Charge Equilibration Dynamics: The Dynamical Dipole Competition of Dissipative Reaction Mechanisms Neck Fragmentation M.Di Toro, PI32 Collab.Meeting, Pisa.

Slides:



Advertisements
Similar presentations
Neck fragmentation time Semi-peripheral reactions: Fragmentation in a smaller region, but with larger cross section ! Possibility to better disantangle.
Advertisements

PROBING THE DENSITY DEPENDENCE OF SYMMETRY ENERGY WITH HIC KITPC Workshop, Beijing, June09, “Recent Progress and New Challenges in Isospin.
Nuclear Symmetry energy and Intermediate heavy ion reactions R. Wada, M. Huang, W. Lin, X. Liu IMP, CAS.
W. Udo Schröder University of Rochester, Rochester, NY Proximity Splitting W. Udo Schröder IWNDT International Workshop on Nuclear Dynamics and.
Probes of EOS in Heavy Ion Collisions : results from transport theories Maria Colonna INFN - Laboratori Nazionali del Sud (Catania) Nuclear Structure &
Isospin dependence of nucleus-nucleus collisions
E. De Filippo (INFN Catania) for the REVERSE / ISOSPIN collaboration Time sequence and isoscaling in neck fragmentation  Fragments production in peripheral.
Neutron Number N Proton Number Z a sym =30-42 MeV for infinite NM Inclusion of surface terms in symmetry.
WCI 2004: 3- SORTING Catania January 2004 WCI 2004 session 3: DATA SORTING Can we extract mechanism? Can we extract sources in space-time? What are the.
EURISOL workshop, ECT* Trento, Jan Two-component (neutron/proton) statistical description of low-energy heavy-ion reactions E. Běták & M.
Clearly state goals and open questions. Questions Which exp. should we perform in order to know how far (how to measure this distance?) we are from eqil.(randomized)
The National Superconducting Cyclotron State University Betty Tsang Constraining neutron star matter with laboratory experiments 2005.
16/1/06Eurisol ECT*1 The nuclear liquid gas phase transition Francesca Gulminelli LPC Caen and Institut Universitaire de France The status of.
Germany's United States 2 Germany 0 FIFA Women’s World Cup Semifinal.
Zbigniew Chajęcki National Superconducting Cyclotron Laboratory Michigan State University Probing reaction dynamics with two-particle correlations.
Constraining the EoS and Symmetry Energy from HI collisions Statement of the problem Demonstration: symmetric matter EOS Laboratory constraints on the.
The study of fission dynamics in fusion-fission reactions within a stochastic approach Theoretical model for description of fission process Results of.
Collective Flow in Heavy-Ion Collisions Kirill Filimonov (LBNL)
Reaction mechanisms in transport theories: a test of the nuclear effective interaction Maria Colonna INFN - Laboratori Nazionali del Sud (Catania) NN2012.
Laura Francalanza Collaborazione EXOCHIM INFN Sezione di Catania - LNS.
Fragmentation mechanism and enhanced mid-rapidity emission for neutron-rich LCPs Yingxun Zhang( 张英逊 ) 中国原子能科学研究院 Colloborator: Chengshuang Zhou 周承双 (CIAE,GXNU),
Maria Colonna Laboratori Nazionali del Sud (Catania) Extracting the symmetry energy from low Extracting the symmetry energy from low and medium energy.
The FARCOS project Collaboration: INFN (CT, LNS, MI, NA; Italy), GANIL (France), Un. Huelva (Spain) Synergies: Fazia, Neutron detectors, Spectrometers,
Longitudinal de-correlation of anisotropic flow in Pb+Pb collisions Victor Roy ITP Goethe University Frankfurt In collaboration with L-G Pang, G-Y Qin,
Peripheral collisions as a means of attaining high excitation –Velocity dissipation is key quantity R. Yanez et al, PRC (in press) Proximity emission as.
Effect of isospin-dependent cluster recognition on the observables in heavy ion collisions Yingxun Zhang ( 张英逊 ) 2012 年 8 月 10 日, 兰州 合作者: Zhuxia Li, (CIAE)
Probing the density dependence of symmetry energy at subsaturation density with HICs Yingxun Zhang ( 张英逊 ) China Institute of Atomic Energy JINA/NSCL,
Maria Colonna Laboratori Nazionali del Sud (Catania) Testing the behavior of n-rich systems away from normal density Eurorib’ 10 June 6-11, Lamoura.
From the Phys.Dept. Jan.2002Etna Double-Face, Aug.07 ISOSPIN DYNAMICS IN HEAVY ION COLLISIONS From Coulomb Barrier to Deconfinement V.Baran, M.Colonna,
Probing the nuclear EOS with fragment production Maria Colonna Laboratori Nazionali del Sud (Catania)
Maria Colonna Laboratori Nazionali del Sud (Catania) Dynamics and Thermodynamics with.
Ln(R 12 ) N Alan McIntosh, Yennello Research Group, TAMU-CI. Nuclear Physics Town Meeting, Aug 2014, College Station, TX Asymmetry Dependence of Thermodynamic.
BNU The study of dynamical effects of isospin on reactions of p Sn Li Ou and Zhuxia Li (China Institute of Atomic Energy, Beijing )
Status of the Subtask 6 Heavy ion reactions in the Fermi-energy domain M. Veselsky, IoP SASc Bratislava Main.
George A. Souliotis Laboratory of Physical Chemistry, Department of Chemistry, National and Kapodistrian University of Athens, Athens, Greece and Cyclotron.
Dynamical fragment production in non-central heavy-ion collisions E *, J PLF* TLF* Sylvie Hudan, Indiana University EvaporationBinary breakupfragmentation.
M.Di Toro, ECT*/Eurisol Jan.06, Isospin Dynamics in Heavy Ion Collisions at Fermi Energies: EOS-sensitive Observables Dissipative Collisions.
Neutron enrichment of the neck-originated intermediate mass fragments in predictions of the QMD model I. Skwira-Chalot, T. Cap, K. Siwek-Wilczyńska, J.
Constraints on the Symmetry Energy from Heavy Ion Collisions Hermann Wolter Ludwig-Maximilians-Universität München 44th Karpacz Winter School of Theoretical.
Probing the symmetry energy with isospin ratio from nucleons to fragments Yingxun Zhang( 张英逊 ) China Institute of Atomic Energy The 11 th International.
Isospin study of projectile fragmentation Content 1 、 Isospin effect and EOS in asymmetry nuclei 2 、 Isotope Yields in projectile ragmentation 3 、 Summary.
Quasifission reactions in heavy ion collisions at low energies A.K. Nasirov 1, 2 1 Joint Institute for Nuclear Research, Dubna, Russia 2 Institute.
Isospin Distillation Mechanism: “direction” of the spinodal unstable mode ! y = proton fraction.
Heavy-ion dynamics at the Fermi energy A theoretical point of view Heavy-ion dynamics at the Fermi energy A theoretical point of view Laboratory for heavy-ion.
Nuclear Isovector Equation-of-State (EOS) and Astrophysics Hermann Wolter Dep. f. Physik, LMU Topics: 1.Phase diagram of strongly interacting matter and.
Isovector reorientation of deuteron in the field of heavy target nuclei The 9th Japan-China Joint Nuclear Physics Symposium (JCNP 2015) Osaka, Japan, Nov.
Z.Q. Feng( 冯兆庆 ), W.F. Li( 李文飞 ), Z.Y. Ming( 明照宇 ), L.W. Chen( 陈列文 ), F. S. Zhang ( 张丰收 ) Institute of Low Energy Nuclear Physics Beijing Normal University.
XII Convegno su Problemi di Fisica Nucleare Teorica
Properties of clustered nuclear matter in nuclear reactions Maria Colonna INFN - Laboratori Nazionali del Sud (Catania) NUFRA October 2015 Kemer.
In-medium properties of nuclear fragments at the liquid-gas phase coexistence International Nuclear Physics Conference INPC2007 Tokyo, Japan, June 3-8,
ATLAS Research projects (DOE milestone NS8) W. Loveland Oregon State University.
COLLECTIVE FEATURES OF NUCLEAR DYNAMICS WITH EXOTIC NUCLEI WITHIN MICROSCOPIC TRANSPORT MODELS Virgil Baran University of Bucharest ROMANIA.
Yoritaka Iwata 1, Naoyuki Itagaki 2, Takaharu Otsuka 1,2,3 1 Department of Physics, University of Tokyo. 2 CNS, University of Tokyo. 3 RIKEN. Competitive.
Lecture 4 1.The role of orientation angles of the colliding nuclei relative to the beam energy in fusion-fission and quasifission reactions. 2.The effect.
Isospin Effects in Dissipative Reactions Maria Colonna INFN - Laboratori Nazionali del Sud (Catania) SPES 2014 Second International Workshop 26 th -28.
Isospin Equilibration Processes and dipolar degree of Freedom 12 C+ 64 Ni 8 Be(2α)+ 72 Ge * 8 MeV/A Incomplete fusion-FastTransfer of isoscalar particles.
Signals for dynamical process from IMF-IMF correlation function
Fragment-fragment correlations
FAST IN-MEDIUM FRAGMENTATION OF PROJECTILE NUCLEI
Transverse and elliptic flows and stopping
28/05/2018 Investigation of the Dynamical Dipole Mode in the 40,48Ca+152,144Sm fusion- evaporation and fission reactions at 11 MeV/nucleon Concetta Parascandolo.
RIZZO CARMELO Isospin effects in heavy ion reactions at low energies
124Sn + 64Ni (35AMeV) b- impact parameter
Midrapidity Dynamics Update
Isospin observables Observables
Reaction Dynamics in Near-Fermi-Energy Heavy Ion Collisions
Nuclear Reactions --Part 2
NECK FRAGMENTATION EVENT
in 124Sn,107Sn + 120Sn collisions at 600 MeV/nucleon
HIC: probing different B regions
Presentation transcript:

Charge Equilibration Dynamics: The Dynamical Dipole Competition of Dissipative Reaction Mechanisms Neck Fragmentation M.Di Toro, PI32 Collab.Meeting, Pisa 05 Isospin Dynamics in Dissipative Heavy Ion Collisions

Symmetry Energy E sym    MeV)     1230 Expansion around   Pressure & compressibility Asy-stiff Asy-soft Pressure gradient

Mean Field & Chemical Potentials 124 Sn “asymmetry”  = 0.2 symmetry part of the mean fieldneutron-proton chemical potentials neutron proton bulk neck

STOCHASTIC MEAN-FIELD TRANSPORT APPROACH VLASOV + COLLISION and PAULI CORRELATIONS FLUCTUATIONS Equilibrium in a phase space cell OK if tot. number of collisions Initial: any time FLUCT.-DISS. THEOREM gainloss Markov NPA 642 (1998)

D(t) : bremss. dipole radiation CN: stat. GDR Initial Dipole Pre-equilibrium Dipole Radiation Charge Equilibration Dynamics: Stochastic : Diffusion vs. Collective : Dipole Oscillations of the Di-nuclear System Fusion Dynamics - Fusion Dynamics (MassAsymmetry) - Anisotropy - Cooling on the way to Fusion

Pre-equilibrium dipole emission (1) Ca + 4 AMeV O + 4,8,14,20 AMeV O AMeV, Simenel et al., PRL86(2001) Baran et al., PRL87(2001) TDHF BNV Quantitative: abs. estimations

S32 + Mo100 (6 AMeV) S32 + Mo100 (9 AMeV) D(t) Dk(t) time(fm/c) Pre-equilibrium dipole emission (2) D.Pierroutsakou et al. (2005) M.Papa et al., AMeV Cooling in hot fusion ?

Fusion - Deep Inelastic Competition E= 30 AMeV, b=0.45 b max 46 Ar + 64 Ni (1.55) (1.29) n-rich 46 V + 64 Ge n-poor M. Colonna et al., PRC57 (1998) Asy-soft Asy-stiff Asy-soft Asy-stiff More fast proton emission

b=4fmb=6fm 124Sn+124Sn 50AMeV, semi-central STOCHASTIC MEAN-FIELD Freeze-out V.Baran et al. NPA 703 (2002) Time-scale matching: Instability growth vs Interaction time Rise and Fall: -with impact parameter - with beam energy Neck Fragmentation Mechanism

NECK FRAGMENTATION: COMPRESSIBILITY EFFECTS the role of volume instabilities K=380MEV soft stiff Central density evolution cube of 10fm side K=200MEV 124 Sn+ 64 Ni 35AMeV b=6fm V.Baran et al. NPA 730 (2004)

NECK FRAGMENTATION EVENTS free cross sectionshalf free cross sections up -early stage of fragment formation down- configurations close to freeze-out Nucleon-nucleon cross sections dependence P=N ternary /N total 124 Sn+ 64 Ni 112 Sn+ 58 Ni 124 Sn+ 64 Ni ; 35AMeV; b=6fm

DEVIATIONS FROM VIOLA SYSTEMATICS r - ratio of the observed PLF-IMF relative velocity to the corresponding Coulomb velocity; r1- the same ratio for the pair TLF-IMF The Neck - IMF is weakly correlated with both PLF and TLF Wilczynski-2 plot ! V.Baran, M.Colonna, M.Di Toro NPA 730 (2004)

REDUCED VELOCITY PLOTS: BNV V. Baran et al. Nucl. Phys A730 (2004) 329 Note: BNV model accounts only for the “prompt” component of IMF’s Chimera 124Sn+64Ni 35AMeV data, same E_loss selections

Gating the reduced plot for light IMFs:

NECK FRAGMENTATION: CM V z -V x CORRELATIONS PLF IMF TLF Large dispersion also along transversal, x, direction 124 Sn + 64 Ni 35 AMeV  <0  >0 Alignement + Centroid at Clear Dynamical Signatures !

Angular distributions: alignment characteristics  plane is the angle, projected into the reaction plane, between the direction defined by the relative velocity of the CM of the system PLF- IMF to TLF and the direction defined by the relative velocity of PLF to IMF Out-of-plane angular distributions for the “dynamical” (gate 1) and “statistical” (gate 2) components: these last are more concentrated in the reaction plane.

124 Sn+ 64 Ni 35AMeV asystiffasysoft 64 Ni 124 Sn superasystiff ISOSPIN COMPOSITION OF THE IMF’S PRODUCED IN NECK FRAGMENTATION: ASY-EOS EFFECT

N  = 0.95 Z=1 Z=3 Z=2 Z=5 Z=7 Z=6 Z=8 Z=4 Z=9 lnR 21 NECK ISOSCALING at 35 MeV/n (b=6,7,8fm) asysoft asystiff superasystiff  V. Baran, M. Colonna, M. Di Toro : NPA 370 (2004) 329

Z ln R 21  = N=2 N=3 N=8 N=7 N=6 N=5 N=4 NECK ISOSCALING at 35 MeV/n (b=6,7,8fm) asysoft asystiff superasystiff 

58Fe+58Fe vs. 58Ni+58Ni b=4fm 47AMeV: Freeze-out Asymmetry distributions Fe Ni Fe Ni White circles: asy-stiff Black circles: asy-soft Asy-soft: small isospin migration Fe: fast neutron emission Ni: fast proton emission R.Lionti et al., nucl-th/

Neck Fragments: N/Z – angle correlation FeFe vs NiNi b=4fm 47AMeV: 40% ternary - Isospin Migration for almost symmetric systems - Minimum N/Z around 90° : earlier formation? R.Lionti et al, nucl-th/

FeFe b=4fm 47AMeV: density contour plots fm/c PLF/TLF residues asymmetry (N-Z)/A System initial t=100fm/c(after pre-eq) freeze-out 58Fe+58Fe binary 1.19 ternary 58Ni+58Ni binary 1.12 ternary n-enrichment of Neck-Fragments even for symmetric systems! R.Lionti et al. nucl-th/