Abstract
The infrared spectra of solid Hg(CN)2 and the mono‐ and di‐substituted C13 and N15 species have been observed. The polarized spectrum of a single crystal of the normal species was also observed. The seven fundamental vibrations of the linear, symmetric Hg(CN)2 molecule have been assigned at 2192, 415, 2193.5, 442, 276, 341, and ca 100 cm—1. From the observed frequencies of the normal and isotopic species, force constants were calculated for two possible structures: N–C–Hg–C–N and C–N–Hg–N–C. It is shown that the latter structure gives unreasonably large values for the CN stretching force constant (> 20 md/A) and the CN, HgN interaction constant (∼2.4 md/A), while the former structure yields quite reasonable force constants, namely: Fcn=17.6, Fhgc=2.61, Fcn, c′n′=—0.1, Fhgc, hgc′=0.1, and Fhgc, cn=0.1 md/A. These results are presented as strong evidence that the cyanides are bound to the mercury through carbon atoms.