AbstractWe describe the electroproduction ratios of baryon–meson states from nucleon, inferring from the sea quarks in the nucleon using an extension of the quark model that takes into account the sea. As a result we provide, with no adjustable parameters, the predictions of ratios of exclusive meson–baryon final states: ΛK+, Σ⁎K, ΣK, pπ0, and nπ+. These predictions are in agreement with the new JLab experimental data showing that sea quarks play an important role in the electroproduction. We also predicted further ratios of exclusive reactions that can be measured and tested in future experiments. In particular, we suggested new experiments on deuterium and tritium. Such measurements can provide crucial tests of different predictions conce...
In this contribution I discuss recent results in light quark baryon spectroscopy involving CLAS data...
Abstract The difference between the strange and antistrange quark distributions, δs(x) = s(x) − s̄(...
The strong decays of excited nonstrange baryons into the final states Lambda K, Sigma K, and for the...
AbstractWe describe the electroproduction ratios of baryon–meson states from nucleon, inferring from...
We measured the ratios of electroproduction cross sections from a proton target for three exclusive ...
We measured the ratios of electroproduction cross sections from a proton target for three exclusive ...
<p>We measured the ratios of electroproduction cross sections from a proton target for three exclusi...
• With the advent of the new generation of electron-scattering facilities, such as CEBAF at JLab, th...
We present results on the electroexcitation of the low mass resonances Δ(1232)P[subscript 33], N(144...
We present some of our results for the electromagnetic properties of excited Σ hyperons, computed wi...
The role of nonvalence, e.g., sea quarks and/or meson degrees of freedom in static electroweak baryo...
Electrocouplings of excited proton states with masses less than 1.8 GeV were determined for the firs...
The flavor asymmetry of the nucleon sea, i e, the excess of d (d) over bar quark-antiquark pairs ove...
We propose the pure sea-quark contributions to the magnetic form factors of Σ baryons, GuΣ− and GdΣ+...
In this contribution I discuss recent results in light quark baryon spectroscopy involving CLAS data...
In this contribution I discuss recent results in light quark baryon spectroscopy involving CLAS data...
Abstract The difference between the strange and antistrange quark distributions, δs(x) = s(x) − s̄(...
The strong decays of excited nonstrange baryons into the final states Lambda K, Sigma K, and for the...
AbstractWe describe the electroproduction ratios of baryon–meson states from nucleon, inferring from...
We measured the ratios of electroproduction cross sections from a proton target for three exclusive ...
We measured the ratios of electroproduction cross sections from a proton target for three exclusive ...
<p>We measured the ratios of electroproduction cross sections from a proton target for three exclusi...
• With the advent of the new generation of electron-scattering facilities, such as CEBAF at JLab, th...
We present results on the electroexcitation of the low mass resonances Δ(1232)P[subscript 33], N(144...
We present some of our results for the electromagnetic properties of excited Σ hyperons, computed wi...
The role of nonvalence, e.g., sea quarks and/or meson degrees of freedom in static electroweak baryo...
Electrocouplings of excited proton states with masses less than 1.8 GeV were determined for the firs...
The flavor asymmetry of the nucleon sea, i e, the excess of d (d) over bar quark-antiquark pairs ove...
We propose the pure sea-quark contributions to the magnetic form factors of Σ baryons, GuΣ− and GdΣ+...
In this contribution I discuss recent results in light quark baryon spectroscopy involving CLAS data...
In this contribution I discuss recent results in light quark baryon spectroscopy involving CLAS data...
Abstract The difference between the strange and antistrange quark distributions, δs(x) = s(x) − s̄(...
The strong decays of excited nonstrange baryons into the final states Lambda K, Sigma K, and for the...