THE GEOMETRY AND MOLECULAR PROPERTIES OF THE ETHYLENE-HCN AND ACETYLENE-HCN DIMERS
dc.creator | Aldrich, P. D. | en_US |
dc.creator | Read, W. G. | en_US |
dc.creator | Kukolich, Stephen G. | en_US |
dc.creator | Campbell, E. J. | en_US |
dc.date.accessioned | 2007-08-31T14:12:49Z | |
dc.date.available | 2007-08-31T14:12:49Z | |
dc.date.issued | 1982 | en_US |
dc.identifier | 1982-RB-12 | en_US |
dc.identifier.uri | http://hdl.handle.net/1811/29208 | |
dc.description.abstract | The microwave spectra of the acetylene-HCN and ethylene-HCN dimers has been observed in the 4-18 GHz region using the pulsed Fourier transform method where the gas mixture is pulsed into a Fahry-Perot cavity. The spectra reveal both dimers to be near prolate asymmetric tops (K = -.99) in their ground vibrational states. Both dimers have a `T' shape for an equilibrium structure with the proton of HCN nearest to acetylene or ethylene. The ethylene-HCN dimer is nonplanar. Hyperfine structure originating from interaction of the nuclear electric quadrupole moment of $^{14}N$ with the surrounding electric field gradient is evident in all transitions. The nucleum quadrupole coupling analysis shows $X_{bb}$ and $X_{cc}$ to be equal within experimental uncertainty in both cases indicating that the proton of HCN experiences a nearly isotropic potential due to ethylene or acetylene. The structure of both dimers is consistent with other acetylene (ethylene)-HX dimers studied in this laboratory in structure and approximate well depth. | en_US |
dc.format.extent | 83403 bytes | |
dc.format.mimetype | image/jpeg | |
dc.language.iso | English | en_US |
dc.publisher | Ohio State University | en_US |
dc.title | THE GEOMETRY AND MOLECULAR PROPERTIES OF THE ETHYLENE-HCN AND ACETYLENE-HCN DIMERS | en_US |
dc.type | article | en_US |
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