2021
DOI: 10.1142/s0219887821300063
|View full text |Cite
|
Sign up to set email alerts
|

Symmetries and reduction Part II — Lagrangian and Hamilton–Jacobi picture

Abstract: Following the analysis we have presented in a previous paper (that we refer to as [I]), we describe a Noether theorem related to symmetries, with the associated reduction procedures, for classical dynamics within the Lagrangian and the Hamilton–Jacobi formalism.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2022
2022
2022
2022

Publication Types

Select...
2

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 62 publications
0
2
0
Order By: Relevance
“…In this section, we review the geometrical theory of symmetries that can be constructed for dynamical systems, admitting a symplectic or presymplectic formulation. We refer to [6,7,21], and references therein, for a more detailed exposition.…”
Section: Symmetries For Presymplectic Dynamicsmentioning
confidence: 99%
See 1 more Smart Citation
“…In this section, we review the geometrical theory of symmetries that can be constructed for dynamical systems, admitting a symplectic or presymplectic formulation. We refer to [6,7,21], and references therein, for a more detailed exposition.…”
Section: Symmetries For Presymplectic Dynamicsmentioning
confidence: 99%
“…These aspects, and many more, have been extensively analyzed in the last two centuries, both within the mathematical and theoretical physics literature: a (far from exhaustive) list of contributions where the previous ideas have been developed include [1][2][3][4][5][6][7][8][9][10][11][12][13][14], where Noether's theorems (that is the relation between symmetries and the so called conservation laws) are also elucidated. In particular, in recent references where classical field theories were analyzed within the setting of jet bundles and their duals, conserved currents associated with symmetries of an action functional are modeled as (m − 1)-forms on a fiber bundle underlying the theory (with m the dimension of the space-time in which the theory is developed, see, for instance, [8,[15][16][17]).…”
Section: Introductionmentioning
confidence: 99%