Polarized deep inelastic scattering (DIS) data are analyzed in leading and next-to-leading order of QCD within the common ``standard'' scenario of polarized parton distributions with a flavor-symmetric light sea (antiquark) distribution δq̄, and a completely SU(3)f broken ``valence'' scenario with totally flavor-asymmetric light sea densities (δ ū \=u≠δd̄≠δs̄). The latter flavor-broken light sea distributions are modeled with the help of a Pauli-blocking ansatz at the low radiative or dynamical input scales of μLO(NLO)²=0.26 (0.40)GeV² which complies with predictions of the chiral quark-soliton model and expectations based on the statistical parton model as well as with the corresponding, well established, flavor-broken unpolarized sea (d̄> ū \=u). Present semi-inclusive DIS data cannot yet uniquely discriminate between those two flavor-symmetric and flavor-broken polarized light sea scenarios.
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Glück et al. (2001) studied this question.
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