Nonstatistical fluctuations for deep inelastic processes in 27 Al + 27 Al collision Introduction Experimental procedures Cross section excitation functions.

Slides:



Advertisements
Similar presentations
Accelerator Physics, JU, First Semester, (Saed Dababneh).
Advertisements

HIGS2 Workshop June 3-4, 2013 Nuclear Structure Studies at HI  S Henry R. Weller The HI  S Nuclear Physics Program.
Marina Barbui Trento, Italy, April 7-11, 2014
Cohen & Fano (CF) Model CF-I: Monoelectronic Process CF-II: LCAO for the bound molecular state CF-III: Free Wave for the ejected electron H H Interferences.
Gamma-Ray Spectra _ + The photomultiplier records the (UV) light emitted during electronic recombination in the scintillator. Therefore, the spectrum collected.
Alpha Stucture of 12 B Studied by Elastic Scattering of 8 Li Excyt Beam on 4 He Thick Target M.G. Pellegriti Laboratori Nazionali del Sud – INFN Dipartimento.
Nucleon knockout reactions with heavy nuclei Edward Simpson University of Surrey Brighton PRESPEC Meeting 12 th January 2011.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
Preliminary results from a study of isospin non-equilibrium E. Martin, A. Keksis, A. Ruangma, D. Shetty, G. Souliotis, M. Veselsky, E. M. Winchester, and.
NECK FRAGMENTATION IN FISSION AND QUASIFISSION OF HEAVY AND SUPERHEAVY NUCLEI V.A. Rubchenya Department of Physics, University of Jyväskylä, Finland.
Higher Order Multipole Transition Effects in the Coulomb Dissociation Reactions of Halo Nuclei Dr. Rajesh Kharab Department of Physics, Kurukshetra University,
1 Role of the nuclear shell structure and orientation angles of deformed reactants in complete fusion Joint Institute for Nuclear Research Flerov Laboratory.
Using GEMINI to study multiplicity distributions of Light Particles Adil Bahalim Davidson College Summer REU 2005 – TAMU Cyclotron Institute.
EURISOL User Group, Florence, Jan Spin-Dependent Pre-Equilibrium Exciton Model Calculations for Heavy Ions E. Běták Institute of Physics SAS,
Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Nuclear Reactions Categorization of Nuclear Reactions According to: bombarding.
Radiation therapy is based on the exposure of malign tumor cells to significant but well localized doses of radiation to destroy the tumor cells. The.
Dinuclear system model in nuclear structure and reactions.
W. Udo Schröder, 2007 Semi-Classical Reaction Theory 1.
Nuclear Level Densities Edwards Accelerator Laboratory Steven M. Grimes Ohio University Athens, Ohio.
Laura Francalanza Collaborazione EXOCHIM INFN Sezione di Catania - LNS.
Study of the Halo Nucleus 6 He using the 6 Li(   ) 6 He Reaction Derek Branford - Edinburgh University for the A2-Collaboration MAMI-B Mainz.
Neutron transfer reactions at large internuclear distances studied with the PRISMA spectrometer and the AGATA demonstrator.
1 New horizons for MCAS: heavier masses and α-particle scattering Juris P. Svenne, University of Manitoba, and collaborators CAP 15/6/2015.
Kazimierz 2011 T. Cap, M. Kowal, K. Siwek-Wilczyńska, A. Sobiczewski, J. Wilczyński Predictions of the FBD model for the synthesis cross sections of Z.
abrasion ablation  σ f [cm 2 ] for projectile fragmentation + fission  luminosity [atoms cm -2 s -1 ]  70% transmission SIS – FRS  ε trans transmission.
Nuclear deformation in deep inelastic collisions of U + U.
Sep. 2003CNS Summer School Feb 分 => Talk なら 35 枚だが、 lecture だと少なめ? 50 分 => Talk なら 35 枚だが、 lecture だと少なめ?
Pygmy Dipole Resonance in 64Fe
POPULATION OF GROUND-STATE ROTATIONAL BANDS OF SUPERHEAVY NUCLEI PRODUCED IN COMPLETE FUSION REACTIONS A.S. Zubov, V.V. Sargsyan, G.G. Adamian, N.V.Antonenko.
Neutrons (Basic Concepts).  It is desirable to classify neutrons according to their kinetic energy into:
1 The results of the study of dp-elastic scattering at the energies from 500 to 1000 MeV/nucleon A.A Terekhin et al. Joint Institute for Nuclear Research,
Neutron enrichment of the neck-originated intermediate mass fragments in predictions of the QMD model I. Skwira-Chalot, T. Cap, K. Siwek-Wilczyńska, J.
Charge Equilibration Dynamics: The Dynamical Dipole Competition of Dissipative Reaction Mechanisms Neck Fragmentation M.Di Toro, PI32 Collab.Meeting, Pisa.
C. Oppedisano for the ALICE Collaboration. 5 Jun 2012 C. Oppedisano 2/10 Centrality in p-A interactions can be defined through the number of collisions.
Accelerator Physics, JU, First Semester, (Saed Dababneh). 1 Electron pick-up. ~1/E What about fission fragments????? Bragg curve stochastic energy.
Some aspects of reaction mechanism study in collisions induced by Radioactive Beams Alessia Di Pietro.
Quasifission reactions in heavy ion collisions at low energies A.K. Nasirov 1, 2 1 Joint Institute for Nuclear Research, Dubna, Russia 2 Institute.
NUCLEAR LEVEL DENSITIES NEAR Z=50 FROM NEUTRON EVAPORATION SPECTRA IN (p,n) REACTION B.V.Zhuravlev, A.A.Lychagin, N.N.Titarenko State Scientific Center.
RNB Cortina d’Ampezzo, July 3th – 7th 2006 Elisa Rapisarda Università degli studi di Catania E.Rapisarda for the Diproton collaboration 18 *
N/Z Dependence of Isotopic Yield Ratios as a Function of Fragment Kinetic Energy Carl Schreck Mentor: Sherry Yennello 8/5/2005 J. P. Bondorf et al. Nucl.
Hadronic interaction studies with the ARGO-YBJ experiment (5,800 m 2 ) 10 Pads (56 x 62 cm 2 ) for each RPC 8 Strips (6.5 x 62 cm 2 ) for each Pad ( 
NS08 MSU, June 3rd – 6th 2008 Elisa Rapisarda Università degli studi di Catania E.Rapisarda 18 2.
Protons Neutrons Nuclear structure at finite temperature probed by the Giant Dipole Resonance G. Benzoni, O. Wieland, A. Bracco, N. Blasi, F. Camera, F.
Reaction studies with low-energy weakly-bound beams Alessia Di Pietro INFN-Laboratori Nazionali del Sud NN 2015Alessia Di Pietro,INFN-LNS.
Fusion of light halo nuclei
Signals of bimodality in fragmentation induced by 3.65 A GeV 12C B.Grabez Institute of Physics Zemun.
Two-proton simultaneous emission from 29 S C.J. Lin 1, G.L. Zhang 1, F. Yang 1, H.Q. Zhang 1, Z.H. Liu 1, C.L. Zhang 1, P. Zhou 1, X.K. Wu 1, X.X. Xu 1,
A. Dokhane, PHYS487, KSU, 2008 Chapter1- Neutron Reactions 1 NEWS Lecture1: Chapter 0 is already on my Website.
Time dependent GCM+GOA method applied to the fission process ESNT janvier / 316 H. Goutte, J.-F. Berger, D. Gogny CEA/DAM Ile de France.
The experimental evidence of t+t configuration for 6 He School of Physics, Peking University G.L.Zhang Y.L.Ye.
Study of repulsive nature of optical potential for high energy 12 C+ 12 C elastic scattering (Effect of the tensor and three-body interactions) Gaolong.
Dynamical Model of Surrogate Reaction Y. Aritomo, S. Chiba, and K. Nishio Japan Atomic Energy Agency, Tokai, Japan 1. Introduction Surrogate reactions.
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.
Lecture 3 1.The potential energy surface of dinuclear system and formation of mass distribution of reaction products. 2.Partial cross sections. 3. Angular.
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
FAST IN-MEDIUM FRAGMENTATION OF PROJECTILE NUCLEI
Extracting β4 from sub-barrier backward quasielastic scattering
M. Sc Physics, 3rd Semester
Fusion-Incomplete Fusion Dissipative binary processes
Ternary Fission and Neck Fragmentation
Yuliya Aksyutina for the LAND-R3B collaboration Motivation
Peripheral collisions Hans-Jürgen Wollersheim
PHL424: Semi-classical reaction theory
Isospin Symmetry test on the semimagic 44Cr
Sensitivity of reaction dynamics by analysis of kinetic energy spectra of emitted light particles and formation of evaporation residue nuclei.
Nuclear Reactions --Part 2
Modification of Fragmentation Function in Strong Interacting Medium
PHL424: Semi-classical reaction theory
Duality in Nuclei: The EMC Effect
Probing correlations by use of two-nucleon removal
Presentation transcript:

Nonstatistical fluctuations for deep inelastic processes in 27 Al + 27 Al collision Introduction Experimental procedures Cross section excitation functions (EFs) 1. Statistical analysis (a) Energy autocorrelation function (EAF): experimental results and discussion (b) Angular analysis: experimental results and discussion 2. Deformation of the di-nuclear system (DNS) Conclusions

Introduction Ericson (Statistical) Fluctuations in the region   >> D (due to random interferences between resonances) (T. Ericson, Ann. Phys.,1963) - channel uncorrelated - Lorentzian pattern of the energy autocorrelation function: N eff - number of the independently microchannels contributing to the cross section  - correlation width of the fluctuations Types of structures (fluctuations) in the Efs: gross (  ~ sec), intermediate (nonstatisical) (  ~ sec), CN (statistical) (  > sec) ħ= Mev sec,    ~ MeV, hundreds of keV, keV – tens of keV for gross, intermediate, CN structures Fluctuation phenomenon unexpected for deep inelastic processes (DIP): amplitude of the fluctuations ~ 1/N eff, N eff very large for DIP However evidence of the fluctuations in EFs of the DIP of the 28 Si + 64 Ni system with nonstatistical features (A. De Rosa et al, Phys. Lett., 1985) : -  of hundreds of keV - channel correlated + non Lorentzian pattern of the energy autocorrelation function

12 C + 24 Mg 19 F + 89 Y 28 Si + 48 Ti 19 F + 63 Cu 28 Si + 28 Si 19 F + 51 V Models for nonstatistical fluctuations from elastic and inelastic scattering of heavy ion as Orbiting Cluster Model (OCM) (N. Cindro, 1980), Number of Open Channels (NOC) Model (Y. Abe, F. Haas, 1981) predict intermediate structures in light heavy ion systems where both partners are  - nuclei Models supposing angular momentum coherence Ericson's theory generalized to deep inelastic reaction (D. M. Brink, K.Dietrich, Z. Phys., 1987), Kun Model (S. Yu. Kun, Phys. Lett. B, 1991) + Partial Overlapping of Molecular Levels (  D) POMLM (G. Pappalardo et al, 1991) explain the persistence and the main features of the fluctuations in the EF of deep inelastic processes. Other studied systems: medium mass or light  - nuclei (A. Glaesner et al, Phys. Lett B, 1986) (T. Suomijavri et al, PRC, 1987) (A. De Rosa et al, PRC, 1988; F. Rizzo et al, Z. Phys. A, 1994) (G. Cardella et al, Z. Phys. A, 1990) (M. Papa et al, Z. Phys. A,1995) (Wang Qi et al, Phys. Lett. B, 1996) Systems studied by us light mass non-  : 19 F + 27 Al (I. Berceanu et al, Phys. Rev. C, 1998), 27 Al + 27 Al

  Integration window: TKEL = ( ) MeV TKEL = E cm – TKE Experimental procedures Incident energy range: E lab = MeV, Energy increment: 250 keV (125 keV in CMS) Targets: 27 Al of 39, 40  g/cm 2 (~ 75 keV), 197 Au of 92  g/cm 2, 12 C of 100  g/cm 2 Beam current measured with a tantalum plated Faraday cup provided with an electron suppressing guard ring Detection and identification of the reaction products: Ionization chambers (ICs) of DRACULA Device ICs center at  lab = 24 o ; 12 o ≤  lab ≤ 36 o ;  gr (132 MeV) = 15 o Carbon deposition on Al target = 6  g/cm 2 The effect on the yield of the Z ≠ 13 products < 1%  E/E = 2.5%;  =0.5  ;   Z=0.3  E lab = 128MeV 

Cross section excitation functions 1. Statistical analysis  N ev /N beam Large CCC  nonstatistical fluctuations Cross Correlation Coefficients (CCC)

 = (150 ± 75) keV, (M.Papa et al, Phys. Rev. C, 2000) Energy autocorrelation function (EAF)  = (128 ± 32) keV,  DNS =  (5.1±1.1) sec  19 F + 27 Al, 27 Al + 27 Al, 27 Al + 27 Al, 28 Si + 28 Si o 19 F + 63 Cu, 19 F + 51 V, 19 F + 89 Y, 28 Si + 48 Ti Points on figure (from the left to the right): Thin line on figure:  = (170 ± 65) keV,  DNS =  (3.9 ± 2.1) sec (D. Shapira et al, Phys Rev. C, 1974)

Angular analysis Average angular distribution Normalized Variance C(0) Relationship between V = (C(0)) 1/2 and the level density in the framework of POMLM:   - the angular momentum window,    /ħ  - the degree of the angular momentum coherence  s,  F - cross sections for slow and fast processes   eV  eV  ~    S /(  S +  F ) = 0.5,  = 2  /D ~ 16,  ~125 MeV -1  ang = sec,  cm < 50 o  ang = sec,  cm > 50 o  ang = sec, Z = 8 Z =   EAF more consistent with  ang for slower processes  EAF = (5.1 ± 1.1) sec

Deformation of the di-nuclear system  T - rotation period of DNS, n – number of DNS revolutions   ħl / J - angular velocity of the di-nucleus, J = J rel + J int, J rel =  r MeVsec -2 - the relative momentum of inertia J int = (2/5) r o 2 (A 3 5/3 + A 4 5/3 ) MeVsec -2 - the intrinsic momentum of inertia A 3, A 4 - the atomic masses of the fragments in final channel  The most probable total kinetic energy: l i = (l gr + l cr )/2 = ( )/2=45.8 ħ l st = l i (1- J int / J tot ) ħ Z = 12, = 41 MeV, l st = 32.5  DNS =  sec, T = sec Z = 8, = 33 MeV, l st = 29.6 to compare with  c =  eV  EAF =  eV  c = 2.0 MeV   F ~ 2.0 MeV to compare with For  DNS ≥ T secondary structures in the EAF of the symmetric systems with period (S. Yu. Kun, Z. Phys. A, 1993 ) :  c = 2nħ  r = 10.9 fm r = 10.0 fm

l cr for light heavy-ion systems has a large spreading: (27ħ – 42ħ) l cr = 35ħ, r = 10.3 (9.5) fm,   c = 1.4 (1.6) MeV  for O + Ar (Mg + Si) a lower value of l cr should be more appropriate to describe the long range oscillations from Z = 8 EAF, while they are quite well reproduced with l cr = 43.7ħ for the fragments with atomic number close to the projectile one J rel ( r) = 1.97 J rel ( R int ), for r ~ 10.9 fm Large deformation of the DNS: RLDM: in mass region “it should be possible to form super- deformed nuclei “ ( S. Cohen, F. Plasil, W. J. Swiatecki, 1974) E. g.: triaxial 54 Fe and 46 Ti CNs for l > 33.6ħ and 29ħ, respectively Comparison with results from the EAF analysis for other systems S. Yu. Kun: 19 F + 89 Y (Phys. Lett. B, 1991 ), 58 Ni + 46 Ti (Z. Phys. A, 1997) no deformation 12 C + 24 Mg (PRC, 1999), 24 Mg + 24 Mg, 28 Si + 28 Si (PRL, 1999) deformation  R int = r o (A 3 1/3 +A 4 1/3 ) - interaction radius for spherical nuclei For system 19 F + 27 Al we obtained r ~ 11 fm (1998)

Intensive experiments studing deformation in mass region Light charged particle spectra emitted by 55 Co, 56 Ni and 59 Cu CNs formed in the reactions 28 Si + 27 Al (D. K. Agnihotri et al, Phys. Lett., 1993 ), 28 Si + 28 Si (C. Bhattcharya et al, Phys. Rev. C, 2001) and 35 Cl + 24 Mg ( D. Mahoub et al, Phys. Rev. C, 2004) could be described by calculating the yrast line with an effective moment of inertia: J eff = J sphere (1 +   1 l 2 +  2 l 4 ),  1,  2 -  the deformability parameters  Experiments at IReS, Strasbourg 16 O + 28 Si: the   spectral shape at three incident energies indicate large deformation of the 44 Ti CN (axis ratio a/b ~ 2) (P. Papka et al, Acta Phys. Pol., 2003) 18 O + 28 Si: the shape of  -ray spectrum from the decay of GDR built in hot 46 Ti could be described supposing an elongated 3-axial equilibrium shape at l = 30 ħ (A. Maj et al, Nucl. Phys. A, 2004) 27 Al + 19 F:  -particle spectra also suggests very elongated shapes around this value of the angular momentum (M. Brekiesz et al, Acta Phys. Pol., 2005)    For systems with mass close to that of the 27 Al + 27 Al For systems with mass close to that of the 19 F + 27 Al J sphere  -  rigid body momentum of inertia J eff ~ 1.5 J sphere for  1,  2 from experiment

Conclusion s The correlation width extracted from the EF is equal to (128±32) keV to which corresponds a DNS lifetime of (5.1 ± 1.1) sec. This lifetime is in good agreement with the DNS lifetime extracted from the average angular distribution. From the analysis of the EAF structure at  > 0 a separation distance value of 10.0 – 10.9 fm has been obtained indicating a large deformation of the excited rotational states as in the case of the previously system 19 F + 27 Al studied by us. The low value of the  /D estimated in the POMLM framework is physically supported by the excitation of the deformed DNS levels in a region at ~ 27 MeV above yrast line. The experimental evidence from the present paper supports a reaction mechanism where special states of rotational (molecular) nature play the role of doorway configurations toward a regime characterized by stochastic exchange of nucleons between interacting nuclei as the main mechanism behind the dissipative phenomena in light heavy ion collisions. Large fluctuations have been evidenced in the EF for deep inelastic processes in the 27 Al+ 27 Al interaction on the incident energy interval ( ) MeV. The large channel cross correlation coefficients and non-Lorentzian pattern of the EAF show the nonstatistical origin of the fluctuations.

I. Berceanu 1, M. Duma 1, D. Moisa 1, M. Petrovici 1, A. Pop 1, V. Simion 1, A. Del Zoppo 2, G. d'Erasmo 3,4, G. Imme 5, G. Lanzano 5, A. Pagano 5, A. Pantaleo 3, and G. Raciti 2,6 1 National Institute of Physics and Nuclear Engineering, Bucharest, Romania 2 Istituto Nazionale di Fisica Nucleare, Laboratorio Nazionale del Sud, Italy 3 Istituto Nazionale di Fisica Nucleare, Sezione di Bari, Italy 4 Dipartimento di Fisica, Universita di Bari, Italy 5 Istituto Nazionale di Fisica Nucleare and Dipartimento di Fisica, Catania, Italy 6 Dipartimento di Fisica, Universita di Catania, Catania, Italy