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(1)

SPACE-LIKE SUBMANIFOLDS WITH CONSTANT SCALAR CURVATURE IN THE DE SITTER SPACES

Liu Ximin

Abstract. Let M

n

be a space-like submanifold in a de Sitter space M

pn+p

(c) with constant scalar curvature. We rstly extend Cheng- Yau’s technique to higher codimensional cases. Then we study the rigidity problem for M

n

with parallel normalized mean curvature vector eld.

1. Introduction

Let M p n+p (c) be an (n+p)-dimensional connected semi-Riemannian man- ifold of constant curvature c whose index is p. It is called an indenite space form of index p and simply a space form when p = 0. If c > 0, we call it as a de Sitter space of index p. Akutagawa [3] and Ramanathan [11]

investigated space-like hypersurfaces in a de Sitter space and proved inde- pendently that a complete space-like hypersurface in a de Sitter space with constant mean curvature is totally umbilical if the mean curvature H sat- ises H 2 ≤ c when n = 2 and n 2 H 2 < 4(n − 1)c when n ≥ 3. Later, Cheng [4] generalized this result to general submanifolds in a de Sitter space.

To our best knowledge, there are almost no intrinsic rigidity results for the space-like submanifolds with constant scalar curvature in a de Sitter space until Zheng [15] obtained the following result.

Theorem. Let M n be an n-dimensional compact space-like hypersur- face in M 1 n+1 (c) with constant scalar curvature. If M n satises

(1) K(M ) > 0,

(2) Ric(M ) ≤ (n − 1)c, (3) R < c,

where R is the normalized scalar curvature of M n , then M n is totally umbilical.

Received February 23, 2000.

2000 Mathematics Subject Classication: 53C40, 53C42, 53C50.

Key words and phrases: space-like submanifold, scalar curvature, normalized mean curvature vector eld.

This project is supported in part by the National Science Foundation of China.

(2)

In [5], Cheng-Yau rstly studied the rigidity problem for a hypersurface with constant scalar curvature in a space form by introducing a self-adjoint second order dierential operator (See Theorems 1 and 2 in [5]). They proved that, for an M n in M n+1 (c), if R is constant and R ≥ c, then

|∇σ| 2 ≥ n 2 |∇H| 2 where σ and H denote the second fundamental form and the length of the mean curvature vector eld of M n respectively. By using Cheng-Yau’s technique, Li [7] [8] studied the pinching problem and also proved some global rigidity theorems for hypersurfaces with constant scalar curvature.

In the present paper, we would like extend Cheng-Yau’s technique to higher codimensional cases and use this result to study the rigidity prob- lem for space-like submanifolds in a de Sitter space with constant scalar curvature.

2. Preliminaries

Let M p n+p (c) be an (n + p)-dimensional semi-Riemannian manifold of constant curvature c whose index is p. Let M n be an n-dimensional Rie- mannian manifold immersed in M p n+p (c). As the semi-Riemannian metric of M p n+p (c) induces the Riemannian metric of M n , M n is called a space- like submanifold. We choose a local eld of semi-Riemannian orthonormal frames e 1 , . . . , e n+p in M p n+p (c) such that at each point of M n , e 1 , . . . , e n

span the tangent space of M n and form an orthonormal frame there. We use the following convention on the range of indices:

1 ≤ A, B, C, . . . ≤ n + p; 1 ≤ i, j, k, . . . ≤ n; n + 1 ≤ α, β, γ ≤ n + p.

Let ω 1 , . . . , ω n+p be its dual frame eld so that the semi-Riemannian metric of M p n+p (c) is given by ds 2 = ∑

i ω 2 i

α ω 2 α = ∑

A ϵ A ω A 2 , where ϵ i = 1 and ϵ α = −1. Then the structure equations of M p n+p (c) are given by

(1) A = ∑

B

ϵ B ω AB ∧ ω B , ω AB + ω BA = 0,

(2) AB = ∑

C

ϵ C ω AC ∧ ω CB 1 2

C,D

K ABCD ω C ∧ ω D ,

(3) K ABCD = c ϵ A ϵ B AC δ BD − δ AD δ BC ).

Restrict these form to M n , we have

(4) ω α = 0, n + 1 ≤ α ≤ n + p,

(3)

the Riemannian metric of M n is written as ds 2 = ∑

i ω i 2 . From Cartan’s lemma we can write

(5) ω αi = ∑

j

h α ij ω j , h α ij = h α ji .

From these formulas, we obtain the structure equations of M n :

(6) i = ∑

j

ω ij ∧ ω j , ω ij + ω ji = 0,

(7) ij = ∑

k

ω ik ∧ ω kj 1 2

k,l

K ijkl ω k ∧ ω l ,

(8) R ijkl = c(δ ik δ jl − δ il δ jk )

α

(h α ik h α jl − h α il h α jk ), where R ijkl are the components of the curvature tensor of M n .

For indenite Riemannian manifolds in detail, refer to O’Neill [9].

Denote L α = (h α ij ) n ×n and H α = (1/n)

i h α ii for α = n + 1, · · · , n + p.

Then the mean curvature vector eld ξ, the mean curvature H and the square of the length of the second fundamental form S are expressed as

ξ =

α

H α e α , H = |ξ|, S =

α,i,j

(h α ij ) 2 ,

respectively. Moreover, the normal curvature tensor {R αβkl }, the Ricci curvature tensor {R ik } and the normalized scalar curvature R are expressed as

R αβkl = ∑

m

(h α km h β ml − h α lm h β mk ), R ik = (n − 1) c δ ik − n

α

(H α )h α ik + ∑

α,j

h α ij h α jk ,

R = c + 1

n(n − 1) (S − n 2 H 2 ).

(9)

Dene the rst and the second covariant derivatives of {h α ij }, say {h α ijk } and {h α ijkl } by

(10) ∑

k

h α ijk ω k = dh α ij + ∑

k

h α kj ω ki + ∑

k

h α ik ω kj + ∑

β

h β ij ω βα ,

(4)

l

h α ijkl ω l = dh α ijk + ∑

m

h α mjk ω mi + ∑

m

h α imk ω mj (11)

+ ∑

m

h α ijm ω mk + ∑

β

h β ijk ω βα .

Then, by exterior dierentiation of (5), we obtain the Codazzi equation

(12) h α ijk = h α ikj .

It follows from Ricci’s identity that (13) h α ijkl − h α ijlk = ∑

m

h α mj R mikl + ∑

m

h α im R mjkl + ∑

β

h β ij R βαkl . The Laplacian of h α ij is dened by h α ij = ∑

k h α ijkk . From (13), we have h α ij = nH α,ij + ∑

k,m

h α km R mijk + ∑

k,m

h α im R mkjk + ∑

k,β

h β ik R βαjk

= nH α,ij + n c h α ij − n c H α δ ij − n

β,m

H β h α im h β mj + ∑

β

S αβ h β ij

−2

β,k,m

h β ik h α km h β mj + ∑

m,k,β

h α im h β mk h β kj + ∑

β,k,m

h β ik h β km h α mj ,

where S αβ = ∑

i,j h α ij h β ij for all α and β. Dene N (A) =

i,j a 2 ij for any real matrix A = (a ij ) n ×n . Then we have

i,j

h α ij h α ij = n

i,j

H α,ij h α ij + n c S α − c n 2 H α 2 − n

β

H β T r(L 2 α L β )

+ ∑

β

S αβ 2 + ∑

β

N (L α L β − L β L α ), (14)

where S α = ∑

i,j (h α ij ) 2 , for every α.

Suppose H > 0 on M n and choose e n+1 = ξ/H. Then it follows that (15) H n+1 = H; H α = 0, α > n + 1.

From (10) and (15) we can see

(16) H n+1,k ω k = dH, H α,k ω k = Hω n+1α α > n + 1.

From (11), (15) and (16) we have

(17) H n+1,kl = H kl 1

H

β>n+1

H β,k H β,l , where dH =

i H i ω i and ∇H k = ∑

l H kl ω l ≡ dH k + H l ω lk for all k.

(5)

Using (14) and (17), we have

i,j

h n+1 ij h n+1 ij = n

i,j

H ij h n+1 ij n H

i,j

β>n+1

H β,i H β,j h n+1 ij +n c S n+1 − c n 2 H 2 − nHf n+1 + S n+1 2 + ∑

β>n+1

S n+1β 2

+ ∑

β>n+1

N (L n+1 L β − L β L n+1 ), (18)

where f n+1 = T r(L n+1 ) 3 .

M. Okumura [10] established the following lemma (see also [2]).

Lemma 2.1. Let {a i } n i=1 be a set of real numbers satisfying

i a i = 0,

i a 2 i = t 2 , where t ≥ 0. Then we have

n − 2

n(n − 1) t 3

i

a 3 i n − 2 n(n − 1) t 3 ,

and the equalities hold if and only if at least (n − 1) of the a i are equal.

Denote the eigenvalues of L n+1 by i } n i=1 . Then we have

(19) nH =

i

λ i , S n+1 = ∑

i

λ 2 i , f n+1 = ∑

i

λ 3 i .

Set L n+1 = L n+1 − H I n , f n+1 = f n+1 − 3HS n+1 + 2nH 3 , S n+1 = S n+1 − nH 2 , and λ i = λ i − H, where I n denotes the identity matrix of degree n. Then (19) changes into

(20) 0 = ∑

i

λ i , S n+1 = ∑

i

λ 2 i , f n+1 = ∑

i

λ 3 i .

By applying Okumura’s Lemma to f n+1 , we have f n+1 n − 2

n(n − 1) S n+1

S n+1 ⇐⇒

f n+1 ≤ 3HS n+1 − 2nH 3 + √ n − 2

n(n − 1) S n+1

S n+1 . So we have

n c S n+1 − c n 2 H 2 − nHf n+1 + S n+1 2 (21)

S n+1 {n c + S n+1 − nH 2 − n(n − 2)H

S n+1

n(n − 1) }.

(6)

It follows from (15) that

(22) ∑

β>n+1

S n+1β 2 = ∑

β>n+1

{

i,j

(h n+1 ij − Hδ ij )h β ij } 2 . Denote S I = ∑

β>n+1 S β . From (22), we have

(23) ∑

β>n+1

S n+1β 2 ≤ S n+1 S I . Let T =

i,j T ij ω i ω j be a symmetric tensor on M n dened by (24) T ij = h n+1 ij − nHδ ij .

We introduce an operator  associated to T acting on f ∈ C 2 (M n ) by

f =

i,j

T ij f ij = ∑

i,j

h n+1 ij f ij − nH f,

where is the Laplacian. Since ( T ij ) is divergence-free, it follows from [5]

that the operator  is self-adjoint relative to the L 2 -inner product of M n . Choosing f = H in above expression, we have

(25) ∑

i,j

h n+1 ij H ij = H + nH H.

Denote S = S n+1 + S I . Substituting (21), (23) and (25) into (18), we get

i,j

h n+1 ij h n+1 ij ≥ nH + 1

2 n 2 ( H 2 ) − n 2 |∇H| 2

n H

β>n+1

i,j

H β,i H β,j h n+1 ij

+ ∑

β>n+1

N (L n+1 L β − L β L n+1 )

+S n+1

{

n c − nH 2 + S n+1 − n(n − 2)H

S n+1

n(n − 1) }

. (26)

3. An extension of Cheng-Yau’s technique

Cheng-Yau [5] gave a lower estimation for |∇σ| 2 , the square of the length

of the covariant derivative of σ, which plays an important role in their

discussion. They proved that, for a hypersurface in a space form of constant

scalar curvature c, if the normalized scalar curvature R is constant and

R ≥ c, then |∇σ| 2 ≥ n 2 |∇H| 2 .

(7)

For the space-like submanifolds in a de Sitter space, we can prove the following

Theorem 3.1. Let M n be a connected submanifold in M p n+p (c) with nowhere zero mean curvature H. If R is constant and R < c, then

(27) |∇σ| 2 = ∑

i,j,k,α

(h α ijk ) 2 ≥ n 2 |∇H| 2

and the symmetric tensor T dened by (24) is negative semi-denite. More- over, if the equality in (27) holds on M n , then H is constant and T is negative denite.

Proof. From (9), we have n 2 H 2 − S = n(n − 1)(c − R) > 0. Taking the covariant derivative on both sides of this equality, we get

n 2 H H k = ∑

i,j,α

h α ij h α ijk , k = 1, · · · , n.

For every k, it follows from Cauchy-Schwarz’s inequality that (28) n 4 H 2 H k 2 = ( ∑

i,j,α

h α ij h α ijk ) 2 ≤ S

i,j,α

(h α ijk ) 2 ,

where the equality holds if and only if there exits a real function c k such that

(29) h α ijk = c k h α ij

for all i, j and α. Taking sum on both sides of (28) with respect to k, we have

(30) n 4 H 2 |∇H| 2 = n 4 H 2

k

H k 2 ≤ S

(i,j,k,α)

(h α ijk ) 2 ≤ n 2 H 2

(i,j,k,α)

(h α ijk ) 2 . Therefore (27) holds on M n .

Denote the eigenvalues of L n+1 by i } n i=1 . Then (λ i ) 2 ≤ S n+1 ≤ S ≤ n 2 H 2 for all i. Hence i | ≤ nH for all i. Therefore T = (T ij ) = L n+1 nHI n is negative semi-denite.

Suppose that ∑

i,j,k,α (h α ijk ) 2 = n 2 |∇H| 2 holds on M n . It follows from (30) that

(31) 0 ≤ n 3 (n − 1)(c − R)|∇H| 2 ≤ S

 ∑

i,j,k,α

(h α ijk ) 2 − n 2 |∇H| 2

 .

Hence (c −R)|∇H| 2 = 0 on M n . Because R < c, |∇H| 2 = 0 on M n . In this case, i | ≤ (S n+1 ) 1/2 ≤ S 1/2 < nH for all i. Thus T is negative denite.

This completes the proof of Theorem 3.1.

(8)

4. Submanifolds with at normal bundle

In this section, we propose to use the extension of Cheng-Yau’s technique given in section 3 to study the rigidity problem for compact submanifolds in the de sitter space M p n+p (c). We continue use the same notations as in section 2. Let M n be a compact submanifold in M p n+p (c) with nowhere zero mean curvature H. Suppose that ξ/H is parallel and choose e n+1 = ξ/H.

Then ω n+1α = 0 for all α. It follows from (11) and (16) that

(32) H α,k = 0, H α,kl = 0,

for all α > n + 1 and k, l = 1, · · · , n.

Suppose in addition that the normal bundle of M n is at. Then

(33) αβ = 1

2 R αβkl ω k ∧ ω l = 0,

for all α and β on M n . For all α and β we have L α L β = L β L α , which is equivalent to that {L α } n+p α=n+1 can be diagonized simultaneously.

We denote the eigenvalues of L α by α 1 , · · · , λ α n } for every α. It follows from [13] that

(34) 1

2 S =

i,j,k,α

(h α ijk ) 2 + n

i,j,α

H α,ij h α ij + ∑

α

i<j

K ij α i − λ α j ) 2 ,

where K ij = c +

β λ β i λ β j denotes the sectional curvature of M n corre- sponding to the plane section spanned by {e i , e j } for every pair of i < j.

Assume that R is constant and R < c. From (25) and (32), we have

i,j,k,α

(h α ijk ) 2 + n

i,j,α

H α,ij h α ij = n H + 1

2 ( n 2 H 2 ) + ∑

i,j,k,α

(h α ijk ) 2 −n 2 |∇H| 2 . Note that S = ( n 2 H 2 ). Therefore (34) turns into

0 = n H +

i,j,k,α

(h α ijk ) 2 − n 2 |∇H| 2 + ∑

i<j

α

K ij α i − λ α j ) 2 . Integrating the both sides of above equality on M n , we have

0 =

M

 ∑

i,j,k,α

(h α ijk ) 2 − n 2 |∇H| 2

 ∗ 1 +

i<j

α

M

K ij α i − λ α j ) 2 ∗ 1.

If K ij ≥ 0 on M n , it follows from (27) and the above equality that

(35) ∑

(i,j,k,α)

(h α ijk ) 2 ≡ n 2 |∇H| 2 ; K ij α i − λ α j ) 2 ≡ 0,

for every α and i < j. Hence we can prove the following theorem

(9)

Theorem 4.1. Let M n be a compact submanifold with non-negative sectional curvature in M p n+p (c). Suppose that the normal bundle N (M ) is at and the normalized mean curvature vector is parallel. If R is constant and R < c, then M n is totally umbilical.

Proof. From the rst equality of (35) and Theorem 3.1, we have that H is constant on M n , then ξ is parallel. From Theorem 3 of [1] we know that M n is totally umbilical.

Remark 4.1. In Theorem 4.1, we have used the assumptions that are dierent from that in Theorem 3 [1] to obtain the same result.

Also, we need the following

Lemma 4.1 [12]. Let A and B be n × n-symmetric matrices satisfying T r A = 0, T r B = 0 and A B − B A = 0. Then

n − 2

n(n − 1) (T r A 2 )(T r B 2 ) 1/2 ≤ T r A 2 B (36)

n − 2

n(n − 1) (T r A 2 )(T r B 2 ) 1/2 , and the equality holds on the right (resp. left) hand side if and only if n −1 of the eigenvalues x i of A and the corresponding eigenvalues y i of B satisfy

|x i | = (T r A

2

)

1/2

n(n −1) , x i x j ≥ 0, y i = (T r B

2

)

1/2

n(n −1) (resp. y i = (T r B

2

)

1/2

n(n −1) ).

Choose a suitable normal frame eld {e β } n+p β=n+2 such that S αβ = 0 for all α ̸= β. Then

(37) ∑

α,β>n+1

S αβ 2 = ∑

β>n+1

S β 2 ≤ S I 2 ,

where the equality holds if and only if at least p − 2 numbers of S α ’s are zero.

Taking sum with respect to α > n + 1 on both-sides of (14), we have

i,j,α>n+1

h α ij h α ij = (n c − n H 2 )S I − nH

α>n+1

T r(L 2 α L n+1 )

+ ∑

α>n+1

S n+1α 2 + ∑

α>n+1

S α 2 . (38)

Using the left hand side of (36) to T r(L 2 α L n+1 ), we have T r(L 2 α L n+1 ) ≤ (n − 2)S α

S n+1

n(n − 1) .

(10)

Substituting this into (38) and using (23) and (37), we have (39)

i,j,α>n+1

h α ij h α ij ≥ S I

{

(n c − n H 2 ) − n(n − 2)H

S n+1

n(n − 1) + S n+1

} . Substituting (32) into (26), we have

i,j

h n+1 ij h n+1 ij ≥ nH + 1

2 ( n 2 H 2 ) − n 2 |∇H| 2

+S n+1 {

(n c − nH 2 ) − n(n − 2)H

S n+1

n(n − 1) + S n+1 }

. (40)

Note that S = ( n 2 H 2 ) and (41) 1

2 S =

i,j,k,α

( h α ijk ) 2

+ ∑

i,j

h n+1 ij h n+1 ij + ∑

i,j,α>n+1

h α ij h α ij . From (39) and (40), we obtain

0 ≥ nH +

(i,j,k,α)

( h α ijk ) 2

− n 2 |∇H| 2

+S {

(n c − nH 2 ) − n(n − 2)H

S n+1

n(n − 1) + S n+1 }

. (42)

Consider the quadratic form Q(u, t) = u 2 n n −2 −1 ut − t 2 . By the orthogonal transformation

{ u = 1

2n {(1 +

n − 1)u + (1 −

n − 1)t}

t = 1 2n {(

n − 1 − 1)u + (

n − 1 + 1)t}

Q(u, t) turns into Q(u, t) = n

2

n −1 (u 2 − t 2 ), where u 2 + t 2 = u 2 + t 2 . Take u =

S n+1 , t =

nH, then nc − nH 2 − n(n − 2)H

S n+1

n(n − 1) + S n+1

= nc + Q(u, t) = nc + n(u 2 − t 2 ) 2

n − 1

= nc + n( −u 2 − t 2 ) 2

n − 1 + nu 2

n − 1

≥ nc − nS n+1

2

n − 1

(43)

(11)

Note that

(44) S n+1 ≤ S n+1 + S I = S.

From (43), (44) and (27) we have

(45) 0 ≥ nH + S

{

nc nS 2

n − 1 }

. Integrating the both sides of (45) on M n , we have

(46) 0

M

S {

nc nS 2

n − 1 }

∗ 1.

Therefore we can prove the following

Theorem 4.2. Let M n (n ≥ 3) be a closed space-like submanifold with parallel normalized mean curvature vector eld immersed into M p n+p (c).

Suppose that R is constant and R = c − R > 0. If the normal bundle N (M ) is at and

(47) S < nH 2 + 2

n − 1c,

then S = nH 2 and M n is umbilical (hence isometric to a sphere).

Proof. Denote R = c − R. Then S = n(n − 1)(H 2 − R) and S = nR + n 2 (H 2 − R). Since n ≥ 3, we have

(48) nc nS 2

n − 1 = n(c n(n − 1)(H 2 − R 2

n − 1 ) = n(c S − nH 2 2

n − 1 ).

It is clear that the condition (47) is equivalent to

(49) nc S

2

n − 1 > 0.

From (46) and (49) we have S = 0 on M n , so H 2 = R and S = nR, that is S = nH 2 . Since H is constant on M n , hence ξ is parallel, from Theorem 3 of [1] we know that M n is totally umbilical.

References

[1] R. Aiyama, Compact space-like submanifolds in a pseudo-Riemannian sphere S

pm+p

(c), Tokyo J. Math. 18 (1995), 81–90.

[2] H. Alencar and M. P. do Carmo, Hypersurfaces with constant mean curvature in spheres, Proc. Amer. Math. Soc. 120 (1994), 1223–1229.

[3] K. Akutagawa, On space-like hypersurfaces with constant mean curvature in the de Sitter space, Math. Z. 196 (1987), 13–19.

[4] Q. M. Cheng, Complete space-like submanifolds in a de Sitter space with parallel

mean curvature vector, Math. Z. 206 (1991), 333–339.

(12)

[5] S. Y. Cheng and S. T. Yau, Hypersurfaces with constant scalar curvature, Math.

Ann. 225 (1977), 195–204.

[6] Z. H. Hou, Hypersurfaces in sphere with constant mean curvature, Proc. Amer. Math.

Soc. 125 (1997), 1193–1196.

[7] H. Li, Hypersurfaces with constant scalar curvature in space forms, Math. Ann. 305 (1996), 665–672.

[8] , Global rigidity theorems of Hypersurfaces, Ark. Mat. 35 (1997), 327–351.

[9] B. O’Neill, Semi-Riemannian Geometry, New York, Academic Press, 1983.

[10] M. Okumuru, Hypersurfaces and a pinching problem on the second fundamental tensor, Amer. J. Math. 96 (1974), 207–213.

[11] J. Ramanathan, Complete space-like hypersurfaces of constant mean curvature in the de Sitter space, Indiana Univ. Math. J. 36 (1987), 349-35.

[12] W. Santos, Submanifolds with parallel mean curvature vector in spheres, Tˆ ohoku Math. J. 46 (1994), 403–415.

[13] K. Yano and S. Ishihara, Submanifolds with parallel mean curvature vector, J. Di.

Geom. 6 (1971), 95–118.

[14] S. T. Yau, Submanifolds with constant mean curvature, Amer. J. Math. 96 (1975), 346–366; 97 (1975), 76–100.

[15] Y. Zheng, Space-like hypersurfaces with constant scalar curvature in the de Sitter spaces, Di. Goem. and its Appl. 6 (1996), 51–54.

Department of Applied Mathematics Dalian University of Technology Dalian 116024, China

and

Institute of Mathematics

Academy of Mathematics and Systems Sciences Chinese Academy of Sciences

Beijing 100080, China

E-mail : [email protected]

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In this regard, I would like to request your full cooperation to Kangnam University when they contact you regarding the verification of enrollment

In this regard, I would like to request your full cooperation to Kangnam University when they contact you regarding the verification of enrollment

The index is calculated with the latest 5-year auction data of 400 selected Classic, Modern, and Contemporary Chinese painting artists from major auction houses..