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Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Techn ology 2012.06.15 KITPC, Beijing

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Page 1: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Nuclear Collective Excitation in a Femi-Liquid Model

Bao-Xi SUN

Beijing University of Technology

2012.06.15 KITPC, Beijing

Page 2: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Content

Fermi-liquid Model based on Landau Theory.

Relation between isoscalar giant resonance and isovector giant resonance

Collective excitation in nuclear matter Collective excitation in finite nuclei Conclusion

Page 3: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Fermi-liquid Model based on Landau Theory

Xiao-Gang Wen,

Quantum field theory of many-body systems,

Oxford University Press, Oxford, 2004.

Page 4: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Boltzmann Equation of quasi-nucleons

Boltzmann equation of nucleons

where

Page 5: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Density of quasi-nucleons

The quasi-nucleon density near the Fermi-surface:

with

Page 6: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Vibrations of Fermi surface

Fk

Page 7: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Linearized liquid equation of motion in the momentum space

with

and

Page 8: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Potential between nucleons in the linear Walecka model

Page 9: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Fermi liquid function

Page 10: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Fermi liquid function

with

and

Page 11: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Fermi energy and Fermi velocity

Page 12: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

C. J. Horowitz and B. D. Serot, Nucl. Phys. A368 (1981) 503

10.47, 13.80,

520 , 783 ,

939 .N

g g

m MeV m MeV

M MeV

Page 13: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

The quasi-nucleon density can be expanded in spherical harmonics:

Page 14: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Liquid equation of motion in spherical harmonics

Page 15: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

The stability of the Fermi liquid requires the diagonal matrix elements of M must be positive definite, and we can write M as M =W WT. Letting

Page 16: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Eigen-energy equation for the nuclear collective excitation

with the Hamiltonian

, , ,i u Hu l m q tt

,

1, 1, 1,

1 12 22 2

* *3 3

, ,(2 ) (2 )

Tl l

lm l l l m l l

F FF F F F

H q W KW

q a a

k kv f l l v f l l

Page 17: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

and

Tu W

Page 18: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Eigenvalues of the Hamiltonian

Page 19: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Since the nucleon near Fermi-surface is easier to be excited, in the following calculation, we set the value of nucleon momentum

Page 20: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Collective excitation energy El .vs. effective mass M*N .

L=0,Dash;L=1,Solid;L=2,Dot.

Page 21: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Collective excitation

* 0.742N NM M

Page 22: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Relation between isoscalar and isovector giant resonances

The nuclear isovector giant resonances correspond to the nuclear collective excitation that the collective excitation of protons is creating with the energy ES(l), while the collective excitation of neutrons is annihilating with the energy ES(l), and vice versa.

Page 23: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Relation between isoscalar and isovector giant resonances

The energy of the nuclear isovector giant resonance is about twice of the corresponding isoscalar giant resonance in the nuclear matter, i.e.,

Page 24: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Giant resonances of finite nuclei

The proton and neutron densities can be written approximately

Page 25: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Giant monopole resonances of finite nuclei

L=0 M*/M E0(p) E0(n) E0(p) +E0(n)

ES EV

Pb208 0.742 16.28 7.05 23.33 14.17

+-0.28

26.0+-3.0

Sm144 0.742 15.26 9.00 24.26 15.39

+-0.28

_

Sn116 0.742 15.26 9.00 24.26 16.07

+-0.12

_

Zr90 0.717 17.57 13.13 30.7 17.89

+-0.20

28.5+-2.6

Ca40 0.717 15.58 15.58 31.16 31.1+-2.2

Page 26: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Giant dipole resonances of finite nuclei

The isovector giant dipole resonance of the nucleus is a shift of the center of mass, which

corresponds to the creation of the L=1 collective excitation of protons or neutrons.

Page 27: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Giant dipole resonances of finite nuclei

The isoscalar giant dipole resonance in Pb-208 with a centroid energy E=22.5MeV should be a compression mode, which corresponds to a creation of the L=1 collective excitation of protons or neutrons and an annihilation of the L=1 collective excitation of neutrons or protons simultaneously.

B. F. Davis et al., PRL 79, 609 (1997)

Page 28: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Giant dipole resonances of finite nuclei

l=1 M*/M E0(p) E0(n) E0(p) +E0(n)

ES EV

Pb208 0.755 15.53 6.57 22.1 22.5 13.5+-0.2

Zr90 0.742 15.56 11.37 26.93 _ 16.5+-0.2

Ca40 0.7 19.58 19.58 39.16 _ 19.8+-0.5

Page 29: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Giant quadrupole resonances of finite nuclei

l=2 M*/M E0(p) E0(n) E0(p) +E0(n)

ES EV

Pb208 0.742 15.02 5.84 20.86 10.9+-0.1 22.0

Zr90 0.742 13.16 8.27 21.43 14.41+-0.1 _

Ca40 0.69 18.54 18.54 37.08 17.8+-0.3 32.5+-1.5

O16 0.69 18.54 18.54 37.08 20.7 _

Page 30: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Mixture of different L state (M*/M=0.742, kF=1.36fm-1)

Page 31: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Conclusion

In the Fermi-liquid model, the exchange interaction between nucleons causes the nuclear collective excitation.

It is different from RMF+RPA.

Of course, we need not take into account the contribution from Dirac sea.

Page 32: Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology 2012.06.15 KITPC, Beijing

Thanks for your attention!