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dc.creatorAdam, A. G.en_US
dc.creatorAllen, T. F.en_US
dc.creatorDownie, L. E.en_US
dc.creatorGranger, A. D.en_US
dc.creatorLinton, C.en_US
dc.creatorTokaryk, D. W.en_US
dc.date.accessioned2011-07-12T17:37:03Z
dc.date.available2011-07-12T17:37:03Z
dc.date.issued2011en_US
dc.identifier2011-WG-11en_US
dc.identifier.urihttp://hdl.handle.net/1811/49583
dc.descriptionAuthor Institution: Chemistry Department, and Centre for Lasers, and Atomic, and Molecular Sciences, University of New Brunswick, Fredericton, NB, E3B 5A3; Physics Department, and Centre for Lasers, and Atomic, and Molecular Sciences, University of New Brunswick, Fredericton, NB, E3B 5A3en_US
dc.description.abstractThe rhodium monobromide molecule, RhBr, has been created in our laser ablation pulsed jet apparatus by ablating a rhodium target rod in the presence of 1\% CH$_3$Br seeded in He. A low-resolution survey spectrum from 415 to 850 nm indicated the presence of a number of bands belonging to RhBr. Thirteen of these band systems, mainly in the blue spectral region, have been recorded at high resolution with our cw dye laser. In addition, dispersed fluorescence spectra have been obtained for these bands. Not all of the bands have been fully analyzed to date, however, from those analyzed, the RhBr ground state has been determined to have $\Omega$=2 consistent with the isovalent RhCl molecule which has a $^3$$\Pi$$_2$ ground state nderline{234}, 99-105 (2005)}. Vibrational and rotational analysis yields the following ground state parameters for the two isotopologues, Rh$^{79}$Br and Rh$^{81}$Br: $\omega^{\prime\prime}$=260 cm$^{-1}$, B$^{\prime\prime}(Rh$^{79}$Br)=0.0655 cm$^{-1}$, and B$^{\prime\prime}(Rh$^{81}$Br)=0.0646 cm$^{-1}$. Further ground and excited state parameters will be presented at the conference.en_US
dc.language.isoenen_US
dc.publisherOhio State Universityen_US
dc.titleHIGH RESOLUTION LASER SPECTROSCOPY OF RHODIUM MONOBROMIDEen_US
dc.typeArticleen_US
dc.typeImageen_US
dc.typePresentationen_US


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