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Volumn 56, Issue 5, 1997, Pages 2858-2864

Finite size effects and the mixed quark-hadron phase in neutron stars

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EID: 0031502581     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.56.2858     Document Type: Article
Times cited : (36)

References (45)
  • 25
    • 85035258821 scopus 로고
    • 64, 271 (1970)
    • (1970) , vol.64 , pp. 271
  • 26
    • 85035277743 scopus 로고    scopus 로고
    • 84, 559(E) (1970)
    • , vol.84 , pp. 559
  • 28
    • 85035270493 scopus 로고
    • 151, 204 (1983).
    • (1983) , vol.151 , pp. 204
  • 33
    • 24844467929 scopus 로고    scopus 로고
    • In the nuclear liquid drop model no curvature energy term is needed in order to fit the mass spectrum, even if every theoretical calculation come up with a curvature term of the same magnitude as the surface term. The explanation is according to W. D. Myers and W. J. Swiatecki, Nucl. Phys. A601, 142 (1996) that still higher order terms tend to counteract the curvature correction and thereby masking its presence. But still (Formula presented) may be ignored in comparison with the quark matter contribution
    • (1996) Nucl. Phys. , vol.A601 , pp. 142
    • Myers, W.D.1    Swiatecki, W.J.2
  • 40
    • 0000456365 scopus 로고
    • J. F. Donoghue and K. Johnson, Phys. Rev. D 21, 1975 (1980); PRVDAQA. W. Thomas, in Advances in Nuclear Physics, edited by J. W. Negele and E. Vogt (Plenum Press, New York, 1984), Vol. 13, pp. 1–137.
    • (1980) Phys. Rev. D , vol.21 , pp. 1975
    • Donoghue, J.F.1    Johnson, K.2
  • 42
    • 85035277883 scopus 로고    scopus 로고
    • When we allow the zero-point energy to change sign from one bulk phase to the other, we obviously break the symmetry between the quark and hadronic slabs at (Formula presented). But one should keep in mind that the approximation altogether of treating one phase as a bulk phase containing a geometry of the other phase becomes poor when the volume fractions approaches 0.5
    • When we allow the zero-point energy to change sign from one bulk phase to the other, we obviously break the symmetry between the quark and hadronic slabs at (Formula presented). But one should keep in mind that the approximation altogether of treating one phase as a bulk phase containing a geometry of the other phase becomes poor when the volume fractions approaches 0.5.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.