1983
DOI: 10.1016/0375-9601(83)90018-x
|View full text |Cite
|
Sign up to set email alerts
|

Superintegrability of the Calogero-Moser system

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

4
208
0
3

Year Published

1993
1993
2016
2016

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 196 publications
(215 citation statements)
references
References 5 publications
4
208
0
3
Order By: Relevance
“…The √ r factor in (2.21) gets cancelled in the similarity transformation (2.12), giving 8) and the angular wave function reads…”
Section: Jhep10(2015)191mentioning
confidence: 99%
See 1 more Smart Citation
“…The √ r factor in (2.21) gets cancelled in the similarity transformation (2.12), giving 8) and the angular wave function reads…”
Section: Jhep10(2015)191mentioning
confidence: 99%
“…Originally defined for the root system of A 1 ⊕ A n−1 , the Calogero model was quickly generalized for any finite Coxeter group of rank n [4]. In particular the rational version is remarkable for its conformal properties and its maximal superintegrability [8,9] (see also [10]). Moreover, when the coupling constant g is integral, the quantum model enjoys additional and algebraically independent conserved quantities, which make it 'analytically integrable' [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…A classical superintegrable system H = ͚ ij g ij p i p j + V͑x͒ on an n-dimensional local Riemannian manifold is one that admits 2n − 1 functionally independent symmetries ͑i.e., constants of the motion͒ S k , k =1, ... ,2n − 1 with S 1 = H. That is, ͕H , S k ͖ = 0 where ͕f,g͖ = ͚ j=1 n ‫ץ͑͑‬ x j f‫ץ‬ p j g − ‫ץ‬ p j f‫ץ‬ x j g͒͒ is the Poisson bracket for functions f͑x , p͒ , g͑x , p͒ on phase space. [1][2][3][4][5][6][7][8] Note that 2n − 1 is the maximum possible number of functionally independent symmetries and, locally, such symmetries always exist. The main interest is in symmetries that are polynomials in the p k and are globally defined, except for lower dimensional singularities such as poles and branch points.…”
Section: Introduction and Examplesmentioning
confidence: 99%
“…if the distribution D is integrable, we have a degenerate integrable system and a commutative diagram (3). An example of such system is the (spinless) Calogero-Moser system [30]. For other examples see [2][5].…”
Section: 2mentioning
confidence: 99%
“…One should emphasize that degenerate integrability is a special structure which is stronger than Liouville integrability: invariant tori now have dimension k < n. In the extreme case of k = 1 all trajectories are periodic. A degenerately integrable system may also be Liouville integrable, as in the case of spinless Calogero-Moser system [30].…”
Section: Introductionmentioning
confidence: 99%