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The disappearance of directed, collective nuclear motion (``flow'') away from the interaction region of heavy-ion collisions has been observed using the Lawrence Berkeley Laboratory Streamer Chamber. We find that flow vanishes at a beam energy near 50 MeV/nucleon for the ¹³⁹La{+}¹³⁹$La system and near 60 MeV/nucleon for the $⁹³Nb+⁹³Nb system. The disappearance of flow may be understood as resulting from a balance between attractive and repulsive scattering strengths. Full calculations with the Boltzmann-Uehling-Uhlenbeck model show that the disappearance of flow is sensitive to the assumed nuclear equation of state (EOS) and to the in-medium scattering cross section (σNN). Also, in the ⁹³Nb{+}⁹³$Nb system, the purely attractive contribution to the reduced flow does not appear to be strongly sensitive to the EOS assumptions.
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Krofcheck et al. (1992) studied this question.
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