Sez.-CT
 GDR pre-equilibrium emission 40Ca+48Ca,46Ti at 25 MeV/A
   S.Tudisco EPL 58 (5), 811(2003)
   M.Papa et al, PRC 68., 034606 (2003)
   F.Amorini et al PRC 69, 014608(2004)

Fusion-Incomplete Fusion                                 Dissipative binary processes
                                 Extra yield at 10 MeV
GDR pre-equilibrium emission 40Ca+48Ca,46Ti at 10 MeV/A
  M.Papa et al, submitted to PRC


  Dissipative binary processes     study of kinematical coincidence
Z=14-22   Elab<160 MeV
       40Ca+46Ti

                       40Ca+46Ti
γ-1f          γ-2f                   40Ca+48Ca
CoMD calculations
TKEL-angular and charge distrib.
b-window→ pre-eq γ Yield
How we can generate the coherent                  Sez.-

               contribution?
                                                       CT


  A simple picture the “Molecular Dipole”
The average ensemble in an harmonic mean field
    The initial conditions for the GDR mode

                            At the contact D1≈D2 ≈0

  n
   p
                 N1/Z1≠N2/Z2




                              if

   If Y=0 NO coherent contribution
Sez.-CT




Coherent contribution         Incoherent contribution
 (ensemble average)           a) Collective
                              b) Microscopic incoherent

Mean field approach            Statistical models
  Fully N-body dynamical approach for 1000 fm/c
Υ-ray average multiplicity in   Sez.-CT


Semi classical Approximation



     The Larmor formula




      Fourier Transform
b=0 fm E/A 25 MeV                      Sez.-CT




                                           Langevin prediction for
                                              the total system

                                         ∗Prediction in the loc. Time
                                              equil. hypothesis

                                         • Prediction according to a
                                            full CoMD approach




                                              g~12


M.Papa et al, PRC 68(2003) 034606
We have also high energy               Sez.-CT

             bremsstrahlung contribution




We have to study the
                       1. We need to define T at long time
      local time
                       2. We need to separate the
spectral properties of
                        incoherent Microscopic contribution
Sez.-CT




High energy results
Multifragmentation
of the hot
 source
M.Papa et al, PRC 50 MeV/A          b=0 fm             Sez.-CT
                      68(2003) 024612




                 ∗
                 •




α obtained from the fit procedure
                                                  Very small
                         or                        Coherent
                                                 contribution
Something is changed in the fundamental
         properties of the formed hot sources….
Degree of collectivity-Degree of coherence as function of t
A new observable related to the properties
  of the dipolar γ-ray emission in different reaction
  mechanisms has been measured




 - Φch represents the ratio between the average and fluctuating dynamics.
 For N-body approaches able to evaluate the two contributions in a self
 consistent way, this parameter should be rather robust with respect some model
 ansatz: semiclassical approximaton, occupation numbers…….
 - On the other hand and we can expect that Φch can depend
 on the dynamics (Forces) governing the equilibration
 Process.
                  From the experiments

Фch(12MeV)=0.6±0.15             10 MeV/A Binary. proc.


Фch(10 MeV)=0.3±0.07            25 MeV/A Inc. fusion.proc.
Collectivity and Coherence for the total system
    limiting energy for the collective motion
    M.Papa et al, PRC 68(2003) 024612,
                                       Black: rather smooth
                                       behaviour
   40Ca + 48Ca Central Collisions
                                       Red:it contains the
                                       Ambiguity related
                                       to the experimental
                 *10                   selections of 1
                                       equilibrated source

                                       Green:high sensitivi
                 Φc(0,tm)              ty, related to the
                 Φc(0,tf)
                                       natural time selection
                 Φch(0,tf)
                                       performed by the
                                       dynamic through
                                       memory effects.
CoMD calculations
TKEL-angular and charge distrib.
b-window→ pre-eq γ Yield
γ-Pre-equilibrium effects and “Isospin-Equlibration”
                           M.Papa et al Sub. PRC

                        Invariant with respect to
                        secondary statistical emission
                        processes
Conclusive remarks                            Sez.-CT




1. An unified description of the pre-equilibrium phenomenon
   (fluctuating average dynamics) has been obtained throgh ComD
   calculations 2.

2. The fluctuation predicted by the model are in agreement with
   Cascade calculations at 25 MeV/A by using g≈12.




2.   φch    rapidly change when the multifragmentation processes set

     in. (much more than φc)




3. The pre-equilibrium extra-yield it is strictly related to the
   isospin equilibration process throgh a quasy-resonant mechanisms.
004

004

  • 1.
    Sez.-CT GDR pre-equilibriumemission 40Ca+48Ca,46Ti at 25 MeV/A S.Tudisco EPL 58 (5), 811(2003) M.Papa et al, PRC 68., 034606 (2003) F.Amorini et al PRC 69, 014608(2004) Fusion-Incomplete Fusion Dissipative binary processes Extra yield at 10 MeV
  • 2.
    GDR pre-equilibrium emission40Ca+48Ca,46Ti at 10 MeV/A M.Papa et al, submitted to PRC Dissipative binary processes study of kinematical coincidence
  • 3.
    Z=14-22 Elab<160 MeV 40Ca+46Ti 40Ca+46Ti γ-1f γ-2f 40Ca+48Ca
  • 4.
    CoMD calculations TKEL-angular andcharge distrib. b-window→ pre-eq γ Yield
  • 5.
    How we cangenerate the coherent Sez.- contribution? CT A simple picture the “Molecular Dipole” The average ensemble in an harmonic mean field The initial conditions for the GDR mode At the contact D1≈D2 ≈0 n p N1/Z1≠N2/Z2 if If Y=0 NO coherent contribution
  • 6.
    Sez.-CT Coherent contribution Incoherent contribution (ensemble average) a) Collective b) Microscopic incoherent Mean field approach Statistical models Fully N-body dynamical approach for 1000 fm/c
  • 7.
    Υ-ray average multiplicityin Sez.-CT Semi classical Approximation The Larmor formula Fourier Transform
  • 8.
    b=0 fm E/A25 MeV Sez.-CT Langevin prediction for the total system ∗Prediction in the loc. Time equil. hypothesis • Prediction according to a full CoMD approach g~12 M.Papa et al, PRC 68(2003) 034606
  • 9.
    We have alsohigh energy Sez.-CT bremsstrahlung contribution We have to study the 1. We need to define T at long time local time 2. We need to separate the spectral properties of incoherent Microscopic contribution
  • 10.
  • 11.
    M.Papa et al,PRC 50 MeV/A b=0 fm Sez.-CT 68(2003) 024612 ∗ • α obtained from the fit procedure Very small or Coherent contribution
  • 12.
    Something is changedin the fundamental properties of the formed hot sources…. Degree of collectivity-Degree of coherence as function of t
  • 13.
    A new observablerelated to the properties of the dipolar γ-ray emission in different reaction mechanisms has been measured - Φch represents the ratio between the average and fluctuating dynamics. For N-body approaches able to evaluate the two contributions in a self consistent way, this parameter should be rather robust with respect some model ansatz: semiclassical approximaton, occupation numbers……. - On the other hand and we can expect that Φch can depend on the dynamics (Forces) governing the equilibration Process. From the experiments Фch(12MeV)=0.6±0.15 10 MeV/A Binary. proc. Фch(10 MeV)=0.3±0.07 25 MeV/A Inc. fusion.proc.
  • 14.
    Collectivity and Coherencefor the total system limiting energy for the collective motion M.Papa et al, PRC 68(2003) 024612, Black: rather smooth behaviour 40Ca + 48Ca Central Collisions Red:it contains the Ambiguity related to the experimental *10 selections of 1 equilibrated source Green:high sensitivi Φc(0,tm) ty, related to the Φc(0,tf) natural time selection Φch(0,tf) performed by the dynamic through memory effects.
  • 15.
    CoMD calculations TKEL-angular andcharge distrib. b-window→ pre-eq γ Yield
  • 16.
    γ-Pre-equilibrium effects and“Isospin-Equlibration” M.Papa et al Sub. PRC Invariant with respect to secondary statistical emission processes
  • 17.
    Conclusive remarks Sez.-CT 1. An unified description of the pre-equilibrium phenomenon (fluctuating average dynamics) has been obtained throgh ComD calculations 2. 2. The fluctuation predicted by the model are in agreement with Cascade calculations at 25 MeV/A by using g≈12. 2. φch rapidly change when the multifragmentation processes set in. (much more than φc) 3. The pre-equilibrium extra-yield it is strictly related to the isospin equilibration process throgh a quasy-resonant mechanisms.