Hyperfine coupling constants, electron-spin g-factors and vertical spectra of the X2Σ+ radicals BeH, MgH, CaH and BZ+, AlZ+, GaZ+ (Z = H, Li, Na, K).: A theoretical study

被引:32
作者
Bruna, PJ [1 ]
Grein, F [1 ]
机构
[1] Univ New Brunswick, Dept Chem, Fredericton, NB E3B 6E2, Canada
关键词
D O I
10.1039/b303698g
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
Hyper. ne coupling constants (hfcc), electron-spin g-factors, excitation energies ( DE) and oscillator strengths (f-values) are calculated for the X(2)Sigma(+) (1sigma(2)2sigma) radicals YH (Y = Be, Mg, Ca) and BZ(+), AlZ(+), GaZ(+) (Z = H, Li, Na, K). Single reference ab initio and density functional theory methods are used for the hfcc's, and multireference configuration interaction wavefunctions for DeltaE's, f-values and g-shifts. In XZ(+) (X = B to Ga; Z = Li to K), the 2sigma unpaired electron is 60-90% p(sigma)(X), resulting in \A(perpendicular to)\ being one order of magnitude larger than \Ak(parallel to)\. The Deltag(perpendicular to)'s are relatively large for just 3 valence electrons, from -3300 to -6100 ppm for BZ(+), -14 100 to -29 600 ppm for AlZ(+), and -93 700 to -198 300 ppm for GaZ(+). Such large Deltag(perpendicular to)(XZ(+))'s relate to the strong coupling between the close-lying X(2)Sigma(+) and I(2)Pi(2sigma --> 1pi) states, which results from the splitting of the P-2(s(2)p) state of X due to its interaction with Z(+). ESR spectra are not available for any of the XZ(+)'s. Calculation on the hydrides YH/XH+ reproduce well the experimental hfcc's and g factors, except for AlH+, which appears to be strongly perturbed in Ar matrices. Several transitions X(2)Sigma(+) --> n(2)Sigma(+) and X(2)Sigma(+) --> n(2)Pi in XZ(+) have large oscillator strengths, mainly caused by intramolecular charge-transfer processes X <----> Z and atomic-like s(g) <----> p(u) excitations.
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页码:3140 / 3153
页数:14
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共 97 条
[1]   EXPERIMENTAL DETERMINATIONS OF HYPERFINE-STRUCTURE IN ALKALI ATOMS [J].
ARIMONDO, E ;
INGUSCIO, M ;
VIOLINO, P .
REVIEWS OF MODERN PHYSICS, 1977, 49 (01) :31-75
[2]   LOW-LYING ELECTRONIC STATES OF MAGNESIUM HYDRIDE [J].
BALFOUR, WJ ;
CARTWRIGHT, HM .
CHEMICAL PHYSICS LETTERS, 1975, 32 (01) :82-85
[3]   THE A 2-PI-X-2-SIGMA SYSTEM OF ALD+ AND THE C 1-SIGMA-A-1-PI SYSTEM OF ALD [J].
BALFOUR, WJ ;
LINDGREN, B .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 1984, 17 (24) :L861-L866
[4]   THE MILLIMETER-WAVE SPECTRUM OF CAH (X2-SIGMA+) [J].
BARCLAY, WL ;
ANDERSON, MA ;
ZIURYS, LM .
ASTROPHYSICAL JOURNAL, 1993, 408 (01) :L65-L67
[5]  
Barone V., 1996, RECENT ADV DENSITY 1
[6]   STUDIES IN CONFIGURATION INTERACTION - FIRST-ROW DIATOMIC HYDRIDES [J].
BENDER, CF ;
DAVIDSON, ER .
PHYSICAL REVIEW, 1969, 183 (01) :23-&
[7]   AB-INITIO STUDY OF THE ELECTRONIC-STRUCTURES OF LITHIUM-CONTAINING DIATOMIC-MOLECULES AND IONS [J].
BOLDYREV, AI ;
SIMONS, J ;
SCHLEYER, PV .
JOURNAL OF CHEMICAL PHYSICS, 1993, 99 (11) :8793-8804
[8]   Predictions of ground states of LiGa and NaGa [J].
Boldyrev, AI ;
Simons, J .
CHEMICAL PHYSICS LETTERS, 1996, 262 (06) :807-812
[9]  
BOLDYREV AI, 1997, DIATOMIC PERIODIC TA
[10]   THEORETICAL-STUDY OF THE LOWEST ELECTRONIC STATES OF CAH AND CAH+ MOLECULES [J].
BOUTALIB, A ;
DAUDEY, JP ;
ELMOUHTADI, M .
CHEMICAL PHYSICS, 1992, 167 (1-2) :111-120