Abstract

The pure rotational spectrum of AsD2in the2B1ground electronic state was measured in the frequency region of 268–398 GHz by microwave spectroscopy. The AsD2radical was generated in a free-space cell by dc-glow discharge of a gaseous mixture of D2and He over arsenic powder. Fifty fine and hyperfine components of nine rotational transitions were measured and analyzed by least-squares methods determining the detailed molecular constants of AsD2: the rotational constants, the centrifugal distortion constants, the spin–rotation coupling constant with the centrifugal distortion terms, and the hyperfine coupling constants associated with the arsenic and deuterium nuclei. The harmonic force field of AsH2was determined from the centrifugal distortion constants, the equilibrium vibrational frequency of ν2mode of AsH2, and the inertial defects of AsH2and AsD2. The harmonic force field was used to calculate vibrational corrections to the rotational constants of both species and thus the zero-point average structures for both species were derived; AsH2: rz(AsH) = 1.53436(15) Å, θz(HAsH) = 90.695(20)°, and AsD2: rz(AsD) = 1.52902(13) Å, θz(DAsD) = 90.722(17)°, where the errors in parentheses are due to residual inertial defects of the corrected moments of inertia. From the difference between the rzstructures for AsH2and AsD2the restructure of AsH2is estimated to be re(AsH) = 1.5158(6) Å, θe(HAsH) = 90.79(8)°.

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