Skip to content
DraconiticResearch
Search Sources API
197,768 studies31 sourcesUpdated 43 min ago
PreprintarXiv licencearXiv

Distribution amplitudes of vector and axial-vector mesons in a nonperturbatively improved symmetry-preserving framework

Abstract

Using continuum Schwinger-function methods with a nonperturbatively improved, symmetry-preserving kernel, we deliver predictions for the leading-twist light-front distribution amplitudes (DAs) of the ρ, K∗, a1(1260), b1(1235), and the unmixed strange partners of the 1++ and 1+− axial-vector (AV) channels, reconstructed from Mellin moments of the associated Bethe--Salpeter wave functions. For vector mesons, polarisation barely affects longitudinal momentum sharing: the longitudinal and transverse DAs are nearly degenerate, and both narrower than the asymptotic distribution in the second-moment sense. The AV sector is different in kind. Charge conjugation compels one projection -- interchanged between the 1++ and 1+− channels -- to vanish at x=1/2 and change sign; breaking SUF(3) symmetry removes this protection, whereupon the zeroth moments become nonzero and the nodes shift from the midpoint. Under a common weighted normalisation, the 1+− zeroth moment is $1.63$ times that of the 1++ channel, and the profile distortion follows the same pattern. A coupling forbidden by charge conjugation in the symmetric limit, fb1=0, becomes fK1+−=0.019GeV in the strange channel: an independent measure of the same symmetry breaking, obtained from a current matrix element rather than from the DA reconstruction. What distinguishes the two sectors is thus a symmetry-enforced zero, not the size of the flavour asymmetry.

Related

  1. Pion and η meson gravitational form factors from GPDs at non-zero skewness and distribution amplitudes within the Graviton Soft-Wall model
    Filippo Fornetti, Matteo Rinaldi, Sergio Scopetta
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
  2. Electromagnetic tails of B-meson light-cone distribution amplitudes
    Max Ferré, Matthias Neubert
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsarXiv
  3. Towards power corrections in the factorization of baryon quasi-distribution amplitudes in LaMET
    Yu-Ji Shi, Jun Zeng
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsarXiv
  4. Medium modification of pseudoscalar meson structure: Distribution amplitudes and parton distribution functions
    Muhammad Ridwan, Parada Tobel Paraduan Hutauruk, Ahmad Jafar Arifi +1
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsNuclear physicsarXiv
  5. Three-particle di-light-cone distribution amplitudes of the B-meson in heavy-quark effective theory
    Riccardo Bartocci, Philipp Böer, Thorsten Feldmann +3
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
BibTeX
@misc{xu2026distribution,
  title = {{Distribution amplitudes of vector and axial-vector mesons in a nonperturbatively improved symmetry-preserving framework}},
  author = {Zhen-Ni Xu and Zhao-Qian Yao and Peng Cheng and Khépani Raya},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.02329},
  eprint = {2609.02329},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.02329},
}
RIS
TY  - UNPB
TI  - Distribution amplitudes of vector and axial-vector mesons in a nonperturbatively improved symmetry-preserving framework
AU  - Zhen-Ni Xu
AU  - Zhao-Qian Yao
AU  - Peng Cheng
AU  - Khépani Raya
PY  - 2026
DA  - 2026/09/03
PB  - arXiv
DO  - 10.48550/arxiv.2609.02329
UR  - https://arxiv.org/abs/2609.02329
AB  - Using continuum Schwinger-function methods with a nonperturbatively improved, symmetry-preserving kernel, we deliver predictions for the leading-twist light-front distribution amplitudes (DAs) of the ρ, K^∗, a_1(1260), b_1(1235), and the unmixed strange partners of the 1^++ and 1^+− axial-vector (AV) channels, reconstructed from Mellin moments of the associated Bethe--Salpeter wave functions. For vector mesons, polarisation barely affects longitudinal momentum sharing: the longitudinal and transverse DAs are nearly degenerate, and both narrower than the asymptotic distribution in the second-moment sense. The AV sector is different in kind. Charge conjugation compels one projection -- interchanged between the 1^++ and 1^+− channels -- to vanish at x=1/2 and change sign; breaking SU_F(3) symmetry removes this protection, whereupon the zeroth moments become nonzero and the nodes shift from the midpoint. Under a common weighted normalisation, the 1^+− zeroth moment is $1.63$ times that of the 1^++ channel, and the profile distortion follows the same pattern. A coupling forbidden by charge conjugation in the symmetric limit, f_b_1=0, becomes f_K_1^+−=0.019GeV in the strange channel: an independent measure of the same symmetry breaking, obtained from a current matrix element rather than from the DA reconstruction. What distinguishes the two sectors is thus a symmetry-enforced zero, not the size of the flavour asymmetry.
ER  -