We report the X-ray study for the pyrochlore oxide Cd2Re2O7. Two symmetry-lowering structural transitions were observed at Ts1=200 K and Ts2=120 K. The former is of the second order from the ideal cubic pyrochlore structure with space group F d3m to a tetragonally distorted structure with I4m2, while the latter is of the first order likely to another tetragonal space group I4122. We discuss the feature of the lattice deformation.A series of pyrochlore oxides A 2 B 2 O 7 show a variety of interesting conductive and magnetic properties, depending on the substitutions of A and B sites [1]. Geometrical frustration on the pyrochlore lattice leads to an exotic ground state such as spin ice for magnetic insulators [2], while for metallic systems a unique heavy carrier behavior is found in spinel LiV 2 O 4 having a pyrochlore lattice made of V atoms [3]. In the pyrochlore structure, the A site occupied by a rare-earth or a post-transition metal cation forms a distorted (6+2) coordination, while the B site occupied by a transition metal cation forms a distorted octahedron BO 6 with an equal B-O distance. The structure comprises two interpenetrating pyrochlore lattices composed of the A or B sites (see Fig. 1).Recently, Hanawa et al. and the others reported the first superconductor Cd 2 Re 2 O 7 (T c =1 K) in the family of pyrochlore oxides [4,5,6]. The compound exhibits two more phase transitions at T s1 =200 K and T s2 =120 K, where electrical and magnetic properties change dramatically [7,8,9]. The former is of the second order, while the latter is of the first order. These transitions are accompanied by structural transitions. Three phases appearing are named as phase I (T >T s1 ), II (T s1 >T >T s2 ), and III (T