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Masses and Fission Barriers of Atomic Nuclei

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Nuclear energy functional<br />

The one-body density <strong>of</strong> a nucleus can be expressed as<br />

∫ ∫ ∫<br />

ρ = A . . . Ψ ⋆ Ψ dτ 2 · · · dτ A<br />

<strong>and</strong> the corresponding energy-density as<br />

∫ ∫ ∫<br />

η = . . . Ψ ⋆ ĤΨ dτ 2 · · · dτ A .<br />

The total energy <strong>of</strong> the nucleus is<br />

∫<br />

B = η d 3 r<br />

V<br />

<strong>Masses</strong> <strong>and</strong> <strong>Fission</strong> <strong>Barriers</strong> <strong>of</strong> <strong>Atomic</strong> <strong>Nuclei</strong> – p.6/33

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