Universality of the baryon axial vector current operator in large-$$N_c$$ chiral perturbation theory

Abstract The baryon axial vector current is computed in a combined formalism in $$1/N_c$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>1</mml:mn> <mml:mo>/</mml:mo> <mml:msub> <mml:mi>N</mml:mi> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> and chiral corrections. Flavor SU (3) symmetry breaking is accounted for in two ways: Implicitly through the integrals occurring in the one-loop graphs and explicitly through perturbative symmetry breaking. Loop integrals can be expanded in a power series in the ratio of the decuplet-octet baryon mass difference to the pseudoscalar meson mass and the first three terms in the series are retained and evaluated. The universal baryon axial vector current so constructed is neither diagonal nor off-diagonal in the sense that it can connect baryon states of either different or equal spins to obtain appropriate axial vector couplings. Processes of interest are found in octet-baryon and decuplet-baryon semileptonic decays and strong decays of decuplet baryons. A fit to the available experimental information is performed to determine the free parameters in the formalism, which allows one to estimate, for instance, the leading axial vector coupling in the semileptonic decays $$\Omega ^- \rightarrow \Xi ^0 \ell ^-\overline{\nu }_\ell $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mi>Ω</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:mo>→</mml:mo> <mml:msup> <mml:mi>Ξ</mml:mi> <mml:mn>0</mml:mn> </mml:msup> <mml:msup> <mml:mi>ℓ</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>ℓ</mml:mi> </mml:msub> </mml:mrow> </mml:math> and $$\Omega ^- \rightarrow {\Xi ^*}^0\ell ^-\overline{\nu }_\ell $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mi>Ω</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:mo>→</mml:mo> <mml:msup> <mml:mrow> <mml:msup> <mml:mi>Ξ</mml:mi> <mml:mo>∗</mml:mo> </mml:msup> </mml:mrow> <mml:mn>0</mml:mn> </mml:msup> <mml:msup> <mml:mi>ℓ</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>ℓ</mml:mi> </mml:msub> </mml:mrow> </mml:math> .

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Journal
The European Physical Journal C
Published
2025-09-24
DOI
https://doi.org/10.1140/epjc/s10052-025-14790-x
Primary Topic
Quantum Chromodynamics and Particle Interactions
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article
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article

Universality of the baryon axial vector current operator in large-$$N_c$$ chiral perturbation theory

Rubén Flores-Mendieta, Guillermo Sánchez-Almanza
The European Physical Journal C
Quantum Chromodynamics and Particle Interactions
article

Universality of the baryon axial vector current operator in large-$$N_c$$ chiral perturbation theory

Rubén Flores-Mendieta, Guillermo Sánchez-Almanza
article en

Abstract

Abstract The baryon axial vector current is computed in a combined formalism in $$1/N_c$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>1</mml:mn> <mml:mo>/</mml:mo> <mml:msub> <mml:mi>N</mml:mi> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> and chiral corrections. Flavor SU (3) symmetry breaking is accounted for in two ways: Implicitly through the integrals occurring in the one-loop graphs and explicitly through perturbative symmetry breaking. Loop integrals can be expanded in a power series in the ratio of the decuplet-octet baryon mass difference to the pseudoscalar meson mass and the first three terms in the series are retained and evaluated. The universal baryon axial vector current so constructed is neither diagonal nor off-diagonal in the sense that it can connect baryon states of either different or equal spins to obtain appropriate axial vector couplings. Processes of interest are found in octet-baryon and decuplet-baryon semileptonic decays and strong decays of decuplet baryons. A fit to the available experimental information is performed to determine the free parameters in the formalism, which allows one to estimate, for instance, the leading axial vector coupling in the semileptonic decays $$\Omega ^- \rightarrow \Xi ^0 \ell ^-\overline{\nu }_\ell $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mi>Ω</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:mo>→</mml:mo> <mml:msup> <mml:mi>Ξ</mml:mi> <mml:mn>0</mml:mn> </mml:msup> <mml:msup> <mml:mi>ℓ</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>ℓ</mml:mi> </mml:msub> </mml:mrow> </mml:math> and $$\Omega ^- \rightarrow {\Xi ^*}^0\ell ^-\overline{\nu }_\ell $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mi>Ω</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:mo>→</mml:mo> <mml:msup> <mml:mrow> <mml:msup> <mml:mi>Ξ</mml:mi> <mml:mo>∗</mml:mo> </mml:msup> </mml:mrow> <mml:mn>0</mml:mn> </mml:msup> <mml:msup> <mml:mi>ℓ</mml:mi> <mml:mo>-</mml:mo> </mml:msup> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>ℓ</mml:mi> </mml:msub> </mml:mrow> </mml:math> .

The European Physical Journal CVol. 85(9)
Autonomous University of San Luis Potosí (MX)
Openalex Percentile: Top 89%
Quantum Chromodynamics and Particle Interactions
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