The crystal structure of the title compound, (2,2 H -bipyridyl-2 N,N H )(tetraallyl 3,3,3 H ,3 H -tetramethyl-1,1 H -bicyclopropane-1,1 H ,-2,2 H -tetracarboxylato-2 C 2 ,C 2 H )palladium(II),[Pd(C 26 H 32 -O 8 )(C 10 H 8 N 2 )], is disordered above 194 K. A doubling of the unit cell is observed on cooling. The structure at 143 K contains two ordered molecules related by a pseudo-translation vector of approximately (0.44,0.00,0.50) or a pseudoinversion center at approximately (0.22,0.00,0.25). Weak intermolecular CÐHÁ Á ÁO interactions are enhanced in the low-temperature structure.
CommentIn an effort to synthesize the ®rst palladepane derivatives and in the course of an investigation covering polymer-bound organometallic catalysts, we reacted diallyl 3,3-dimethylcyclopropene-1,2-dicarboxylate with a Pd 0 compound. One of the two products was the desired palladepane derivative, the other turned out to be the title compound, (I) (Hashmi et al., 1999). Compound (I) is also a promising substrate for the formation of polymer-bound organometallic catalysts by cometathesis with other 1,n-dienes. During X-ray diffraction experiments on (I), a reversible phase transition was observed at 194 K. The crystal structure of the high-temperature phase has been determined at room temperature (292 K) and at 205 K. The high-temperature phase has one molecule in the asymmetric unit ( Fig. 1). Two propene side chains are disor-dered. The structures at 292 and 205 K are similar. Thus, the room-temperature results are not reported here.The crystal structure of the low-temperature phase has been determined at 143 K. At this temperature, the crystal structure contains two independent ordered molecules (Fig. 2). The cell axes transform according to: a low = a high , b low = Àc high and c low = 2b high À a high . The fractional coordinates between the lowand the high-temperature phases are related by: x low = x high + 1 2 y high , y low = Àz high and z low = 1 2 y high . Thus, the low-temperature structure should be approximately B-centered. Surprisingly, the re¯ection intensities do not show approximate Bcentering. The two independent molecules are related by a pseudo-translation of about (0.44,0.00,0.50).A combination of this pseudo-translation vector with the crystallographic inversion center at (0,0,0) results in a noncrystallographic pseudo-inversion center at (0.22,0.00,0.25) (Desiraju et al., 1991). The presence of this pseudo-center is con®rmed by the program BUNYIP (Hester & Hall, 1996). The conformations of both independent molecules are very similar. The molecules differ mainly in the orientations of the propene groups attached to O2, O10, O8 and O16. Those are the propene groups which are disordered above the phasetransition temperature. Below the phase-transition temperature, both molecules are fully ordered. The conformations of the molecules in the high-temperature and low-temperature phases are compared in Fig. 3. This ®gure shows the relative positions of the molecules of the low-temperature structure as they would appear...