Although the distributions of sea quarks and antiquarks generated by l
eading-twist QCD evolution through gluon splitting g --> (q) over bar
q are necessarily CP symmetric, the distributions of nonvalence quarks
and antiquarks which are intrinsic to the nucleon's bound state wavef
unction need not be identical. In this paper we investigate the sea qu
ark-antiquark asymmetries in the nucleon wavefunction which are genera
ted by a light-cone model of energetically-favored meson-baryon fluctu
ations. The model predicts striking quark-antiquark asymmetries in the
momentum and helicity distributions for the down and strange contribu
tions to the proton structure function: the intrinsic d and s quarks i
n the proton sea are predicted to be negatively polarized, whereas the
intrinsic (d) over bar and (s) over bar antiquarks give zero contribu
tions to the proton spin, Such a picture is supported by experimental
phenomena related to the proton spin problem and the violation of the
Ellis-Jaffe sum rule. The light-cone meson-baryon fluctuation model al
so suggests a structured momentum distribution asymmetry for strange q
uarks and antiquarks which could be relevant to an outstanding conflic
t between two different determinations of the strange quark sea in the
nucleon. The model predicts an excess of intrinsic d (d) over bar pai
rs over u (u) over bar pairs, as supported by the Gottfried sum rule v
iolation. We also predict that the intrinsic charm and anticharm helic
ity and momentum distributions are not identical.