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Self-consistency and covariance of light-front quark models: Testing via P , V , and A meson decay constants, and P → P weak transition form factors
In this paper, we test the self-consistencies of the standard and the covariant light-front quark model and study the zero-mode issue via the decay constants of pseudoscalar (P), vector (V) and axial-vector (A) mesons, as well as the P → P weak transition form factors. With the traditional type-I co...
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Published in: | Physical review. D 2018-12, Vol.98 (11), p.1, Article 114018 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In this paper, we test the self-consistencies of the standard and the covariant light-front quark model and study the zero-mode issue via the decay constants of pseudoscalar (P), vector (V) and axial-vector (A) mesons, as well as the P → P weak transition form factors. With the traditional type-I correspondence between the manifestly covariant and the light-front approach, the resulting fV as well as f1A and f3A obtained with the λ = 0 and λ = ± polarization states are different from each other, which presents a challenge to the self-consistency of the covariant light-front quark model. However, such a self-consistency problem can be “resolved” within the type-II scheme, which requires an additional replacement M → M0 relative to the type-I case. Moreover, the replacement M → M0 is also essential for the self-consistency of the standard light-front quark model. In the type-II scheme, the valence contributions to the physical quantities (Q) considered in this paper are always the same as that obtained in the standard light-front quark model, [Q] val = [Q] SLF, and the zero-mode contributions to fV,1A,3A and f− (q2) exist only formally but vanish numerically, which further implies that [Q]val ˙ = [Q] full. In addition, the manifest covariance of the covariant light-front quark model is violated in the traditional type-I scheme, but can be recovered by taking the type-II correspondence. |
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ISSN: | 2470-0010 2470-0029 |
DOI: | 10.1103/PhysRevD.98.114018 |