ﻻ يوجد ملخص باللغة العربية
The extracted value for the $g^{eff}_{omega rhopi}$ effective coupling from experimental data, considering only the $rho$ meson, resumes not only the $rho$ meson effect but also all its additional radial excitation modes. By explicitly adding the radial excitations of the $rho$ meson, considering a particular form of the spectrum and relations among the couplings, we identify the single $g_{omega rho pi}$ and the $rho$ radial excitations effect in the $omega rightarrow pi^0 gamma$ decay. We obtain that the individual coupling is in the range $g_{omegarhopi}= 8.2 - 8.6 {text GeV}^{-1}$, which is about 40% smaller than the effective $g^{eff}_{omegarhopi}$. We verify the consistency with the chiral approach in the $pi^0 rightarrow gammagamma$ and $gamma^* rightarrow 3pi$ processes. Besides the model dependence, our description succeeds in exhibiting how each contribution came into the game. In particular, we show that for the $gamma^* rightarrow 3 pi$ decay, the usual relation $mathcal{A}^{VMD}_{gamma3pi}=(3/2)mathcal{A}^{WZW}_{gamma3pi}$, encodes all the vector contributions and not only the $rho$ meson one. In addition, we find that there is an almost exact (accidental) cancelation between the radial excitations and the contact term contributions.
The atomic nucleus capability of responding by hydromagnetic vibrations, that has been considered long ago by Hannes Alfven, is re-examined in the context of current development of nuclear physics and pulsar astrophysics.
We argue that an expanding quark-gluon plasma has an anomalous viscosity, which arises from interactions with dynamically generated colour fields. The anomalous viscosity dominates over the collisional viscosity for large velocity gradients or weak c
We study the origin of the resonances associated with pole singularities of the scattering amplitude in the chiral unitary approach. We propose a natural renormalization scheme using the low-energy interaction and the general principle of the scatter
We present results for kaon decay widths of baryon resonances from a relativistic study with constituent quark models. The calculations are done in the point-form of Poincare-invariant quantum mechanics with a spectator-model decay operator. We obtai
Constituent quark models provide a reasonable description of the baryon mass spectra. However, even in the light- and strange-flavor sectors several intriguing shortcomings remain. Especially with regard to strong decays of baryon resonances no consi