Peter Egelhof GSI Darmstadt, Germany 8th. International ... - Bulgaria

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Introduction: Phenomena and Burning QuestionsSensitivity of the Skin Thickness on Parameters of the EOS of Nuclear Matter:2 4E(ρ , α)= E(ρ,0) + S ( ρ)α + Ο(α ) , α =21 ∂ E(ρ,α)S2 ( ρ)= | =22 ∂αα = 0p0∆K0= a4+ ( ρ − ρ0)+ ( ρ − ρ0)22ρ 18ρ0+ ...example: Sn isotopesat the nuclear surface:almost pure neutron matter probe isospin dependence ofeffective in-medium interactions sensitivity to the symmetry energy(parameter a 4of the EOS)02N − ZA2 (S 2= Symmetry Energy)Skin thickness R n- R ptheoretical prediction: P.-G. Reinhard
Introduction: Phenomena and Burning QuestionsThe Nuclear Equation of State and its Dependence on n-p Asymmetry and Density:Neutron Starsymmetry energy and its density dependence close to saturation density→ properties of n-rich nuclei ?symmetry energy at higher densities→ reactions with n-rich nuclei ?
Page 1 and 2: Nuclear Structure Studies on Exotic
Page 3 and 4: I. Introductionmethods of nuclear s
Page 5 and 6: Introduction: Phenomena and Burning
Page 9 and 10: Halo-Nuclei - a New Phenomenonof th
Page 11: The Radial Shape of Nuclei: from St
Page 15 and 16: The Collective Response of the Nucl
Page 17 and 18: The Collective Response of the Nucl
Page 19 and 20: The Radial Shape of Nuclei: from St
Page 21 and 22: New Magic Number N = 16N=20 shell g
Page 27 and 28: Light-Ion Induced Direct Reactions
Page 29 and 30: The Present Radioactive Beam Facili
Page 31 and 32: Production of Radioactive Beams at
Page 33 and 34: Why Fast Radioactive Beams?Producti
Page 35 and 36: II. Experimental TechniquesExperime
Page 37 and 38: Application of Active TargetsConcep
Page 39 and 40: The Experimental Storage Ring ESR a

Peter Egelhof GSI Darmstadt, Germany 8th. International ... - Bulgaria

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