To examine the correlation between the atomic displacement parameters of oxygen atom and oxide-ion conductivity of rare-earth-oxide-doped ceria materials, Ce 0.8 R 0.2 O 1.9 (R ) La, Nd, Sm, Gd, Y, and Yb), their crystal structures have been refined by the Rietveld analyses of high-resolution (d > 0.38 Å) synchrotron powder diffraction data measured in air in situ at 29.5, 408.0, and 675.0 °C. As a reference material, pure nondoped ceria CeO 2 was also investigated by the same method. Both atomic displacement parameters of cations and anions increase with temperature, which indicates the thermal vibrations and dynamic positional disorders. At a given temperature, the thermal parameters of cation in Ce 0.8 R 0.2 O 1.9 , U C (R), are larger than those in CeO 2 , U C (CeO 2 ), which indicates that the positional disorder of cations in Ce 0.8 R 0.2 O 1.9 is also larger compared with that in CeO 2 . Similarly, at a given temperature, the atomic displacement parameters of anions in Ce 0.8 R 0.2 O 1.9 , U O (R), are larger than those in CeO 2 , U O (CeO 2 ), which indicates that the positional disorder of oxide ions in Ce 0.8 R 0.2 O 1.9 is larger than that in CeO 2 . The larger positional disorders of oxide ions in Ce 0.8 R 0.2 O 1.9 would be the structural origin of higher ionic conductivities of Ce 0.8 R 0.2 O 1.9 , compared with those of undoped CeO 2 . In Ce 0.8 R 0.2 O 1.9 , both atomic displacement parameters of cations U C (R) and of anions U O (R) decrease with increasing ionic radius of R 3+ ions for the coordination number of eight r(R) from R ) Yb to R ) Gd, while they increase with r(R) from R ) Gd to R ) La. Thus, both U C (R) and U O (R) exhibit minima at R ) Gd in the range from R ) Yb to R ) La. The mismatch between dopant rare-earth oxide and host ceria would yield the positional disorder, local distortion, and lattice strain, which leads to the larger atomic displacement parameters. The present paper discusses the correlation between the oxygen thermal parameter U O (R) and oxide-ion conductivity of Ce 0.8 R 0.2 O 1.9 .