Title: Diapositive 1
1Giant resonances, exotic modes astrophysics
1) The dipole strength r-process
Ultra-High Energy
Cosmic Rays 2) Exotic modes SuperGiant
Resonances Giant
Pairing Vibrations 3) Surprise ?
E. Khan
21) The dipole strength
3The role of dipole strength in nuclei(de)-excitat
ion
- r-process (n,g) rates in the non-equilibrium
canonical model - Nuclei photodisintegration
- Statistical model of compound nuclear reaction
Hauser-Feshbach
Tn
SnEn
(Z,A) n
Tg TE1(E) r(E) dE
Sn
0
(Z,A1)
Photon transmission coefficient sensitive
to
Tg
- the E1 strength distribution TE1(E)
- the level density r(E)
4Why using microscopic calculations ?
- Microscopic
- Efforts consuming ?
- More suited to extrapolate
- far from stability neutron skin
- Characterize the n-n interaction on the whole
nuclear chart - Test the model validity on a large scale
- Phenomenologic
- Fast and simple to use
- Extrapolations ?
- No feedback about nuclear structure
E1
E1
5 Impact on astrophysical predictions
GDRPR
GDR
Maxwellian averaged (n,g) rates
r-abundance distributions
Effect of the Pygmy Resonance
S. Goriely, PLB436 (1998) 10
6Experiment 1
- Systematics E1 strength measurements for neutron
rich unstable nuclei - below Sn
- Relativistic Coulomb excitation
AGATA
70Ni
High Z
70-100 MeV/u
7 Meanwhile microscopic prediction of the E1
strength
- Collective excitation in superfluid system
- QRPA in linear response small amplitude limit
of the perturbed TD-HFB equations
harmonic oscillations - Connected to the Density Functional Theory
er,k - Since Year 2000
- Skyrme functionnal
- ?lt?(r)?(r)gt particle density
-
- ?lt?(r)?(r)gt pairing density
E (MeV)
r (fm-3)
E. Khan, N. Sandulescu, Nguyen Van Giai, M.
Grasso PRC66 (2002) 024309
8Comparison with experiment
GDR centroids (cf experiment 1)
SLy4
rms on GDR centroids SIII 2267 keV SGII 573
keV SLy4 457 keV MSk7 564 keV
BSk7 rms on 2135 masses 676 keV rms on
48 GDR centroids 485 keV interactions
developed with both ground and excited states
features on a large scale
(48 spherical nuclei)
9Experiment 2
- Inputs E1, level densities, masses, optical
model potential -
- Validity high level density
Sn not too small - Direct captures are not negligible for
neutron-rich nuclei
Low energy section of EURISOL masses, b decay,
...
10(n,g) rates
QRPA/Hybrid
Discrepancy pheno/micro
QRPA/QRPA
Agreement HFBCS QRPA / HFB QRPA
T1.5 109 K
Deviation up to a factor 10
S. Goriely, E. Khan, M. Samyn, NPA739 (2004) 331
11 Are Ultra-High Energy Cosmic Rays made of
nuclei ?
The Pierre Auger collaboration
12Ultra High energy Cosmic Rays
E1018-21 eV
GZK
Ankle
E-3
Redressed spectrum (x E3)
13Composition, acceleration propagation
- Open question !
- Extra-galactic particles protons
- nuclei (56Fe, ) ?
COMPOSITION
- Open question !
- Gamma Ray Bursts, Active Galaxy Nucleus ?
- N(E)E-b
ACCELERATION
- Quantitative answers
- Interaction with the 2.7 K Cosmic microwave
background - Extra-galactic Magnetic fields
PROPAGATION
Comparison with the measured spectrum on Earth
(AUGER, )
14Propagation of UHECR
2.7 K Cosmic Microwave Background
Photodisintegration cross section
g2.1010
GDR
56Fe 1021 eV
Photons density
Lorentz boosted
10
100
0.1
1
10
100
1000
E (MeV)
E (MeV)
Photodisintegration rate (1h-1)
15Photodisintegration (I)
- Pheno. and microscopic models to predict the GDR
strength - Photodisintegration calculated within
Hauser-Feshbach formalism
55Mn (g,1nx)
51V (g,1nx)
Full network with beta decay rate ( r-process)
16Photodisintegration (II)
17Experiment 3
- E1 strength for Alt56 nuclei close to the valley
of stability - Very High intensity 109 pps for 37,39Ar
UHECR campain ? Usefull for many other
applications
18Impact on astroparticle propagation
Source 56Fe
E. Khan, S. Goriely, D. Allard, E. Parizot, et
al, Astr. Phys. 23 (2005) 191
19Interpretation of the ankle
Protons only b2.6
Protons Nuclei b2.3
Needs for a galactic CR Ankle is the
galactic/extra-galactic transition
D. Allard, E. Parizot, A.V. Olinto, E. Khan, S.
Goriely, AA 443 (2005) 29
202) Exotic modes
21 SuperGiant Resonances in neutron stars
Nuclear matter not only a toy for theoreticians
22 The inner crust
r0
0.5 r0
Wigner-Seitz cells
23 Supergiant resonances
L1
Excitations of drip-line nuclei immersed in
neutron gas
E. Khan, N. Sandulescu, Nguyen Van Giai, PRC71
(2005 042801
24Experiment 4
- Specific heat spectroscopy of drip-line nuclei
drives - the excitation spectrum of the Wigner-Seitz cells
- (low-lying states)
- Coulex or integrated (p,p)
- on the most neutron-rich Sn available (138Sn)
25Giant pairing vibrations
22O2n
- 2n transfer
- GPV high energy mode
- never observed
Khan PRC69(2004)014314
26Experiment 5
- Exotic nuclei Q value matched for high energy
states - Search for the GPV
- 208Pb(12Be,10Be) at 10 MeV/u
273) Surprise
28GMR in unstable nuclei
MAYA active target
56Ni(d,d) at 50 MeV/u (GANIL)
2956Ni excitation energy spectrum
Charlotte Monrozeau PhD thesis
30 Outlook
- Dipole modes plays a crucial role in nuclei
de-excitation - Microscopic treatment necessary to draw
conclusions on - r-process abundances
- Nature of UHECR
- Needs for
- Masses, b decay
- Systematic E1 data
- Low lying states close to the drip-line
- 2 neutron transfer reactions with exotic nuclei
Collective excitations in stable nuclei
exotic nuclei drip-line nuclei Fermi gas
31Microscopic models improvements
Neutron average pairing field
- Finite temperature effects
- HFBQRPA
- Future - microscopic treatment of the width
- - better treatment for odd nuclei
- - microscopic treatment of the deformation
- - phonon coupling calculations
- - drip-line nuclei coupling between
continuum and pairing effects - exact continuum calculations
124Sn
Dn (MeV)
Pairing phase transition
T (MeV)
32Comparison with the data
- Monte-Carlo using a extragalactic source with
energy distribution E-b - CMB Protons p photoproduction and e-e-
pairs production - Nuclei photodisintegration and
e-e- production - Infra Red background
Non-negligible effect with the forthcoming AUGER
data
33 Next
- Magnetic field effect on the propagation of UHECR
- Nuclei in the acceleration process
- Comparison with the AUGER data
34 Low and high density WS cells
- Size of the WS cells
- 1800Sn 28 fm
- 982Ge 14 fm
- Skyrme-HFB calculations with density dependent
pairing interaction - Non-zero value of r at the border of the WS cell
N. Sandulescu PRC 69 (2004) 045802
35 Specific heat of collective modes
1800Sn
Entropy ScollSQRPA-SHFB
36Température dans les noyaux
Transition de phase superfluide
Noyaux exotiques chauds pairingcontinuumtempér
ature
E. Khan, Nguyen Van Giai, M. Grasso
NPA731(2004)311
37Accelerators of the Universe
38 The QRPA residual interaction
Skyrme force and surface pairing interaction
h
SLy4 force
EQP lt 60 MeV