1995
DOI: 10.1088/0954-3899/21/10/007
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The hole spectral function and the relationship between overlap functions, natural orbitals and the one-body density matrix in nuclei

Abstract: A method to calculate the hole spectral function in the discrete part of the spectrum is suggested within the natural orbital representation of the one-body density matrix of the A-nucleon system using its relationship with the overlap functions of the eigenstates in the (A-1)-nucleon system.

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Cited by 4 publications
(7 citation statements)
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“…2m (6) and the spectroscopic factor S n0lj = φ n0lj | φ n0lj . The procedure also yields the next bound state overlap functions with the same multipolarity if they exist.…”
Section: Correlated Nuclear Wave Functionsmentioning
confidence: 99%
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“…2m (6) and the spectroscopic factor S n0lj = φ n0lj | φ n0lj . The procedure also yields the next bound state overlap functions with the same multipolarity if they exist.…”
Section: Correlated Nuclear Wave Functionsmentioning
confidence: 99%
“…[1][2][3][4] and also in other domains of many-body physics, as e.g. atomic and molecular physics [5][6][7][8][9][10][11][12].…”
Section: Introductionmentioning
confidence: 99%
“…The same one-body operator has been used also in [28] [Eq. ( 14) of this reference] for realistic study of the nuclear transparency and the distorted momentum distributions in the semi-inclusive process 4 He(e, e ′ p)X.…”
Section: A Correlated One-body Density Matrixmentioning
confidence: 99%
“…For instance, NN correlations are responsible for the reduction of the spectroscopic strengths of the nuclear hole states [1,2,3]. The theoretical understanding of this fact requires the knowledge of the removal spectral function which can be represented in a natural way by both overlap functions and single-nucleon spectroscopic factors [4]. They are directly related to observable quantities such as (p, d), (e, e ′ p) and (γ, p) reaction cross sections.…”
Section: Introductionmentioning
confidence: 99%
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