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1)  generalized vector Fritz-John saddle point
广义向量Fritz-John鞍点
1.
In ordered linear spaces,generalized vector Fritz-John saddle point and generalized vector Kuhn-Tucker saddle point of set-valued optimization problems with generalized inequality constraints were defined,and the relations between them were established.
在序线性空间中定义了带广义不等式约束集值优化问题的广义向量Fritz-John鞍点和广义向量Kuhn-Tucker鞍点,建立了二者之间关系。
2)  vector Fritz John saddle point
向量Fritz-John鞍点
3)  generalized vector Kuhn-Tucker saddle point
广义向量Kuhn-Tucker鞍点
1.
In ordered linear spaces,generalized vector Fritz-John saddle point and generalized vector Kuhn-Tucker saddle point of set-valued optimization problems with generalized inequality constraints were defined,and the relations between them were established.
在序线性空间中定义了带广义不等式约束集值优化问题的广义向量Fritz-John鞍点和广义向量Kuhn-Tucker鞍点,建立了二者之间关系。
4)  Generalized saddle point
广义鞍点
1.
Super efficient point in vector optimization problems with set-valued maps characterized by generalized saddle point;
集值向量优化问题超有效点的广义鞍点刻画
2.
By using the properties of generalized saddle points and a separation theorem,a property of generalized saddle points is proved with set separation.
本文研究集值优化问题严有效解的广义鞍点刻画问题。
5)  Fritz John condition
Fritz John条件
1.
With Fritz John condition, we change the condition into an algebraic one in terms of the solutions of equations and inequality, which is easy to verify.
首先将系统的二次稳定性转化为等价的带约束非线性规划问题 ,给出了系统二次稳定的充分必要条件 ;然后利用 Fritz John条件 ,将该充要条件转化为较易检验的以代数方程和不等式的解表示的代数条件 ,最后举例说明了该代数条件的使用 。
6)  generalized weak saddle point
广义弱鞍点
1.
This paper establishes one kind of constructions for vector Lagrangian functionals in a class of multiobjective fractional optimal control problems, called generalized Lagrangian functionals, and the relationship between the weak efficiency and generalized weak saddle points of such a kind of generalized Lagrangian functionals is discussed.
给出一类多目标分式最优控制问题的向量 Lagrange泛函的构造 ,称为广义 Lagrange泛函 ,并且讨论弱有效性和这样一种广义 Lagrange泛函的广义弱鞍点之间的关
补充资料:鞍点
分子式:
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性质:数学上同时具备极大与极小性质的点。应用于三维势能面及裂变核势能曲面上,与反应坐标相垂直的方向上过渡态位于势能的最低点,发生对称伸缩振动。在沿反应坐标方向上过渡态位于势能的最高点,发生不对称伸缩振动。过渡态在势能面所处的这一点即势能面的鞍点。

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