Ultrafast time-domain thermoreflectance (TDTR) is utilized to extract the through-plane thermal conductivity (Λ LSCO ) of epitaxial La 0.5 Sr 0.5 CoO 3−δ (LSCO) of varying thickness (<20 nm) on LaAlO 3 and SrTiO 3 substrates. These LSCO films possess ordered oxygen vacancies as the primary means of lattice mismatch accommodation with the substrate, which induces compressive/tensile strain and thus controls the orientation of the oxygen vacancy ordering (OVO). TDTR results demonstrate that the room-temperature Λ LSCO of LSCO on both substrates (1.7 W m −1 K −1 ) are nearly a factor of four lower than that of bulk single-crystal LSCO (6.2 W m −1 K −1 ). Remarkably, this approaches the lower limit of amorphous oxides (e.g., 1.3 W m −1 K −1 for glass), with no dependence on the OVO orientation. Through theoretical simulations, origins of the glass-like thermal conductivity of LSCO are revealed as a combined effect resulting from oxygen vacancies (the dominant factor), Sr substitution, size effects, and the weak electron/phonon coupling within the LSCO film. The absence of OVO dependence in the measured Λ LSCO is rationalized by two main effects: (1) the nearly isotropic phononic thermal conductivity resulting from the imperfect OVO planes when δ is small; (2) the missing electronic contribution to Λ LSCO along the through-plane direction for these ultrathin LSCO films on insulating substrates.fraction of the metals in the periodic table on either the A or B cationic site. This flexibility allows for the tuning of many functionalities by substitution of A and/ or B site cations, as well as by control of oxygen stoichiometry (i.e., by inducing oxygen vacancies or interstitials). One such example is in strontium-doped lanthanum cobaltite, La 1−x Sr x CoO 3−δ (LSCO), in which divalent Sr 2+ substitution for La 3+ hole-dopes the initially insulating and nonferromagnetic LaCoO 3 (LCO), increases the formal Co valence, and induces metallic ferromagnetism via a spin-state transition. [11] Control of the oxygen stoichiometry has been shown similarly effective in tuning the properties of LSCO. Oxygen vacancies compensate Sr-induced holes, destabilizing metallicity, and ferromagnetism, and thus controlling both. Moreover, the presence of oxygen vacancies has been shown to critically influence the high oxygen conductivity that makes LSCO an excellent candidate for gas separation membranes, [12] gas sensors, [13] and solid oxide fuel cell cathodes. [7,14] Oxygen vacancies readily form above x = 0.5 in LSCO due to the general instability of Co 4+ in octahedral coordination. [15] This is also evidenced by the very high oxygen pressure needed to form SrCoO 3 (x = 1), [16] and the tendency of SrCoO 3−δ to form Sr 2 Co 2 O 5 (SrCoO 2.5 ), the so-called Brownmillerite structure, with ordered oxygen vacancies. [17] The Brownmillerite structure is derived from perovskite when oxygen vacancies form in alternating (001) Co-O planes, along staggered [110] lines, resulting in alternating planes of tetrahedrally-and octahedrally coordinated ...