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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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