TY - JOUR
T1 - Doubly virtual (π0,η,η′) →γ∗γ∗ transition form factors in the light-front quark model
AU - Choi, Ho Meoyng
AU - Ryu, Hui Young
AU - Ji, Chueng Ryong
N1 - Publisher Copyright:
© 2019 authors. Published by the American Physical Society.r(s) and the published article's title, journal citation, and DOI. Funded by SCOAP .
PY - 2019/4/1
Y1 - 2019/4/1
N2 - We report our investigation on the doubly virtual transition form factors (TFFs) FPγ∗(Q12,Q22) for the P→γ∗(q1)γ∗(q2)(P=π0,η,η′) transitions using the light-front quark model (LFQM). Performing a LF calculation in the exactly solvable manifestly covariant Bethe-Salpeter (BS) model as the first illustration, we use the q1+=0 frame and find that both LF and manifestly covariant calculations produce exactly the same results for FPγ∗(Q12,Q22). This confirms the absence of the LF zero mode in the doubly virtual TFFs. We then map this covariant BS model to the standard LFQM using the more phenomenologically accessible Gaussian wave function provided by the LFQM analysis of meson mass spectra. For the numerical analyses of FPγ∗(Q12,Q22), we compare our LFQM results with the available experimental data and the perturbative QCD (pQCD) and vector meson dominance (VMD) model predictions. As (Q12,Q22)→, our LFQM result for doubly virtual TFF is consistent with the pQCD prediction, i.e., FPγ∗(Q12,Q22)∼1/(Q12+Q22), while it differs greatly from the result of the VMD model, which behaves as FPγ∗VMD(Q12,Q22)∼1/(Q12Q22). Our LFQM prediction for Fη′γ∗(Q12,Q22) shows an agreement with the very recent experimental data obtained from the BABAR Collaboration for the ranges of 2<(Q12,Q22)<60 GeV2.
AB - We report our investigation on the doubly virtual transition form factors (TFFs) FPγ∗(Q12,Q22) for the P→γ∗(q1)γ∗(q2)(P=π0,η,η′) transitions using the light-front quark model (LFQM). Performing a LF calculation in the exactly solvable manifestly covariant Bethe-Salpeter (BS) model as the first illustration, we use the q1+=0 frame and find that both LF and manifestly covariant calculations produce exactly the same results for FPγ∗(Q12,Q22). This confirms the absence of the LF zero mode in the doubly virtual TFFs. We then map this covariant BS model to the standard LFQM using the more phenomenologically accessible Gaussian wave function provided by the LFQM analysis of meson mass spectra. For the numerical analyses of FPγ∗(Q12,Q22), we compare our LFQM results with the available experimental data and the perturbative QCD (pQCD) and vector meson dominance (VMD) model predictions. As (Q12,Q22)→, our LFQM result for doubly virtual TFF is consistent with the pQCD prediction, i.e., FPγ∗(Q12,Q22)∼1/(Q12+Q22), while it differs greatly from the result of the VMD model, which behaves as FPγ∗VMD(Q12,Q22)∼1/(Q12Q22). Our LFQM prediction for Fη′γ∗(Q12,Q22) shows an agreement with the very recent experimental data obtained from the BABAR Collaboration for the ranges of 2<(Q12,Q22)<60 GeV2.
UR - http://www.scopus.com/inward/record.url?scp=85065169014&partnerID=8YFLogxK
U2 - 10.1103/PhysRevD.99.076012
DO - 10.1103/PhysRevD.99.076012
M3 - Article
AN - SCOPUS:85065169014
SN - 2470-0010
VL - 99
JO - Physical Review D
JF - Physical Review D
IS - 7
M1 - 076012
ER -