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Learn about collective excitations in nuclei, deformed shapes, rotational vibrations, Fermi gas model, and Fermi level in a thermodynamic context. Discover the dynamics of highly excited nuclei.
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Lesson 6 The Collective Model and the Fermi Gas Model
Evidence for Nuclear Collective Behavior • Existence of permanently deformed nuclei, giving rise to “collective excitations”, such as rotation and vibration • Systematics of low lying 2+ states in many nuclei • Large transition probabilities for 2+0+ transitions in deformed nuclei • Existence of giant multipole excitations in nuclei
Deformed Nuclei • Which nuclei? A=150-190, A>220 • What shapes?
Rotational Excitations • Basic picture is that of a rigid rotor
Are nuclei rigid rotors? • No, irrotational rigid
Nuclear Vibrations Types of vibrations
Nilsson model • Build a shell model on a deformed h.o. potential instead of a spherical potential Superdeformed nuclei Hyperdeformed nuclei
Fermi Gas Model • Treat the nucleus as a gas of non-interacting fermions • Suitable for predicting the properties of highly excited nuclei
Details Consider a box with dimensions Lx,Ly,Lz in which particle states are characterized by their quantum numbers, nx,ny,nz. Change our descriptive coordinates to px,py,pz, or their wavenumbers kx,ky,kz where ki=ni/Li The highest occupied level Fermi level.
Thermodynamics of a Fermi gas • Start with the Boltzmann equation S=kBln • Applying it to nuclei • The evaluation of this expression requires some detailed considerations of the • statistical thermodynamics of the system, which are outlined in the book.
Relation between Temperature and Level Density • Lang and LeCouteur • Ericson