New Positive and Negative Hierarchies of Integrable Differential-Difference Equations and Conservation Laws

2009 ◽  
Vol 51 (1) ◽  
pp. 17-22 ◽  
Author(s):  
Li Xin-Yue ◽  
Zhao Qiu-Lan
2019 ◽  
Vol 2019 ◽  
pp. 1-14
Author(s):  
J. J. H. Bashingwa ◽  
A. H. Kara

We present geometric based methods for solving systems of discrete or difference equations and introduce a technique for finding conservation laws for such systems.


2006 ◽  
Vol 39 (45) ◽  
pp. 14055-14066 ◽  
Author(s):  
Olexandr G Rasin ◽  
Peter E Hydon

Author(s):  
E L Mansfield ◽  
A Rojo-Echeburúa ◽  
P E Hydon ◽  
L Peng

Abstract We consider the calculation of Euler–Lagrange systems of ordinary difference equations, including the difference Noether’s theorem, in the light of the recently-developed calculus of difference invariants and discrete moving frames. We introduce the difference moving frame, a natural discrete moving frame that is adapted to difference equations by prolongation conditions. For any Lagrangian that is invariant under a Lie group action on the space of dependent variables, we show that the Euler–Lagrange equations can be calculated directly in terms of the invariants of the group action. Furthermore, Noether’s conservation laws can be written in terms of a difference moving frame and the invariants. We show that this form of the laws can significantly ease the problem of solving the Euler–Lagrange equations, and we also show how to use a difference frame to integrate Lie group invariant difference equations. In this Part I, we illustrate the theory by applications to Lagrangians invariant under various solvable Lie groups. The theory is also generalized to deal with variational symmetries that do not leave the Lagrangian invariant. Apart from the study of systems that are inherently discrete, one significant application is to obtain geometric (variational) integrators that have finite difference approximations of the continuous conservation laws embedded a priori. This is achieved by taking an invariant finite difference Lagrangian in which the discrete invariants have the correct continuum limit to their smooth counterparts. We show the calculations for a discretization of the Lagrangian for Euler’s elastica, and compare our discrete solution to that of its smooth continuum limit.


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