2004
DOI: 10.1002/prop.200310124
|View full text |Cite
|
Sign up to set email alerts
|

Representations of the Schrödinger algebra and Appell systems

Abstract: We investigate the structure of the Schrödinger algebra and its representations in a Fock space realized in terms of canonical Appell systems. Generalized coherent states are used in the construction of a Hilbert space of functions on which certain commuting elements act as self-adjoint operators. This yields a probabilistic interpretation of these operators as random variables. An interesting feature is how the structure of the Lie algebra is reflected in the probability density function. A Leibniz function a… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
28
0

Year Published

2011
2011
2022
2022

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 28 publications
(28 citation statements)
references
References 12 publications
0
28
0
Order By: Relevance
“…The theorem of Stone and von Neumann (see appendix A) implies that, given the mass m, there is a unique UIR of the Heisenberg subalgebra. The authors of [47] proved that any massive representation of the Schrödinger algebra is equivalent to the following realisation of the remaining generatorŝ 5) where the operatorsL ij ,L ± andL 0 commute with all the other generators and provide a representation of o(d) ⊕ sl(2, R) with usual notations. In a sense, the latter operators correspond to the "spinning" or "internal" part of the generators while the "orbital" part is entirely built out of the translation and boost generators.…”
Section: Jhep02(2012)113mentioning
confidence: 99%
“…The theorem of Stone and von Neumann (see appendix A) implies that, given the mass m, there is a unique UIR of the Heisenberg subalgebra. The authors of [47] proved that any massive representation of the Schrödinger algebra is equivalent to the following realisation of the remaining generatorŝ 5) where the operatorsL ij ,L ± andL 0 commute with all the other generators and provide a representation of o(d) ⊕ sl(2, R) with usual notations. In a sense, the latter operators correspond to the "spinning" or "internal" part of the generators while the "orbital" part is entirely built out of the translation and boost generators.…”
Section: Jhep02(2012)113mentioning
confidence: 99%
“…The lowest weight vector w 0 of the factor module V d,r /I 0 satisfies the condition 22) and the basis of V d,r /I 0 is given by…”
Section: Irreducible Modulesmentioning
confidence: 99%
“…We mention the followings: Projective representations of the Schrödinger group in 3 spatial dimension were constructed in [19]. Irreducible representations of the Schrödinger algebras up to 3 spatial dimension were investigated in [20][21][22]. The author of [23] studied the highest weight representations of the N = 2 super Schrödinger algebra in 2 spatial dimension ("exotic" algebra in the terminology of [14]).…”
Section: Introductionmentioning
confidence: 99%
“…where a, b ∈ C with |a| < 2 and Φ is the Fock vacuum such that B 2 Φ, is given by (see Theorem 6.1 of [9] for c = μ(I) / 2 and a, b ∈ R; for a detailed proof see [10])…”
Section: The Schrödinger Algebra In Terms Of the Rhp W N Generatorsmentioning
confidence: 99%
“…the avoidance of the RHP W N no-go theorems, in what follows we will use the notation B 3. The Schrödinger kernel and the no-go theorem for Heis and RSW N As shown in [9], for μ(I) = 0 the operators…”
Section: The Schrödinger Algebra In Terms Of the Rhp W N Generatorsmentioning
confidence: 99%