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NSR database version of May 1, 2024.

Search: Author = M.L.Cescato

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1998CE01      Phys.Rev. C57, 134 (1998)

M.L.Cescato, P.Ring

Density Dependent Relativistic Mean Field Theory in Deformed Nuclei

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁹⁰Zr, ¹¹⁸Sn, ¹⁴⁰Ce, ^208,214Pb, ²⁰Ne, ^142,162Dy, ¹⁶⁸Er, ²³⁴U, ²³⁸Pu; calculated binding energy, radii, deformation. Comparison with data. Density dependent relativistic mean-field theory.

doi: 10.1103/PhysRevC.57.134
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1994ST22      J.Phys.(London) G20, L149 (1994)

M.V.Stoitsov, M.L.Cescato, P.Ring, M.M.Sharma

Nuclear Breathing Mode in the Relativistic Mean-Field Theory

NUCLEAR STRUCTURE ²⁰⁸Pb, ⁹⁰Zr, ⁴⁰Ca, ¹⁶O; calculated breathing mode collective mass incompressibility. Relativistic mean field theory.

doi: 10.1088/0954-3899/20/12/003
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1991CE08      Nucl.Phys. A533, 455 (1991)

M.L.Cescato, Y.Sun, P.Ring

Cranked Hartree-Fock-Bogoliubov Calculations for Dy Isotopes

NUCLEAR STRUCTURE ^{154,156,158,160,162,164}Dy; calculated transition energies, n-, p-gap parameters, g factors, B(λ), pair-transfer matrix elements. Cranked HFB calculations.

doi: 10.1016/0375-9474(91)90528-E
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1984CE01      Phys.Rev. C29, 49 (1984)

M.L.Cescato, M.C.Hermida, M.Ruiz, J.L.Foster, Jr., F.Krmpotic

¹⁴⁴Sm(p, p') Scattering Isobaric Analog Resonances and the Structure of ¹⁴⁵Sm

NUCLEAR STRUCTURE ¹⁴⁵Sm; calculated low-lying parent state spectroscopic factors. Input from ¹⁴⁴Sm(p, p') data analysis.

NUCLEAR REACTIONS ¹⁴⁴Sm(p, p), (p, p'), E=8.5-14 MeV; measured σ(θ), σ(θ) vs E; deduced optical model parameters. ¹⁴⁵Eu deduced IAR, J, π, Γp, Γp', Γ, spectroscopic factors.

doi: 10.1103/PhysRevC.29.49
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1984HE01      Phys.Rev. C29, 64 (1984)

M.C.Hermida, M.Ruiz, M.L.Cescato, J.L.Foster, Jr., F.Krmpotic

¹³⁰Te(p, p') Reaction on Analog Resonances

NUCLEAR STRUCTURE ¹³¹Te; calculated low-lying parent state spectroscopic amplitudes.

NUCLEAR REACTIONS ¹³⁰Te(p, p), (p, p'), E=7.5-14 MeV; measured σ(θ), σ(θ) vs E; deduced optical model parameters. ¹³¹I deduced IAR, Γp, Γp', Γ, spectroscopic amplitudes.

doi: 10.1103/PhysRevC.29.64
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