Broad Range Of Momentum Transfers Research Articles

Strong three-meson couplings ofJ/ψandηc

We discuss the strong couplings $g_{PPV}$ and $g_{VVP}$ for vector ($V$) and pseudoscalar ($P$) mesons, at least one of which is a charmonium state $J/\psi$ or $\eta_c$. The strong couplings are obtained as residues at the poles of suitable form factors, calculated in a broad range of momentum transfers using a dispersion formulation of the relativistic constituent quark model. The form factors obtained in this approach satisfy all constraints known for these quantities in the heavy-quark limit. Our results suggest sizably higher values for the strong meson couplings than those reported in the literature from QCD sum rules.

Pion elastic and(π0,η,η′)→γγ*transition form factors in a broad range of momentum transfers

We analyze $F_\pi(Q^2)$ and $F_{P\gamma}(Q^2)$, $P=\pi,\eta,\eta'$, within the local-duality (LD) version of QCD sum rules, which allows one to obtain predictions for hadron form factors in a broad range of momentum transfers. To probe the accuracy of this approximate method, we consider, in parallel to QCD, a potential model: in this case, the exact form factors may be calculated from the solutions of the Schr\"odinger equation and confronted with the results from the quantum-mechanical LD sum rule. On the basis of our quantum-mechanical analysis we conclude that the LD sum rule is expected to give reliable predictions for $F_\pi(Q^2)$ and $F_{\pi\gamma}(Q^2)$ in the region $Q^2 \ge 5-6$ GeV$^2$. Moreover, the accuracy of the method improves rather fast with growing $Q^2$ in this region. For the pion elastic form factor, the data at small $Q^2$ indicate that the LD limit may be reached already at relatively low values of momentum transfers, $Q^2\approx 4-8$ GeV$^2$; we therefore conclude that large deviations from LD in the region $Q^2=20-50$ GeV$^2$ reported in some recent theoretical analyses seem unlikely. The data on the ($\eta,\eta')\to\gamma\gamma^*$ form factors meet very well the expectations from the LD model. Surprisingly, the {\sc BaBar} results for the $\pi^0\to\gamma\gamma^*$ form factor imply a violation of LD growing with $Q^2$ even at $Q^2\approx 40$ GeV$^2$, at odds with the $\eta,\eta'$ case and the experience from quantum mechanics.

Multipole resonances in open-shell nuclei: Connection with direct-reaction spectroscopy

Probability distributions for the excitation of the 1ħω multipole resonances E1, M6, and M2 in the sd-shell nuclei 18O, 22Ne, 24Mg, 26Mg, 27Al, 28Si, 32S, and 40Ca were obtained by means of the spectroscopy of direct pickup reactions within the particle-core coupling (PCC) version of the multiparticle shell model. The deviation of the ground state of a nucleus featuring A nucleons from the case of closed shells or subshells manifests itself in a broad range of the energy distribution of holes among states of (A − 1) nuclei. This energy spread is the main source of the fragmentation of multipole resonances in open-shell nuclei. A comparison of PCC theoretical results with experimental data confirms the applicability of the approach used over a broad range of momentum transfers and proves the existence of connections between direct and resonance processes.

Separated structure functions for the exclusive electroproduction ofK+ΛandK+Σ0final states

We report measurements of the exclusive electroproduction of $K^+\Lambda$ and $K^+\Sigma^0$ final states from a proton target using the CLAS detector at the Thomas Jefferson National Accelerator Facility. The separated structure functions $\sigma_T$, $\sigma_L$, $\sigma_{TT}$, and $\sigma_{LT}$ were extracted from the $\Phi$- and $\epsilon$-dependent differential cross sections taken with electron beam energies of 2.567, 4.056, and 4.247 GeV. This analysis represents the first $\sigma_L/\sigma_T$ separation with the CLAS detector, and the first measurement of the kaon electroproduction structure functions away from parallel kinematics. The data span a broad range of momentum transfers from $0.5\leq Q^2\leq 2.8$ GeV$^2$ and invariant energy from $1.6\leq W\leq 2.4$ GeV, while spanning nearly the full center-of-mass angular range of the kaon. The separated structure functions reveal clear differences between the production dynamics for the $\Lambda$ and $\Sigma^0$ hyperons. These results provide an unprecedented data sample with which to constrain current and future models for the associated production of strangeness, which will allow for a better understanding of the underlying resonant and non-resonant contributions to hyperon production.

Plasmon excitation in beryllium: inelastic x-ray scattering experiments and first-principlescalculations

An experimental and theoretical study of collective electronic excitations in Be ispresented. The plasmon energy and linewidth were measured by means of inelastic x-rayscattering spectroscopy. Measurements were performed on a polycrystalline sample and ina broad range of momentum transfers within the plasmon excitation regime.Theoretical plasmon dispersion and its linewidth in the whole Brillouin zone werederived from ab initio evaluations of the electron density response function. Thecalculations were performed with full inclusion of the electron band structure within therandom-phase approximation. Good agreement of experimental plasmon energy andlinewidth dispersions with direction-averaged theoretical results in all investigatedq-range is obtained. We conclude that, in Be, the band structureeffects alone can account for the observed finite plasmon lifetime atq = 0, as well as for the linewidth dispersion in the long-wavelength domain.

Distortion of the quasi-elastic peak in hadron scattering

The distortion, due to the strong absorption, of the quasi-elastic peak for hadronic reactions on nuclei is systematically analyzed, within the Glauber theory framework, for a broad range of momentum transfers. We observe a momentum dependent shift of the peak position, solely dye to the reaction mechanism, that dominates over the dynamical shift caused by the residual interaction in the random phase approximation.