We study the effects of the degeneracy of the eg orbitals as well as the double exchange interaction with t2g spins in perovskite transition-metal oxides. In addition to the spin field Si, the isospin field Ti is introduced to describe the orbital degrees of freedom. The isospin is the quantum dynamical variable, and is represented by the boson with a constraint. The dispersion of this boson is flat along (π/a, π/a, kz) (a: lattice constant) and the other two equivalent directions. This enables the orbital disordered phase down to low temperatures. We interpret some of the anomalous experiments, i.e., optical absorption and d.c. resistivity, in the low temperature ferromagnetic phase of La1−xSrxMnO3 with x > 0.2 in terms of this orbital liquid picture. 71.27.+a, 71.30.+h, 75.30.Et The colossal negative magneto-resistance observed in transition-metal oxides with perovskite structure, e.g., the double exchange system La 1−x Sr x MnO 3 , has revived the interest in these systems [1][2][3][4]. The valency of Mn ion is Mn 3+ for x = 0, whose electron configuration is (t 2g ) 3 (e g ) 1 , and all the spins are aligned ferromagnetically due to the strong Hund coupling. Because of the strong on-site repulsion, the double occupancy of e g orbitals is forbidden [5,6], and the system is a Mott insulator. When one La is replaced by Sr, one hole is introduced to Mn and Mn 3+ turns into Mn 4+ . These doped holes, which contribute to the conduction, can not be described in terms of the one-body theory. For a single band case, which is relevant to high-Tc cuprates, extensive studies have been focused on these doped holes to a Mott insulator. One of the promising approaches is resonating valence bond (RVB) theory [7,8], where the spin and charge are separated. In the orbital-degenerate case, this idea can be generalized also to the orbital degrees of freedom as shown below [9].Experimentally the orbital ordering has been established in the low hole-concentration region, i.e., x ∼ 0.0 [10], where the system is insulating with the A-type antiferromagnetic long range ordering (AFLRO) [11]. As x increases the system becomes more and more conductive, and finally shows the metallic conduction below the ferromagnetic transition temperature T c . In this metallic state (x > 0.2), there are several anomalous features.(1) The optical conductivity shows a narrow coherent peak up to around 0.02eV followed by a broader "Drude like" band up to around 1eV [12]. The integrated oscillator strength for this two-component Drude absorption changes down to the very low temperature where the ferromagnetic moment already saturates, which suggests that other degrees of freedom still remain active.(2) The photoemission spectra shows only a small discontinuity at the Fermi energy E F followed by a gap like behavior [13][14][15]. On the other hand, the specific heat is not enhanced with γ ∼ 5mJ/K 2 mol [15]. (3) The anisotropy of the conduction and the spin excitation, which is expected with the orbital ordering, is not observed even at low temperature...