LONG-RANGE INTERACTION OF THE K-39(4S)-39(4P) ASYMPTOTE BY PHOTOASSOCIATIVE SPECTROSCOPY .1. THE O-G(-) PURE LONG-RANGE STATE AND THE LONG-RANGE POTENTIAL CONSTANTS(K)
H. Wang et al., LONG-RANGE INTERACTION OF THE K-39(4S)-39(4P) ASYMPTOTE BY PHOTOASSOCIATIVE SPECTROSCOPY .1. THE O-G(-) PURE LONG-RANGE STATE AND THE LONG-RANGE POTENTIAL CONSTANTS(K), The Journal of chemical physics, 106(19), 1997, pp. 7899-7912
This paper reports on a comprehensive study of the long-range interact
ion of the K-39(4s) + K-39(4p) asymptotic system. We present a detaile
d discussion of the R-dependent angular momentum couplings and correla
tion between the Hund's case (a) and case (c) molecular states. Analyt
ical expressions for the 16 adiabatic Hund's case (c) long-range poten
tial curves are derived including the higher order dispersion forces a
nd the effects of retardation. Experimentally, six Hund's case (c) lon
g-range molecular states (0(u)(+), 1(g), and 0(g)(-) dissociating to t
he 4 S-2(1/2) + 4 P-2(3/2) asymptote and 0(u)(+), 1 g and 0(g)(-) to t
he 4 S-2(1/2) + 4 P-2(1/2) limit) are observed with rovibrational reso
lution by photoassociative spectroscopy of ultracold K-39 atoms in a h
igh density magneto-optical trap (MOT). Among the six observed long-ra
nge states, the upper 0(g)(-) ''pure long-range'' state has negligible
short-range chemical exchange contributions and the measured molecula
r binding energies (v = 0-26) are used to precisely determine the long
-range potential constants of the 4s + 4p interaction. We determine: C
-3(Pi) = 8.436(14) a.u., C-3(Sigma) = 16.872(28) a.u., C-6(Pi) = 6272(
94) a.u., and C-6(Sigma) = 9365(141) a.u. Molecular constants for the
three special pure long-range states, the 0(g)(-) and 1(u) (dissociati
ng to the 4 P-2(3/2) limit and with potential minimum) and the 1(u) (d
issociating to the 4 P-2(1/2) and with potential maximum), are reporte
d. The internal consistency of the theoretical model used in this work
is confirmed by the excellent agreement between the long-range potent
ial curve of the 1(g) state obtained in present work (from the 0(g)(-)
srate) and the long-range portion of the RKR potential curve of the 1
(1) Pi(g) state previously determined by conventional molecular spect
roscopy. The radiative lifetime of the K 4p state derived from the n i
s also in excellent agreement with a recent fast-beam dipole-dipole in
teraction constant C-3(Pi) is also in excellent agreement with a recen
t fast-beam measurement. (C) 1997 American Institute of Physics. measu
rement.