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國立臺灣大學 數學系 預印本 Department of Mathematics, National Taiwan University

www.math.ntu.edu.tw/ ~ mathlib/preprint/2011- 13.pdf

Asymptotic Tian-Yau-Zelditch Expansions on Singular Riemann Surfaces

Chiung-Ju Liu and Zhiqin Lu

April, 2011

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ASYMPTOTIC TIAN-YAU-ZELDITCH EXPANSIONS ON SINGULAR RIEMANN SURFACES

CHIUNG-JU LIU AND ZHIQIN LU

Abstract. We give both lower and upper bound estimates of the Bergman kernel for a degeneration of Riemann surfaces with constant curvature −1. As a result, we gave a geometric proof of the Riemann-Roch Theorem for singular Riemann surface.

Contents

1. Introduction 1

2. The holomorphic plumbing fixture 2

3. Subharmonic functions 4

4. Main results 6

4.1. Riemann-Roch Theorem on singular surface 8

4.2. The upper bound of the Bergman Kernel 9

References 10

1. Introduction

Let M be a compact complex manifold of dimension n and let (L, h) → M be a positive Hermitian line bundle. Let g be the K¨ahler metric on M corresponding to the K¨ahler form ωg = Ric(h). For each m ∈ N, h induces a Hermitian metric hm on Lm. Let {S0, · · · , Sdm−1} be any orthonormal basis of H0(M, Lm) with respect to the inner product

(Si, Sj) = Z

M

hSi(x), Sj(x)ihmdVg,

where dm = dimH0(M, Lm) and dVg = n!1ωgn is the volume form of g. The sequence of functions,

Bm(x) =

dm−1

X

i=0

kSi(x)k2hm, is called the Bergman kernel of the manifold.

Catlin [2] and Zelditch [12] proved that for any given point x ∈ M there is a complete asymptotic expansion for the Bergman kernel:

Bm(x) ∼ a0(x)mn+ a1(x)mn−1+ a2(x)mn−2+ · · · (1.1)

1Subject Classification. Primary 53C55; Secondary 32S30 Date: March 31, 2011.

Key words and phrases. Asymptotic Expansion, Singular Riemann Surface.

1

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for certain smooth coefficients aj(x) with a0 = 1. The asymptotic expansion is conver- gent in the following sense: for any positive integers k and l, there exists a constant C, depending on k, l and the manifold M , such that

Bm(x) − mn+ a1(x)mn−1+ · · · + ak(x)mn−k

Cl(M ) ≤ Cmn−k−1. (1.2) In [8], the first several coefficients of the above expansion were computed. Moreover, aj(x), for any j, is a polynomial of the curvature and their covariant derivatives at x. Thus, the expansion of Catlin and Zelditch is local. On the other hand, the Bergman kernel itself contains global information of the manifold M . Thus the asymptotic expansion, in general, is not uniform. The constant in (1.2) may go to infinity when the metric varies.

One of the main applications of the above expansion is the theorem of Tian [9], which is equivalent to

∂ ¯∂ log Bm(x) = O 1 m

 .

A necessary condition for the above equality to be true uniformly is the uniform lower bound of the Bergman kernel. For general line bundle L, if for some positive integer m, Bm(x) > 0, then Lm is called base point free. By the work of Demailly and Siu, for an ample line bundle L there is a constant c(n), depending only on the dimension n of M , such that for any m > c(n), Lm is base point free. For a family of manifolds, it is interesting to see whether there is a constant ε > 0, depending only on the geometry of the family, such that

dm−1

X

i=0

kSi(x)k2hm > ε.

In K¨ahler-Einstein geometry, the above estimate is very important. Similar estimate is called strong partial C0 estimate in [10] and is called tamed in the paper of Chen-Wang [1].

In this paper, we study the behavior of the Bergman kernels on a degeneration family of Riemann surfaces, polarized by their canonical bundles. This is the prototype case for the volume collapsing family of K¨ahler manifolds. We proved that there is no strong partial C0 estimate in this case and we believe that the same statement is true for the Bergman kernels in all volume collapsing cases.

We give both lower and upper bounds estimates of the Bergman kernel for a family of Riemann surfaces in this paper (Theorem 4.1 and Theorem 4.3). Using the techniques developed, we are able to study the limiting behaviors of the holomorphic sections of the pluri-canonical bundles. Let Xt be a degeneration of smooth Riemann surfaces such that X0 is a single Riemann surface with one ordinary double point. We obtain

dim HL02(X0, KXm0) = dim H0(Xt, KXmt) − 1.

We are able to single out one of the holomorphic section whose L2 normal blows up at t = 0.

Throughout this paper, a constant C is a positive real number which is independent to t but may differ line by line.

2. The holomorphic plumbing fixture

Consider a holomorphic degeneration family π : X → ∆ of Riemann surfaces, where

∆ = {t ∈ C : |t| < 1} and for any 0 6= t ∈ ∆, Xt= π−1(t) is a smooth Riemann surface of

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w1

w2

w1w2= t

γ

w1

w2

w1w2= 0

x0

Figure 1. Algebra pictures vs. geometric pictures of Xt near the singu- larity point x0

genus greater than 1. We assume that X is smooth and the central fiber X0 is a singular Riemann surface which has only one ordinary double point x0.

Near x0, Xt can be represented by the curve {w1w2 = t} within the unit ball of C2. In particular, X0 is the zero locus of {w1w2 = 0}.

On the other hand, from the differential geometric point of view, near x0, X0 is the union of two cusps, each of which is biholomorphic to the punctured unit disk with the Poincar´e metric

4dz ⊗ d¯z

|z|2(log |z|−2)2. (2.1)

Please see Figure 1. To unify the above two view points, we start with the following Collar Theorem of Keen [5, page 264]:

Theorem 2.1 (Keen). Consider the region T of U , the upper half plane, bounded by the curve r = 1, r = el, θ = θ0 and θ = π − θ0. Let γ be a closed geodesic on M with length l. Then there is a conformal isometric mapping ϕ : T → M such that ϕ(iy) = γ. The image ϕ(T ) of T is called a collar. Then we can choose θ0 small enough such that the area of the Collar is at least 8

5.

Topologically, a collar CR is the cylinder (−R, R) × S1, where 2R is the length of the collar. For the rest of the paper, we write CR = (−R, R) × [0, 2π) for the sake of convenience. There is a holomorphic embedding

pt: CR→ Xt for each t. We identify CR with its image pt(CR).

The Gaussian curvature of CR is −1 with respect to the above Poincar´e metric. Let γ be the shortest closed geodesic line of CR in Xt and let 4πσ0 be its length. Then the

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Riemannian metric on CR, with the natural coordinates (ρ, θ), can be written as ds2 = dρ2+ (2σ0cosh ρ)2(dθ)2.

By Wolpert [11, page 13], we have (up to a constant) σ0 = π

log |t|−2. Let

x = θ + 1

0, y = 1 σ0



arctan eρ− π 4

 ,

where t = |t|e0 and let z = x + iy. Then under coordinate z, the metric ds2 can be written as

ds2 = (2σ0cosh ρ)2(dz ⊗ d¯z). (2.2) By the conformal structure of Riemann surface, we conclude that z = x + iy is either holomorphic or anti-holomorphic. With the suitable orientation, we assume that z is holomorphic.

Let

p(ρ, θ) = (w1, w2) be the embedding. Then we have

w1 = eσ01 (π2−arctan eρ)−iθ; w2 = t

w1, (2.3)

The area of the collar CR is

A = 8πσ0sinh R = ε1 = 8

√5.

As t goes to zero, the sequences of collars CR preserves the areas while the length 2R goes to infinity and the injective radius 2πσ0 goes to zero. For the rest of the paper, the real number R is related to σ0 (also in terms of t) by the above equation, and ε1 is the absolute constant 8/√

5.

3. Subharmonic functions

The injectivity radius of the singular Riemann surface X0 is 0. In order to make use of the ¯∂-estimate, we need to construct suitable subharmonic functions on X0 (Note that on Riemann surfaces, subharmonic functions and plurisubharmonic functions are the same thing). The main result of this section is Proposition 3.2, which is a generalization of [7, Proposition 4.2] in the singular case.

For t 6= 0, let x1 = (R − ρ1, θ) for some fixed 4 ≤ ρ1 < R and p0 = (R − 1, 0) in CR. As t approaches zero, let wx1, wp0 be the corresponding limit points in

D1\ {0} = {0 < |w1| < eε1} ⊂ X0, respectively. By taking the limit in (2.3), We have

wx1 = eε1eρ1−iθ wp0 = e4eπε1

In [7], the following result was proved (with slightly different notations)

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Proposition 3.1. Let X be a compact Riemann surface of genus g ≥ 2 and constant curvature −1. Then for any x1 ∈ M , there is a function ϕt = ϕt,x1

ϕt(w1) = log

wx1

w1 − 1

−2 arctan eR−ρ1

π log

wp0

w1 − 1 , such that

(1) In a neighborhood Ux1 of x1, ϕt can be written as ϕt= 2 log d(x) + ψ,

where ψ is a smooth function on Ux1 and d(x) is the distance function to x1. Consequently

Z

Ux1

e−ϕt = +∞;

(2) There is a constant C such that

√−1

2π ∂ ¯∂ϕt≥ −Cωg on M \{x1}, where ωg is the K¨ahler form of M ; (3) ϕt satisfies

ϕt ≤ C on X and

ϕt ≥ 2 log d(x) − 2π δx1 − C for d(x) ≤ δx1 and the injectivity radius δx1 at x1.

 Since ρ1 is fixed, we have

2 arctan eR−ρ1

π → 1

as t → 0. Thus point-wisely, the functions ϕt have the following limit

ϕ = log |wx1 − w1| − log |wp0 − w1| (3.1) on X0.

Since the Poincar´e metric

ds20 = 4

|w1|2(log |w1|−2)2dw1⊗ dw1, is the limit of the metric in (2.2), we concluded the following result.

Proposition 3.2. Suppose X0 is a singular Riemann surface with singular point x0 of genus g ≥ 2 and constant curvature −1 except at the singular point. Then for any x1 ∈ X0, there is a function ϕ on X0\ {x0, x1} such that

(1) In a neighborhood Ux1 of x1, ϕ can be written as ϕ = 2 log d + ψ, where ψ is a smooth function on Ux1 and

Z

Ux1

e−ϕ = +∞; (3.2)

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(2) There is a constant C such that

√−1

2π ∂ ¯∂ϕ ≥ −Cωg0 (3.3)

on X0\ {x0, x1}, where g0 is the complete K¨ahler metric of X0; (3) ϕ satisfies

ϕ ≤ C (3.4)

on X0 and

ϕ ≥ 2 log d − 2π δx1 − C for d ≤ δx1.

Remark 3.1. Since the (global) injectivity radius of X0 is zero, the existence of the sub- harmonic function is not trivial. We don’t know how to use the method in high dimensions.

On the other hand, by our construction, we obtained a smooth family of subharmonic func- tions over X . The functions ϕt,x1 naturally extends to the punctured unit ball of C2 such

that √

−1∂ ¯∂ϕt,x1 ≥ −Cωt, for sufficiently large constant C.

 4. Main results

We need the following H¨ormander’s L2 estimate.

Proposition 4.1. Suppose X0 is a singular Riemann surface of genus g ≥ 2 with ordinary double point x0 . Let L be a line bundle over X0 with the Hermitian metric h such that Ric(h) is a complete metric. Let ψ be plurisubharmonic function on X0, which can be approximated by a decreasing sequence of smooth functions {ψ`}1≤`≤∞. If



∂ ¯∂ψ`+ 2

√−1(Ric(h) + Ric(ωg0)), v ∧ ¯v



g0

≥ Ckvk2.

for any tangent vector v of type (1, 0) at X0 \ {x0} for each `, where C is a constant independent of `, and h·, ·ig0 is the inner product induced by g0, then for any C L-valued (0, 1)-form τ on X0 with ¯∂τ = 0 and R

X0kτ k2e−ψdVg0 < +∞, there exists a C L-valued u on X0 such that ¯∂u = τ and

Z

X0

kuk2e−ψdVg0 ≤ 1 C

Z

X0

kτ k2e−ψdVg0, where dVg0 is the volume form of g0.

 With the above estimate and the existence of the subharmonic function in Proposi- tion 3.2, we are able to generalize [7, Theorem 1.3] into the singular case in Theorem 4.1 below.

We apply Proposition 4.1 to the case that L = KXm0, h = g0−m for m ≥ 2, where g0 is the complete K¨ahler metric on X0 with scalar curvature −1. By Proposition 3.2, we have



∂ ¯∂ϕ + 2

√−1(Ric(h) + Ric(ωg0)), v ∧ ¯v



≥ (m − C − 1)kvk2.

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We choose m ≥ 2C.

Theorem 4.1. Suppose X0 is a singular Riemann surface of genus g ≥ 2 with ordinary double point x0 and constant scalar curvature −1. Then there exists constant D such that for any x1 ∈ X0\ x0, the Bergman kernel Bm(x) satisfies

Bm(x1) ≥ m D

 1 + e

δx1

4x1

 , (4.1)

where δx1 is the injectivity radius of x1.

Proof. The result is obviously true if x1 is away from the singular point. Thus we only need to prove the theorem under the assumption that |wx1| < eε1.

Let Vx1 = {x | dist(x, x1) < δx1}. Let z1 be the holomorphic function on Vx1 under which the K¨ahler metric can be represented as

ds2 = 2

(1 − |z1|2)2dz1⊗ d¯z1. (4.2) For sufficiently large m, let

τ = ¯∂η 2|z1| δx1



(dz1)m, where the smooth cut-off function

η(t) =

( 1 for t ≤ 12 0 for t ≥ 1 such that |η0| < 4 and |η00| < 4. Then ¯∂τ = 0 and

kτ k2 ≤ 16 δ2x

1

1 − |z1|22m+2

for 14δx1 ≤ |z1| ≤ 12δx1. The L2-norm of τ with respect to the weight ϕ given in Proposition 3.2 is

Z

X0

kτ k2e−ϕdVg0 ≤ Ce

δx1

x4

1

. By Proposition 4.1, for m large, there exists u ∈ C(X0, KXm

0) such that ¯∂u = τ and Z

X0

kuk2e−ϕdVg0 ≤ Ce

δx1

m2δx4

1

. (4.3)

Let S = η

2|z|

δx1



(dz1)m− u. Thus S ∈ H0(X0, KXm0). SinceR

X0e−ϕdVg0 = +∞, u(x1) = 0.

Therefore

kSk2(x1) = 1. (4.4)

By parallelogram law, we have kSk2L

2 ≤ 2

Z

X0

kuk2dVg0 + Z

X0

kη · (dz1)mk2dVg0

 .

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By (4.3) and Proposition 3.2, we have Z

X0

kuk2dVg0 ≤ Ce

δx1

m2δx41. (4.5)

Z

X0

kη · (dz1)mk2dVg0 ≤ Z

Vx1

k(dz1)mkdVg0 ≤ π

m − 12. (4.6)

By (4.4)-(4.6), there exists a constant D such that kSk2(x1)

kSk2L2

≥ m

D

 1 + e

δx1

x14

 . The theorem is proved.

 4.1. Riemann-Roch Theorem on singular surface. The canonical line bundle KX0 of X0 is defined as follows. Let Uj, j = 1, · · · , N be an open cover of X0. We assume that U0 is a neighborhood of x0 , and

U1 = {(w1, w2) | w1 6= 0; w2 = 0}; U2 = {(w1, w2) | w1 = 0; w2 6= 0}

Moreover, we assume that x1 ∈ U/ j for j > 2. Let V be an open set of X0. A section f of KX0 over V is define as

(1) On Uj∩ V 6= ∅, f is a holomorphic 1 form;

(2) On U1, f is represented by the meromorphic function f1 of the form f1(w1) = a

w1 + ˜f1(w1),

where ˜f1(w1) is a holomorphic function of w1 in the unit disk;

(3) Similarly, on U2 f is represented by the meromorphic function f2 of the form f2(w2) = − a

w2 + ˜f2(w2),

where ˜f2(w2) is a holomorphic function of w2 in the unit disk.

By the flatness of the family X , we concluded that

dim H0(X, KXm0) = dim H0(Xt, KXmt) = (2m − 1)(g − 1).

We prove the following result.

Theorem 4.2. Let HL02(X0, KXm

0) be the space of L2 holomorphic sections of KXm

0. Then dim HL02(X0, KXm0) = dim H0(X0, KXm0) − 1 = (2m − 1)(g − 1) − 1.

Proof. Define a local section u of KXm

0 on U1∪ U2 by f1(w1) = 1

w1m on U1; f2(w2) = − 1

w2m on U2.

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Let ρ be a cut-off function such that in a neighborhood of x0, ρ is identically equal to 1.

Let

τ = ¯∂ρ · u.

By Proposition 4.1, there exists a u1 ∈ C(X0, KXm0) such that

∂u¯ 1 = ¯∂ρ · u.

We claim that

S = ρu − u1 is not in L2. To see this, we first observe that

Z

X0

||u1||2dVg0 ≤ C m

Z

X0

||τ ||2dVg0 < +∞.

On the other hand, we have Z

X0

||ρu||2dVg0 = Z

|w1|<δ

|w1|2m(log |w1|−2)2m· 1

|w1|2m · 2√

−1dw1∧ d ¯w1

|w1|2(log |w1|−2)2 = +∞.

Thus we have

dim HL02(X0, KXm

0) ≤ dim H0(X0, KXm

0) − 1.

To prove the other direction of the inequality, let T be an arbitrary section of KXm0. Then for a suitable choice of complex number α, T − αS has the pole of order at most m − 1 near w1 = 0. Therefore we have

Z

X0

||T − αS||2dVg0 ≤ C1

+ C2 Z

|w1|<δ

|w1|2m(log |w1|−2)2m· 1

|w1|2m−2 · 2√

−1dw1∧ d ¯w1

|w1|2(log |w1|−2)2 < +∞

for some positive constants C1 and C2. The theorem is proved.

 4.2. The upper bound of the Bergman Kernel. We end this paper by proving the family version of upper bounds of the Bergman kernel.

Theorem 4.3. Let X be a Riemann surface with genus g ≥ 2 and constant scalar curva- ture −1. Let KX be the canonical line bundle of X and h be a positive Hermitian metric on KX. Then we have

Bm(x) ≤ 2m − 1 π (1 − e−(2m−1)δ2x). Proof. Given any x ∈ X, we have

Bm(x) ≤ sup

S∈H0(X,KXm)

kSk2(x) kSk2L2

.

Let z1 be the holomorphic coordinate on Vx = {y ∈ X | dist(x, y) < δx} centered at x and let the metric under z1 be defined as in (4.2). Any section S ∈ H0(X, KXm) restricted to Vx can be written as

S|Vx = f (z1)(dz1)m

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for some holomorphic function f (z1) defined on Ux. Thus we have kSk2(x)

kSk2L2

≤ kSk2(x) kSk2L2(Bxx))

= |f (0)|2

R

Bxx)|f (z)|2h(z)m−1

−1

2 dz ∧ d¯z, where

h(z) = (1 − |z|2)2. In polar coordinates, we have

Z

Bxx)

|f |2hm−1

√−1

2 dz ∧ d¯z = Z δx

0

Z

|z|=r

|f |2hm−1rdθdr.

By the mean value inequality, we have Z

Bxx)

|f |2hm−1

√−1

2 dz ∧ d¯z ≥ 2π|f (0)|2 Z δx

0

(1 − r2)2m−2rdr

≥ π|f (0)|2 2m − 1



1 − e(2m−1)δx2 , which proves the theorem.

 Acknowledgement. The first author is partially supported by the NSC grant 100- 2115-M-002-010- in Taiwan. The second author is partially supported by the NSF grant DMS-09-04653. The authors thank Zheng Huang for his help for explaining the concept holomorphic plumbing structure in the book of Wolpert [11].

References

[1] X.X. Chen and B. Wang, K¨ahler-Ricci flow on Fano Manifolds (I). arXiv:0909.2391v2, to appear in Journal of European Mathematical Society.

[2] David Catlin, The Bergman kernel and a theorem of Tian, Analysis and geometry in several complex variables (Katata, 1997), Trends Math., Birkh¨auser Boston, Boston, MA, 1999, pp. 1–23. MR1699887 (2000e:32001)

[3] Jean-Pierre Demailly, Holomorphic Morse inequalities, Several complex variables and complex ge- ometry, Part 2 (Santa Cruz, CA, 1989), Proc. Sympos. Pure Math., vol. 52, Amer. Math. Soc., Providence, RI, 1991, pp. 93–114. MR1128538 (93b:32048)

[4] S. K. Donaldson, Scalar curvature and projective embeddings. I, J. Differential Geom. 59 (2001), no. 3, 479–522. MR1916953 (2003j:32030)

[5] Linda Keen, Collars on Riemann surfaces, Discontinuous groups and Riemann surfaces (Proc. Conf., Univ. Maryland, College Park, Md., 1973), Princeton Univ. Press, Princeton, N.J., 1974, pp. 263–268.

Ann. of Math. Studies, No. 79. MR0379833 (52 #738)

[6] Chiung-ju Liu, The asymptotic Tian-Yau-Zelditch expansion on Riemann surfaces with constant curvature, Taiwanese J. Math. 14 (2010), no. 4, 1665–1675. MR2663940

[7] Zhiqin Lu, On the lower bound estimates of sections of the canonical bundles over a Riemann sur- face, Internat. J. Math. 12 (2001), no. 8, 891–926, DOI 10.1142/S0129167X01001064. MR1863285 (2002j:32018)

[8] , On the lower order terms of the asymptotic expansion of Tian-Yau-Zelditch, Amer. J. Math.

122(2000), no. 2, 235–273. MR1749048 (2002d:32034)

[9] Gang Tian, On a set of polarized K¨ahler metrics on algebraic manifolds, J. Differential Geom. 32 (1990), no. 1, 99–130. MR1064867 (91j:32031)

[10] G. Tian, On Calabi’s conjecture for complex surfaces with positive first Chern class, Invent. Math.

101(1990), no. 1, 101–172, DOI 10.1007/BF01231499. MR1055713 (91d:32042)

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[11] Scott A. Wolpert, Families of Riemann surfaces and Weil-Petersson geometry, CBMS Regional Conference Series in Mathematics, vol. 113, Published for the Conference Board of the Mathematical Sciences, Washington, DC, 2010. MR2641916 (2011c:32020)

[12] Steve Zelditch, Szeg˝o kernels and a theorem of Tian, Internat. Math. Res. Notices 6 (1998), 317–331, DOI 10.1155/S107379289800021X. MR1616718 (99g:32055)

(Chiung-ju Liu) Department of Mathematics, National Taiwan University, Taipei, Taiwan 106

E-mail address: cjliu4@ntu.edu.tw

(Zhiqin Lu) Department of Mathematics, University of California, Irvine, CA 92697-3875 E-mail address: zlu@uci.edu

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