2002
DOI: 10.1103/physreva.65.023412
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Magnetic-field imaging of weakly bound levels of the ground-stateNa2dimer

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Cited by 26 publications
(32 citation statements)
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“…(2) with R-dependent interaction potentials and coupling terms. The R-dependent functions are found in a fit to all known Feshbach resonances and existing spectroscopic data of more deeply bound rovibrational levels of the X 1 + g and a 3 + u potentials [8][9][10][11][12]. Data from conventional spectroscopy by Kush and Hessel [39] and by Barrow et al [40] for the ground-state X 1 + g potential and by Li Li et al [41] for the lowest triplet state a 3 + u potential are also included.…”
Section: Coupled-channels Calculationmentioning
confidence: 99%
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“…(2) with R-dependent interaction potentials and coupling terms. The R-dependent functions are found in a fit to all known Feshbach resonances and existing spectroscopic data of more deeply bound rovibrational levels of the X 1 + g and a 3 + u potentials [8][9][10][11][12]. Data from conventional spectroscopy by Kush and Hessel [39] and by Barrow et al [40] for the ground-state X 1 + g potential and by Li Li et al [41] for the lowest triplet state a 3 + u potential are also included.…”
Section: Coupled-channels Calculationmentioning
confidence: 99%
“…We find that all the observed Feshbach resonances can be described by a single vibrational triplet level below the |1,1 + |1,1 dissociation threshold. In fact, it is the v a = 14 level with l = 0, 2, and 4 [10]. From a least-squares fit including all resonances we obtain for the rotational structure of this vibrational level three fitted energies: ε 1,0 14 /h = −4976 MHz, ε 1,2 14 /h = −3679 MHz, and ε 1,4 14 /h = −765 MHz, where the energies are given with respect to the |1,1 + |1,1 dissociation threshold.…”
Section: Moerdijk Modelmentioning
confidence: 99%
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