1997
DOI: 10.1103/physrevlett.79.3142
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Electronic Structure Critical Parameters From Finite-Size Scaling

Abstract: We present finite-size scaling and phenomenological renormalization equations for calculations of the critical points of the electronic structure of atoms and molecules. Results show that the method is efficient and very accurate for estimating the critical screening length for one-electron screened Coulomb potentials and the critical nuclear charge for two-electron atoms. The method has potential applicability for many-body quantum systems. [S0031-9007 (97)04408-6] PACS numbers: 31.15. -p, 05.70.Jk

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Cited by 51 publications
(52 citation statements)
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“…2. This behavior is different from that of our previous results [7,8] for the heliumlike atoms where the ionization energy bends sharply to zero at the helium critical l ͑He͒ c Ӎ 1.0976. The different behavior of the energy as a function of the Hamiltonian parameter, l, suggests, an analogy with standard phase transitions in statistical mechanics, that the transition from a ground bound state to a continuum in the heliumlike atoms resemble first order phase transitions, while for lithiumlike atoms, the transition is continuous.…”
Section: (Received 4 March 1998)contrasting
confidence: 79%
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“…2. This behavior is different from that of our previous results [7,8] for the heliumlike atoms where the ionization energy bends sharply to zero at the helium critical l ͑He͒ c Ӎ 1.0976. The different behavior of the energy as a function of the Hamiltonian parameter, l, suggests, an analogy with standard phase transitions in statistical mechanics, that the transition from a ground bound state to a continuum in the heliumlike atoms resemble first order phase transitions, while for lithiumlike atoms, the transition is continuous.…”
Section: (Received 4 March 1998)contrasting
confidence: 79%
“…Although there is no unique recipe to define such a sequence, in this Letter we used two methods: (i) the first order method (FOM), which can be applied if the threshold energy is known [7,17]. In this method one defines l ͑N͒ as the value in which the ground state energy in the Nth-order approximation, E ͑N͒ 0 ͑l͒, is equal to the threshold energy E T ,…”
Section: (Received 4 March 1998)mentioning
confidence: 99%
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“…Three-body problems have been studied in a variety of context, such as three-body Coulomb systems [1][2][3], and nuclear three-body systems [4][5][6]. Efimov predicted that a system with three particles may have a large number of trimer states even when the dimer potential does not posses any bound states [7][8][9].…”
Section: Introductionmentioning
confidence: 99%