1996
DOI: 10.1006/jmsp.1996.0168
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High-Resolution Study of theX21 →X10+Fine-Structure Transition of BiF

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Cited by 19 publications
(16 citation statements)
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“…The HF splitting, is described by anãI Á J a term, whereã is a coupling constant describing the interaction (it simplifies toãI z J az , where I z and J az are the I and J a components along the internuclear axis). In some couplings (mostly Hund's cases (a) and (c)), the HF splitting of the rotational energy levels decreases as J increases, as was observed for the a1 state in 207 Pb 16 O ( 3 R + 1 R + transition) [28] or the X 2 1-X 1 0 + (X 3 R À ) system in 209 Bi 19 F [29]. For the former, the first-order HF splitting due to the magnetic dipole-dipole interaction changes as 2J þ1…”
Section: Resultsmentioning
confidence: 61%
“…The HF splitting, is described by anãI Á J a term, whereã is a coupling constant describing the interaction (it simplifies toãI z J az , where I z and J az are the I and J a components along the internuclear axis). In some couplings (mostly Hund's cases (a) and (c)), the HF splitting of the rotational energy levels decreases as J increases, as was observed for the a1 state in 207 Pb 16 O ( 3 R + 1 R + transition) [28] or the X 2 1-X 1 0 + (X 3 R À ) system in 209 Bi 19 F [29]. For the former, the first-order HF splitting due to the magnetic dipole-dipole interaction changes as 2J þ1…”
Section: Resultsmentioning
confidence: 61%
“…They pointed out that the measured values of both nuclear quadrupole coupling constants and nuclear spin-rotation constants are really effective values including contributions from electronnuclear hyperfine constants. This difference was also noted by Fink et al in their definitive high resolution near-infrared study of the X 2 1 À X 1 0 + fine structure transition of BiF [23].…”
Section: Introductionmentioning
confidence: 58%
“…High-resolution spectra (0.02 cm Ϫ1 ) show that the bands of the 9350 cm Ϫ1 system consist of P and R branches only, whereas the 7600 cm Ϫ1 system contains P, Q, and R branches (Figs Seven bands of the A 2 3 X 1 (0 -0, 0 -1, 1-0, 1-1, 1-2, 2-1, 2-3) and five bands of the A 2 3 X 2 (0 -0, 0 -1, 1-1, 1-2, 2-3) systems were measured at high resolution (0.02 cm Ϫ1 ) and rotationally analyzed. In the spectra of BiH and BiF, magnetic hyperfine splitting in the X 2 1 state leads to strong hfs splitting of the low J lines of all transitions ending in this state (2,4). Except for a weak broadening of the low J lines in the Q and R branches, no such hfs splitting is observed in the A 2 3 X 2 bands of BiNa (Fig.…”
Section: Experimental Results and Analysesmentioning
confidence: 84%
“…3 Numbers in parentheses are the standard deviations of the parameters in units of the last digit. 4 Data marked with a star were fixed in the fit.…”
Section: Theoretical Calculationsmentioning
confidence: 99%
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