g′is the real version of g andFurthermore,the Jacobian matrix of g could be denoted as

        According to Step 4,it is not difficult to obtain

        that is,

        that is,

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