SciELO - Scientific Electronic Library Online

 
vol.46 número1On the relationship between disjunctive relaxations and minors in packing and covering problemsEta series and eta invariants of Z4-manifolds índice de autoresíndice de materiabúsqueda de artículos
Home Pagelista alfabética de revistas  

Servicios Personalizados

Revista

Articulo

Indicadores

  • No hay articulos citadosCitado por SciELO

Links relacionados

  • No hay articulos similaresSimilares en SciELO

Compartir


Revista de la Unión Matemática Argentina

versión impresa ISSN 0041-6932versión On-line ISSN 1669-9637

Rev. Unión Mat. Argent. v.46 n.1 Bahía Blanca ene./jun. 2005

 

The Bergman Kernel on Tube Domains

Ching-I Hsin,

Minghsin University of Science and Technology, Taiwan.

Abstract
Let Ω  be a bounded strictly convex domain in  n  R  , and        n  TΩ ⊂ C  the tube domain over Ω  . In this paper, we show that the Bergman kernel of T Ω   can be expressed easily by an integral formula.

2000 Mathematics Subject Classification : 32A07, 32A25.

Key words and phrases. Bergman kernel; Tube domain.

1. Introduction

Let        n  T  ⊂ C  be a domain. The Bergman kernel (see for instance [4]) K : T × T - →  C  is one of the important holomorphic invariants associated to T  , but it is often difficult to compute K  . We shall show that if T  is a tube domain over a bounded strictly convex domain, then an easy computation leads quickly to its Bergman kernel.

Let Ω ⊂ Rn  be a bounded strictly convex domain. We are interested in domains T = T        Ω   of the type
TΩ = {x +  iy ; y ∈ Ω}  ⊂ Cn,
(1.1)

known as the tube domain over Ω  . Let K(z, w)  be the Bergman kernel of T Ω   . The main result of this paper is as follows.

Theorem The Bergman kernel on the tube domain TΩ   is given by
             1   ∫   eit(z- ¯w)                 ∫  K(z, w) =  ----n-    -------dt,  where   γt =   e -2txdx.             (2π)   Rn   γt                      Ω
(1.2)

Given a function h  on T Ω   , we shall say that K(z, w)  reproduces h  if

∫        K(z, w)h(w) dV   =  h(z),   w∈TΩ
(1.3)

where dV  is the Lebesgue measure on T Ω   . Let A2(TΩ)  denote the Bergman space, namely the Hilbert space of all holomorphic functions h  on TΩ   in which
∫             2    z∈T  ∣h(z)∣ dV.      Ω
(1.4)

The Bergman kernel K(z, w)  is uniquely characterized by the following three properties:

(i)           --------  K(z, w) = K(w,  z)  for all z,w ∈ TΩ   ;

(ii) K(z,  w)  reproduces every element in A2(T Ω)  in the sense of (1.3);

(iii)              2  K( - ,w) ∈  A (TΩ)  for all w ∈  TΩ   .

Our formulation of K(z, w)  in (1.2) clearly satisfies condition (i). Therefore, to prove the theorem, we need to check conditions (ii) and (iii). This will be done by Propositions 2.4 and 2.5 in the next section.

2. The Bergman kernel on tube domains

Let Ω  be a bounded strictly convex domain in Rn  , and let TΩ   be the tube domain as defined in (1.1). Since Ω  is strictly convex, TΩ   is strictly pseudoconvex.

Let γ   t  and K(z, w)  be defined as in (1.2). The Bergman space A2(T  )       Ω  consists of holomorphic functions h  which satisfy (1.4). In this section, we show that K(z, w)  satisfies conditions (ii) and (iii) stated in the Introduction. Let P  denote the polynomial functions, and we define

   -z2           -z2  P e    =  {p(z)e    ; p(z) polynomial }.

Lemma 2.1 K(z, w)  reproduces every element of   - z2  Pe   .

Proof: The following identity shall be useful:
∫                  √ --        2      e-p2x2+zxdx =  (--π)n exp(-z--) , p > 0,z ∈ Cn.   Rn                 p        4p2
(2.1)

Here x2, zx,z2   denote the usual dot product. In deriving this identity, we observe that both sides of (2.1) are holomorphic in z ∈ Cn  . Therefore, it suffices to check that it holds on the totally real subspace z ∈ Rn  . This can be obtained from standard integration tables ([3], 3.323 ♯  2).

Write w = x +  iy  on T   Ω   , where x,y  are variables on Rn, Ω  respectively. Then

∫        K(z, w)e- w2dV   w∈TΩ  ∫       ∫                          2  = (21π)n- (x,y)∈TΩ t∈Rn eit(z-(x-iy))γ-t 1e- (x+iy)dt dx dy    --1--∫   ∫  ∫                2                           2  -1  = (2π)n  Rn  Ω( Rn exp(- itx - x  - 2ixy)dx) exp(itz - ty + y )γt dy dt  = --√1--∫   ∫  exp(- (t+2y)2)exp(itz - ty + y2)γ-1dy dt                 by (2.1)    (2 π)n∫Rn ∫Ω          4                      t  = --√1-n   n   exp(- t2-  2ty + itz)γ-t 1dy dt    (2 π) ∫R   Ω     2 4  = (2√1π)n Rn exp(- t4 + itz)dt     -z2  = e   .                                                                by (2.1)

Consequently,
∫                2         2        K(z, w)e- w dV  = e-z  ,  z ∈ T Ω.   w∈TΩ
(2.2)

From (2.2), substitute z ∈ T Ω   with z + c ∈ TΩ   , where c ∈ Rn  . This gives

  1  ∫      ∫    eit(z+c-w¯)    2              2  ----n-           ---------e- w dtdV  = e-(z+c).  (2 π)   w∈TΩ  t∈Rn     γt

Changing the variable w  to w + c  in LHS gives

  1   ∫     ∫     eit(z- ¯w)  ------            -------e-(w+c)2dt dV =  e-(z+c)2.  (2π)n  w∈TΩ  t∈Rn   γt

Apply ddc∣c=0   to both sides, we see that K(z,  w)  reproduces the function        2  - 2ze-z   . We carry out the procedure -dk  dck∣c=0   for k =  1,2,...  , and Lemma 2.1 follows.

We plan to show that K(z, w)  reproduces every element of   2  A  (TΩ)  . In view of Lemma 2.1, this will follow if we can show that    -z2  P e   is a dense subset of the Hilbert space A2(T Ω)  . This will be established by the next two lemmas. Our strategy is to convert the problem on A2(T Ω)  to another Hilbert space L2(Rn, γt)  by Lemma 2.2, and obtain a result on   2  n  L  (R ,γt)  by Lemma 2.3. We then transfer this result back to   2  A  (TΩ)  , by Proposition 2.4.

Let L2(Rn, γt)  denote the Hilbert space of L2   functions on Rn  , with weight γt  given in (1.2). Namely,

                  ∫    2  n                     2  L  (R  ,γt) = {f ;  Rn ∣f (t)∣ γtdt <  ∞}.

Lemma 2.2 (T. G. Genchev) The transformation
          ∫  g(t)  ↦-→       eiztg(t) dt             Rn
(2.3)

is an isometry from L2(Rn, γt)  to A2(TΩ)  , preserving the Hilbert space norms.

Proof: Given h(z) ∈ A2(T Ω)  , there exists g(t) ∈ L2(Rn, γt)  such that
       ∫  h(z) =     eiztg(t)dt,          Rn
(2.4)

see [1],[2]. This means that the transformation in (2.3) is surjective. In order to see that (2.3) is well-defined, injective and preserves the norms, we shall prove that in (2.4), ∥h ∥A2(TΩ) = ∥g ∥L2(Rn,γt)   .

Write z = x + iy  , and (2.4) gives

              ∫                     -ixt  -yt  h(- x + iy) =   n e   (e   g(t))dt.                 R

Thus for every fixed y ∈ Ω  , h(- x + iy)  is the Fourier transform of  -yt  e   g(t)  . By Plancherel's theorem,

∫                     ∫      ∣h(- x + iy)∣2dx =     ∣e-ytg(t)∣2dt.   Rn                     Rn

Apply ∫  dy   Ω  to both sides, we get

             ∫  ∫  ∥h∥2A2(TΩ)  =  Ω  Rn ∣h( - x + iy)∣2dx dy               ∫  ∫    - yt    2             =  Ω  Rn ∣e   g(t)∣ dtdy             = ∫   ∣g(t)∣2γ dt                Rn        t             = ∥g ∥22 n   .                   L (R ,γt)

This proves Lemma 2.2. □

Next we define

  - t2-          - t2  Pe  4  =  {p(t)e 4 ; p(t) polynomial }.

Lemma 2.3      t2-  P e- 4   is dense in the Hilbert space L2(Rn, γt)  .

Proof: We shall show that
{tke- t24 }, ∣k∣ = 0,1,2,...
(2.5)

is a complete basis of  2   n  L (R  ,γt)  , and the lemma follows.

Let f(t) ∈ L2(Rn, γt)  , and suppose that
∫        t2      tke- 4 f (t)γtdt =  0    Rn
(2.6)

for all ∣k ∣ = 0,1, 2,...  . It is easy to see that    2  e- t2 γ2t  is bounded, so

∫     - t2     2        ∫        2    - t2-2   Rn ∣e 4 f(t)γt∣ γtdt  =   Rn ∣f(t)∣γt(e 2 γt) dt                        ≤ c ∫   ∣f (t)∣2γ dt                             Rn        t                        < ∞,    as f(t) ∈ L2(Rn, γt).

Therefore,  - t2         2  n  e  4 f(t)γt ∈ L (R ,γt)  . Let
       ∫        t2  h(z) =     eizte- 4 f(t)γtdt.          Rn
(2.7)

By Lemma 2.2, h(z) ∈ A2(T Ω)  . We may assume that 0 ∈ TΩ   , and consider the power series expansion

       ∑      k  h(z) =    akz

near 0  . Then

ak  = k1!h(k)(0)        -1 ∣k∣∫    k - t2      = k!i   Rn t e 4 f(t)γtdt  by (2.7)      = 0.                       by (2.6)

So h(z)  vanishes near 0  . However, since h(z)  is holomorphic, it follows that h ≡  0  . By Lemma 2.2,

 - t2-  e  4 f(t)γt ≡  0.

Since   t2  e- 4   and γt  are always positive,

f ≡  0.

This shows that the functions in (2.5) form a complete basis of   2  n  L (R  ,γt)  , and the lemma is proved. □

We combine Lemmas 2.1, 2.2 and 2.3 to show that:

Proposition 2.4 The function K(z, w)  of (1.2) reproduces every element of   2  A  (TΩ)  .

Proof: We claim that    -z2  P e   is dense in   2  A  (TΩ)  . Identity (2.1) implies that

∫       izt- t42      √ --n -z2   Rn e     dt = (2  π) e   .

Applying d-  dz  repeatedly to both sides, we see that if p(t)  is a polynomial, then

∫       izt    - t24-          - z2     2   Rn e  p(t)e   dt = p1(z)e    ∈ A  (TΩ),

for another polynomial p (z)   1  . Namely, the isometry in Lemma 2.2 sends every

p(t)e- t24-∈ P e- t24 ⊂ L2(Rn, γ )                              t

to some

      -z2      -z2    2  p1(z)e    ∈ P e   ⊂  A (TΩ).

By Lemma 2.3,     t2  Pe -4   is dense in L2(Rn, γt)  . Hence      2  P e-z   is dense in A2(T Ω)  as claimed.

By Lemma 2.1, K(z, w)  reproduces every element of    -z2  P e   . Therefore, since   - z2  Pe   is dense in   2  A  (T Ω)  , it follows that K(z, w)  reproduces every element of   2  A  (TΩ)  . □

With this result, condition (ii) of K(z, w)  stated in the Introduction is verified. Therefore, to prove the theorem, it remains only to check condition (iii). This is done by the following proposition.

Proposition 2.5 For each fixed w ∈  T ,        Ω

K( - ,w) ∈ A2(T  ).                  Ω

Proof: Fix w ∈ T Ω   , and consider K( - ,w)  . For any fixed      n  ξ ∈ R  , formula (1.2) satisfies

K Ω(z,w)  = K Ω+ξ(z + iξ,w + iξ)

for all z, w ∈ TΩ   . Further, z + ξ,w +  ξ ∈ T Ω   and K(z, w) = K(z  + ξ,w + ξ)  . Therefore, without loss of generality, we may assume that w = 0 ∈ T Ω ⊂ Cn  in the statement of this proposition. We want to show that K(z, 0) ∈ A2(T Ω)  . But

            1   ∫   eizt  K(z, 0) = -----n    ----dt,            (2π)   Rn  γt

and with Lemma 2.2, we get

∥K(z, 0)∥2L2(TΩ)  =  (21π)n∥γ1∥2L2(Rn,γt)                      1  ∫ t  1                  =  (2π)n- Rnγtdt                    =  K(0, 0)                  <  ∞,   as 0 ∈ TΩ.

We have shown that, for each w  ∈ TΩ   ,              2  K( - ,w) ∈ A  (TΩ)  .

This result verifies condition (iii) of the Introduction, and the theorem follows.

References

[1]   T. G. Genchev, Integral representations for functions holomorphic in tube domains, C. R. Acad. Bulgare Sci. 37 (1984), 717-720.         [ Links ]

[2]   T. G. Genchev, Paley-Wiener type theorems for functions in Bergman spaces over tube domains, J. Math. Anal. and Appl. 118 (1986), 496-501.         [ Links ]

[3]   I. S. Gradshteyn, I. M. Ryzhik, Table of Integrals, Series and Products, Academic Press, (1980).         [ Links ]

[4]   S. Krantz, Function Theory of Several Complex Variables, 2ed. Wadsworth & Brooks/Cole, Pacific Grove 1992.         [ Links ]

Ching-I Hsin
Division of Natural Science,
Minghsin University of Science and Technology.
Hsinchu County 304, Taiwan.
hsin@must.edu.tw

Recibido: 6 de mayo de 2004
Aceptado: 28 de marzo de 2005

Creative Commons License Todo el contenido de esta revista, excepto dónde está identificado, está bajo una Licencia Creative Commons