We present a theory for the transition between two ferromagnetic phases obs
erved experimentally in lightly doped La1-xSrxMnO3. Starting from an electr
onic model, the instabilities to various types of orbital orderings are stu
died within the random-phase approximation. In most cases, the instabilitie
s occur in the region of strong correlations. A phase diagram is calculated
in the case of strong correlation by means of the projected perturbation t
echnique and the Schwinger boson technique. A phase transition between two
types of orbital ordering occurs at a low doping, which may be closely rele
vant to recent experimental observations.