Reproducing kernel technique for extracting accurate potentials from spectral data: Potential curves of the two lowest states X (1)Sigma(+)(g) and a (3)Sigma(+)(u) of the sodium dimer
Ts. Ho et al., Reproducing kernel technique for extracting accurate potentials from spectral data: Potential curves of the two lowest states X (1)Sigma(+)(g) and a (3)Sigma(+)(u) of the sodium dimer, J CHEM PHYS, 112(14), 2000, pp. 6218-6227
This work describes an extension of the Reproducing Kernel Hilbert Space (R
KHS) method, in conjunction with the Tikhonov regularization, for construct
ing potential energy surfaces, with correct asymptotic forms, from high qua
lity experimental measurements. The method is applied to the construction o
f new, global potential energy curves of the two lowest states X (1)Sigma(g
)(+) and a (3)Sigma(u)(+) of the sodium dimer using rovibrational spectral
measurements. The exchange interaction of Na-2 at intermediate and long ran
ges is accordingly derived and adopted for determining the ionization energ
y of the corresponding valence electron. It is found that the resulting gro
und-state X (1)Sigma(g)(+) dissociation energy 6022.025 (+/- 0.049) cm(-1)
of Na-2 agrees within the experimental errors with the most recent experime
ntal value [6022.0286 (+/- 0.0053) cm(-1), Jones , Phys. Rev. A 54, R1006 (
1996)]. The well depth of the a (3)Sigma(u)(+) state is determined to be 17
4.96 (+/- 1.18) cm(-1), compared to the Rydberg-Klein-Rees (RKR) value of 1
74.45 (+/- 0.36) cm(-1) [Li , J. Chem. Phys. 82, 1178 (1985)]. Moreover, th
e equilibrium positions of both RKHS potential curves, 3.0796 (+/- 0.0010)
Angstrom for the X (1)Sigma(g)(+) state and 5.089 (+/- 0.062) Angstrom for
the a (3)Sigma(u)(+) state, are in excellent agreement with previously dete
rmined RKR results of 3.079 53 Angstrom [Babaky and Hussein, Can. J. Phys.
67, 912 (1989)] and 5.0911 Angstrom (Li ), respectively. The experimentally
determined values of the equilibrium position and well depth for the a (3)
Sigma(u)(+) state differ from recent theoretical values of 5.192 Angstrom a
nd 177.7 cm(-1) obtained by highly accurate ab initio calculations [Gutowsk
i, J. Chem. Phys. 110, 4695 (1999)]. Finally, both RKHS potential curves at
large distances reproduce very recent theoretical dispersion coefficients
within 1.0x10(-5) percentage errors. (C) 2000 American Institute of Physics
. [S0021-9606(00)00114-8].