The Q branches of the Raman bands associated to the 2 1 :4 2 0 : 1 ϩ2 2 0 Fermi resonance of 12 C 16 O 2 have been observed in the gas phase at 2543, 2671, and 2797 cm Ϫ1 and, in addition, at 2514 cm Ϫ1 , one hot band from their first excited vibrational state is seen. From the analysis of their cross sections, jointly with those of the main Fermi diad, 1 :2 2 0 and its hot bands, an improved description of the molecular polarizability surface has been achieved. The following derivatives of the mean polarizability have been obtained:␣ץ ¯/ץq 1 ϭ12.43ϫ10 Ϫ42 CV Ϫ1 m 2 ; ץ 2 ␣ ¯/ץq 2 2 ϭ2.81ϫ10 Ϫ42 CV Ϫ1 m 2 ͑ϭa,b͒; ץ 2 ␣ ¯/ץq 1 2 ϭ0.45ϫ10 Ϫ42 CV Ϫ1 m 2 ; ץ 2 ␣ ¯/ץq 3 2 ϭ0.67 or 0.15ϫ10 Ϫ42 CV Ϫ1 m 2 ; ץ 3 ␣ ¯/ץq 1 ץq 2 2 ϭϪ0.06ϫ10 Ϫ42 CV Ϫ1 m 2 , in terms of the dimensionless normal coordinates, and, in terms of the symmetry coordinates. The thermal dependence of the mean polarizability is discussed in terms of these quantities.