2006
DOI: 10.1142/s0129055x06002802
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The Schwinger Representation of a Group: Concept and Applications

Abstract: The concept of the Schwinger Representation of a finite or compact simple Lie group is set up as a multiplicity-free direct sum of all the unitary irreducible representations of the group. This is abstracted from the properties of the Schwinger oscillator construction for SU (2), and its relevance in several quantum mechanical contexts is highlighted. The Schwinger representations for SU (2), SO(3) and SU (n) for all n are constructed via specific carrier spaces and group actions. In the SU (2) case connection… Show more

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Cited by 39 publications
(29 citation statements)
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“…Here, S applies to any two degrees of freedom, which relates to the Schwinger representation of two harmonic oscillators; see Ref. [28] for a review. We have…”
Section: Essential Quantum Correlationsmentioning
confidence: 99%
See 1 more Smart Citation
“…Here, S applies to any two degrees of freedom, which relates to the Schwinger representation of two harmonic oscillators; see Ref. [28] for a review. We have…”
Section: Essential Quantum Correlationsmentioning
confidence: 99%
“…Let us also mention that the Stokes operators have the properties of a spin angular momentum algebra [26][27][28], withĴ =Ŝ/2 andĴ 2 =Ĵ ·Ĵ = (N /2)(N /2 +1). As we restrict ourselves to linear scenarios, let us also briefly comment on other types of interference schemes.…”
Section: Essential Quantum Correlationsmentioning
confidence: 99%
“…In this paper, we extend these ideas to spinlike systems, where the classical phase space is the unit sphere. We stress that this is not a mere academic curiosity, since the underlying SU(2) symmetry plays a pivotal role in numerous models in physics [27].…”
Section: Introductionmentioning
confidence: 95%
“…Here we aim to devise an algorithm to construct the D-functions of arbitrary representations of SU(n) for arbitrary n. We approach the problem of limited availability of SU(n) D-functions 47,48 by presenting (i) a mapping of the weights of an irrep to a graph, (ii) a graph-theoretic algorithm to compute boson realizations of the canonical basis states of SU(n) for arbitrary n (Algorithm 2 in Subsection IV B) and (iii) an algorithm that employs the constructed boson realizations to compute expressions for D-functions as polynomials in the matrix elements of the defining representation (Algorithm 3 in Subsection IV C).…”
Section: Introductionmentioning
confidence: 99%