1994
DOI: 10.1002/qua.560510405
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Accurate upper and lower bounds to the 2S states of the lithium atom

Abstract: The first nonrelativistic lower bound to the ground state of the lithium atom is given with EO > -7.47816 au using the method of variance minimization and an extension of Temple's formula. With large Hylleraas-CI basis sets, high-precision upper bounds and isotope shifts are calculated for the three lowest 2S states of the lithium atom, which are the best to date.

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Cited by 64 publications
(35 citation statements)
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“…Usually just the former is used in calculations. The impact of not including the latter triplet has been studied by many authors [13][14][15][16][17]. Their common conclusion is that including the triplet spin coupling explicitly will not enhance the convergence of the energy significantly, but it will strongly affect the expectation values of other operators which are spin dependent, such as the Fermi contact term.…”
Section: Introductionmentioning
confidence: 99%
“…Usually just the former is used in calculations. The impact of not including the latter triplet has been studied by many authors [13][14][15][16][17]. Their common conclusion is that including the triplet spin coupling explicitly will not enhance the convergence of the energy significantly, but it will strongly affect the expectation values of other operators which are spin dependent, such as the Fermi contact term.…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately, the explicitly correlated bases mentioned above are specific for two-electron atoms and two-electron diatomics and have not been successfully generalized to larger systems, except for recent Hylleraas-CI calculations on Li and Be. [12][13][14] At present, the only explicitly correlated basis that can be practically and without approximations applied to manyelectron polyatomic systems is the set of correlated Gaussian functions, introduced to quantum chemistry by Boys and Singer. 15 In the two-electron case such functions are usually referred to as Gaussian-type geminals ͑GTG͒ and have a general form g͑r 1 ,r 2 ͒ϭx 1A l 1 y 1A m 1 z 1A n 1 x 2B l 2 y 2B m 2 z 2B n 2 ϫexp͓Ϫ␣͑r 1 ϪA͒ 2 Ϫ␤͑r 2 ϪB͒ 2 Ϫ␥r 12 2 ͔, ͑1͒…”
Section: Introductionmentioning
confidence: 99%
“…case s 0, and ensuring that Eqs. 48 and 49 12 are satisfied, gives an immediate indication of the expected optimal values of the parameters for this particular wave function. The fact that the parameter g does not contribute to C should be noted.…”
Section: R Correlated Wave Functions 12mentioning
confidence: 97%
“…The definition is motivated by the standard form w x of the electron᎐electron cusp condition 30 12 To obtain a finite E , C must satisfy the condi- pendent terms do not offset the detrimental contribution yg 2 . Examination of the limit of the right Ž .…”
Section: R Correlated Wave Functions 12mentioning
confidence: 99%