AbstractThe crystal structures of [C(NH2)3]CdI3(1) and [4-ClC6H5NH3]3CdBr5(2) have been determined at 100 K: monoclinic,Cc,a= 828.75(3) pm,b= 1615.31(5) pm,c= 810.64(3) pm, andβ= 106.5820(10)° for1; monoclinic,P21/c,a= 1486.93(5) pm,b= 794.31(3) pm,c= 2290.59(7) pm, andβ= 99.6830(10)° for2. The structure of1has an infinite chain of anions consisting of [CdI4] tetrahedra sharing two corners. The structure of2has an infinite chain of anions consisting of [CdBr6] octahedra sharing two corners in cispositions. In both structures, isolated cations are connected to the anion chains through weak hydrogen bonds Cd–X···H to result in three-dimensional network structures. In accordance with the crystal structures, three127I (m= ±1/2 ↔m= ±3/2), five81Br, and three35Cl nuclear quadrupole resonance (NQR) lines were observed for1and2. The NQR spectra reflect the anion chain structures and their weak hydrogen bonds. The MO calculations of the models [Cd5I16]6–for1and [Cd3Br16]10–for2estimate only about half the values for the NQR frequencies but give accurate electric field gradient directions.