Abstract
We investigate $\phi$-meson electroproduction off the proton target, i.e., $\gamma^* p \to \phi p$, by employing a tree-level effective Lagrangian approach in the kinematical ranges of $Q^2$ = (0$-$4) $\mathrm{GeV}^2$, $W$ = (2$-$5) GeV, and $|t| \leq 2\,\mathrm{GeV}^2$. In addition to the universally accepted Pomeron exchange, we consider various meson exchanges in the $t$ channel with the Regge method. Direct $\phi$-meson radiations in the $s$- and $u$-channels are also taken into account. We find that the $Q^2$ dependence of the transverse ($\sigma_{\mathrm{T}}$) and longitudinal ($\sigma_{\mathrm{L}}$) cross sections are governed by Pomeron and $(a_0,f_0)$ scalar meson exchanges, respectively. Meanwhile, the contributions of $(\pi,\eta)$ pseudoscalar- and $f_1(1285)$ axial-vector-meson exchanges are much more suppressed. The results of the interference cross sections ($\sigma_{\mathrm{LT}}, \sigma_{\mathrm{LT}}$) and the spin-density matrix elements indicate that $s$-channel helicity conservation holds at $Q^2$ = (1$-$4) $\mathrm{GeV}^2$. The result of the parity asymmetry yield $P \simeq 0.95$ at $W$ = 2.5 GeV, meaning that natural-parity exchange dominates the reaction process. Our numerical results are in fair agreement with the experimental data and thus the use of our effective Reggeized model is justified over the considered kinematical ranges of $Q^2$, $W$, and $t$.
Highlights
Exclusive electroproduction of vector mesons is a suitable place to test model predictions in a kinematic region where the transition between the hadronic and partonic domains is involved according to the ranges of the photon virtuality Q2 and the photon center-of-mass (c.m.) energies W
We find that the Q2 dependence of the transverse and longitudinal cross sections are governed by Pomeron and (a0, f0) scalar-meson exchanges, respectively
The production mechanisms under consideration are drawn with the relevant Feynman diagrams in Fig. 2, which includes Pomeron (P ) (a), Reggeized f1(1285) axial-vector (AV) meson, (π, η) pseudoscalar (PS) meson, and (a0, f0) scalar (S) meson exchanges in the t channel (b), and direct φ-meson radiations via the proton in the s and u channels (c and d)
Summary
Exclusive electroproduction of vector mesons is a suitable place to test model predictions in a kinematic region where the transition between the hadronic and partonic domains is involved according to the ranges of the photon virtuality Q2 and the photon center-of-mass (c.m.) energies W. We take a similar approach for φ-meson electroproduction and test whether our hadronic description is applicable or not in the kinematical ranges of Q2 = (0–4) GeV2, W = (2–5) GeV, and |t| 2 GeV2. We examine the Q2 and t dependences on the transverse, longitudinal, and interference parts of the cross sections The latter enables us to test s-channel helicity conservation (SCHC). Parity asymmetry is calculated to check the relative strengths of natural to unnatural parity exchanges in the t channel For this purpose, we utilize our recent results for φ-meson photoproduction, γ p → φ p [23], where the relative contributions among the Pomeron and various meson exchanges were discussed in detail by analyzing a vast amount of CLAS data [24,25].
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