The Nuclear Surface Energy

Świa̧tecki, W.J.

doi:10.1088/0370-1298/64/3/302

Cited by 59 publications

(22 citation statements)

References 4 publications

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“…(J) where the total energy E of the nucleus is a function of the mass number A, the Fermi momentum kf, and the surface area S. This definition is practically in accordance with the definition given by Swiatecld and other authors [3,6,7,9] …”

supporting

confidence: 69%

“…where the total energy E of the nucleus is a function of the mass number A, the Fermi momentum kf, and the surface area S. This definition is practically in accordance with the definition given by Swiatecld and other authors [3,6,7,9] but differs from that one used by Hill and Wbeeler [4], Guruits et al [8] and Lanzi [5] which we believe to be inappropriate to nuclear physics. (Furthermore, the method of LanzI is entirely wrong so that with definition (1) he would get u = 0.)…”

supporting

confidence: 64%

“…Several authors [3][4][5][6][7][8][9] have attempted to explain this term by a surface tension of nuclear matter. As these authors, we start with the Fermi-gas model but take a realistic, energydependent shell model potential.…”

mentioning

confidence: 99%

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Surface tension of nuclear matter

et al. 1966

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The surface tension (] and the surface density thickness t of nuclear matter have been calculated in the Fermi-gas model, the nucleons moving in a self-made shell model potential with a realistic slope and velocity dependence (parameters a and. (J) where the total energy E of the nucleus is a function of the mass number A, the Fermi momentum kf, and the surface area S. This definition is practically in accordance with the definition given by Swiatecld and other authors [3,6,7,9]

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supporting

confidence: 69%

supporting

confidence: 64%

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Surface tension of nuclear matter

et al. 1966

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“…Then one has to write Eqs. (10) (12) Let us define a function w(r) such that the portion of the box that is in the shell between rand r + dr is given by w(r) dr. Then the correction may be written as…”

Section: Tmentioning

confidence: 99%

On the microscopic and macroscopic aspects of nuclear structure with applications to superheavy nuclei

Tsang

1969

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“…We consider here the linear potential model [9,10] approximation to the effective potential at a metal surface (Fig. 1).…”

Section: Introductionmentioning

confidence: 99%

Metal Surface Dipole Moment and Work Function in the Linear Potential Model

1991

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Jellium metal surface properties such as the surface dipole barrier and work function are obtained in the linear potential approximation to the effective potential at the surface. The metal surface position and field strength are determined respectively by the requirement of overall charge neutrality and the constraint set on the electrostatic potential by the Budd-Vannimenus theorem. The calculations are primarily analytic and these properties are given in terms of universal functions of the field strength. The results obtained employing the Ceperly-Alder expression for the correlation energy closely approximate those of Lang and Kohn.

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The Nuclear Surface Energy

Cited by 59 publications

References 4 publications

Surface tension of nuclear matter

Surface tension of nuclear matter

On the microscopic and macroscopic aspects of nuclear structure with applications to superheavy nuclei

Metal Surface Dipole Moment and Work Function in the Linear Potential Model

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