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RuoffRodney Scott

Ruoff, Rodney S.
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dc.citation.endPage 1562 -
dc.citation.number 3 -
dc.citation.startPage 1552 -
dc.citation.title JOURNAL OF CHEMICAL PHYSICS -
dc.citation.volume 95 -
dc.contributor.author CHUANG, C -
dc.contributor.author KLOTS, TD -
dc.contributor.author RUOFF, RS -
dc.contributor.author EMILSSON, T -
dc.contributor.author GUTOWSKY, HS -
dc.date.accessioned 2023-12-22T13:08:06Z -
dc.date.available 2023-12-22T13:08:06Z -
dc.date.created 2021-10-20 -
dc.date.issued 1991-08 -
dc.description.abstract Rotational spectra have been observed for eight isotopic species of the diborane-HCl complex with a Balle-Flygare, pulsed nozzle, Fourier transform microwave spectrometer. The dimer has a linear, or at most slightly bent B-B...H/DCl equilibrium structure with the H/D end of the HCl attracted symmetrically to a terminal BH2 group of the diborane. Three B2H6-HCl species homonuclear in the boron were observed to tunnel while those with (BBH6)-B-10-B-11 or DCl did not. The tunneling splits each rotational transition into two components of comparable intensity, separated by several MHz depending on J and K. The a-dipole transitions are characteristic of a prolate, very near symmetric top; only K = 0 and +/- 1 transitions were found. Rotational constants are reported for all species. The BBAR, D(J), H, (B-C), and D(JK) constants determined for (B2H6)-B-11-(HCl)-Cl-35 are for the A1 tunneling state 1273.364(1) MHz, 5.56(5) kHz, 1.0(8) Hz, 5.3(2) MHz, and -2.1(3) MHz; for the A2 tunneling state 1273.856(1) MHz, 11.64(7) kHz, 33.1(9) Hz, 5.70(4) MHz, and -3.21(5) MHz. The chlorine hyperfine structure gives the average torsional displacement of the H/DCl from the a axis to be 26.3-degrees for the HCl complexes and 22.5-degrees for the DCl. The torsional displacement of the B2H6 was found by an inertial analysis of the complexes with HCl. It is very anisotropic, being close to 0-degrees in the ethylene plane and about 9-degrees in the BH2B bridging plane. It is suggested that in the tunneling the B2H6 reorients by 180-degrees in the bridging plane, coupled with a gear-like counter rotation of the HCl by 360-degrees. The B...H distance is 2.693 angstrom in the dimers with HCl and the B...D distance is slightly longer, 2.702 angstrom. -
dc.identifier.bibliographicCitation JOURNAL OF CHEMICAL PHYSICS, v.95, no.3, pp.1552 - 1562 -
dc.identifier.doi 10.1063/1.461070 -
dc.identifier.issn 0021-9606 -
dc.identifier.scopusid 2-s2.0-0005588985 -
dc.identifier.uri https://scholarworks.unist.ac.kr/handle/201301/54576 -
dc.identifier.url https://aip.scitation.org/doi/10.1063/1.461070 -
dc.identifier.wosid A1991GA10600015 -
dc.language 영어 -
dc.publisher AMER INST PHYSICS -
dc.title TUNNELING IN A LINEAR B2H6-HCL DIMER -
dc.type Article -
dc.description.isOpenAccess FALSE -
dc.relation.journalWebOfScienceCategory Chemistry, Physical; Physics, Atomic, Molecular & Chemical -
dc.relation.journalResearchArea Chemistry; Physics -
dc.type.docType Article -
dc.description.journalRegisteredClass scie -
dc.description.journalRegisteredClass scopus -
dc.subject.keywordPlus ROTATIONAL SPECTRUM -
dc.subject.keywordPlus MOLECULAR-STRUCTURE -
dc.subject.keywordPlus MICROWAVE-SPECTRUM -
dc.subject.keywordPlus WATER DIMER -
dc.subject.keywordPlus COMPLEX -

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