The intrinsic quark-antiquark pairs generated by the minimal energy nonperturbative meson-baryon fluctuations in the nucleon sea provide a consistent framework for understanding a number of empirical anomalies observed in the deep inelastic quark-parton structure of nucleons: the flavor asymmetry of the nucleon sea implied by the violation of Gottfried sum rule, the proton spin problem implied by the violation of the Ellis-Jaffe sum rule, and the outstanding conflict between two different determinations of the strange quark sea in the nucleon
We investigate the effect of intrinsic sea quark-antiquark pairs on the magnetic moments of the SU(3...
The proton is a composite object made of fundamental, strongly-interacting quarks. Many of the featu...
Nontrivial q{anti q} sea effects have their origin in the low-Q{sup 2} dynamics of strong QCD. The a...
The intrinsic quark-antiquark pairs generated by the minimal energy nonperturbative meson-baryon flu...
Sea quark distributions in the nucleon have naively been expected to be generated perturbatively by ...
Sea quark distributions in the nucleon have naively been expected to be generated perturbatively by ...
The effects of “quark sea” in determining the flavor structure of the octet baryons have been invest...
The effects of “quark sea” in determining the flavor structure of the octet baryons have been invest...
After a pedagogical review of the simple constituent quark model and deep inelastic sum rules, we de...
Although the distributions of sea quarks and antiquarks generated by leading-twist QCD evolution thr...
It is shown that the proton spin problem raised by the Ellis-Jaffe sum rule violation does not in co...
Recent deep inelastic scattering and Drell-Yan experiments have revealed asurprisingly large asymmet...
The flavor asymmetry of the nucleon sea, i e, the excess of d (d) over bar quark-antiquark pairs ove...
AbstractThe flavor asymmetry of the nucleon sea, i.e., the excess of dd¯ quark–antiquark pairs over ...
AbstractDifference between the u¯ and d¯ sea quark distributions in the proton was first observed in...
We investigate the effect of intrinsic sea quark-antiquark pairs on the magnetic moments of the SU(3...
The proton is a composite object made of fundamental, strongly-interacting quarks. Many of the featu...
Nontrivial q{anti q} sea effects have their origin in the low-Q{sup 2} dynamics of strong QCD. The a...
The intrinsic quark-antiquark pairs generated by the minimal energy nonperturbative meson-baryon flu...
Sea quark distributions in the nucleon have naively been expected to be generated perturbatively by ...
Sea quark distributions in the nucleon have naively been expected to be generated perturbatively by ...
The effects of “quark sea” in determining the flavor structure of the octet baryons have been invest...
The effects of “quark sea” in determining the flavor structure of the octet baryons have been invest...
After a pedagogical review of the simple constituent quark model and deep inelastic sum rules, we de...
Although the distributions of sea quarks and antiquarks generated by leading-twist QCD evolution thr...
It is shown that the proton spin problem raised by the Ellis-Jaffe sum rule violation does not in co...
Recent deep inelastic scattering and Drell-Yan experiments have revealed asurprisingly large asymmet...
The flavor asymmetry of the nucleon sea, i e, the excess of d (d) over bar quark-antiquark pairs ove...
AbstractThe flavor asymmetry of the nucleon sea, i.e., the excess of dd¯ quark–antiquark pairs over ...
AbstractDifference between the u¯ and d¯ sea quark distributions in the proton was first observed in...
We investigate the effect of intrinsic sea quark-antiquark pairs on the magnetic moments of the SU(3...
The proton is a composite object made of fundamental, strongly-interacting quarks. Many of the featu...
Nontrivial q{anti q} sea effects have their origin in the low-Q{sup 2} dynamics of strong QCD. The a...