1) Hugehes-hartogs algorithm
Hugehes-Hartogs算法
2) Hartogs domain
Hartogs域
1.
The purpose of this paper is to prove that every proper holomorphic self-mapping of certain Hartogs domains must be an automorphism.
对C2中某类Hartogs域的逆紧全纯自映射证明了刚性定理,即逆紧全纯自映射必定为全纯自同构。
3) Cartan-Hartogs domain
Cartan-Hartogs域
1.
The Cartan-Hartogs domain Y_Ⅱ(N,p;K)is the special cases of Hua domains, when K=p/2+1/(p+1),the solution of the Dirichlet problem of complex Monge-Ampère equation for domain Y_Ⅱ(N,p;K),and the explicit formula of complete K■hler-Einstein metric of Y_Ⅱ(N,p;K) is obtained.
华罗庚域的特殊类型Cartan-Hartogs域Y_Ⅱ(N,p;K)当K=p/2+1/(p+1)时,求解了该域上的复Monge-Ampère方程的边值问题,从而得到该域的完备K■hler-Einstein度量的显表达式,并且得到此度量下的全纯截曲率的负的上下确界,最后证明了此K■hler-Einstein度量与Bergman度量等价。
2.
In this paper,some extremal problems between the Cartan-Hartogs domain on k＜1 and the unit ball are studied,and the extremal mapping and extremal value in explicit formulas are obtained.
在本文中,k＜1时Cartan-Hartogs域与单位超球间的极值与极值映照被得到。
3.
By means of holomorphic automorphic map to compute the determinant of Bergman metic matrix detT for domains Y_(II),which are Cartan-Hartogs domains of the second type,in explicit formulas and the biholomorphic invariant J_(Y_(II)) for the domains Y_(II) are obtained.
利用全纯自同构映射,求出了第二类Cartan-Hartogs域YII上Bergman度量矩阵行列式detT(W,Z;W,Z)的显表达式,从而得到YII上的双全纯不变量JYII。
4) Hartogs phenomenon
Hartogs现象
1.
If H≤2|u|2u3,then M obeys the Hartogs phenomenon.
若H≤2｜ u｜2u3,则M满足Hartogs现象。
5) phenomenon of Hartogs extension
Hartogs延拓现象
6) generalized Hartoges polyhedral
广义Hartogs多面体
补充资料：[3-(aminosulfonyl)-4-chloro-N-(2.3-dihydro-2-methyl-1H-indol-1-yl)benzamide]
分子式：C16H16ClN3O3S
分子量：365.5
CAS号：26807-65-8
性质：暂无
制备方法：暂无
用途：用于轻、中度原发性高血压。
分子量：365.5
CAS号：26807-65-8
性质：暂无
制备方法：暂无
用途：用于轻、中度原发性高血压。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条