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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
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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
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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.
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