Hamilton系统Mei对称性的一种新守恒量  

A new type of conserved quantity of Mei symmetry for Hamilton system

作　　者：方建会[1] 丁宁[1] 王鹏[1] 

机构地区：[1]中国石油大学(华东)物理科学与技术学院,东营257061

出　　处：《物理学报》2007年第6期3039-3042,共4页Acta Physica Sinica

摘　　要：研究Hamilton系统的Mei对称性直接导致的一种新守恒量.给出Hamilton系统的Mei对称性的定义和判据方程,引入谐调函数,得到系统Mei对称性直接导致新守恒量的条件和形式,并给出应用算例.结果表明,谐调函数可根据寻找规范函数的需要适当选取,从而使规范函数的寻求变得比较容易,而且由于谐调函数的选取具有多样性,因此能够找到系统Mei对称性的更多的守恒量.A new type of conserved quantity which is directly induced by Mei symmetry of Hamilton system is studied. Firstly, the definition and criterion of Mei symmetry for Hamilton system are given. Secondly, a coordination function is introduced; the conditions from which the new type of conserved quantity can be induced by Mei symmetry and the form of the new type of conserved quantity are obtained. Lastly, an illustration example is given. The result indicates that the coordination function should be selected properly according to the demand of the gauge function, thereby the gauge function can be find out more easily. Furthermore, since the choice of the coordination function is not unique more conserved quantities of Mei symmetry for Hamilton system can be obtained.

关 键 词：HAMILTON系统 MEI对称性 新守恒量 

分 类 号：O316[理学—一般力学与力学基础]