Exochim & Farcos collaboration: L. Acosta, F. Amorini, A. Anzalone, L. Auditore, G. Cardella, A....
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Exochim & Farcos collaboration: L. Acosta, F. Amorini, A. Anzalone, L. Auditore, G. Cardella, A. Chbihi, E. De Filippo, L. Francalanza, E. Geraci, C. Guazzoni,
Exochim & Farcos collaboration: L. Acosta, F. Amorini, A.
Anzalone, L. Auditore, G. Cardella, A. Chbihi, E. De Filippo, L.
Francalanza, E. Geraci, C. Guazzoni, E. La Guidara, G. Lanzalone,
I. Lombardo, S. Lo Nigro, D. Loria, I. Martel, T. Minniti, E.V.
Pagano, A. Pagano, M. Papa, S. Pirrone, G. Politi, F. Porto, F.
Rizzo, P. Russotto, S. Santoro, A. Trifir, M. Trimachi, G. Verde,
M. Venhart, M. Veselsky, M. Vigilante NSCL-Michigan State
University Z. Chajecki, P. Danielewicz and B. Barker
Acknowledgements
Slide 2
Dynamics and correlation studies @ INFN-Catania Catania LNS
Tandem (15 MV)EA 10 MeV Superconducting Cyclotron K800 G. Verde
& Exochim coll., INFN-CT, INFN-LNS, Univ. of Catania, LNS
Slide 3
Chimera our Alice for intermediate energies 1m 1 30 TARGET 176
Beam 1192 Si-CsI(Tl) Telescopes 18 rings in the range 1 30 17 rings
in the range 30 176 (sphere) High granularity and efficiency up to
94% 4 Z identification up to beam charge (E-E) Z and A
identification by E-E up to Z 9 Z and A identification in CsI up to
Z 4 Mass identification with low energy threshold (< 0.3 MeV/u)
by ToF Z identification for particles stopping in Si (pulse
shape)
Slide 4
Si CsI(Tl) E(Si)-E(CsI) Charge Z for particles punching
throught the Si detector PSD in CsI(Tl) Z and A for light charged
particles E(Si)-ToF Mass for particles stopping in the Si detector
E(Si)-Rise time Charge Z for particle stopping in Si detectors
(NEW) E(Si)-E(CsI) Charge Z and A for light ions (Z
Asy-Stiff Asy-Soft Producing density gradients in HIC SMF -
Baran, Colonna, Di Toro, Greco Intermediate energies: E/A=20-100
MeV Ganil, Eurisol, Frib, Lns, Nscl, Spiral2, Tamu, High energies:
E/A>200 MeV CSR, GSI/Fair, NSCL/FRIB, Riken, Neutron Stars Radii
Frequencies of crustal vibrations Composition, thickness of inner
crust URCA processes Phases within the star Densities ~ 0.01 0 - 6
0 Large Gradients!!!
Slide 10
Probes of the symmetry energy Probes at Intermediate energies:
sub-saturation density Asy-EoS ( 0 ) + /- and K + /K 0 emission
ratios n/p elliptic flow n/p pre-equilibrium emission 0 ~ 0.17 fm
-3
Slide 11
Effects of the E sym at high density N/Z of high density
regions sensitive to E sym () High 0 : asy-stiff more repulsive on
neutrons - opposite of sub-saturation trend stiffness B.A. Li et
al., PRC71 (2005) (/ 0 )
Slide 12
Elliptic flow: competition between in plane (V 2 >0) and
out-of-plane ejection (V 2
Event characterization TLFPLFIMFTLFPLFIMF TLF~ PLF~ IMF~ IMF
Characterize IMF emission IMF times 3 M c 6 *b red >0.6 7 M c 12
0.2
Neutron-proton emission chronology Time delay between emissions
t0 - Example: p emitted first p p p n V p > V n n p V p < V n
Stronger interaction particle catch-up Interaction attenuated
Slide 28
Lednicky recipe: p-n correlations 1+R + (q) 1+R (q) Ratio +/-
Ratio R+/R- tells us which is emitted first R. Lednicky et al.,
Phys. Lett. B373, 30 (1996) Nuclear FSI q (MeV/c) n first +100
fm/cn first +50 fm/cp first -100 fm/c p-n
Slide 29
Isospin effects on p-p R 48Ca+ 48Ca > R 40Ca+ 40Ca 48 Ca+ 48
Ca vs 40 Ca+ 40 Ca E/A=80 MeV - Central CorrelationsEmitting
sources Larger size for more n-rich system: N/Z effect? Size
effect? Asy-EoS? NN Z. Chajecki, et al. Phys. Rev. C (2012)
Slide 30
Multi-Particle Correlation Spectroscopy (MPCS) non-femtoscopic
stuff HIC and correlations as a spectroscopic tool Cluster states
in stable and exotic nuclei BEC, Hoyle Expansion Not only EoS
Several unbound species in just one single experiment! 10 C*
Slide 31
8 B unbound state: spin determination States of 8 B p+ 7 Be p+
7 Be 0.774 1.4 (?) 2.32 8B8B 1+1+ 3+3+ p- 7 Be correlations W.P.
Tan et al. Phys. Rev. C69, 061304 (2004) 7 Be 8B8B p Xe+AuE/A50 MeV
Central collisions
Slide 32
Sequential decay modes: multi-particle correlation functions
Peripheral projectile fragmentation 12 C+ 24 MgE/A=53, 95 MeV
(Indra@GANIL) Decay of 12 C and 10 C quasi projectiles (QP*) 12 C*
+ + 10 C* + + p + p + 8 Be + 2p+ 8 Be + p+ 9 B + +p + 6 Be +2p 2+2p
direct + + direct Hoyle states? Boson condensate?
Slide 33
2-2p correlations : states in 10 C* E k (MeV) 10 C 6 Be+ (2p+)
10 C 8 Be+p+p (+)+ p 10 C 9 B+p ( + ) p F. Grenier et al., Nucl.
Phys. A811 (2008) 233
Slide 34
Search for Hoyle states in N nuclei Three-alpha correlations 12
C* + + Gated 8 Be* + No direct three-body decay of Hoyle state in
12 C J. Manfredi, R.C. Charity et al., PRC 2012 A. Raduta et al.,
Phys. Lett. B705, 65, 2011 40 Ca+ 12 C, E/A=25 MeV @ Chimera 12 C 3
alpha ~ 7.5% direct three-body decay (BC?)
Slide 35
Conclusions Probes of symmetry energy at high density: GSI
energies: n/p flow Chimera-LAND@GSI + /- and K + /K 0 emission
ratios Understand where and when s and Ks are produced correlation
techniques (?) Probes of symmetry energy at low density:
Intermediate energies: Isospin diffusion and drift; moderately soft
symmetry energy (~0.6-0.9) Still missing probes from femtoscopy
future projects non-femtoscopic correlations to learn about new
phenomena and exotic nuclear systems