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A generalized Bethe-Weizsaecker mass formula for strange hadronic matter

Technical Report ·
OSTI ID:10142547
 [1];  [2]
  1. Brookhaven National Lab., Upton, NY (United States)
  2. Hebrew Univ., Jerusalem (Israel)
The Bethe-Weizsaecker nuclear mass formula is extended to strange hadronic matter composed of nucleons, lambdas and cascade hyperons. The generalized formula contains several volume and symmetry terms constrained by phenomenologically determined {lambda}-nuclear, {xi}-nuclear and {lambda}{lambda} interaction parameters and by hyperon-hyperon ({lambda}{lambda}, {lambda}{xi}, {xi}{xi}) interaction parameters suggested by One-Boson-Exchange models. We find that hypernuclei are generally unstable to {lambda}{lambda} {yields} {xi}N conversion. For strange hadronic matter, as function of the baryon number A, the line of strong-interaction stability, along which a large strangeness fraction {vert_bar}S{vert_bar}/A {approx} 0.5 - 1.1 and a low charge fraction q/A {approx_lt} 0.2 hold, and no fission occurs, is determined. The binding energy per baryon increases monotonically to its bulk limit, B/A {yields} 38 MeV, {vert_bar}S{vert_bar}/A {yields} 1.1 and q/A {yields} 0 for the parameters adopted here assuming that the hyperon species saturate at densities similar to those of protons and neutrons in nuclei. Even in the extreme limit of vanishingly small hyperon-hyperon interaction strengths, strange hadronic matter with B/A {yields} 15 MeV, {vert_bar}S{vert_bar}/A {yields} 0.7 and q/A {yields} 0 in the bulk limit should exist; the mass formula reproduces semi-quantitatively recent mean-field calculations which implicitly assumed weak hyperon-hyperon interactions.
Research Organization:
Washington Univ., Seattle, WA (United States). Inst. for Nuclear Theory
Sponsoring Organization:
USDOE, Washington, DC (United States)
DOE Contract Number:
FG06-90ER40561; AC02-76CH00016
OSTI ID:
10142547
Report Number(s):
DOE/ER/40561--096; ON: DE93011010; IN: INT-92-08-02
Country of Publication:
United States
Language:
English

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