Lower Rydberg {sup 2}D states of the lithium atom: Finite-nuclear-mass calculations with explicitly correlated Gaussian functions
- Department of Chemistry and Biochemistry, University of Arizona, Tucson, Arizona 85721 (United States)
- Department of Physics and Astronomy, Vanderbilt University, Nashville, Tennessee 37235 (United States)
Very accurate variational nonrelativistic calculations are performed for the five lowest Rydberg {sup 2}D states (1s{sup 2}nd{sup 1}, n=3,...,7) of the lithium atom ({sup 7}Li). The finite-nuclear-mass approach is employed and the wave functions of the states are expanded in terms of all-electron explicitly correlated Gaussian function. Four thousand Gaussians are used for each state. The calculated relative energies of the states determined with respect to the {sup 2}S 1s{sup 2}2s{sup 1} ground state are systematically lower than the experimental values by about 2.5 cm{sup -1}. As this value is about the same as the difference between the experimental relative energy between {sup 7}Li{sup +} and {sup 7}Li in their ground-state energy and the corresponding calculated nonrelativistic relative energy, we attribute it to the relativistic effects not included in the present calculations.
- OSTI ID:
- 21529066
- Journal Information:
- Physical Review. A, Vol. 83, Issue 1; Other Information: DOI: 10.1103/PhysRevA.83.012506; (c) 2011 American Institute of Physics; ISSN 1050-2947
- Country of Publication:
- United States
- Language:
- English
Similar Records
Explicitly correlated Gaussian calculations of the {sup 2}D Rydberg states of the boron atom
Prediction of {sup 1}P Rydberg energy levels of beryllium based on calculations with explicitly correlated Gaussians
Related Subjects
ELECTRONS
GAUSS FUNCTION
GROUND STATES
LITHIUM 7
LITHIUM IONS
RELATIVISTIC RANGE
RYDBERG STATES
VARIATIONAL METHODS
WAVE FUNCTIONS
CALCULATION METHODS
CHARGED PARTICLES
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY RANGE
EXCITED STATES
FERMIONS
FUNCTIONS
IONS
ISOTOPES
LEPTONS
LIGHT NUCLEI
LITHIUM ISOTOPES
NUCLEI
ODD-EVEN NUCLEI
STABLE ISOTOPES