2004
DOI: 10.1103/physrevd.70.114002
|View full text |Cite
|
Sign up to set email alerts
|

Octet, decuplet, and antidecuplet magnetic moments in the chiral quark soliton model reexamined

Abstract: We reanalyse the magnetic moments of the baryon octet, decuplet, and antidecuplet within the framework of the chiral quark-soliton model, with SU(3) symmetry breaking taken into account. We consider the contributions of the mixing of higher representations to the magnetic moment operator arising from the SU (3)

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

3
38
0

Year Published

2006
2006
2023
2023

Publication Types

Select...
5
3

Relationship

2
6

Authors

Journals

citations
Cited by 34 publications
(41 citation statements)
references
References 51 publications
3
38
0
Order By: Relevance
“…In a χSM, the collective operators for the HSD vector and axial-vector constants can be expressed in terms of the SU(3) Wigner D functions [20,36,37]:…”
Section: (213)mentioning
confidence: 99%
See 1 more Smart Citation
“…In a χSM, the collective operators for the HSD vector and axial-vector constants can be expressed in terms of the SU(3) Wigner D functions [20,36,37]:…”
Section: (213)mentioning
confidence: 99%
“…In fact, the analyses of the magnetic moments in a similar scheme to the present one were carried out in Refs. [36][37][38]. However, it was then not possible to determine all relevant parameters uniquely, so that the results were shown as functions either of m s or of the πN sigma term.…”
Section: Analysis Of the Hsd Constants For The Baryon Octetmentioning
confidence: 99%
“…[12,13,14,15,16] for additional theoretical approaches to γp → pπ 0 γ ′ ). On the theoretical side, predictions for the delta magnetic moment have been obtained in various approaches such as SU(6) symmetry [9], several quark models [17,18,19,20,21,22,23,24,25,26,27,28], the Skyrme model [29], the 1/N c expansion [30], lattice QCD [31,32,33], QCD sum rules [34,35], heavy-baryon chiral perturbation theory (HBChPT) [32,36,37], quenched ChPT [38], and chiral effective field theory [16]. The aim of this letter is to calculate the magnetic moment of the ∆(1232) up to and including chiral order p 3 in a manifestly Lorentz-invariant formulation of baryon chiral perturbation theory with explicit ∆ degrees of freedom (∆ChPT) [39].…”
Section: Introductionmentioning
confidence: 99%
“…The measurements of the baryon decuplet magnetic moments were reported for CC [223] and [224], to yield a new avenue for understanding hadron structure. The magnetic moments of baryon decuplet were theoretically investigated in several models such as quenched lattice gauge theory [225], quark models [226,227], chiral bag model [120], chiral perturbation theory [228], QCD sum rules [229,230], chiral quark model [231] and a chiral quark soliton model [232]. Moreover, by including effect of decuplet intermediate states of spin 3/2 baryons explicitly, heavy baryon chiral expansion of baryon octet magnetic moments [233] and charge radii [234] were investigated.…”
Section: Chapter 8 Phenomenological Solitonmentioning
confidence: 99%