This paper continues the study of the consequences of the Bjorken-Gottfried
hypothesis for the HBT parameters measured in e(+)e(-) annihilation. It is
shown that introducing a natural cut-off for transverse momenta of emitted
particles, one can describe the observed ratio of transverse and longitudi
nal HBT radii for pions without destroying the good description of the mass
dependence of the HBT parameters for heavier particles.