Experimental studies of the NaK 1 3Δ state

被引:23
作者
Huennekens, J
Prodan, I
Marks, A
Sibbach, L
Galle, E
Morgus, T
Li, L
机构
[1] Lehigh Univ, Dept Phys, Bethlehem, PA 18015 USA
[2] Tsinghua Univ, Dept Phys, Beijing 100084, Peoples R China
关键词
D O I
10.1063/1.1310609
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The NaK 1 (3)Delta state has been studied by the perturbation-facilitated optical-optical double resonance technique. Mixed singlet-triplet levels, A(2)(1)Sigma (+)(upsilon (A),J)similar tob(1)(3)Pi>(*) over bar *(upsilon (b),J), were pumped from thermally populated rovibrational levels of the ground state, X(1)(1)Sigma (+)(upsilon (X),J +/-1), using a single-mode cw dye laser. A single-mode cw Ti:Sapphire laser was then used to further excite the NaK molecules to various 1 (3)Delta>(*) over bar *(upsilon (Delta),N-Delta,J(Delta)) rovibrational levels which were detected by observing collision-induced (3)Lambda -->a(1)(3)Sigma (+) fluorescence in the green part of the spectrum. The measured energies of the 1 (3)Delta>(*) over bar *(upsilon (Delta),N-Delta) levels were fit to a Dunham expansion, and the Dunham coefficients were used to construct the RKR potential curve. Absolute numbering of the 1 (3)Delta state vibrational levels was established by a comparison of experimental and calculated 1 (3)Delta>(*) over bar *(upsilon (Delta),N-Delta,J(Delta))<--b(1)(3)Pi>(*) over bar *(upsilon (b),J(b)) absorption line strengths. A deperturbation program was used to determine the vibration-dependent 1 (3)Delta state spin-orbit interaction parameter. Hyperfine structure of the 1 (3)Delta state was studied, and the Fermi-contact interaction term for this state was determined to be similar to0.0111 cm(-1). (C) 2000 American Institute of Physics. [S0021-9606(00)00140-9].
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收藏
页码:7384 / 7397
页数:14
相关论文
共 122 条
[1]   Vibrational wave packet dynamics in NaK:: The A 1Σ+ state [J].
Andersson, LM ;
Karlsson, HO ;
Goscinski, O ;
Berg, LE ;
Beutter, M ;
Hansson, T .
CHEMICAL PHYSICS, 1999, 241 (01) :43-54
[2]  
[Anonymous], 1978, ATLAS SPECTRE ABSORP
[3]  
[Anonymous], 1969, ROTATIONAL STRUCTURE
[4]   HYPERFINE-STRUCTURE OF THE 625 NM BAND IN THE A3PI-U[-X1SIGMA-G TRANSITIONS OF NA-2 [J].
ATKINSON, JB ;
BECKER, J ;
DEMTRODER, W .
CHEMICAL PHYSICS LETTERS, 1982, 87 (02) :128-133
[5]   DOPPLER-FREE SPECTRUM OF THE B1-PI-X1-SIGMA+ TRANSITION OF NAK, AND THE PERTURBATION AND HYPERFINE SPLITTING [J].
BABA, M ;
TANAKA, S ;
KATO, H .
JOURNAL OF CHEMICAL PHYSICS, 1988, 89 (12) :7049-7055
[6]   EFFECTS OF MAGNETIC-FIELD ON THE PERTURBATION BETWEEN THE B 1-PI AND C 3-SIGMA+ STATES OF NAK [J].
BABA, M ;
NISHIZAWA, K ;
YOSHIE, N ;
ISHIKAWA, K ;
KATO, H .
JOURNAL OF CHEMICAL PHYSICS, 1992, 96 (02) :955-960
[7]   LASER-INDUCED FLUORESCENCE AND 2-PHOTON IONIZATION SPECTROSCOPY OF THE C(3)1-SIGMA+ STATE OF THE NAK MOLECULE [J].
BARROW, RF ;
CLEMENTS, RM ;
DELACRETAZ, G ;
EFFANTIN, C ;
DINCAN, J ;
ROSS, AJ ;
VERGES, J ;
WOSTE, L .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 1987, 20 (13) :3047-3055
[8]   Femtosecond laser spectroscopy on the vibrational wave packet dynamics of the A(1)Sigma(+) state of NaK [J].
Berg, LE ;
Beutter, M ;
Hansson, T .
CHEMICAL PHYSICS LETTERS, 1996, 253 (3-4) :327-332
[9]  
Bernath P.F., 2020, Spectra of atoms and molecules
[10]   RYDBERG STATES OF LI-7(2) BY PULSED OPTICAL OPTICAL DOUBLE-RESONANCE SPECTROSCOPY - MOLECULAR-CONSTANTS OF LI-7(2+) [J].
BERNHEIM, RA ;
GOLD, LP ;
TIPTON, T .
JOURNAL OF CHEMICAL PHYSICS, 1983, 78 (06) :3635-3646