1988
DOI: 10.1016/0092-640x(88)90024-1
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Mass predictions by modified ensemble averaging

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Cited by 42 publications
(8 citation statements)
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“…Otherwise, we try the mass estimations [12] one after the other, and then we compare the results. The following mass codes are conventionally adopted: C = 3 for the estimations of Jänecke and Masson [13], C = 2 for Masson and Jänecke [14], C = 4 for Spanier and Johansson [15], C = 5 for Tachibana et al [16], C = 6 for Satpathy and Nayak [17], C = 7 for Comay, Kelson, and Zidon [18], and C = 8 for Möller et al [19].…”
Section: Resultsmentioning
confidence: 99%
“…Otherwise, we try the mass estimations [12] one after the other, and then we compare the results. The following mass codes are conventionally adopted: C = 3 for the estimations of Jänecke and Masson [13], C = 2 for Masson and Jänecke [14], C = 4 for Spanier and Johansson [15], C = 5 for Tachibana et al [16], C = 6 for Satpathy and Nayak [17], C = 7 for Comay, Kelson, and Zidon [18], and C = 8 for Möller et al [19].…”
Section: Resultsmentioning
confidence: 99%
“…Authors [2][3][4] use the results of the phenomenological shell model description for AEc reported in I- 6,7]. In the case of diagonal nuclei, protons and neutrons of which are disposed in the same shell, the shell model expression for AEc takes the form…”
Section: M(z N) = M(n Z) + ~ [M(n + In + I --mentioning
confidence: 99%
“…However, if one considers nuclei far from stability it turns out that the predictions of M(Z, N) values differ greatly even in works which allow for properties of mirror nuclei. As an example, root-mean-square value (6) which characterizes the differences of mass predictions given in [2] and [5] calculated on 313 nuclei amounts to 0.78 MeV. Considerable discrepancies between mass values of nuclei with Z >N predicted in various works limit their use and raise the question of reasons which account for such discrepancies.…”
Section: Introductionmentioning
confidence: 98%
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